# Small Data Solutions of the Vlasov-Poisson System and the Vector Field Method

## Abstract

The aim of this article is to demonstrate how the vector field method of Klainerman can be adapted to the study of transport equations. After an illustration of the method for the free transport operator, we apply the vector field method to the Vlasov-Poisson system in dimension 3 or greater. The main results are optimal decay estimates and the propagation of global bounds for commuted fields associated with the conservation laws of the free transport operators, under some smallness assumption. Similar decay estimates had been obtained previously by Hwang, Rendall and Velázquez using the method of characteristics, but the results presented here are the first to contain the global bounds for commuted fields and the optimal spatial decay estimates. In dimension 4 or greater, it suffices to use the standard vector fields commuting with the free transport operator while in dimension 3, the rate of decay is such that these vector fields would generate a logarithmic loss. Instead, we construct modified vector fields where the modification depends on the solution itself. The methods of this paper, being based on commutation vector fields and conservation laws, are applicable in principle to a wide range of systems, including the Einstein-Vlasov and the Vlasov-Nordström system.

## Introduction

A standard approach to the study of asymptotic stability of stationary solutions of non-linear evolution equations consists in an appropriate linearization of the system togetherFootnote 1 with

1. 1.

a robust method for proving decay of solutions to the linearized equations,

2. 2.

an appropriate set of estimates for the non-linear terms of the original system, using the linear decay estimates obtained previously.

For systems of non-linear wave equations such as the Einstein vacuum equations $$Ric(g)=0$$, several methods for proving decay of solutions to the linear wave equation $$\square \psi =0$$ where $$\displaystyle {\square =-\partial _t^2+\sum _{i=1}^n\partial _{x^i}^2}$$ is the wave operator of the flat Minkowski spaceFootnote 2 are a priori available. One of the classical methods to derive decay estimates is to use an explicit representation of the solutions, such as the Fourier representation, together with specific estimates for singular or oscillatory integrals. While this method provides very precise estimates on the solutions, it does not seem sufficiently robust to be applicable to quasilinear system of wave equations such as the Einstein equations, and the method of choiceFootnote 3 for proving decay in view of such applications is the commutation vector field method of Klainerman [12] and its extensions using multiplier vector fields, see for instance [5, 20, 21]. The method of Klainerman is based on

1. 1.

A coercive conservation law: the standard energy estimate in the case of the wave equation.

2. 2.

Commutation vector fields: these are typically associated with the symmetries of the equations. In the case of the wave equation, these are the Killing and conformal Killing fields of the Minkowski space.

3. 3.

Weighted vector field identities and weighted Sobolev inequalities: the usual vector fields $$\partial _t, \partial _{x^i}$$ are rewritten in terms of the commutation vector fields. The coefficients involved in these decompositions contain weights in t and |x| and the presence of these weights leads to weighted Sobolev inequalities, that is to say decay estimates.

The typical method used in the study of the Vlasov-Poisson and other systems of transport equations such as the Vlasov-Nordström system is the method of characteristics. This is an explicit representation of the solutions and thus, in our opinion, should be compared with the Fourier representation for solutions of the wave equation. What would then be the analogue of the vector field method for transport equations? The aim of this article is twofold. First, we will provide a vector field method for the free transport operator. In fact, in a joint work with J. Joudioux and D. Fajman, we have developed a vector field approach to decay of averages not only for the free (non-relativistic) transport operator but also for the massive and massless relativistic transport operators, see [7]. In this paper, we will give two different proofs of Klainerman-Sobolev inequalities. The easier proof will give us a decay estimate for velocity averages of sufficiently regular distribution functions, i.e. quantities such as $$\int _{v \in {\mathbb {R}}^n} f(t,x,v)dv$$. However, this proof fails in the case of velocity averages of absolute values of distribution functions, i.e. quantities such as $$\int _{v \in {\mathbb {R}}^n} |f|(t,x,v)dv$$, because higher derivatives of |f| will typically not lie in $$L^1$$ even if f is in some high regularity Sobolev space. On the other hand, the decay estimate obtained via the method of characteristics can be applied equally well to f and |f|. We shall therefore give a second proof of Klainerman-Sobolev inequalities for velocity averages which will be applicable to absolute values of regular distribution functions. The first approach, which is closer to the standard proof of the Klainerman-Sobolev inequality for wave equations, consists essentially of two steps, a weighted Sobolev type inequality for functions in $$L^1_x$$ and an application of this inequality to velocity averages, exploiting the commutation vector fields. The improvement in the second approach comes from mixing the two steps together.

In the second part of this paper, we will apply our method to the Vlasov-Poisson system in dimension $$n \ge 3$$

\begin{aligned}&\displaystyle \partial _t f + v.\nabla _x f + \mu \nabla _x \phi . \nabla _v f =0, \end{aligned}
(1)
\begin{aligned}&\displaystyle \Delta \phi = \rho (f), \end{aligned}
(2)
\begin{aligned}&\displaystyle f(t=0)=f_0. \end{aligned}
(3)

where $$\mu =\pm 1$$, $$\displaystyle {\Delta =-\sum _{i=1}^n \partial ^2_{x^i}}$$, $$f=f(t,x,v)$$ with $$t \in {\mathbb {R}}$$, $$x,v \in {\mathbb {R}}^n$$, $$f_0$$ is a sufficiently regular function of xv and $$\rho (f)$$ is given by

\begin{aligned} \rho (f)(t,x):= \int _{v \in {\mathbb {R}}^n} f(t,x,v) d^n v. \end{aligned}

Our main result can be summarized as follows (a more precise version is given in Section 4.2).

### Theorem 1.1

Let $$n \ge 3$$ and $$N \ge \frac{5n}{2}+2$$ if $$n \ge 4$$ and $$N \ge 14$$ if $$n=3$$. Let $$0< \delta < \frac{n-2}{n+2}$$. Then, there exists $$\epsilon _0 > 0$$ such that for all $$0 \le \epsilon \le \epsilon _0$$, if $$E_{N,\delta }[f_0] \le \epsilon$$, where $$E_{N,\delta }[f_0]$$ is a normFootnote 4 containing up to N derivatives of $$f_0$$, then the classical solution f(txv) of (1)–(3) exists globally in timeFootnote 5 and satisfies the estimates, $$\forall t \in {\mathbb {R}}$$ and $$\forall x \in {\mathbb {R}}^n$$,

1. 1.

Global bounds

\begin{aligned} \quad E_{N,\delta }[f](t) \le 2 \epsilon . \end{aligned}
(4)
2. 2.

Space and time pointwise decay of averages of $$\rho (f)$$

\begin{aligned} \text {for any multi-index }&\alpha \text { with } |\alpha | \le N-n,\\&|\rho ( Z^\alpha f)(t,x) | \le \frac{C_{N,n,\delta } \epsilon }{\left( 1+|t|+|x| \right) ^{n}}, \end{aligned}

where $$Z^\alpha$$ is a differential operator of order $$\alpha$$ obtained as a combination of $$|\alpha |$$ commuting vector fields and $$C_{N,n,\delta } > 0$$ is a constant depending only on $$N,n,\delta$$.

3. 3.

Improved decay estimates for derivatives of f

\begin{aligned} \text {for any multi-index }&\alpha \text { with } |\alpha | \le N-n,\\&|\rho ( \partial _{x}^\alpha f)(t,x) | \le \frac{C_{N,n,\delta } \epsilon }{\left( 1+|t|+|x| \right) ^{n+|\alpha |}}. \end{aligned}
4. 4.

Boundedness of the $$L^{1+\delta }$$ norms of $$\nabla ^2 \phi$$ and $$\nabla ^2 Z^\alpha \phi$$

\begin{aligned} \text {for any multi-index } \alpha \hbox { with } |\alpha | \le N, \quad ||\nabla ^2 Z^\alpha \phi (t) ||_{L^{1+\delta }({\mathbb {R}}^n)} \le C_{N,n,\delta } \epsilon . \end{aligned}
5. 5.

Space and time decay of the gradient of the potential and its derivatives

\begin{aligned} \text {for any multi-index } \alpha \text { with }&|\alpha | \le N-(3n/2+1), \\&| \nabla Z^\alpha \phi (t,x) | \le \frac{C_{N,n,\delta } \epsilon }{t^{(n-2)/2}\left( 1+|t|+|x| \right) ^{n/2}}, \end{aligned}

as well as the improved decay estimates

\begin{aligned} |\partial ^\alpha _x \nabla \phi (t,x) | \le \frac{C_{N,n,\delta } \epsilon }{t^{(n-2)/2}\left( 1+|t|+|x| \right) ^{n/2+|\alpha |}}. \end{aligned}

### Remark 1.1

Stronger bounds can be propagated by the equations provided the data enjoy additional integrability conditions. More precisely, the improved decay estimates for derivatives of $$\rho (f)$$ can be improved to

\begin{aligned} |\rho ( \partial _t^\tau \partial _{x}^\alpha f)(t,x) | \le \frac{C_N \epsilon }{\left( 1+|t|+|x| \right) ^{n+|\alpha |+\tau }} \end{aligned}

and the improved decay estimates for derivatives of the gradient of $$\phi$$ can be improved to

\begin{aligned} |\partial ^\tau _t\partial ^\alpha _x \nabla \phi (t,x) | \le \frac{C_N \epsilon }{t^{(n-2)/2}\left( 1+|t|+|x| \right) ^{n/2+|\alpha |+\tau }}, \end{aligned}

the point being that additional t derivatives now bring additional decay in t and |x|. These stronger estimates hold provided the initial data have stronger decay in xv than what is needed in the proof of Theorem 1.1. Similarly, one can propagates $$L^p$$ norms with $$p \ge 2$$ for $$\nabla \phi$$ and $$\nabla Z^\alpha \phi$$ provided additional v decay of the initial data is assumed.

### Remark 1.2

Similar time decay estimates have been obtained in [11] for derivatives of $$\rho (f)$$ and $$\phi$$ using the method of characteristics under different assumptions on the initial data. On the other hand, the optimal decay rates in space and the propagation of the global bounds (4) were, as far as we know, not known prior to our work.

### Remark 1.3

As is clear from the proof below and is typical of strategies based on commutation formulae and conservation laws, the method is very robust. In particular, we are not using the method of characteristics, nor the conservation of the total energy for the system (1)–(3). An illustration of this robustness will be given in [7] where we will apply a similar approach to the study of the Vlasov-Nordström system.

### Previous Work on the Vlasov-Poisson System and Discussion

There exists a large literature on the Vlasov-Poisson system. We refer to the introduction in [22] for a good introduction to the subject and only quote here the most important results from the point of view of this article. In the pioneered work [1], small data global existence in dimension 3 for the Vlasov-Poisson system was established together with optimal time decay rates for $$\rho (f)$$ and $$\nabla \phi$$ but no decay was obtained for their derivatives. The optimal time (but not spatial) decay rates for derivatives of $$\rho (f)$$ and $$\nabla \phi$$ has been only much later obtained in [11], covering at the same time all dimensions $$n \ge 3$$. Both these works use decay estimates obtained via the method of characteristics. In fact, in [1] and even more in [11], precise estimates on the deviation of the characteristics from the characteristics of the free transport operator are needed in order to obtain the desired decay estimates. Parallely to these works giving information on the asymptotics of small data solutions, let us mention that under fairly weak assumption on the initial data (in particular, no smallness assumption is needed), it is known that global existence holds in dimension 3 for the solutions of (1)–(3), see [18, 24]. The strongest results concerning the stability of non-trivial stationary solutions of (1)–(3) with $$\mu =-1$$ have been obtained in [15]. They are not based on decay estimates but on a variational characterisation of the stationary solutions. On the other hand, this type of method does not provide asymptotic stability of the solutions but orbital stability. It is likely that any result addressing the question of asymptotic stability will need to go back to an appropriate linearization of the equations combined with robust decay estimatesFootnote 6. We believe that, once again, the vector field method would be totally appropriate for the derivation of such decay estimates. Finally, let us mention the celebrated work [23] on Landau damping concerning the stability of stationary solutions to (1)-(3) with periodic initial data.

### Outline of the Paper

In Section 2, we introduce the vector fields commuting with the free transport operator and the notations that we will use throughout the paper. In Section 3, we present and prove decay estimates for velocity averages of solutions to the transport equation. In the following section, we present our results on the Vlasov-Poisson system. The following two sections are devoted to the proof of these results, first in dimension $$n \ge 4$$ and then in dimension 3 using modified vector fields. Finally, in the last section, we present some open problems related to the use of vector field techniques for kinetic transport equations.

## Preliminaries

Throughout this article, f will denote a sufficiently regular function of (txv) with $$t \in {\mathbb {R}}$$ and $$(x,v) \in {\mathbb {R}}^n \times {\mathbb {R}}^n$$. By sufficiently regular, we essentially mean that f is such that all the terms appearing in the equations make sense as distributions and that all the norms appearing in the estimates are finite. For simplicity, the reader might just assume that f is smooth with compact support in xv (but any sufficient fall-off will be enough).

We will denote by T the free transport operator i.e.

\begin{aligned} T(f):=\partial _tf + \sum _{i=1}^n v^i \partial _{x^i} f, \end{aligned}

where $$\partial _t f= \frac{\partial f}{\partial t}$$ and for all $$1\le i \le n$$, $$\partial _{x^i}f= \frac{\partial f}{\partial x^i}$$. Similarly, for any sufficiently regular scalar function $$\phi$$, $$T_\phi$$ will denote the perturbed transport operator

\begin{aligned} T_\phi (f):= T(f) + \mu \nabla _x \phi . \nabla _v f, \end{aligned}
(5)

where $$\mu =\pm 1$$, corresponding to an attractive or repulsive force. Since we are dealing only with small data solutions, the sign of $$\mu$$ will play no role in the rest of this article.

The notation $$A \lesssim B$$ will be used to specify that there exists a universal constant $$C>0$$ such that $$A \le CB$$, where typically C will depends only on the number of dimensions n and a few other fixed constants, such as the maximum number of commutations.

### Macroscopic and Microscopic Vector Fields

Consider first the following set of vector fields

• Translations in space and time   $$\partial _t$$, $$\partial _{x^i}$$,

• Uniform motion in one spatial directionFootnote 7    $$t\, \partial _{x^i}$$,

• Rotations   $$x^i \partial _{x^j}-x^j \partial _{x^i}$$,

• Scaling in space   $$\displaystyle {\sum _{i=1}^n x^i \partial _{x^i}}$$,

• Scaling in space and time   $$t \partial _t + \displaystyle {\sum _{i=1}^n x^i \partial _{x^i}}$$.

The above set of vector fields is associated with the Gallilean invariance of macroscopic fields and equations. We will denote by $$\Gamma$$ the set of all such vector fields

\begin{aligned} \Gamma =\left\{ \partial _t, \partial _{x^i}, t\, \partial _{x^i}, x^i \partial _{x^j}-x^j \partial _{x^i}, \sum _{i=1}^n x^i \partial _{x^i}, t \partial _t + \sum _{i=1}^n x^i \partial _{x^i}, \,\, 1\le i,j \le n\right\} . \end{aligned}

One easily check that while the translations commute with T, uniform motions, rotations or the scaling in space do not. The correct replacement for these vector fields is most easily explained using the language of differential geometry; the interested reader may consult [7, 28] for detailed constructions (in the case of the relativistic transport operator). We shall here only present the resulting objects which are the vector fields

• Uniform motions in one direction in microscopic form $$t \partial _{x^i} + \partial _{v^i}$$,

• Rotations in microscopic form $$x^i \partial _{x^j}-x^j \partial _{x^i}+ v^i \partial _{v^j}-v^j \partial _{v^i}$$,

• Scaling in space in microscopic form $$\displaystyle {\sum _{i=1}^n x^i \partial _{x^i}+v^i\partial _{v^i}}$$.

One can then easily check

### Lemma 2.1

(Commutation with the transport operator)

• If Z is any of the translations, microscopic uniform motions or microscopic rotations, then $$[T,Z]=0$$.

• If Z is the microscopic scaling in space, then $$[T,Z]=0$$.

• If Z is the scaling in space and time, then $$[T,Z]=T$$.

### Remark 2.1

From the two scaling commuting vector fields, it follows automatically that $$t\partial _t - \sum _{i=1}^n v^i\partial _{v^i}$$ also commutes with T in the sense that

\begin{aligned}{}[ T, t\partial _t - \sum _{i=1}^n v^i\partial _{v^i} ]=T. \end{aligned}

This vector field will be used to obtain improved decay for t derivatives of velocity averages.

To ease the notation, we will denote by $$\Omega _{ij}^{x}:=x^i \partial _{x^j}-x^j \partial _{x^i}$$ the rotation vector fields in x and by $$\Omega _{ij}^{v}:=v^i \partial _{v^j}-v^j \partial _{v^i}$$ the rotation vector fields in v. The full microscopic rotation vector fields are thus of the form $$\Omega _{ij}^{x}+\Omega _{ij}^{v}$$. Similarly, we will denote by $$S^{x}+S^{v}:=\displaystyle {\sum _{i=1}^n x^i \partial _{x^i}+v^i\partial _{v^i}}$$ the scaling in space in microscopic form, with $$S^{x}=\displaystyle {\sum _{i=1}^n x^i \partial _{x^i}}$$ and $$S^{v}=\displaystyle {\sum _{i=1}^n v^i\partial _{v^i}}$$.

Let now $$\gamma$$ be the set of all the above microscopic vector fields including the translations and the space and time scaling i.e.

\begin{aligned} \gamma =\left\{ \partial _t, \partial _{x^i}, t\partial _{x^i} + \partial _{v^i}, \Omega _{ij}^{x}+\Omega _{ij}^{v}, S^{x}+S^{v} , t \partial _t + \sum _{i=1}^n x^i \partial _{x^i}, 1\le i,j \le n \right\} . \end{aligned}

### Multi-Index Notations

Let $$Z^i,i=1,\ldots ,2n+3+n(n-1)/2$$ be an ordering of $$\Gamma$$. For any multi-index $$\alpha$$, we will denote by $$Z^\alpha$$ the differential operator of order $$|\alpha |$$ given by the composition $$Z^{\alpha _1} Z^{\alpha _2}\ldots$$.

In view of the above discussion, to any vector field of $$\Gamma$$, we can associate a unique vector field of $$\gamma$$. More precisely,

\begin{aligned} \partial _t\rightarrow & {} \partial _t, \\ \partial _{x^i}\rightarrow & {} \partial _{x^i},\\ t \partial _{x^i}\rightarrow & {} t \partial _{x^i} + \partial _{v^i}, \\ \Omega _{ij}^x\rightarrow & {} \Omega _{ij}^x+\Omega _{ij}^v, \\ S^x\rightarrow & {} S^x+ S^v, \\ t\partial _t + \sum _{i=1}^n x^i \partial _{x^i}\rightarrow & {} t\partial _t + \sum _{i=1}^n x^i \partial _{x^i}. \end{aligned}

Thus, to any ordering of $$\Gamma$$ we can associate an ordering of $$\gamma$$. We will by a small abuse of notation, denote again by $$Z^i$$ the elements of such an ordering since it will be clear that, if $$Z^i$$ is applied to a macroscopic quantity, such as a velocity average, then $$Z^i \in \Gamma$$ and if $$Z^i$$ is applied to a microscopic quantity, i.e. any function depending on (xv) (and possibly t), then $$Z^i \in \gamma$$. Similarly, for any multi-index $$\alpha$$, we will also denote by $$Z^\alpha$$ the differential operator of order $$|\alpha |$$ given by the composition $$Z^{\alpha _1} Z^{\alpha _2}\ldots$$ obtained from the vector fields of $$\gamma$$.

For some of the estimates below, it will be sufficient to only consider a subset of all the vector fields of $$\Gamma$$ and $$\gamma$$. Let us thus denote by $$\Gamma _s$$ the set of all the macroscopic vector fields apart from $$\partial _t$$ and $$t \partial _t + \displaystyle {\sum _{i=1}^n x^i \partial _{x^i}}$$, which are the only vector fields containing time derivatives and by $$\gamma _s$$ the corresponding set of microscopic vector fields, i.e.

\begin{aligned} \Gamma _s= & {} \left\{ \partial _{x^i}, t\, \partial _{x^i}, x^i \partial _{x^j}-x^j \partial _{x^i}, \sum _{i=1}^n x^i \partial _{x^i}, \, 1\le i,j \le n\right\} ,\\ \gamma _s= & {} \left\{ \partial _{x^i}, t\partial _{x^i} + \partial _{v^i}, \Omega _{ij}^{x}+\Omega _{ij}^{v}, S^{x}+S^{v} , \, 1\le i,j \le n \right\} . \end{aligned}

The notation $$Z^\alpha \in \Gamma ^{|\alpha |}_s$$ (respectively $$Z^\alpha \in \gamma ^{|\alpha |}_s$$) will be used to denote a generic differential operator of order $$|\alpha |$$ obtained as a composition of $$|\alpha |$$ vector fields in $$\Gamma _s$$ (respectively in $$\gamma _s$$). The standard notation $$\partial _x^\alpha$$ will also be used to denote a differential operator of order $$|\alpha |$$ obtained as a composition of $$|\alpha |$$ translations among the $$\partial _{x^i}$$ vector fields.

The following lemmas can easily be checked.

### Lemma 2.2

(Commutation within $$\Gamma$$) For any $$Z^\alpha \in \gamma ^{|\alpha |}$$, $$Z^{\alpha '} \in \gamma ^{|\alpha '|}$$ , where $$\alpha , \alpha '$$ are multi-indices, we have

\begin{aligned}{}[Z^\alpha , Z^{\alpha '}]=\sum _{|\beta |\le |\alpha |+|\alpha '|-1} c_\beta ^{\alpha ,\alpha '} Z^\beta , \end{aligned}

for some constant coefficients $$c_\beta ^{\alpha , \alpha '}$$. Moreover, if $$Z^\alpha , Z^{\alpha '} \in \gamma _s$$, then all the $$Z^\beta$$ of the right-hand side belongs to $$\gamma _s$$.

### Lemma 2.3

(Commutation of $$Z^\alpha$$ and weightsFootnote 8 in v)

Let $$q>0$$. For any sufficiently regular function f of (txv) and for any $$Z^\alpha \in \gamma ^{|\alpha |}$$ where $$\alpha$$ is a multi-index, we have

\begin{aligned} \left| Z^\alpha \left[ (1+v^2)^{q/2} f\right] \right| \lesssim (1+v^2)^{q/2} \sum _{|\beta | \le |\alpha |} \left| Z^\beta (f) \right| . \end{aligned}

Moreover, if $$Z^\alpha \in \gamma _s^{|\alpha |}$$ then all the $$Z^\beta$$ belong to $$\gamma _s^{|\beta |}$$ in the above inequality.

### Velocity Averages and Commutators

For any integrable function f of $$v \in {\mathbb {R}}^n$$, we will denote by $$\rho (f)$$ the quantity

\begin{aligned} \rho (f):= \int _{v \in {\mathbb {R}}^n} f d^nv \end{aligned}

We have the following lemma.

### Lemma 2.4

For any sufficiently regular function f of (xv) we have

• for all $$1 \le i \le n$$,

\begin{aligned} \partial _{x^i} \rho (f)= \rho ( \partial _{x^i} f), \end{aligned}
• for all $$t \in {\mathbb {R}}$$ and all $$1 \le i \le n$$,

\begin{aligned} t \partial _{x^i}\rho (f)=\rho \left( \left( t \partial _{x^i}+ \partial _{v^i} \right) f \right) , \end{aligned}
• for all $$1 \le i, j \le n,$$

\begin{aligned} \Omega _{ij}^{x} \rho (f)= \rho \left( \left( \Omega _{ij}^{x}+\Omega _{ij}^{v} \right) (f) \right) , \end{aligned}
• for all $$t \in {\mathbb {R}}$$ and $$x \in {\mathbb {R}}^n$$,

\begin{aligned} \left( t \partial _t +\sum _{i=1}^n x^i \partial _{x^i}\right) \rho (f)= \rho \left( \left( t \partial _t +\sum _{i=1}^n x^i \partial _{x^i}\right) (f) \right) , \end{aligned}
• and finally

\begin{aligned} S^{x}\rho (f)=\rho \left( \left( S^{x}+S^{v} \right) (f) \right) +n\rho (f), \end{aligned}

where $$S^x$$ and $$S^x+S^v$$ are the spatial scaling vector fields in macroscopic and microscopic forms.

### Proof

The proof is straightforward and consist in identifying total derivatives in v. For instance, we have

\begin{aligned} \rho \left( S^{v} \right) (f)=\int _{v \in {\mathbb {R}}^n} \left( \sum _{i=1}^n v^i \partial _{v^i} f\right) d^nv=\int _{v \in {\mathbb {R}}^n} -n f d^n v, \end{aligned}

where we have integrated by parts in each of the $$v^i$$. Similarly, in the case of rotations, it suffices to note that for any $$1 \le i, j \le n$$, $$\Omega ^v_{ij}$$ is an angular derivative in v and therefore, $$\int _{v \in {\mathbb {R}}^n} \Omega _{ij}^v(f)d^nv=0.$$ $$\square$$

In the remainder of this paper, we shall write the preceding lemma as

\begin{aligned} Z\rho (f)=\rho (Z(f))+c_Z \rho (f), \end{aligned}

where we are using, by a small abuse of notation, the letter Z to denote a generic macroscopic vector field and its corresponding microscopic version and where $$c_Z=0$$ unless Z is the spatial scaling vector field, in which case $$c_Z=n$$.

### Vector Field Identities

The following well-known identity will be used later

### Lemma 2.5

For any $$1\le j \le n$$, we have

\begin{aligned} |x|^2 \partial _{x^j} = \sum _{i=1}^n x^i \Omega _{ij}^{x}+ x^j S^{x}, \end{aligned}
(6)

and thus, at any $$x \ne 0$$,

\begin{aligned} |x|\partial _{x^j}=\sum _{i=1}^n \frac{x^i}{|x|} \Omega _{ij}^{x}+\frac{x^j}{|x|}S^{x}, \end{aligned}

where the coefficients $$\frac{x^i}{|x|}$$ are all homogeneous of degree 0 and therefore uniformly bounded.

The following higher order version will be used often in the derivation of the Klainerman-Sobolev inequalities of the next section.

### Lemma 2.6

For any multi-index $$\alpha$$,

\begin{aligned} (t+|x|)^\alpha \partial _x^\alpha = \sum _{|\beta | \le |\alpha |, Z^\beta \in \Gamma ^{|\beta |}_s} C_\beta Z^\beta , \end{aligned}

where the coefficients $$C_\beta$$ are all uniformly bounded.

### Proof

The lemma is a consequence of the previous decomposition, the fact $$t \partial _{x^i}$$ is part of our algebra of commuted vector fields and that $$\left[ \partial _{x^i},t+|x| \right]$$ is homogeneous of degree 0. $$\square$$

### The Commuted Equations

We now turn to the study of the transport operator $$T_\phi$$ defined by (5). Many of the estimates below are only valid provided $$\phi$$ has sufficient regularity. In the applications to the Vlasov-Poisson system of this article, we will eventually control the regularity of $$\phi$$ via a bootstrap argument. For all the estimates below, we therefore assume that $$\phi$$ is a sufficiently regularFootnote 9 function of (tx) defined on $$[0,T] \times {\mathbb {R}}^n_x$$, for some $$T > 0$$, which decays sufficiently fast as $$|x| \rightarrow +\infty$$.

The following lemma can then easily be checked.

### Lemma 2.7

Let f be a sufficiently regular function of (t,x,v) and let $$\alpha$$ be a multi-index. Then, there exists constant coefficients $$C^\alpha _{\beta \gamma }$$ such that,

\begin{aligned}{}[T_\phi ,Z^\alpha ] f = \sum _{|\beta | \le |\alpha |-1,} \sum _{|\gamma |+|\beta | \le |\alpha |} C^\alpha _{\beta \gamma }\nabla _x Z^\gamma \phi . \nabla _v Z^\beta f. \end{aligned}

Moreover if $$Z^\alpha \in \Gamma _s^{|\alpha |}$$, then $$Z^\gamma \in \Gamma _s^{|\gamma |}$$ and $$Z^\beta \in \gamma _s^{|\beta |}$$ in the above decomposition.

Similarly one has

### Lemma 2.8

Let f be a sufficiently regular function of (txv) and let $$\psi$$ be the solution to the Poisson equation $$\Delta \psi = \rho (f)$$. Then, for any multi-index $$\alpha$$, $$Z^\alpha \psi$$ is solution to an equation of the form

\begin{aligned} \Delta Z^\alpha \psi = \sum _{|\beta | \le |\alpha |} C_{\beta }^\alpha Z^\beta \rho (f), \end{aligned}
(7)

where $$C_{\beta }^\alpha$$ are constants.

### Proof

The lemma is an easy consequence of the fact that all macroscopic vector fields apart from the two scalings commute with $$\Delta$$ while for the spatial scaling $$S^{x}$$ and the space-time scaling $$t\partial _t+ S^{x}$$ we have $$[\Delta , S^{x}]=2 \Delta$$ and $$[\Delta , t\partial _t+ S^{x}]=2 \Delta$$$$\square$$

### Conservation Laws

We shall use the following (approximate) conservation laws.

### Lemma 2.9

For any sufficiently regular function f of (txv), we have, for all $$t \in [0,T]$$,

\begin{aligned} || f(t) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)} \le || f(0) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}+\int _0^t || T_\phi (f)(s) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}ds. \end{aligned}

Similarly, we have for all $$p \ge 1$$, for all $$t \in [0,T]$$,

\begin{aligned} || f(t) ||^p_{L^p( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}\le || f(0) ||^p_{L^p( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}+p \int _0^t || f^{p-1} T_\phi (f)(s) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}ds, \end{aligned}

and for all $$q\ge 1$$,

\begin{aligned} ||(1+v^2)^{q/2} f^p(t) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}\lesssim & {} ||(1+v^2)^{q/2} f^p(0) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)} \nonumber \\&\hbox {}+\int _0^t || (1+v^2)^{(q-1)/2} f^{p-1} T_\phi (f)(s) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )} ds \nonumber \\&\hbox {}+\int _0^t || f^{p} (1+v^2)^{(q-1)/2} \partial _x \phi (s) ||_{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}ds .\nonumber \\ \end{aligned}
(8)

Note in particular that the conclusions of the lemma hold true when $$T_\phi =T$$ (i.e. when $$\partial _x \phi =0$$).

### Proof

These are classical estimates so we only sketch their proofs.

One has (in the sense of distribution),

\begin{aligned} T_\phi \left[ (1+v^2)^{q/2} |f|^p \right] \lesssim (1+v^2)^{q/2} |f|^{p-1} |T_\phi (f)|+ (1+v^2)^{(q-1)/2}|\partial _x \phi | |f|^p. \end{aligned}

Using a standard procedureFootnote 10, one can regularize the previous inequality. We shall therefore neglect regularity issues here. Integrating the previous line in (txv) leads to

\begin{aligned}&\int _0^t \int _x \int _v T_\phi \left[ (1+v^2)^{q/2} |f|^p \right] dv dx ds \lesssim \nonumber \\&\quad \quad \, \int _0^t \int _x \int _v \left[ (1+v^2)^{q/2} |f|^{p-1} |T_\phi (f)|+ (1+v^2)^{(q-1)/2}|\partial _x \phi | |f|^p \right] dv dx ds.\nonumber \\ \end{aligned}
(9)

On the other-hand, remembering that $$T_\phi =\partial _t\,+\,\sum _{i=1}^n v^i \partial _x^i\,+\, \mu \nabla _x \phi . \nabla _v$$ and integrating by parts in x and v, we obtain

\begin{aligned} \int _0^t \int _x \int _v T_\phi \left[ (1+v^2)^{q/2} |f|^p\right] dv dx ds= & {} ||(1+v^2)^{q/2} f^p(t)||_{L^1({\mathbb {R}}_x^n \times {\mathbb {R}}_v^n)}\\&\hbox {}-||(1+v^2)^{q/2} f^p(0)||_{L^1({\mathbb {R}}_x^n \times {\mathbb {R}}_v^n)}, \end{aligned}

which combined with (9) leads to the desired estimate (8). $$\square$$

## Decay of Velocity Averages for the Free Transport Operator via the Vector Field Method

Since the main purpose of this article is to illustrate how the vector field method can lead to robust decay estimates for velocity averages, let us for the sake of comparison recall the Bardos-Degond decay estimate and its proof.

### Proposition 3.1

([1]) Let f be a sufficiently regular solution of $$T(f)=0$$. Then, we have the estimate, for all $$t > 0$$ and all $$x \in {\mathbb {R}}^n$$,

\begin{aligned} |\rho (f)|(t,x) \le \frac{1}{t^n} \int _{x \in {\mathbb {R}}^n} \sup _{v \in {\mathbb {R}}^n} |f(0,x,v)| d^n x. \end{aligned}
(10)

### Proof

The proof of this classical estimate is based on the method of characteristics. More precisely, if f is a regular solution to $$T(f)=0$$, then it follows that

\begin{aligned} f(t,x,v)=f(0,x-vt,v), \end{aligned}

for all $$t \in {\mathbb {R}}$$, $$x,v \in {\mathbb {R}}^n$$.

We then have

\begin{aligned} |\rho (f)|(t,x)= & {} \left| \int _{v \in {\mathbb {R}}^n} f(t,x,v) d^n v \right| \\= & {} \left| \int _{v \in {\mathbb {R}}^n} f(0,x-vt,v) d^n v \right| \\\le & {} \int _{v \in {\mathbb {R}}^n} \sup _{w \in {\mathbb {R}}^n} |f(0,x-vt,w)| d^n v. \end{aligned}

Applying now the change of coordinates $$y=vt$$ for $$t> 0$$ leads to

\begin{aligned} |\rho (f)|(t,x)\le & {} \frac{1}{t^n} \int _{y \in {\mathbb {R}}^n} \sup _{w \in {\mathbb {R}}^n} |f(0,x-y,w)| d^n y=\frac{1}{t^n} \int _{x \in {\mathbb {R}}^n} \sup _{v \in {\mathbb {R}}^n} |f(0,x,v)| d^n x . \end{aligned}

$$\square$$

In the above proof, the two key ingredients are

• the explicit representation obtained via the method of characteristics,

• the change of variables $$y=vt$$.

Note that in the presence of a perturbation of the free transport operator, to exploit a similar change of variables would require estimates on the Jacobian associated with the differential of the characteristic flow, see [1, 11].

Let us now show how the vector field method can be used as an alternative to obtain similar decay estimates. As explained in the introduction, we will give two different proofs.

The first proof will give us decay estimates for quantities of the form $$\int _{v \in {\mathbb {R}}^n} f dv$$. The starting point of this approach is the following Klainerman-Sobolev inequality using $$L^1({\mathbb {R}}^n)$$ norms of commuted fields.

### Lemma 3.1

[$$L^1$$ Klainerman-Sobolev inequality] For any sufficiently regular function $$\psi$$ defined on $${\mathbb {R}}^n_x$$, we have

\begin{aligned} |\psi |(x) \lesssim \frac{1}{\left( 1+t+|x| \right) ^n} \sum _{|\alpha | \le n, Z^\alpha \in \Gamma _s} || Z^\alpha (\psi ) ||_{L^1( {\mathbb {R}}^n_x)}. \end{aligned}

### Proof

This is relatively standard material and we adapt here the presentation given in [30] Chap.2 to our setting.

Fix $$(t,x) \in {\mathbb {R}}_t \times {\mathbb {R}}_x^n$$ and let $$\widetilde{\psi }$$ be the function

\begin{aligned} \widetilde{\psi }:\, {\mathbb {R}}^n\rightarrow & {} {\mathbb {R}} \end{aligned}
(11)
\begin{aligned} y\rightarrow & {} \widetilde{\psi }(y):=\psi (x+(t+|x|)y). \end{aligned}
(12)

Applying a standardFootnote 11 Sobolev inequality, we have

\begin{aligned} |\psi (t,x)| = |\widetilde{\psi }(0) | \lesssim \sum _{|\alpha | \le n} ||\partial _y^\alpha \widetilde{\psi } ||_{L^1(B_n(0,1/2))}, \end{aligned}
(13)

where $$B_n(0,1/2)$$ denote the ball in $${\mathbb {R}}^n_y$$ of radius 1 / 2. On the other hand, we have $$\partial _{y^i}\widetilde{\psi }(y)= (t+|x|) \partial _{x^i} \psi (x+(t+|x|)y)$$ and thus, for $$y \in B_n(0,1/2)$$,

\begin{aligned} |\partial _y^\alpha \widetilde{\psi }(y)|\lesssim & {} \sum _{|\beta | \le |\alpha |} (t+|x|)^\beta \left| \partial _x^\beta \psi \left( x+(t+|x|)y\right) \right| , \\\lesssim & {} \sum _{|\beta | \le |\alpha |} (t+|x+(t+|x|)y|)^\beta \left| \partial _x^\beta \psi \left( x+(t+|x|)y\right) \right| ,\\\lesssim & {} \sum _{|\beta | \le |\alpha |, Z^\beta \in \Gamma _s} \left| Z^\beta \psi \left( x+(t+|x|)y\right) \right| , \end{aligned}

where we have used Lemma 2.6 in the last step and the fact that $$t+|x|$$ and $$t+\left| x+(t+|x|)y\right|$$ are comparable for $$y \in B_n(0,1/2)$$. Inserting the last line in the Sobolev inequality (13) and applying the change of variables $$z=(t+|x|)y$$ conclude the proof of the lemma. $$\square$$

Using Lemma 2.4, we now note that for any vector field Z and any sufficiently regular function f of xv, we have

\begin{aligned} || Z (\rho (f)) ||_{L^1({\mathbb {R}}^n_x)} = || \rho (Z(f))+c_Z\rho (f) ||_{L^1({\mathbb {R}}^n_x)} \end{aligned}

and thus,

\begin{aligned} || Z (\rho (f)) ||_{L^1({\mathbb {R}}^n_x)} \lesssim || Z(f) ||_{L^1\left( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v\right) }+|| \rho (f)||_{L^1\left( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v\right) }. \end{aligned}

Combined with the previous Klainerman-Sobolev inequality, we obtain

### Proposition 3.2

(Global Klainerman-Sobolev inequality for velocity averages)

For any sufficiently regular function f defined on $${\mathbb {R}}^n_x \times {\mathbb {R}}^n_v$$, we have, for all $$t > 0$$ and all $$x \in {\mathbb {R}}^n$$,

\begin{aligned} |\rho (f)|(x) \lesssim \frac{1}{\left( 1+t+|x| \right) ^n} \sum _{|\alpha | \le n, Z^\alpha \in \gamma _s^{|\alpha |}} || Z^\alpha f ||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}. \end{aligned}
(14)

Note that the above inequality cannot be applied to |f| even is f is say a smooth, compactly supported function. Indeed, if |f| is say in $$W^{n,p}$$, then |f| is in $$W^{1,p}$$ but, unless f has some extra special properties, $$|f| \notin W^{n,p}$$ when $$n \ge 2$$. On the other hand, (10) clearly holds both for f and for |f|.

Two distinct steps lead to the proof of (14), the $$L^1$$ Klainerman-Sobolev inequality of Lemma 3.1 and the special commutation properties of the velocity averaging operator as described in Lemma 2.4. To improve upon (14), the strategy is to try to use at the same time arguments similar to those of Lemma 3.1 and Lemma 2.4, instead of applying them one after the other. This will lead to us to the following improvement.

### Proposition 3.3

(Global Klainerman-Sobolev inequality for velocity averages of absolute values) For any sufficiently regular function f defined on $${\mathbb {R}}^n_x \times {\mathbb {R}}^n_v$$, we have, for all $$t > 0$$ and all $$x \in {\mathbb {R}}^n$$,

\begin{aligned} |\rho (|f|)|(x) \lesssim \frac{1}{\left( 1+t+|x| \right) ^n} \sum _{|\alpha | \le n, Z^\alpha \in \gamma _s^{|\alpha |}} || Z^\alpha f ||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}. \end{aligned}
(15)

### Proof

Let us assume that f is smooth and compactly supported for simplicity.

Define $$\widetilde{\psi }$$ similarly to (11 12) as

\begin{aligned}&\displaystyle \widetilde{\psi }:\, B_n(0,1/2) \rightarrow {\mathbb {R}} \\&\displaystyle y \rightarrow \widetilde{\psi }(y):=\int _{v \in {\mathbb {R}}^n}|f|(x+(t+|x|)y,v)d^n v. \end{aligned}

Next, recall that for any $$\psi \in W^{1,1}$$, $$|\psi | \in W^{1,1}$$ and $$\partial |\psi |= \frac{\psi }{|\psi |} \partial \psi$$ (in the sense of distribution, see for instance [16], Chap 6.17) so that in particular $$\left| \partial |\psi | \right| \le |\partial \psi |$$. Let us write $$y=(y_1,\ldots ,y_n)$$ and let $$\delta = \frac{1}{4n}$$. Using a 1 dimensional Sobolev inequality, we have

\begin{aligned} |\widetilde{\psi }(0)|\lesssim \int _{|y_1| \le \delta ^{1/2}}\left( \left| \partial _{y_1}\widetilde{\psi }(y_1,0,\ldots ,0)\right| + \left| \widetilde{\psi }(y_1,0,\ldots ,0)\right| \right) dy_1. \end{aligned}
(16)

Now,

\begin{aligned} \partial _{y_1}\widetilde{\psi }(y_1,0,\ldots ,0)= & {} \int _{v \in {\mathbb {R}}^n} (t+|x|)\partial _{x_1}|f|\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) d^n v, \nonumber \\= & {} \int _{v \in {\mathbb {R}}^n} t\partial _{x_1}|f|\left( t,x+(t+|x|)(y_1,0,\ldots ,0)\right) d^n v \nonumber \\&\hbox {}+\int _{v \in {\mathbb {R}}^n} |x|\partial _{x_1}|f|\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) d^n v. \end{aligned}
(17)

As before, we can introduce total derivatives in v. For instance,

\begin{aligned}&\int _{v \in {\mathbb {R}}^n} t\partial _{x_1}|f|\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) d^n v\\&\quad = \int _{v \in {\mathbb {R}}^n}\left( t\partial _{x_1}+\partial _{v_1} \right) |f|\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) d^n v, \\&\quad \le \int _{v \in {\mathbb {R}}^n}\left| \left( t\partial _{x_1}+\partial _{v_1} \right) f\left( t,x+(t+|x|)(y_1',0,\ldots ,0)\right) \right| d^n v, \end{aligned}

and, using that $$(y_1,0,\ldots ,0) \in B_n(0,1/2)$$ if $$|y_1| \le \delta ^{1/2}$$, a similar argument can be used to handle the second term on the right-hand side of (17). This gives us

\begin{aligned} \left| \partial _{y_1}\widetilde{\psi }(y_1,0,\ldots ,0) \right|\le & {} \sum _{Z_s \in \gamma _s} \int _{v \in {\mathbb {R}}^n}\left| Z f\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) \right| d^n v. \end{aligned}

Combined with (16), we have obtained that

\begin{aligned} |\widetilde{\psi }(0)|\lesssim & {} \sum _{Z_s \in \gamma _s}\int _{|y_1| \le \delta ^{1/2}} \int _{v \in {\mathbb {R}}^n}\left| Z f\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) \right| d^n v dy_1\\&\hbox {}+ \int _{|y_1| \le \delta ^{1/2}} \int _{v \in {\mathbb {R}}^n}\left| f\left( x+(t+|x|)(y_1,0,\ldots ,0)\right) \right| d^n v dy_1 . \end{aligned}

We now repeat the same argument varying the variable $$y_2$$.

\begin{aligned} |\widetilde{\psi }(0)|\lesssim & {} \int _{|y_1| \le \delta ^{1/2}}\int _{|y_2| \le \delta ^{1/2}}\sum \limits _{\mathop {|\alpha |\le 2,}\limits _{Z^{\alpha } \in \gamma ^{|\alpha |}_s}} \\&\quad \times \,\int _{v \in {\mathbb {R}}^n}\left| Z^\alpha f\left( x+(t+|x|)(y_1,y_2,0,\ldots ,0)\right) \right| d^n v dy_1 dy_2. \end{aligned}

Iterating again this argument until all variables $$y_i$$ appears in the integral of the right-hand side, we obtain

\begin{aligned} |\widetilde{\psi }(0)| \lesssim \int _{y \in B_n(0,1/2)} \sum \limits _{\mathop { |\alpha |\le n,}\limits _{Z^{\alpha } \in \gamma ^{|\alpha |}_s}} \int _{v \in {\mathbb {R}}^n}\left| Z^\alpha f\left( x+(t+|x|)y\right) \right| d^n v dy, \end{aligned}

and the conclusion of the proof follows as in the proof of Lemma 3.1 by the change of variable $$z=(t+|x|)y$$$$\square$$

We now recall that if f is a solution to $$T(f)=0$$, then, in view of the commutation properties of Lemma 2.1 and standard properties of differentiation of the absolute value, so are |f| and the commuted fields $$|Z^\alpha f|$$. Thus, from Lemma 2.9, all the norms on the right-hand side of (15) are preserved by the flow and we have obtained the decay estimate

### Proposition 3.4

(Decay estimates for velocity averages) For any sufficiently regular solution f to $$T(f)=0$$, we have, for all $$t > 0$$ and all $$x \in {\mathbb {R}}^n$$,

\begin{aligned} |\rho (|f|)|(t,x) \lesssim \frac{1}{\left( 1+t+|x| \right) ^n} \sum _{|\alpha | \le n, Z^\alpha \in \gamma ^{|\alpha |}_s} || Z^\alpha f(t=0) ||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}. \end{aligned}
(18)

### Remark 3.1

If we restrict the set of vector fields only to the uniform motions $$t \partial _{x^i} + \partial _{v^i}$$, then we still obtain the time decay estimate,

\begin{aligned} |\rho (|f|)|(t,x) \lesssim \frac{1}{t^n} \sum \limits _{\mathop {|\alpha | \le n,}\limits {Z^{\alpha _i}=t \partial _{x^j} + \partial _{v^j}}} ||Z^\alpha f(t=0)||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}. \end{aligned}
(19)

Now, note that the vector fields of the form $$t \partial _{x^j} + \partial _{v^j}$$ degenerate to $$\partial _{v^j}$$ when evaluated at $$t=0$$. Since from the Sobolev inequality, we have that

\begin{aligned} || f(x,.) ||_{L^\infty ({\mathbb {R}}^n_v)} \lesssim \sum _{|\alpha | \le n} || \partial _{v}^\alpha f(x,.) ||_{L^1({\mathbb {R}}_v)}, \end{aligned}

it follows that (19) is strictly weaker than the inequality (10). In some sense, the fact that our method gives us a slightly worse estimate reflects its robustness and thus its appropriateness to deal with non-linear problems.

### Remark 3.2

Estimates similar to (18) hold for the relativistic transport operator $$T_{m}=\sqrt{m^2+|v|^2} \partial _t + \sum _{i=1}^n v^i \partial _{x^i}$$, where $$m=0$$ for massless particlesFootnote 12 and $$m>0$$ for massive particles. These estimates are presented in [7] together with non-linear applications to the Vlasov-Nordström system. Interestingly, in the case of the relativistic transport operator, the estimates obtained have additional benefits. Decay estimates for relativistic operators in the style of the Bardos-Degond estimate (10) typically require the extra assumptions of compact support in v of the solution, while for the estimates obtained via the vector field method, only the finiteness of the $$L^1_{x,v}$$ norms of the commuted fields are required. See [7].

As is classical, derivatives enjoy better decay properties as followsFootnote 13

### Proposition 3.5

(Improved decay estimates for derivatives) For any sufficiently regular function f defined on $${\mathbb {R}}^n_x \times {\mathbb {R}}^n_v$$, we have, for all $$x \in {\mathbb {R}}^n$$ and all multi-index $$\alpha$$

\begin{aligned} |\rho (\partial _{x}^\alpha (f) )|(x) \lesssim \frac{1}{\left( 1+t+|x| \right) ^{n+| \alpha |}} \sum _{|\beta | \le n+|\alpha |, Z^\beta \in \gamma ^{|\beta |}_s} || Z^\beta f ||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}, \end{aligned}

Similarly, for any sufficiently regular function f defined on $${\mathbb {R}}_t \times {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v$$, we have, for all $$t \ge 0$$ all $$x \in {\mathbb {R}}^n$$ and all $$\tau \in \mathbb {N}$$,

\begin{aligned} |\rho (\partial _{x}^\alpha \partial _{t}^\tau (f) )|(t,x)\lesssim & {} \frac{1}{\left( 1+t+|x| \right) ^{n+|\alpha |} \left( 1+t\right) ^{\tau }}\\&\quad \times \,\sum _{|\beta | \le n+\tau +|\alpha |, Z^\beta \in \gamma ^{|\beta |}} || Z^\beta f ||_{L^1( {\mathbb {R}}_x \times {\mathbb {R}}_v )}, \end{aligned}

### Proof

The first part of the proposition is a consequence of Lemma 2.6, Lemma 2.4 and the global Klainerman Sobolev inequality (14).

The second part of the proposition follows similarly, using that

\begin{aligned} t \partial _t \rho (f)= \rho (t \partial _t f)= \rho \left[ t \partial _t f -\sum _{i=1}^n v^i \partial _{v^i}f-n f \right] \end{aligned}

with $$t \partial _t -\sum _{i=1}^n v^i \partial _{v^i}$$ being a linear combination of commuting vector fields as explained in Remark 2.1$$\square$$

### Remark 3.3

In the above proposition, additional t derivatives yield only additional t decay and no improvement in terms of |x| decay. This improvement can also be achieved assuming stronger decay in v of the initial data. More precisely, if f is a solution to $$T(f)=0$$ then

\begin{aligned} \partial _t f= -\sum _{i=1}^n v^i \partial _{x^i} f=\sum _{i=1}^n \partial _{x^i} (-v^i f). \end{aligned}

Note now that if f is a solution, so is $$v^i f$$, for any $$v^i$$. Thus, for all i, $$\int _{v} \partial _{x^i} (-v^i f) dv$$ enjoys the additional decay $$(t+|x|)$$ as stated in Proposition 3.5, provided that the $$L^1$$ norms of $$Z^\alpha (v^i f )$$ are finite for $$|\alpha | \le n+1$$. Iterating the procedure, we obtain that each $$\partial _t$$ derivatives gives an additional decay of $$(t+|x|)$$.

For the applications to the Vlasov-Poisson system of this paper, we will also need an $$L^2$$ based Klainerman-Sobolev inequality to estimate $$\nabla Z^\alpha \phi$$ pointwise, for $$\phi$$ a solution to the Poisson equation (2). The estimate that we will used is contained in the following lemma.

### Lemma 3.2

For any sufficiently regular function of $$\psi$$ defined on $${\mathbb {R}}^n_x$$, we have, for all $$t\ge 0$$,

\begin{aligned} |\psi (x)| \lesssim \frac{1}{\left( 1+t+|x| \right) ^{n/2}} \sum _{|\alpha | \le (n+2)/2, Z^\alpha \in \Gamma _s} || Z^\alpha (\psi ) ||_{L^2({\mathbb {R}}_x^n)}. \end{aligned}

### Proof

The proof is similar to that of Lemma 3.1, considering the function $$\widetilde{\psi }: y \rightarrow \psi (x+(t+|x|)y)$$ and replacing the $$L^1$$ Sobolev inequality with the $$L^2$$ Sobolev inequality

\begin{aligned} |\psi (x)|^2=|\widetilde{\psi }(0)|^2 \lesssim \sum _{|\alpha | \le (n+2)/2} \int _{B_n(0,1/2)}|\partial ^\alpha (\widetilde{\psi })|^2 dy. \end{aligned}

$$\square$$

## Small Data Solutions of the Vlasov-Poisson System

### The Norms

The vector fields presented in Section 2.1 and the resulting decay estimates of the previous section will be sufficient to prove global existence of solutions to the Vlasov-Poisson system and derive their asymptotics for all dimension $$n \ge 4$$. On top of the boundedness of the $$L^1$$ norms of commuted fields $$Z^\alpha (f)$$, which are needed in order to obtain pointwise decay from the vectorfield method, we will also need a little bit of additional integrability to prove the $$L^p$$ boundedness of the gradient of the commuted potentials $$\nabla Z^\alpha \phi$$.

With this in mind, for any $$n \ge 4$$, $$N \in \mathbb {N}$$ and $$\delta > 0$$, let us consider, for any sufficiently regular function g of (xv), the norm $$E_{N,\delta }$$ defined by

\begin{aligned} E_{N,\delta }[g]:= & {} \sum _{|\alpha |\le N, Z^\alpha \in \gamma _s^{|\alpha |} } || Z^\alpha (g) ||_{L^1({\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}\\&+\,\sum _{|\alpha |\le N, Z^\alpha \in \gamma _s^{|\alpha |} } || (1+|v|^2)^{\frac{\delta (\delta +n)}{2(1+\delta )} } Z^\alpha (g) ||_{L^{1+\delta }({\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}. \end{aligned}

As we shall see below, applying a similar strategy would fail in dimension 3 due to the lack of sufficiently strong decay. In order to close the estimates, it will thus be necessary to improve the commutation relation between our commutation vector fields and our perturbed transport operator. This led us to the introduction of modified vector fields, denoted Y (and $$Y^\alpha$$ for a combination of $$|\alpha |$$ such vector fields) below. Our main results are then similar to the $$n \ge 4$$ case, replacing the Z vector fields by the Y ones. In dimension 3, the norm $$E_{N,\delta }$$ will therefore be defined as

\begin{aligned} E_{N,\delta }[g]:= & {} \sum _{|\alpha |\le N, Y^\alpha \in \gamma _{m,s}^{|\alpha |} } || Y^\alpha (g) ||_{L^1({\mathbb {R}}^3_x \times {\mathbb {R}}^3_v)}\nonumber \\&\quad +\,\sum _{|\alpha |\le N, Y^\alpha \in \gamma _{m,s}^{|\alpha |} } || (1+|v|^2)^{\frac{\delta (\delta +3)}{2(1+\delta )}} Y^\alpha (g) ||_{L^{1+\delta }({\mathbb {R}}^3_x \times {\mathbb {R}}^3_v)}. \end{aligned}
(20)

The precise definitions of the modified vector fields Y and of the algebra $$\gamma _{m,s}$$ are given in Section 6.2.

### Remark 4.1

In order to close our main estimates, we will not need to commute with any vector field containing t derivatives, i.e. commuting with vector fields in $$\gamma _s$$ if $$n\ge 4$$ (respectively $$\gamma _{m,s}$$ if $$n=3$$) will be sufficient. Commutations with vector fields containing t derivatives are of course useful if one wants to obtain decay estimates of t-derivatives of $$\rho (f)$$ and $$\nabla \phi$$. In that case, one would simply modify the norms, replacing the algebra $$\gamma _s$$ (respectively $$\gamma _{m,s}$$) by the algebra $$\gamma$$ (respectively $$\gamma _{m}$$). The interested reader can then verify that all the arguments below still hold. For these reasons, we will sometimes omit in the following section to specify whether the vector fields considered lie in $$\gamma$$ (respectively $$\gamma _{m}$$) or in $$\gamma _s$$ (respectively $$\gamma _{m,s}$$).

### The Main Results

Our main results are the following

### Theorem 4.1

Let $$n \ge 3$$, $$0< \delta < \frac{n\,-\,2}{n\,+\,2}$$, and $$N \ge 5n/2+2$$ if $$n\ge 4$$, $$N \ge 14$$ if $$n=3$$. Then, there exists $$\epsilon _0 > 0$$ such that for all $$0< \epsilon <\epsilon _0$$, if $$E_{N,\delta }[f_0] \le \epsilon$$, then the classical solution f(txv) of (1)-(3) exists globally in time and satisfies the estimates

1. 1.

Global bounds

\begin{aligned} \forall t \in {\mathbb {R}},\quad E_{N,\delta }[f(t)] \lesssim \epsilon . \end{aligned}
2. 2.

Space and time pointwise decay of averages of f

\begin{aligned} \text {for any multi-index } \alpha \text { of order } |\alpha | \le N-n, \quad |\rho ( Z^\alpha f)(t,x) | \lesssim \frac{\epsilon }{\left( 1+|t|+|x| \right) ^{n}}, \end{aligned}

as well as the improved decay estimates

\begin{aligned} |\rho ( \partial _{x}^\alpha f)(t,x) | \lesssim \frac{\epsilon }{\left( 1+|t|+|x| \right) ^{n+|\alpha |}}. \end{aligned}
3. 3.

Boundedness for $$L^{1+\delta }$$ norms of $$\nabla ^2 Z^\alpha \phi$$

\begin{aligned} \text {for any multi-index } \alpha \text { of order } |\alpha | \le N, \quad ||\nabla ^2 Z^\alpha \phi ||_{L^{1+\delta }({\mathbb {R}}^n)} \lesssim \epsilon . \end{aligned}
4. 4.

Space and time decay of the potential and its derivatives

\begin{aligned} \text {for any multi-index } \alpha \text { with }&|\alpha | \le N-(3n/2+1), \\&|Z^\alpha \nabla \phi (t,x) | \lesssim \frac{\epsilon }{t^{(n-2)/2}\left( 1+|t|+|x| \right) ^{(n)/2}} \end{aligned}

as well as the improved decay estimates

\begin{aligned} |\partial ^\alpha _x \nabla \phi (t,x) | \lesssim \frac{\epsilon }{t^{(n-2)/2}\left( 1+|t|+|x| \right) ^{n/2+|\alpha |}}. \end{aligned}

Finally, all the constants in the above inequalities depend only on $$N,n,\delta$$.

As explained above, when $$n \ge 4$$, the proof is easier and can be performed using only the commuting vector fields of the free transport operator while in the $$n=3$$ case, we will need to use modified vector fields. The modified vector fields approach would of course work also in the $$n \ge 4$$ case but are not necessary there. In order to better explain the general framework, we will treat first the dimension $$n \ge 4$$ before turning to the proof in the $$n=3$$ case.

## Proof When $$n \ge 4$$

In this section, we assume that $$n \ge 4$$, that the assumptions of Theorem 4.1 are satisfied for some initial data $$f_0$$ and we denote by f the classical solution of (1)-(3) arising from $$f_0$$.

### Bootstrap Assumption

We will assume the following bootstrap assumption on the norm of the solution $$E_{N,\delta }[f(t)]$$. Let $$T \ge 0$$ be the largest time such that the following bounds hold

\begin{aligned} \forall t \in [0,T],\quad E_{N,\delta }[f(t)] \le 2 \epsilon . \end{aligned}
(21)

It follows from the smallness assumptions on $$E_{N,\delta }[f_0]$$ and a continuity argument that $$T> 0$$.

### Immediate Consequence of the Bootstrap Assumption

Applying our decay estimate (15) to $$\left| Z^\alpha f \right|$$ and $$\left| Z^\alpha f \right| ^p (1+v^2)^{q/2}$$ as well as the improved decay estimates of Proposition 3.5, we automatically obtain from our bootstrap assumption (21)

### Lemma 5.1

For any multi-index $$\alpha$$ of order $$|\alpha | \le N-n$$ and for all $$t \in [0,T]$$,

\begin{aligned} \left| \rho \left( \left| Z^\alpha f \right| \right) (t,x) \right| \le \frac{C_n \epsilon }{\left( 1+|t|+|x| \right) ^{n}}, \end{aligned}
(22)
\begin{aligned} \left| \rho \left( \left| Z^\alpha f \right| ^{1+\delta } (1+v^2)^{\frac{\delta (\delta +n)}{2}}\right) (t,x) \right| \le \frac{C_n \epsilon ^{1+\delta }}{\left( 1+|t|+|x| \right) ^{n}}, \end{aligned}
(23)

for some constant $$C_n >0$$ depending on n, as well as the improved decay estimates,

\begin{aligned} \left| \rho \left( \partial ^\alpha f\right) (t,x) \right| \le \frac{C_n \epsilon }{\left( 1+|t|+|x| \right) ^{n+|\alpha |}}. \end{aligned}

#### Estimates on $$Z^\alpha (\phi )$$

From standard elliptic estimates, we can also bound an $$L^p$$ norm of $$\nabla ^2 Z^\alpha \phi$$

### Lemma 5.2

For any multi-index $$\alpha$$ with $$|\alpha |\le N$$ and for all $$t \in [0,T]$$,

\begin{aligned} ||\nabla ^2 Z^\alpha \phi (t) ||_{L^{1+\delta }({\mathbb {R}}^n)} \le C_{N,n,\delta } \epsilon , \end{aligned}

where $$C_{N,n,\delta } > 0$$ is a constant depending on N, n and $$\delta$$.

### Remark 5.1

In the present small data context, there is no difficulty in propagating higher $$L^p$$ norms of $$\,\nabla ^2 Z^\alpha \phi$$ for $$p> 1+\delta$$ provided the initial data for f satisfy additional integrability and decay in v. However, to close the estimates of our main theorem, all that is needed is the above $$L^{1+\delta }$$ bound on $$\nabla ^2 Z^\alpha \phi$$.

### Proof

Let $$p=1+\delta$$. From the commuted equation for $$Z^\alpha \phi$$ and the Calderón-Zygmund inequality, we have

\begin{aligned} || \nabla ^2 Z^\alpha \phi ||_{L^p( {\mathbb {R}}^n)}\lesssim & {} \sum _{|\beta | \le |\alpha |}|| Z^\beta ( \rho (f)) ||_{L^p({\mathbb {R}}^n)},\\\lesssim & {} \sum _{|\beta | \le |\alpha |}|| \rho \left( \left| Z^\beta (f ) \right| \right) ||_{L^p({\mathbb {R}}^n)} \end{aligned}

using Lemma 2.4. Thus the bounds on $$\nabla ^2 Z^\alpha \phi$$ follow if we can prove $$L^p$$ bounds on the $$\rho \left( \left| Z^\beta f \right| \right)$$. For this, let us note that for any weight function $$\chi (v)$$, we have, using the Hölder inequality with $$1/p+1/q=1$$

\begin{aligned} \int _x \left( \int _v |Z^\beta (f)| dv \right) ^p dx \le \int _x \left( \int _v \frac{1}{\chi (v)} dv \right) ^{p/q} dv \int _v \chi (v)^{p/q} |Z^\beta (f)|^p dv dx. \end{aligned}

Thus, we need $$\frac{1}{\chi (v)}$$ to be integrable in v and we choose $$\chi (v)=(1+|v|^2)^{(\delta +n)/2}$$. The lemma then follows from the bound on $$E_{N,\delta }[f(t)]$$ noting that with $$p=1+\delta$$, we have $$p/q=\delta$$$$\square$$

Applying the Gagliardo-Nirenberg inequality, we have immediately

### Corollary 5.1

Let $$q=\frac{n(1+\delta )}{n-(1+\delta )}$$. For all $$t\in [0,T]$$,

\begin{aligned} ||\nabla Z^\alpha \phi (t) ||_{L^q({\mathbb {R}}^n)} \le C_{N,n,\delta } \epsilon . \end{aligned}

Applying $$L^2$$ estimates for solutions to the Poisson equation (7) and the previous pointwise estimates on $$\rho \left( \left| Z^\alpha (f) \right| \right)$$, we can also obtain $$L^2$$ decay estimates for $$\nabla Z^\alpha \phi$$ provided $$|\alpha |$$ is not too large.

### Lemma 5.3

For all multi-index $$\alpha$$ such that $$|\alpha | \le N-n$$

\begin{aligned} ||\nabla Z^\alpha \phi ||_{L^2({\mathbb {R}}^n)} \lesssim \frac{ \epsilon }{t^{(n-2)/2}}. \end{aligned}

### Proof

Multiply the Poisson equation satisfied by $$Z^\alpha \phi$$ by $$Z^\alpha \phi$$ and integrate by parts to obtain

\begin{aligned} ||\nabla Z^\alpha ( \phi ) ||_{L^2({\mathbb {R}}^n)}^2= & {} -\int _{x \in {\mathbb {R}}^n}Z^\alpha ( \phi )Z^\alpha ( \rho (f)) dx \\\le & {} ||Z^\alpha ( \phi )||_{L^{\frac{2n}{n-2}}({\mathbb {R}}^n)}||Z^\alpha ( \rho (f))||_{L^{\frac{2n}{n+2}}({\mathbb {R}}^n)}. \end{aligned}

Using the Gagliardo-Nirenberg inequality $$||\psi ||_{L^{\frac{2n}{n-2}}({\mathbb {R}}^n)} \lesssim || \nabla \psi ||_{L^2({\mathbb {R}}^n)}$$ and Lemma 2.4, we obtain

\begin{aligned} ||\nabla Z^\alpha ( \phi ) ||_{L^2({\mathbb {R}}^n ) }\lesssim & {} ||Z^\alpha ( \rho (f))||_{L^\frac{2n}{n+2}({\mathbb {R}}^n)} \nonumber \\\lesssim & {} \sum _{|\beta | \le |\alpha |} ||\rho (Z^\beta (f))||_{L^\frac{2n}{n+2}({\mathbb {R}}^n)} \end{aligned}
(24)

Since

\begin{aligned} \int _{x \in {\mathbb {R}}^n } \frac{dx}{\left( 1+|x|+t \right) ^{\frac{2n^2}{n+2}}} \lesssim t^{-\left( \frac{2n^2}{n+2}-n\right) } \int _{x \in {\mathbb {R}}^n } \frac{d(x/t)}{\left( |x/t|+1 \right) ^{\frac{2n^2}{n+2}}} \lesssim t^{-\left( \frac{2n^2}{n+2}-n\right) }, \end{aligned}

the lemma now follows by estimating the right-hand side of (24) using the pointwise estimates (22) on $$\rho (Z^\beta (f))$$$$\square$$

The previous lemma combined with the $$L^2$$ based Klainerman-Sobolev inequality of Lemma 3.2 gives the pointwise estimates on $$\nabla Z^\alpha ( \phi )$$ claimed in the theorem.

### Corollary 5.2

For any multi-index $$|\alpha | \le N-(3n/2+1)$$ and $$Z^\alpha \in \Gamma _s^{|\alpha |}$$, we have for all $$t \in [0,T],$$

\begin{aligned} \left| \nabla Z^\alpha \phi \right| \lesssim \frac{ \epsilon }{(1+|x|+t)^{n/2}t^{(n-2)/2}}. \end{aligned}

### Improving the Global Bounds

#### $$L^1$$ estimates of $$Z^\alpha f$$

We first consider the $$L^1$$ estimate on $$Z^\alpha (f)$$. From Lemma 2.9, we have for all multi-index $$|\alpha | \le N$$, and all $$t\in [0,T]$$,

\begin{aligned} || Z^\alpha f(t) ||_{L^1_{x,v}} \le || Z^\alpha f(0) ||_{L^1_{x,v}} + \int _0^t || T_\phi (Z^\alpha (f) )||_{L^1_{x,v}}. \end{aligned}

Thus, we only need to prove that the term below the integral is integrable in t.

Now, from the commutation formula of Lemma 2.7, we know that

\begin{aligned} || T_\phi (Z^\alpha (f) )||_{L^1_{x,v}} \le C_N \sum _{|\beta | \le |\alpha |-1,} \sum _{|\gamma |+|\beta | \le |\alpha |}| C_{\beta \gamma }^\alpha | ||\nabla _x Z^\gamma \phi \nabla _v Z^\beta f ||_{L^1_{x,v}} . \end{aligned}

Note that we have so far no estimates on v derivatives of $$Z^\beta f$$. To circumvent this difficulty, let us rewrite any v derivative as

\begin{aligned} \partial _{v^i} Z^\beta (f)= (t \partial _{x^i} + \partial _{v^i} ) Z^\beta (f) -t \partial _{x^i} Z^\beta (f). \end{aligned}

Since both $$t \partial _{x^i} + \partial _{v^i}$$ and $$\partial _{x^i}$$ are part of our algebra of commuting vector fields, we have

\begin{aligned} || T_\phi (Z^\alpha (f) )||_{L^1_{x,v}} \le C_N (1+t ) \mathop {\mathop {\sum }\limits _{|\beta | \le |\alpha |,|\gamma | \le |\alpha |}}\limits _{|\gamma | +|\beta |\le |\alpha |+1} | C_{\beta \gamma }^\alpha | ||\nabla _x Z^\gamma (\phi ) Z^\beta (f) ||_{L^1_{x,v}} . \end{aligned}
(25)

Now, since $$N \ge 5n/2+2$$ and $$|\gamma | +|\beta |\le |\alpha |+1 \le N+1$$, we always have at least either $$|\gamma | \le N-(3n/2+1)$$ or $$|\beta | \le N -n$$.

Case 1: $$|\gamma | \le N-(3n/2+1)$$

In that case, we have access, thanks to Corollary 5.2 to the pointwise estimates, for all $$t \in [0,T]$$,

\begin{aligned} | \nabla _x Z^\gamma \phi (t,x) | \le \frac{C_N \epsilon }{(1+t)^{n-1}}. \end{aligned}

Thus, we get the estimates

\begin{aligned} ||\nabla _x Z^\gamma (\phi ) Z^\beta (f) ||_{L^1_{x,v}}\le \frac{C_N \epsilon }{(1+t)^{n-1}} \sum _{|\beta | \le |\alpha |} ||Z^\beta f ||_{L^1_{x,v}} \end{aligned}
(26)

and we see that if $$n \ge 4$$, then the error is integrable.

Case 2: $$|\beta | \le N-n$$

In that case, we estimate the error term as follows. First,

\begin{aligned} ||\nabla _x Z^\gamma (\phi ) Z^\beta (f) ||_{L^1_{x,v}}= & {} \int _x \int _v |\nabla _x Z^\gamma (\phi ) | | Z^\beta (f)| dx dv \\= & {} \int _x |\nabla _x Z^\gamma (\phi ) | \rho \left( | Z^\beta (f)| \right) dx, \end{aligned}

since $$Z^\gamma (\phi )$$ is independent of v. Now applying the Hölder inequality with $$1/p+1/q=1$$, we obtain

\begin{aligned} ||\nabla _x Z^\gamma (\phi ) Z^\beta (f) ||_{L^1_{x,v}}\le & {} || \nabla _x Z^\gamma (\phi ) ||_{L^q_x} \left| \left| \rho \left( | Z^\beta (f)| \right) \right| \right| _{L^p_x} \end{aligned}

We would like to take $$q=2$$, since the $$L^2$$ bounds are so easy to obtain for solutions to the Poisson equation. Using the pointwise bounds to estimate $$|| \rho \left( | Z^\beta (f)| \right) ||_{L^2_x}$$, we would obtain

\begin{aligned} \left| \left| \rho \left( | Z^\beta (f)| \right) \right| \right| _{L^2_x} \le C_N \epsilon t^{-n/2}. \end{aligned}

On the other hand, we would get no decay a priori on $$||\nabla _x Z^\gamma (\phi )||_{L^2_x}$$, since $$|\gamma |$$ is a priori too large to have access to decay estimates for the source term of the Poisson equation satisfied by $$Z^\gamma (\phi )$$. With the extra weight of t in (25), we see that if $$n=4$$, we only get 1 / t decay and we would get a logarithmic loss.

To avoid this problem, we want to take $$q < 2$$. Recalling the $$L^q$$ bounds of Corollary 5.1, we see that since $$\delta < \frac{n-2}{n+2}$$, we have $$q=\frac{n(1+\delta )}{n-(1+\delta )} < 2$$ and thus,

\begin{aligned} || \rho \left( | Z^\beta (f)| \right) ||_{L^p_x} \le \frac{C_N \epsilon }{(1+ t)^{n/2+\sigma }}, \end{aligned}

for some $$\sigma > 0$$, which has enough decay so that it remains integrable in t even when multiplied by the extra t weight of (25). Putting everything together, we have obtain

\begin{aligned} || T_\phi (Z^\alpha (f) )||_{L^1_{x,v}} \le \frac{C_N \epsilon }{(1+ t)^{n-2}} E_{N,\delta }[f(t)]+\frac{C_N \epsilon ^2}{(1+ t)^{n/2-1+\sigma }} \lesssim \frac{C_N \epsilon ^2}{(1+ t)^{n/2-1+\sigma }}, \end{aligned}

using the bootstrap assumptions to bound $$E_{N,\delta }[f(t)]$$.

#### v Weighted $$L^{p}$$ Estimates of $$Z^\alpha f$$

Let $$p=1+\delta$$ and $$q=\delta (\delta +n)$$. Recall from (8) the inequality,

\begin{aligned}&\left| \left| (1+v^2)^{q/2} |Z^\alpha f(t)|^p \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}\\&\quad \lesssim \left| \left| (1+v^2)^{q/2} |Z^\alpha f(0)|^p \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)} \\&\qquad +\int _0^t \left| \left| (1+v^2)^{q/2} |Z^\alpha f |^{p-1} T_\phi (Z^\alpha f) \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}ds \\&\qquad +\int _0^t \left| \left| \,\, | Z^\alpha f |^{p} (1+v^2)^{(q-1)/2} \partial _x \phi \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}ds, \\&\quad \lesssim \left| \left| (1+v^2)^{q/2} |Z^\alpha f(0)|^p \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v)}+I_1+I_2, \end{aligned}

where

\begin{aligned} I_1=\int _0^t \left| \left| (1+v^2)^{q/2} |Z^\alpha f |^{p-1} T_\phi (Z^\alpha f) \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )} \end{aligned}

and

\begin{aligned} I_2=\int _0^t \left| \left| \, \,| Z^\alpha f |^{p} (1+v^2)^{(q-1)/2} \partial _x \phi \right| \right| _{L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v )}. \end{aligned}

To estimate the error term $$I_1$$, we proceed as in the previous section, replacing $$T_\phi (Z^\alpha f)$$ using the commutation formula of Lemma 2.7 and rewriting the terms of the form $$\partial _v^i Z^\beta f$$ as $$\left( t\partial _{x^i}+ \partial _v \right) Z^\beta (f)- t \partial _{x^i} Z^\beta f$$. We are then left with error terms of the form

\begin{aligned} (1+t)\int _{x} \int _{v} |\partial _x Z^\gamma \phi | |Z^\beta f|(1+v^2)^{q/2} |Z^\alpha f|^{p-1} dxdv, \end{aligned}
(27)

which need to be integrable in t. Using Young inequality, we have that

\begin{aligned} \int _v |Z^\beta f|(1+v^2)^{q/2} |Z^\alpha f|^{p-1} dv\lesssim & {} \int _v |Z^\beta f|^p(1+v^2)^{q/2} dv\\&\quad +\,\int _v |Z^\alpha f|^p(1+v^2)^{q/2} dv. \end{aligned}

Note moreover that, as in the previous section, if $$|\alpha | \le N-n$$, we have access to the pointwise estimates (23). With this in mind, all the error terms coming from $$I_1$$ can then be estimated as in the previous section.

The estimates on the error term $$I_2$$ are easier and rely on the pointwise estimates of $$\partial \phi$$ of Lemma 5.2.

### Conclusions of the Proof of the $$n \ge 4$$ Case

Thus, we have obtained

\begin{aligned} E_{N,\delta }(t) \le E_{N,\delta }(0)+ C_N \int _0^t \frac{\epsilon ^2}{(1+ s)^{n/2+\sigma }} ds, \end{aligned}

for some $$\sigma > 0$$. Using the smallness assumption $$E_{N,\delta }(0) \le \epsilon$$, it follows that $$E_{N,\delta }(t) \le \epsilon + C \epsilon ^2 \le \frac{3}{2} \epsilon$$, provided $$\epsilon$$ is sufficiently small, which improves our original bootstrap assumption (21) and concludes the proof.

## The Three Dimensional Case

### Strategy of the Proof

Repeating the previous argument in the $$n=3$$ case would fail as seen from inequality (26). Moreover, the non-linear terms do not seem to possess any special structure that would allow better decay such as the null condition for non-linear waves in 3d, and it does not seem possible to close the estimates allowing the norms to grow slowly, using some hierarchy in the equations, as it sometimes happen for some system of non-linear evolution equations (for instance in [17]). Thus, it seems that one is forced to try to improve the commutation relations so as to remove the most problematic error terms. This will be done using modified vector fields. In hindsight, this strategy is reminiscent of the strategy of [3] where modified vector fields are constructed by solving transport equations along null cones.

To understand and motivate the definitions of the modified vector fields that we will use here, let us consider a solution f to the transport equation $$T_\phi (f)=0$$ and commute this equation with $$Z_i=t \partial _{x^i} + \partial _{v^{i}}$$. We obtain

\begin{aligned} T_\phi ( Z_i(f))= & {} T( Z_i(f)) + \mu \nabla _x\phi . \nabla _v Z_i(f) \\= & {} Z_i(T(f)) + \mu Z_i (\nabla _x \phi .\nabla _v f) - \mu \nabla _x (Z_i \phi ). \nabla _v f \\= & {} Z_i ( T_\phi (f)) -\mu \sum _{j=1}^n \partial _{x^j} Z_i( \phi ). ( t\partial _{x^j}+\partial _{v^j} )f + \mu \sum _{j=1}^n \partial _{x^j} Z_i( \phi ). t \partial _{x^j} f \end{aligned}

Thus, the error terms on the right-hand side are of two forms. The good terms are of the form $$\partial _x Z_i(\phi ) Z'f$$, where the $$Z'$$ are some of the commuting vector fields. These have enough decay so that they can be estimated as before. The bad terms are of the form $$t\partial _x Z_i (\phi ) Z'f$$ where, in view of the extra t factor, the previous arguments would lead to logarithmic growth.

The aim of the modified vector fields will be to avoid the introduction of such bad terms. Note that on the other hand, commutations with vector fields such as $$\partial _t$$ or $$\partial _{x^i}$$ would be better, because $$\partial \partial \phi$$ enjoys improved decay. As a consequence, we will only need to modify the homogeneous vector fields.

Let us consider, for all $$1 \le i \le n$$, vector fields of the form

\begin{aligned} Y_i=t \partial _{x^i} + \partial _{v^i} - \sum _{j=1}^n \Phi ^{j}_i(t,x,v) \partial _{x^j}, \end{aligned}

where the coefficients $$\Phi ^{j}_i(t,x,v)$$ are sufficiently regular functions to be specified below.

Since $$\partial _{x^j}$$ commute with the free transport operator, we have the commutation formula

\begin{aligned}{}[T_\phi , Y_i](f)= & {} -\mu \sum _{j=1}^n \partial _{x^j} Z_i(\phi ) Z_j(f) +\mu \sum _{j=1}^n \Phi ^{j}_i \partial _{x^j}(\nabla _x\phi ).\nabla _{v}f \nonumber \\&\hbox {}-\sum _{j=1}^n T_\phi ( \Phi ^{j}_i) \partial _{x^j}f + \mu \sum _{j=1}^n \partial _{x^j} Z_i ( \phi ) t \partial _{x^j} f \end{aligned}
(28)

where $$Z_j = t \partial _{x^j} + \partial _{v^j}$$. The first term on the right-hand can be handled as before as it does not have v derivatives leading to the extra power of t. Note moreover that since $$t \partial _{x^j }$$ is part of the algebra of macroscopic commuting vector field, the second term can be rewritten as

\begin{aligned} \sum _{j=1}^n \Phi ^{j}_i t^{-1} \nabla _x Z_j \phi \nabla _v f \end{aligned}

and thus is expected to be integrable by the previous arguments provided $$\Phi ^{j}_i$$ are uniformly bounded by any power of t strictly less 1.

The key idea is then to choose appropriately the $$\Phi ^{j}_i$$ so as to be able to cancel the last two terms in (28). For this, we impose that each $$\Phi ^{j}_i$$ is obtained as the unique solution to the inhomogeneous transport equation

\begin{aligned} T_\phi (\Phi ^{j}_i )= \mu t \partial _{x^j} Z_i(\phi ) \end{aligned}

with 0 initial data. Note that the right-hand side of this equation only decay like 1 / t, so we expect $$\Phi ^{j}_i$$ to actually grow logarithmically in t.

Assuming that this holds, we see that all the error terms in (28) are now integrable and thus, we should expect to control our norms $$E_{N,\delta }[f(t)]$$ provided all the original commutation vector fields Z are replaced by their modified form Y, hence the definition of the norm in the 3d case given by (20). A few difficulties remain

1. 1.

Since the $$\Phi ^j_i$$ (and in fact all the coefficients involved in the construction of the modified vector fields) are growing logarithmically, it is a priori not clear how to exploit the new energies obtained after commutation with modified vector fields to obtain pointwise decay. The idea is again to rewrite the extra terms such as $$\Phi ^{j}_i \partial _{x^j}(f)$$ in the form

\begin{aligned} \Phi ^{j}_i \partial _{x^j}(f)= \frac{\Phi ^j_i}{t} \left( t \partial _{x^j} + \partial _{v^j} \right) (f)-\frac{\Phi ^j_i}{t} \partial _{v^j}(f) \end{aligned}

and to use an integration by parts in v for the last term to push the v derivatives on the $$\Phi ^j_i$$ coefficient. See Section 6.4 below.

2. 2.

The Poisson equation $$\Delta \phi =\rho (f)$$ cannot be commuted with modified vector fields, since the coefficients in the modified vector fields depend on v, while $$\phi$$ and $$\rho (f)$$ are macroscopic quantities depending only on (tx). Thus, we keep commuting this equation with non-modified vector fields. Quantities such as $$Z^\alpha \rho (f)$$ are then rewritten as $$\rho ( Y^\alpha (f))$$ plus error terms. The structure of these error terms is the subject of Lemma 6.3.

3. 3.

As is seen from the statement of Lemma 6.3, some of the error terms will depend on $$Y^\alpha (\varphi )$$, where $$\varphi$$ is a coefficient obtained by solving a transport equation of the form $$T_\phi (\varphi )= t \partial _x Z \phi$$ and $$Y^\alpha$$ is a composition of $$|\alpha |$$ modified vector fields. Commuting the transport equation satisfied by $$\varphi$$ by $$|\alpha |$$ vector fields, we see that we need to control $$t Y^\alpha \partial _x Z (\phi )$$. This poses a problem at the top order, when $$|\alpha |=N$$, since it looks as if one needs to control $$\partial Z^\alpha Z(\phi )$$, which would a priori require to commute the Poisson equation by $$N+1$$ vector fields, and therefore would forbid us to close the estimates. On the other hand, using directly the Poisson equation satisfied by $$Z^\alpha (\phi )$$, we may hope to control $$\partial ^2 Z^\alpha (\phi )$$. To exploit this fact and close the top order estimates, we devote some time to describe the structure of the top order terms of Lemma 6.3 in Lemma 6.4.

4. 4.

Finally, numerous terms of the form $$Y^\alpha (\varphi ) Y^\beta (f)$$, where $$\varphi$$ is a coefficient obtained by solving a transport equation as above, will appear in the equations. This creates another difficulty to close the top order estimates, since we do not have access to pointwise estimates on $$Y^\alpha (\varphi )$$ when $$|\alpha |$$ is large, nor do we have access to $$L^p_{x,v}$$ estimates on $$Y^\alpha (\varphi )$$ because the source terms in their transport equations are not integrable in v. We will circumvent this difficulty by considering directly a transport equation satisfied by the product $$Y^\alpha (\varphi ) Y^\beta (f)$$. See Section 6.5 below.

We now turn to the details of the proof.

### Definitions and Properties of the Modified Vector Fields Algebra

As explained above, our new algebra of microscopic vector fields will consist in

1. 1.

Standard translations $$\partial _t$$, $$\partial _{x^i}$$,

2. 2.

Modified uniform motions $$Y_i:=t \partial _{x^i}+ \partial _{v^i}-\sum _{k=1}^n \Phi ^{k}_i \partial _{x^k}$$,

3. 3.

Modified rotations $$\Omega _{i,j}^{x}+\Omega _{i,j}^{v}-\sum _{k=1}^n \omega ^{k}_{i,j} \partial _{x^k}$$,

4. 4.

Modified scaling in space $$S^{x}+S^{v}-\sum _{k=1}^n \sigma ^{k} \partial _{x^k}$$,

5. 5.

Modified scaling in space and time $$t\partial _t + \sum _{i=1}^n x^i \partial _{x^i} - \sum _{k=1}^n \theta ^{k} \partial _{x^k}$$,

where the coefficients $$\Phi ^{k}_i$$, $$\omega ^{k}_{i,j}$$, $$\sigma ^{k}$$, $$\theta ^{k}$$ are solutions of the following inhomogeneous equations with 0 data at $$t=0$$

\begin{aligned} T_\phi ( \Phi ^{k}_i )= & {} \mu t \partial _{x^k}\left[ Z_i(\phi ) \right] , \\ T_\phi ( \omega ^{k}_{i,j})= & {} \mu t \partial _{x^k} \left[ \Omega _{i,j}^{x} ( \phi )\right] , \\ T_\phi ( \sigma ^{k} )= & {} \mu t \partial _{x^k} \left[ S^{x} (\phi )-2\phi \right] , \\ T_\phi ( \theta ^{k})= & {} \mu t \partial _{x^k}\left[ \left( t\partial _t + \sum _{i=1}^n x^i \partial _{x^i} \right) ( \phi )\right] . \end{aligned}

#### Further Notations

Since the sign of $$\mu$$ will play no role in the analysis to come, we will assume without loss of generality that $$\mu =1$$ in the rest of this article, to simplify the notation.

We will denote by $${\mathscr {M}}$$ the set of all the coefficients $$\Phi ^{k}_i$$, $$\omega ^{k}_{i,j}$$, $$\sigma ^{k}$$, $$\theta ^{k}$$ and by $$\varphi$$ a generic coefficient among them. Similarly to the set $$\gamma$$ and $$\gamma _s$$, we define the sets $$\gamma _{m}$$ and $$\gamma _{m,s}$$ where $$\gamma _{m}$$ is the set of all modified vector fields (including the translations) and $$\gamma _{m,s}$$ is the set of all modified vector fields minus the time translation and the space-time scaling.

If Z is an original, non-modified vector field, we will sometimes write schematically $$Y=Z+\varphi \partial _x$$ to denote the associated modified vector field, where by convention $$\varphi \partial _x=0$$ is Z is any of the translations, $$\varphi \partial _x=\displaystyle {\sum _{k=1}^n \Phi ^{k}_i \partial _{x^k}}$$ if Z is one of the uniform motions and similarly for the other vector fields.

Finally, we will use the notation $$P(\bar{\varphi })$$ to denote a function depending on all the coefficients in $$\gamma _m$$ or $$\gamma _{m,s}$$.

#### Improved Commutation Formulae

With these definitions, we now have the following improved commutation formulaFootnote 14.

### Lemma 6.1

For any $$Y \in \gamma _{m}$$ and any sufficiently regular function g of (txv), $$[T_\phi ,Y](g)$$ can be written as a linear combination with constant coefficients of terms of the form $$\partial _{x} Z(\phi ) Y(g)$$, $$\varphi \partial _{x} Z(\phi ) Y(g)$$ or $$\varphi ^2 \partial _{x} Z(\phi ) Y(g)$$ where $$\varphi \in {\mathscr {M}}$$, $$\varphi ^2$$ denotes a generic product of two coefficients in $${\mathscr {M}}$$, $$Z \in \Gamma$$ and $$Y \in \gamma _{m}$$.

### Proof

If Y is a translation, for instance $$Y=\partial _{x^k}$$, then

\begin{aligned}{}[T_\phi , Y](g)= & {} -(\partial _{x^k} \nabla _x \phi ).\nabla _v g, \\= & {} -\sum _{i=1}^n \partial _{x^i} \partial _{x^k} \phi . \left( t \partial _{x^i}g+\partial _{v^i}g-\sum _{j=1}^n \Phi ^{j}_i \partial _{x^j} g \right) \\&\hbox {}+\sum _{i=1}^n \partial _{x^i} \partial _{x^k} \phi . \left( t \partial _{x^i}g-\sum _{j=1}^n \Phi ^{j}_i \partial _{x^j} g \right) \\= & {} -\sum _{i=1}^n \partial _{x^i} \partial _{x^k} \phi . Y_i(g) \\&\hbox {}+\sum _{i=1}^n \partial _{x^i} t \partial _{x^k} \phi . \partial _{x^i}g-\sum _{i=1}^n\sum _{j=1}^n \Phi ^{j}_i \partial _{x^i} \partial _{x^k} (\phi ). \partial _{x^j} g, \end{aligned}

which is of the desired form since $$t \partial _{x^k} \in \Gamma$$. If $$Y=Y_i=t \partial _{x^i}+\partial _{v^i}-\sum _{j=1}^n \Phi ^{j}_i \partial _{x^j}$$, then it follows from (28) and the definition of the coefficients $$\Phi ^{j}_i$$ that

\begin{aligned}{}[T_\phi , Y_i](g)= -\sum _{j=1}^n \partial _{x^j} Z_i(\phi ) Z_j(g) +\sum _{j=1}^n \Phi ^{j}_i \partial _{x^j}(\nabla _x\phi ).\nabla _{v}g. \end{aligned}
(29)

where $$Z_i(\phi )= t \partial _{x^i} \phi$$ and $$Z_j(g)=t \partial _{x^i}g+\partial _{v^j} g$$. Since $$Z_j(g)=Y_j(g)+\sum _{i=1}^n \Phi ^i_j\partial _{x^i}(g)$$, the first term term on the right-hand side of (29) is of the desired form while for the last one, we have

\begin{aligned} \sum _{j=1}^n \Phi ^{j}_i \partial _{x^j}(\nabla _x\phi ).\nabla _{v}g= & {} \sum _{j=1}^n\sum _{k=1}^n \Phi ^{j}_i \partial _{x^j}\partial _{x^k}\phi .\partial _{v^k}g \\= & {} \sum _{j=1}^n\sum _{k=1}^n \Phi ^{j}_i \partial _{x^j}\partial _{x^k}\phi .Y_k(g) \\&\hbox {}-\,\sum _{j=1}^n\sum _{k=1}^n \Phi ^{j}_i \partial _{x^j}\partial _{x^k}\phi .\left( t \partial _{x^k}g-\sum _{l=1}^n \Phi ^{l}_i \partial _{x^l} g \right) ,\\= & {} \sum _{j=1}^n\sum _{k=1}^n \Phi ^{j}_i \partial _{x^j}\partial _{x^k}\phi .Y_kg -\sum _{j=1}^n\sum _{k=1}^n \Phi ^{j}_i \partial _{x^j}(t\partial _{x^k}\phi ). \partial _{x^k}g\\&\hbox {}+\,\sum _{j=1}^n\sum _{k=1}^n\sum _{l=1}^n \Phi ^{l}_i \Phi ^{j}_i \partial _{x^j}(\partial _{x^k}\phi ) \partial _{x^l} g, \end{aligned}

which is of the desired form. The commutation with the other modified vector fields can be computed similarly. Note that in the case of the spatial vector field, we have $$[T_\phi , S^x+S^v]=- \nabla _x S^x(\phi ).\nabla _v + 2 \nabla _x \phi . \nabla _v$$, which explains the extra term in the definition of the coefficients $$\sigma ^k$$ compared to the other vector fields. $$\square$$

If we apply several times the previous formula in order to compute $$[T_\phi ,Y^\alpha ]$$, many products of the form $$Y^\rho (\varphi ) Y^{\nu }(\varphi ')$$ will appear. In order to simplify the presentation below, it will be useful to use the following definition.

### Definition 6.1

We will say that $$P(\bar{\varphi })$$ is a multilinear form of degree d and signature less than k if $$P(\bar{\varphi })$$ is of the form

\begin{aligned} P(\bar{\varphi })=\mathop {\mathop {\sum }\limits _{\rho \in I^d,}}\limits _{\rho =(\rho _1, \ldots ,\rho _d)} C_\rho \mathop {\mathop {\prod }\limits _{j=1,\ldots ,d,}}\limits _{\varphi \in {\mathscr {M}}} Y^{\rho _j}(\varphi ), \end{aligned}

where I denotes the set of all multi-indices (thus $$\rho _j$$ is a multi-index for each j), for each $$\rho$$ in the above formula $$\displaystyle \sum _{i=1}^d |\rho _j| \le k$$ and where the $$C_\rho$$ are constants.

Thus, with the help of this definition, we can summarized Lemma 6.1 as saying that $$[T_\phi , Y](g)$$ can be written as a linear combination of terms of the form $$\partial _{x} Z( \phi ) Y(g)$$, for some Z and Y vector fields, with coefficients which are all multilinear forms of degree 2 and signature 0 (the degree keeps track of the number of products and the signature of the total number of derivatives).

From Lemma 6.1, we now obtain

### Lemma 6.2

For any multi-index $$\alpha$$, we have

\begin{aligned}{}[T_\phi ,Y^\alpha ]= \sum _{d=0}^{|\alpha |+1}\sum _{i=1}^n \sum \limits _{\mathop {|\gamma | \le |\alpha |,}\limits _{|\beta | \le |\alpha |}} P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\beta , \end{aligned}
(30)

where the $$P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi })$$ are multilinear forms of degree d and signature less than k such that $$k \le |\alpha |-1$$ and $$k+|\gamma |+|\beta | \le |\alpha |+1$$.

### Proof

This is a classical proof by induction for which we will just sketch the details. Lemma 6.1 shows that (30) holds when $$|\alpha |=1$$. Assume that (30) holds for some multi-index $$\alpha$$ and let $$Y \in \gamma$$ be an arbitrary modified vector field. We have

\begin{aligned}{}[T_\phi , Y Y^\alpha ]=[T_\phi , Y]Y^\alpha +Y[T_\phi , Y^\alpha ]. \end{aligned}

One easily see that the first term on the right-hand side has the correct form using Lemma 6.1. The second term will generate three types of terms. The terms of the form

\begin{aligned} Y\left( P^{\alpha ,i}_{d \gamma \beta }\right) \partial _{x^i} \left( Z^\gamma (\phi ) \right) Y^\beta \end{aligned}

are of the correct form, the multilinear form being of the same degree and its signature being increased by 1 at most. For the terms of the form

\begin{aligned} P^{\alpha ,i}_{d\gamma \beta }Y\left( \partial _{x^i}( Z^\gamma (\phi ))\right) Y^\beta , \end{aligned}

we recall that Y is schematically of the form $$Z+\varphi \partial _x$$. Thus,

\begin{aligned} P^{\alpha ,i}_{d\gamma \beta }Y( \partial _{x^i} Z^\gamma (\phi )) Y^\beta = \sum _{|\gamma '| \le |\gamma |+1}P'_{\gamma '}\partial _{x^i} Z^{\gamma '}(\phi )) Y^\beta , \end{aligned}

where $$P'_{\gamma '}$$ are multilinear forms of degree at most $$d+1$$ and we have not changed the signature, so that these terms are of the desired form.

Finally, the last terms are of the form $$P^{\alpha ,i}_{d\gamma \beta } \partial _{x^i} \left( Z^\gamma (\phi ) \right) Y Y^\beta$$, which clearly satisfied the required properties. $$\square$$

As explained above, we also need to revisit our commutation relations for the Poisson equation satisfied by the potential $$\phi$$. Contrary to f, we cannot commute with a modified vector field, because the coefficients of the modified vector fields depend on v, while $$\phi$$ is a macroscopic quantity and depends only on (tx). Thus, we keep commuting with $$Z^\alpha$$. We have

### Lemma 6.3

Let g be a sufficiently regular function of (txv) and let $$\phi _g$$ solves

\begin{aligned} \Delta \phi _g =\rho (g). \end{aligned}

For any multi-index $$\alpha$$ with $$|\alpha | \le N$$, we have, for all $$0 < t \le T$$,

\begin{aligned} \rho (Z^\alpha (g))= \sum _{j=1}^{|\alpha |} \sum _{d=1}^{|\alpha |+1} \sum _{|\beta | \le |\alpha | } \frac{1}{t^j} \rho \left( P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) \right) + \sum _{d=0}^{|\alpha |}\sum _{|\beta | \le |\alpha | } \rho \left( Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right) \end{aligned}
(31)

and

\begin{aligned} \Delta Z^\alpha (\phi ) = \sum _{j=1}^{|\alpha |} \sum _{d=1}^{|\alpha |+1} \sum _{|\beta | \le |\alpha | } \frac{1}{t^j} \rho \left( \tilde{P}^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) \right) + \sum _{d=0}^{|\alpha |}\sum _{|\beta | \le |\alpha | } \rho \left( \tilde{Q}^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right) , \end{aligned}
(32)

where $$P^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ and $$\tilde{P}^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ are multilinear forms of degree d and signature less than k satisfying

\begin{aligned} k \le |\alpha |, \quad k+|\beta | \le |\alpha | \end{aligned}

and where the $$Q^{\alpha }_{d\beta }(\partial _x\bar{\varphi })$$ and $$\tilde{Q}^{\alpha }_{d\beta }(\partial _x\bar{ \varphi })$$ are all multilinear forms of degree d of the form

\begin{aligned} Q(\partial _x\bar{\varphi })=\mathop {\mathop {\sum }\limits _{\rho \in I^d,}}\limits _{rho=(\rho _1, \ldots , \rho _d)} C_\rho \mathop {\mathop {\sum }\limits _{j=1,\ldots ,n,}}\limits _{\varphi \in {\mathscr {M}}} Y^{\rho _j}(\partial _{x^{r_j}} \varphi ), \end{aligned}
(33)

where the $$C_\rho$$ are constants, $$1 \le r_j \le 3$$, and such that $$\displaystyle k':=\sum _{j=1}^d |\rho _j|$$ satisfies

\begin{aligned} k' \le |\alpha |-1, \quad d+k'+|\beta | \le |\alpha |. \end{aligned}

### Proof

First, recall that if $$Z \in \Gamma$$, then

\begin{aligned} \Delta Z(\phi _g)= Z \Delta \phi _g + d_Z \Delta \phi _g, \end{aligned}

where $$d_Z=0$$ unless Z is one of the two scaling vector fields, in which case $$d_Z=2$$, and

\begin{aligned} Z( \rho (g))= \rho (Z(g))+c_Z \rho (g), \end{aligned}

where $$c_Z=0$$ unless Z is the spatial scaling vector field, in which case $$c_Z=3$$. Since $$\Delta \phi _g=\rho (g)$$, it follows that (31) implies (32).

In the next lines of computations, given $$Z \in \gamma$$ and Y the modified vector field corresponding to Z, we will use the schematic notations $$Y=Z-\varphi \partial _x$$ and $$Z=Y+\varphi \partial _x$$ instead of any of the lengthy formulae given at the beginning of Section 6.2, such as $$Y_i=t \partial _{x^i}+ \partial _{v^i}-\sum _{k=1}^n \Phi ^{k}_i \partial _{x^k}$$. We will also use the notation $$t \partial _{x}+ \partial _{v}-\varphi \partial _x$$ to denote a generic vector field among the $$Y_i$$, the letter $$Y'$$ to denote a generic modified vector field and the letter $$\varphi '$$ to denote a generic coefficient belonging to $${\mathscr {M}}$$.

We now compute, for any $$Z \in \gamma$$

\begin{aligned} \int _v Z(g)dv= & {} \int _v \left( Z+\varphi \partial _x-\varphi \partial _x \right) (g) dv \\= & {} \int _v Y(g)dv - \int _v \varphi \partial _x g dv \\= & {} \int _v Y(g)dv - \int _v \frac{\varphi }{t} \left( t \partial _x g+ \partial _v g-\varphi \partial _x g -\partial _v g +\varphi \partial _xg \right) dv\\= & {} \int _v Y(g) dv - \frac{1}{t} \int _v \varphi \left( Y'(g)+\varphi \partial _xg \right) dv + \int _v \frac{\varphi }{t} \partial _v g d v \end{aligned}

The first and second terms on the right-hand side of the last line have the correct forms. For the last term, we integrate by parts in v

\begin{aligned} -\int _v \frac{\varphi }{t} \partial _v g d v= & {} \frac{1}{t} \int _v \partial _v \varphi g d v \\= & {} \frac{1}{t} \int _v \left( t \partial _x+ \partial _v - \varphi ' \partial _x-t \partial _x + \varphi ' \partial _x\right) (\varphi ) g d v \\= & {} \frac{1}{t} \int _v \left( Y'+ \varphi ' \partial _x\right) (\varphi ) g d v -\int _v \partial _x (\varphi ) g dv, \end{aligned}

where now all terms are of the correct forms. This prove (31) when $$|\alpha |=1$$. We now assume that (31) is true for some $$\alpha$$. Let Z be a non-modified vector field. Using again that $$Z \rho ( Z^\alpha (g))= \rho ( ZZ^\alpha (g)) + c_Z \rho ( Z^\alpha (g))$$, we only need to prove that $$Z \rho ( Z^\alpha (g))$$ is of the correct form. Assume first that Z contains no t-derivativeFootnote 15, i.e. $$Z\ne \partial _t$$ and $$\displaystyle Z\ne t\partial _t +\sum _{i=1}^n x^i \partial _{x^i}$$. Using the induction hypothesis and writing $$Y=Z+\varphi \partial _x$$ to denote the associated modified vector field, we have

\begin{aligned} Z \rho ( Z^\alpha (g))= & {} Z \left( \sum _{j=1}^{|\alpha |} \sum _{d=1}^{|\alpha |+1} \sum _{|\beta | \le |\alpha | } \frac{1}{t^j} \rho \left( P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) \right) \right. \nonumber \\&\quad \left. +\,\sum _{d=1}^{|\alpha |}\sum _{|\beta | \le |\alpha | } \rho \left( Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right) \right) \nonumber \\= & {} \sum _{j=1}^{|\alpha |} \sum _{d=1}^{|\alpha |+1} \sum _{|\beta | \le |\alpha | } \frac{1}{t^j} \rho \left( Z \left[ P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g)\right] \right) \nonumber \\&\quad +\,\sum _{d=1}^{|\alpha |}\sum _{|\beta | \le |\alpha | } \rho \left( Z \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g)\right] \right) + c_Z \rho ( Z^\alpha (g)). \end{aligned}
(34)

If now Z contains t-derivatives, we would get extra terms in (34) which arise when $$\partial _t$$ hits the $$\frac{1}{t^j}$$ factors. Since these extra terms are all of the correct forms, we only need to analyse the terms on the right-hand side of (34).

The last term in (34) has already the right form. Next, replacing Z by $$Y+\varphi \partial _x$$ in the terms $$\rho \left( Z \left[ P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) \right] \right)$$, one easily see that they also have the desired form. For the terms $$\rho \left( Z\left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g)\right] \right)$$, we have

\begin{aligned} \rho \left( Z \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g)\right] \right)= & {} \rho \left( (Y+\varphi \partial _x ) \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \\= & {} \rho \left( Y \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) + \rho \left( \varphi \partial _x \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \end{aligned}

The first term on the right-hand side is easily seen to have the correct form. For the second term, we write $$\varphi \partial _x=\frac{\varphi }{t} \left( t \partial _x \,+\, \partial _v-\varphi ' \partial _x \, +\, \varphi ' \partial _x - \partial _v \right) = \frac{\varphi }{t} Y'- \frac{\varphi }{t} \partial _v + \frac{\varphi \varphi '}{t} \partial _x$$ so that

\begin{aligned} \rho \left( \varphi \partial _x \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right)= & {} \frac{1}{t}\rho \left( \left( \varphi Y'+\varphi \varphi ' \partial _x \right) \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \\&+\frac{1}{t} \rho \left( \partial _v \varphi \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \end{aligned}

using an integration by parts in v. The first term on the right-hand side has now the right-form. For the second term, we again write $$\partial _v \varphi = \left( t \partial _x + \partial _v -\varphi ' \partial _x \right) \varphi - t \partial _x \varphi + \varphi ' \partial _x \phi$$ so that

\begin{aligned} \frac{1}{t} \rho \left( \partial _v \varphi \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right)= & {} \frac{1}{t} \rho \left( Y'(\varphi ) \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \\&-\,\rho \left( \partial _x(\varphi ) \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \\&+\,\frac{1}{t} \rho \left( \varphi ' \partial _x(\varphi ) \left[ Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right] \right) \end{aligned}

where all terms now have the correct form. $$\square$$

Recall that we do not hope to have any good estimate on $$Y^{\alpha }(\varphi )$$ if $$|\alpha |=N$$, since its transport equation would then contain a source term of the form $$\nabla Z^\alpha Z \phi$$ and we only hope to have estimates for $$\nabla Z^\beta \phi$$ up to $$\beta =N$$. On the other hand, using directly the Poisson equation satisfied by $$Z^\alpha (\phi )$$, we will have good estimates on $$\partial _x \partial _x Z^\alpha (\phi )$$. To take advantage of that factFootnote 16, we will need later the following technical lemma, which improves upon Lemma 6.3 by describing the structure of the P multilinear forms a little further.

### Lemma 6.4

With the notations of Lemma 6.3, the multilinear forms $$P^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ and $$\tilde{P}^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ can be written as

\begin{aligned} P^{\alpha ,j}_{d\beta }(\bar{\varphi })= & {} P_1(\bar{\varphi })+\sum _{\varphi \in {\mathscr {M}}}\sum _{i=1}^n C_{i,\varphi } Y_{i} Y^{\rho _{i,\varphi }}(\varphi )+ \sum _{\varphi \in {\mathscr {M}}}\sum _{i=1}^n \mathscr {P}_{i \varphi }(\bar{\varphi }) \partial _{x^i} Y^{\eta _{i,\varphi ,\varphi '}}(\varphi ), \\ \tilde{P}^{\alpha ,j}_{d\beta }(\bar{\varphi })= & {} \tilde{P}_1(\bar{\varphi })+\sum _{\varphi \in {\mathscr {M}}}\sum _{i=1}^n \tilde{C}_{i,\varphi } Y_i Y^{\tilde{\rho }_{i,\varphi }}(\varphi )+ \sum _{\varphi \in {\mathscr {M}}}\sum _{i=1}^n \widetilde{\mathscr {P}}_{i\varphi }(\bar{\varphi }) \partial _{x^i} Y^{\tilde{\eta }_{i,\varphi ,\varphi ' }}(\varphi ) , \end{aligned}

where

1. 1.

$$P_1$$ and $$\tilde{P}_1$$ are multilinear forms of degree d and signature less than k satisfying $$k \le |\alpha |-1, k+|\beta | \le |\alpha |$$,

2. 2.

$$Y_i$$ are the modified uniform motions defined at the beginning of Section 6.2, i.e. $$Y_i=t \partial _{x^i}+ \partial _{v^i}-\sum _{k=1}^n \Phi ^{k}_i \partial _{x^k}$$,

3. 3.

$$|\rho _{i,\varphi }|=|\alpha |-1$$, $$\tilde{\rho }_{i,\varphi }=|\alpha |-1$$, $$|\eta _{i,\varphi ,\varphi '}| \le |\alpha |-1$$, $$|\tilde{\eta }_{i,\varphi ,\varphi '}| \le |\alpha |-1$$,

4. 4.

$$C_{i,\varphi }$$, $$\tilde{C}_{i, \varphi }$$ are constants and $$\mathscr {P}_{i\varphi }(\bar{\varphi })$$, $$\widetilde{\mathscr {P}}_{i\varphi }(\bar{\varphi })$$ are polynomial of degree at most $$|\alpha |$$ in the $$\varphi ' \in {\mathscr {M}}$$.

### Proof

This is an easy proof by induction. The case $$|\alpha |=1$$ has already been proven in the proof of the previous lemma. Assume that the statement of this lemma holds for some $$\alpha$$ and let $$Z \in \Gamma$$. As before, it is sufficient to consider only $$Z\left( \rho (Z^\alpha ) \right)$$. We will only be interested in the top order terms, that is to say terms containing $$Y^\eta (\varphi )$$ with $$\eta =|\alpha |+1$$. Note that they can only be generated by applying a vector field to terms containing $$Y^{\eta '}(\varphi )$$ with $$\eta '=|\alpha |$$.

Using the induction hypothesis, the top order terms coming from the P multilinear forms will give terms of the form

\begin{aligned} \sum _{\varphi \in {\mathscr {M}}}\sum _{i=1}^n C_{i,\varphi } Z \left[ Y_{i} Y^{\rho _{i,\varphi }}(\varphi ) \right] \end{aligned}
(35)

and

\begin{aligned} \sum _{\varphi , \varphi ' \in {\mathscr {M}}}\sum _{i=1}^n D_{i,\varphi ,\varphi '} Z\left[ \varphi ' \partial _{x^i} Y^{\eta _{i,\varphi ,\varphi '}}(\varphi )\right] . \end{aligned}
(36)

For the first type of terms, we have

\begin{aligned} Z \left[ Y_{i} Y^{\rho _{i,\varphi }}(\varphi ) \right] = (Y+ \varphi '' \partial _x) \left[ Y_{i} Y^{\rho _{i,\varphi }}(\varphi ) \right] = Y Y_{i} Y^{\rho _{i,\varphi }}(\varphi ) + \varphi '' \partial _x Y_{i} Y^{\rho _{i,\varphi }}(\varphi ). \end{aligned}

Now the second term on the right-hand side has the right structure. The first term also has the right structure, since $$[Y, Y_i]$$ can be written as a linear combinations of terms of the form $$\partial _x$$, the modified uniform motions $$Y_j$$ and $$\varphi '' \partial _x$$ and $$Y'(\varphi ) \partial _x$$.

The terms of the type (36) can be treated similarly, the only dangerous terms being of the form $$\varphi ' Y \partial _{x^i} Y^{\eta _{i,\varphi ,\varphi '}}(\varphi )$$, where the Y and $$\partial _{x^i}$$ can be commuted up to lower order terms.

The top order terms coming from the Q multi-linear forms will give terms of the form

\begin{aligned} \rho \left( Z [Y^{\eta } ( \partial _x \varphi ) Y^\beta (g)]\right)= & {} \rho \left( \left( Y+ \varphi '' \partial _x \right) \left[ Y^{\eta }(\partial _x \varphi ) Y^\beta (g)\right] \right) \\= & {} \rho \left( Y \left[ Y^{\eta }(\partial _x \varphi ) Y^\beta (g)\right] \right) + \rho \left( \varphi '' \partial _x \left[ Y^{\eta }(\partial _x \varphi ) Y^\beta (g)\right] \right) , \end{aligned}

where $$|\eta |=|\alpha |-1$$. Now the first term on the right-hand side will contribute only the Q forms so it can be ignored here. While the second term, repeating the argument of the previous lemma, gives the following contribution to the P forms

\begin{aligned} \frac{1}{t} \rho \left( Y(\varphi )'' Y^\eta (\partial _x \varphi ) Y^\beta (g)\right) \end{aligned}

which, since $$|\eta |\le |\alpha |-1$$ is not of top order and

\begin{aligned} \frac{1}{t} \rho \left( \varphi '' Y Y^\eta (\partial _x \varphi ) Y^\beta (g)\right) \end{aligned}

as well as

\begin{aligned} \frac{1}{t} \rho \left( \varphi ' \varphi '' \partial _x\left[ Y^\eta (\partial _x \varphi ) Y^\beta (g)\right] \right)= & {} \frac{1}{t} \rho \left( \varphi ' \varphi '' \partial _x\left[ Y^\eta (\partial _x \varphi )\right] Y^\beta (g)\right) \nonumber \\&\hbox {}+ \frac{1}{t} \rho \left( \varphi ' \varphi '' Y^\eta (\partial _x \varphi ) \partial _x\left[ Y^\beta (g)\right] \right) \end{aligned}
(37)

which are all of top order. Again, we use that $$\partial _x$$ essentially commutes with any modified vector field up to lower order terms, to put these last terms in the right form. $$\square$$

The following commutation property will also be useful later.

### Lemma 6.5

For any multi-index $$\alpha$$ and any $$1 \le i \le 3$$, we have

\begin{aligned}{}[\partial _{x^i}, Y^\alpha ]= \sum _{d=0}^{|\alpha |} \,\, \sum \limits _{\mathop {|\beta | \le |\alpha |-1,}\limits _{1 \le j \le 3}} P_{i,d\beta }^{\alpha ,j}(\partial _x \bar{\varphi }) Y^\beta \partial _{x^j}, \end{aligned}

where the $$P_{i,d\beta }^{\alpha ,j}(\partial _x \bar{\varphi })$$ are multilinear forms of degree d of the form (33) with a signature less than k such that $$k+|\beta | \le |\alpha |-1$$ .

### Proof

We prove the $$|\alpha |=1$$ case, the general case following by an easy induction argument. Let Y be modified vector field. We will write schematically $$Y=Z+\varphi \partial _x$$, where Z is a non-modified vector field and $$\varphi \partial _x$$ stands for a linear combination of products of some $$\varphi \in {\mathscr {M}}$$ and some $$\partial _{x^k}$$. For simplicity, assume that Z commutes with $$\partial _{x^i}$$ (the cases where Z do not commute with $$\partial _{x^i}$$ can be treated similarly, since the resulting error terms do not involve any terms depending on the coefficients in $${\mathscr {M}}$$.) An easy computation then shows that

\begin{aligned}{}[ \partial _{x^i}, Y]=[ \partial _{x^i}, \varphi \partial _x]= \partial _{x^i} (\varphi ) \partial _x, \end{aligned}

which is of the desired form. $$\square$$

Finally, let us also remark that

### Lemma 6.6

For any multi-index $$\alpha$$,

\begin{aligned} Y^\alpha \nabla \phi = Z^\alpha \nabla \phi +\frac{1}{t}\sum _{d=1}^{|\alpha |} P^\alpha _{d\beta } ( \bar{\varphi } ) Z^\beta \nabla \phi , \end{aligned}

where $$P^\alpha _{d\beta } ( \bar{\varphi } )$$ are multilinear forms of degree d and signature less than k such that $$k \le |\alpha |-1$$ and $$k+|\beta | \le |\alpha |$$.

### Proof

We only do the $$|\alpha |=1$$ case, the rest of the proof being an easy induction. Let $$Y'$$ be a modified vector field and write schematically $$Y'=Z'+\varphi \partial _x$$. We have

\begin{aligned} Y' \nabla \phi =\left( Z' +\varphi \partial _x\right) \nabla \phi =Z'\nabla \phi +\frac{\varphi }{t}[t\partial _x]\nabla \phi , \end{aligned}

which is of the correct form since $$t\partial _x \in \Gamma$$$$\square$$

### Bootstrap Assumptions and Beginning of the Proof

Let now f be a solution to the Vlasov-Poisson system in dimension $$n=3$$ such that the hypotheses of Theorem 4.1 are satisfied.

We consider the following bootstrap assumptions. Let $$T \ge 0$$ be the largest time so that, for all $$t \in [0,T]$$ and all $$x \in {\mathbb {R}}^3$$,

1. 1.
\begin{aligned} E_{N,\delta }[f(t)] \le 2 \epsilon , \end{aligned}
(38)
2. 2.

For all $$0 < \delta ' \le \delta$$, there exists a $$C_{\delta '} > 0$$ such that for all multi-index $$\alpha$$ with $$|\alpha | \le N$$,

\begin{aligned} ||\nabla ^2 Z^\alpha \phi (t) ||_{L^{1+\delta '}} \le C_{\delta '} \epsilon ^{1/2}. \end{aligned}
(39)
3. 3.

For all multi-index $$\alpha$$ with $$|\alpha | \le N-(9/2+1)$$,

\begin{aligned} | \nabla Z^\alpha \phi (t,x) | \lesssim \frac{\epsilon ^{1/2}}{1+t^2} \end{aligned}
(40)

and

\begin{aligned} | Y^\alpha \nabla \phi (t,x)| \lesssim \frac{\epsilon ^{1/2}}{1+t^2} \end{aligned}
(41)
4. 4.

For all multi-index $$\alpha$$ with $$|\alpha | \le N-(9/2+2)$$, we have for all $$\varphi \in {\mathscr {M}}$$,

\begin{aligned} \left| Y^\alpha (\varphi )(t,x,v) \right| \lesssim \epsilon ^{1/2} \left| 1+ \log (1+t) \right| , \end{aligned}
(42)
5. 5.

For all $$\varphi \in {\mathscr {M}}$$, all $$1 \le i \le 3$$ and all multi-index $$|\alpha | \le N-(9/2+3)$$ ,

\begin{aligned} \left| \partial _{x^i} Y^\alpha (\varphi )(t,x,v) \right| \lesssim \epsilon ^{1/2} , \end{aligned}
(43)

It follows from the initial data assumption and standard arguments that $$T>0$$. In the rest of the proof, we will try to improve each of the above assumptions, which would show that $$T=+\infty$$.

Note that in view of Lemma 6.5, (43) is equivalent to

\begin{aligned} \left| Y^\alpha \partial _{x^i} (\varphi )(t,x,v) \right| \lesssim \epsilon ^{1/2} \end{aligned}

and we will switch freely between the two in the rest of the article. Note moreover than in view of the Gagliardo-Nirenberg inequality, assumption (39) immediately implies that

\begin{aligned} || \nabla Z^\alpha \phi ||_{L^{q}} \le C_q\, \epsilon ^{1/2}, \end{aligned}
(44)

where $$q=3/2$$ satisfies $$q< \frac{3(1+\delta ')}{2-\delta '} < 2$$ in view of the definition of $$\delta$$. In particular, q can be taken as close to 3 / 2 as wanted.

Finally, the notation $$A \lesssim B$$ used in (40), (41), (42), (43) stand for $$A \le C_{N, \delta , n}B$$ where $$C_{N, \delta , n}$$ is a constant depending only on $$N,n,\delta$$ (with here $$n=3$$). We will eventually improve each of these inequalities by replacing the $$\epsilon ^{1/2}$$ on the right-hand sides of (40), (41), (42), (43) by $$\epsilon$$, choosing $$\epsilon$$ sufficiently small to absorb the $$C_{N, \delta , n}$$.

### Klainerman-Sobolev Inequalities with Modified Vector Fields

Using the bootstrap assumptions above, we have

### Proposition 6.1

For all multi-index $$|\alpha | \le N-3$$,

\begin{aligned} \rho \left( \left| Y^\alpha f(t) \right| \right)\lesssim & {} \frac{1}{\left( 1+t+|x| \right) ^3}\sum _{|\beta | \le |\alpha |+3} || Y^\beta f(t)||_{L^1({\mathbb {R}}^3_x \times {\mathbb {R}}^3_v)},\\\lesssim & {} \frac{1}{\left( 1+t+|x| \right) ^3}\sum _{|\beta | \le N} || Y^\beta f(t)||_{L^1({\mathbb {R}}^3_x \times {\mathbb {R}}^3_v)}. \end{aligned}

### Proof

Similarly to the proof of Proposition 3.3, let us fix $$(t,x) \in {\mathbb {R}} \times {\mathbb {R}}^3$$ and let $$\widetilde{\psi }$$ be defined by $$\widetilde{\psi }: B_{3}(0,1/2) \ni y \rightarrow \rho \left( \left| Y^\alpha f\right| \right) \left( t,x+(t+|x|)y \right) .$$ We fix $$\delta '=\frac{1}{12}$$ and apply a 1d Sobolev inequality

\begin{aligned} \rho (| Y^\alpha f| )(t,x) \lesssim \int _{|y_1| \le {\delta '}^{1/2}}\left( \left| \partial _{y_1} \widetilde{\psi } \right| + |\widetilde{\psi }| \right) (y_1,0,0) dy_1, \end{aligned}

where as before

\begin{aligned} \partial _{y_1}\widetilde{\psi }(y)= & {} (t+|x|) \partial _{x_1}\rho (| Y^\alpha f| )\left( t,x+(t+|x|)y \right) \\= & {} t \int _{v} \partial _{x_1}\left( | Y^\alpha f| \right) \left( t,x+(t+|x|)y,v \right) dv\\&\quad +\,|x|\int _{v} \partial _{x_1}\left( | Y^\alpha f|\left( t,x+(t+|x|)y,v \right) \right) dv . \end{aligned}

Now,

\begin{aligned} t \int _{v} \partial _{x_1}\left( | Y^\alpha f| \right) dv= & {} \int _{v}\left[ \left( t\partial _{x_1}+\partial _{v_1}-\sum _{i=1}^n \Phi _1^j \partial _{x^j} + \sum _{j=1}^n \Phi _1^j \partial _{x^j}\right) \left( | Y^\alpha f| \right) \right] dv \\= & {} \int _{v} Y_1 \left( | Y^\alpha f| \right) dv + \int _v \sum _{j=1}^n \Phi _1^j \partial _{x^j}\left( | Y^\alpha f| \right) dv. \end{aligned}

The first term on the right-hand side is simply estimated by

\begin{aligned} \left| \int _{v} Y_1 \left( | Y^\alpha f| \right) dv \right| \le \int _{v} | Y_1 Y^\alpha f| dv. \end{aligned}

For the second term, we again try to force the apparition of our modified vector fields

\begin{aligned} \int _v \Phi _1^j \partial _{x^j}\left( | Y^\alpha f| \right) dv= & {} \int _v \frac{\Phi _1^j}{t} \left( t \partial _{x^j}+ \partial _{v^j}- \sum _{k=1}^n \Phi ^k_j \partial _{x^k} \right) \left( | Y^\alpha f| \right) dv \\&\hbox {}- \int _v \frac{\Phi _1^j}{t}\left( \partial _{v^j}- \sum _{k=1}^n \Phi ^k_j \partial _{x^k} \right) \left( | Y^\alpha f| \right) dv \\= & {} \int _v \frac{\Phi _1^j}{t} Y_j \left( | Y^\alpha f| \right) dv \\&\hbox {}- \int _v \frac{\Phi _1^j}{t}\left( \partial _{v^j}- \sum _{k=1}^n \Phi ^k_j \partial _{x^k} \right) \left( | Y^\alpha f| \right) dv. \end{aligned}

The first term on the right-hand side can then be estimated as above, using that $$|\frac{\Phi _1^j}{t}|$$ is uniformly bounded from the bootstrap assumptions (42). For the remainder terms, we first note than in view of the bootstrap assumptions (42), the terms of the form

\begin{aligned} \int _v \frac{\Phi _1^j}{t}\Phi ^k_j \partial _{x^k} \left( | Y^\alpha f| \right) \end{aligned}

can be estimated by

\begin{aligned} \int _v \left| \partial _{x^k} \left( | Y^\alpha f| \right) \right| dv. \end{aligned}

For the last type of terms, we integrate by parts in v

\begin{aligned} \int _v \frac{\Phi _1^j}{t} \partial _{v^j} \left( | Y^\alpha f| \right) dv=-\int _v \frac{\partial _{v^j}\Phi _1^j}{t} \left( | Y^\alpha f| \right) dv. \end{aligned}

We now rewrite $$\partial _{v^j}\Phi _1^j$$ as

\begin{aligned} \partial _{v^j}\Phi _1^j= & {} \left( t \partial _{x^j} + \partial _{v^j}-\sum _{k=1}^n \Phi _j^k \partial _{x^k} \right) \Phi _1^j - \left( t \partial _{x^j}-\sum _{k=1}^n \Phi _j^k \partial _{x^k} \right) \Phi _1^j \\= & {} Y_j (\Phi _1^j)- \left( t \partial _{x^j}-\sum _{k=1}^n \Phi _j^k \partial _{x^k} \right) \Phi _1^j. \end{aligned}

The first term only grow like $$|1+ \log (1+ t)|$$ according to (42) and this growth can be absorbed thanks to the 1 / t factor. For the second term, using (43) and (42)

\begin{aligned} \left| t \partial _{x^j} (\Phi _1^j) \right| + \left| \Phi _j^k \partial _{x^k} ( \Phi _1^j) \right| \le \epsilon ^{1/2} t + \epsilon ^{1/2} |1+ \log (1+t)|, \end{aligned}

and again we can absorb the growth using the 1 / t factor.

Putting everything together we have obtained that

\begin{aligned}&\rho (| Y^\alpha (f)|)(t,x)\\&\quad \lesssim \int _{|y_1| \le {\delta '}^{1/2} } \int _v \left( |Y Y^\alpha (f) | + |Y^\alpha (f)| \right) \left( t,x+(t+|x|)(y_1,0,0) \right) dv dy_1. \end{aligned}

The remaining of the proof follows as in the proof of Proposition 3.3, repeating the previous arguments for each of the variables and applying the usual change of coordinates. $$\square$$

### Estimates on Products of Type $$Y^{\alpha }(\varphi ) Y^{\beta }(f)$$

Due to the form of the commutators of Section 6.2.2, we will need to estimate terms of the form $$Y^{\alpha }(\varphi ) Y^{\beta }(f)$$. When $$\alpha$$ is sufficiently small, we will have access to pointwise estimates on $$Y^{\alpha }(\varphi )$$ so there is no difficulty. When $$\alpha$$ is large, say $$\alpha =N$$, we have for the moment no estimate on $$Y^{\alpha }(\varphi )$$ and we can certainly not hope to prove pointwise estimates for these quantities, because, in view of the transport equations satisfied by the coefficients $$\varphi$$, these estimates would in turn require pointwise estimates on $$\nabla Y^\alpha (\phi )$$, and these estimates do not hold at the top order. Instead, we will prove directly estimates on the products $$Y^{\alpha }(\varphi ) Y^{\beta }(f)$$, taking advantage of the fact that $$Y^{\beta }(f)$$ are integrable in v. More precisely,

### Proposition 6.2

Let $$\sigma > 0$$. Then, there exists a $$C_{\sigma }> 0$$ such that for any multi-indices $$\alpha , \beta$$, $$|\alpha | \le N-1$$, $$|\beta | \le 9/2 +3$$ and any $$\varphi \in {\mathscr {M}}$$, we have for all $$t \in [0,T]$$ and all $$1 \le i \le 3$$,

\begin{aligned} || Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }\le & {} C_{\sigma } (1+t)^{\sigma } \epsilon , \\ ||Y_i Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }\le & {} C_{\sigma } (1+t)^{\sigma } \epsilon , \\ ||\partial _{x^i} Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }\le & {} C_{\sigma } (1+t)^{\sigma } \epsilon , \end{aligned}

### Proof

Let $$\sigma > 0$$ and let $$\alpha$$ be a multi-index satisfying $$|\alpha |\le N$$ and such that if $$|\alpha |=N$$ then $$Y^\alpha =Y_j Y^{\alpha '}$$ or $$Y^\alpha = \partial _{x^j} Y^{\alpha '}$$ with $$|\alpha '|=N-1$$.

We have

\begin{aligned} T_\phi \left( Y^{\alpha }(\varphi ) Y^{\beta }(f) \right) = T_\phi \left( Y^\alpha (\varphi ) \right) Y^\beta (f)+Y^\alpha (\varphi ) T_\phi \left( Y^{\beta }(f) \right) =I_1+I_2, \end{aligned}

where $$I_1= T_\phi \left( Y^\alpha (\varphi ) \right) Y^\beta (f)$$ and $$I_2=Y^\alpha (\varphi ) T_\phi \left( Y^{\beta }(f) \right)$$. In view of Lemma 2.9, it suffices to show that

\begin{aligned} ||I_1, I_2||_{L^1_{x,v}} \le C_\sigma (1+t)^{\sigma -1}. \end{aligned}
1. 1.

Estimates on $$I_1$$ We have

\begin{aligned} I_1= & {} [T_\phi , Y^\alpha ](\varphi ) Y^\beta (f)+ Y^{\alpha } [T_\phi ( \varphi )] Y^\beta (f) \\= & {} I_{1,1}+I_{1,2}, \end{aligned}

with $$I_{1,1}=[T_\phi , Y^\alpha ](\varphi ) Y^\beta (f)$$ and $$I_{1,2}=Y^{\alpha }[T_\phi ( \varphi )] Y^\beta (f)$$. For $$I_{1,1}$$, we use the commutation formula (30)

\begin{aligned} I_{1,1}=\sum _{d=0}^{|\alpha |+1}\sum _{i=1}^n \mathop {\mathop {\sum }\limits _{|\gamma | \le |\alpha |,}}\limits _{|\eta | \le |\alpha |} P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\eta (\varphi )Y^\beta (f) , \end{aligned}

where $$P^{\alpha ,i}_{d \gamma \eta }$$ satisfies the requirement of Lemma 6.2, in particular, it has signature less than k such that $$k\le |\alpha |-1$$ and $$k +|\gamma |+|\eta | \le |\alpha |+1$$. Case 1: $$|\gamma | \le N-\left( 9/2 +1 \right)$$. It then follows from the bootstrap assumption (40), that we have the pointwise estimate

\begin{aligned} \left| \partial _{x^i} Z^\gamma (\phi ) \right| \le \frac{\epsilon ^{1/2}}{1+t^2}. \end{aligned}

Moreover, since $$k + |\eta | \le |\alpha |+1 \le N+1$$, either $$k \le N-(9/2+2)$$, and we have access to the pointwise estimate

\begin{aligned} \left| P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi }) \right| \le \epsilon ^{d/2}\left( 1+ \log (1+t) \right) ^{d} \end{aligned}

or $$k > N-(9/2+2)$$. In this case, we have $$|\eta | \le N+1-k \le N-(9/2+2)$$, since $$N \ge 14$$, so that we now have access to pointwise estimates on $$Y^\eta (\varphi )$$. Note also that since $$k \le N+1$$, there is at most one factor in each of products of $$Y^{\rho _j}(\bar{\varphi })$$ in the decomposition of $$P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi })$$ for which we do not have access to pointwise estimates. In conclusion, it follows that we have an estimate of the form

\begin{aligned} \left| P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\eta (\varphi ) \right| \lesssim \epsilon ^{1/2} \frac{\left( 1+ \log (1+t) \right) ^d}{1+t^2} \sum _{|\rho | \le |\alpha |-1} |Y^\rho (\varphi )|. \end{aligned}

Case 2: $$\gamma > N-\left( 9/2 +1 \right)$$.

Then, $$k+|\eta | \le N+1-|\gamma | \le N-(9/2+2)$$ since $$N \ge 14$$ and we can bound $$P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi })$$ and $$Y^{\eta }(\varphi )$$ pointwise. Since $$|\beta | \le 9/2+3$$, we have access to pointwise bound on $$\rho (|Z^\beta (f)|)$$, so that we can estimate

\begin{aligned}&|| P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\eta (\varphi )Y^\beta (f) ||_{L^1_{x,v}} \lesssim \\&\quad \quad \quad \quad \quad \quad \quad \quad \quad \quad \epsilon ^{1/2}\left( 1+ \log (1+t) \right) ^{d+1} ||\partial _{x^i} Z^\gamma (\phi )||_{L^q_x} || \rho \left( |Y^\beta (f)| \right) ||_{L^p_x}, \end{aligned}

where $$1/q+1/p=1$$. Taking q as in (44) with $$\delta '$$ as small as needed (depending only on $$\sigma$$), we obtain, using the pointwise estimates of Proposition 6.1, that

\begin{aligned} || \rho \left( |Y^\beta (f)| \right) ||_{L^p_x} \lesssim C_\sigma \frac{\epsilon }{(1+t)^{2-\sigma }}, \end{aligned}

so that

\begin{aligned} || P^{\alpha ,i}_{d \gamma \eta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\eta (\varphi )Y^\beta (f) ||_{L^1_{x,v}} \lesssim \epsilon ^{2}\frac{\left( 1+ \log (1+t) \right) ^{d+1}}{(1+t)^{2-\sigma }}, \end{aligned}

which, assuming $$\sigma <1$$, is integrable in t. We now turn to the estimates on $$I_{1,2}$$. Recall that we have $$T_\phi (\varphi )=t \partial _{x^i} Z(\phi )$$ for some Z and some $$x^i$$, unless Z is the spatial scaling vector field, in which case $$T_\phi (\varphi )=t \partial _{x^i} \left( Z(\phi )-2\phi \right)$$. Since the extra term can be handled similarly, we will only treat the case of the non spatial scaling vector fields below. Applying Lemma 6.6, we have

\begin{aligned} Y^\alpha \left( T_\phi (\varphi ) \right)= & {} t Y^\alpha \partial _{x^i} Z(\phi ) \nonumber \\= & {} t Z^\alpha \partial _{x^i} Z(\phi ) +t \frac{1}{t}\sum _{d=1}^{|\alpha |} P^\alpha _{d\eta } ( \bar{\varphi } ) Z^\eta \partial _{x^i} Z(\phi ), \nonumber \\= & {} t Z^\alpha \partial _{x^i} Z(\phi ) +\sum _{d=1}^{|\alpha |} P^\alpha _{d\eta } ( \bar{\varphi } ) Z^\eta \partial _{x^i} Z(\phi ), \end{aligned}
(45)

where $$P^{\alpha }_{d \eta }(\bar{\varphi })$$ is a multi-linear form of degree d and signature less than k with $$k \le |\alpha |-1$$ and $$k+|\eta | \le |\alpha |$$. Assume first that $$|\alpha | \le N-1$$. For the first term on the right-hand side of (45), we have

\begin{aligned} |t Z^\alpha \partial _{x^i} Z(\phi )| \lesssim t \sum _{|\eta | \le |\alpha |} |\partial _{x^i} Z^\eta Z(\phi ) |. \end{aligned}

Since $$|\alpha | \le N-1$$, we have $$|\eta |+1 \le N$$ in the above sum. Thus, $$|t Z^\alpha \partial _{x^i} Z(\phi )| | Z^\beta (f) |$$ can be estimated as before using the Hölder inequality, pointwise estimates on $$\rho ( | Z^\beta (f) | )$$ and the estimate (44). If now $$|\alpha |=N$$, then by assumption, $$Y^\alpha = Y^jY^{\alpha '}$$ or $$Y^\alpha = \partial _{x^j}Y^{\alpha '}$$ with $$|\alpha '|=N-1$$, so that $$Z^\alpha =t \partial _{x^i} Z^{\alpha '}$$ or $$Z^\alpha = \partial _{x^i} Z^{\alpha '}$$. Thus,

\begin{aligned} |t Z^\alpha \partial _{x^i} Z(\phi )|\lesssim & {} t(1+t) \sum _{|\eta | \le N-1} |\partial _x \partial _{x^i} Z^\eta Z(\phi ) |, \\\lesssim & {} t(1+t) \sum _{|\eta | \le N} |\partial ^2_x Z^\eta (\phi ) |. \end{aligned}

We can now estimate $$|t Z^\alpha \partial _{x^i} Z(\phi )| \rho ( | Z^\beta (f) | )$$ using Hölder inequality with $$p=\frac{3}{3-\sigma }=1+\sigma '$$ with $$\sigma '=\frac{\sigma }{3-\sigma }> 0$$ assuming $$\sigma < 3$$ and $$q=\frac{3}{\sigma }$$. Recall that $$|| \partial ^2_x Z^\eta (\phi ) ||_{L^p}$$ is bounded thanks to the bootstrap assumption (39) provided $$\sigma$$ is sufficiently small. Moreover, using the pointwise estimate on $$\rho (| Z^\beta (f) | )$$, we have

\begin{aligned} || \rho (| Z^\beta (f) |) ||_{L^q({\mathbb {R}}^3_x)} \lesssim \epsilon (1+t)^{\sigma -3}. \end{aligned}

Whether $$|\alpha |\le N-1$$ or $$|\alpha |=N$$, the above estimates gives

\begin{aligned} \int _{x,v} |t Z^\alpha \nabla Z(\phi )|| Z^\beta (f) | dxdv\le C_\sigma \frac{ \epsilon ^{3/2}}{(1+t)^{1-\sigma }} \end{aligned}

which, after integration, gives rise to the $$t^\sigma$$ growth in the statement of the proposition. For the second term on the right-hand side of (45), we have either $$|\eta |+1 \le N-(9/2+1)$$, in which case, we have access to the pointwise estimate

\begin{aligned} |\partial _{x^i} Z^\eta Z(\phi ) | \lesssim \frac{\epsilon ^{1/2}}{(1+t)^2} \end{aligned}

and thus,

\begin{aligned} P^\alpha _{d\eta }(\bar{\varphi }) |\partial _{x^i} Z^\eta Z(\phi ) | Z^{\beta }(f)| \lesssim \frac{\epsilon ^{1/2}\left( 1+\log (1+t) \right) ^{d}}{(1+t)^2} \sum _{|\rho | \le N-1} |Y^\rho (\varphi )|| Z^{\beta }(f)|, \end{aligned}

where we have used the fact that there is at most one term in $$P^\alpha _{d\eta }(\bar{\varphi })$$ for which we do not have access to pointwise estimates, or we have $$|\eta |+1 > N-(9/2+1)$$, in which case $$k \le N-(9/2+2)$$ and we can bound pointwise $$P_{d \eta }(\bar{\varphi })$$ as

\begin{aligned} | P_{d \eta }(\bar{\varphi }) | \lesssim \left( 1+\log (1+t) \right) ^{d}. \end{aligned}

$$P^\alpha _{d\eta }(\bar{\varphi }) |\partial _{x^i} Z^\eta Z(\phi ) | Z^{\beta }(f)|$$ can then be estimated as before, using Hölder inequality, pointwise estimates on $$\rho ( | Z^\beta (f) | )$$ and the estimate (44).

2. 2.

Estimates on $$I_2$$. Using (30) again, we have

\begin{aligned} | I_2 | \lesssim \sum _{d=0}^{|\beta |+1}\sum _{i=1}^n \sum \limits _{\mathop {|\gamma | \le |\beta |,}\limits _{|\eta | \le |\beta |}} | P^{\beta ,i}_{d \gamma \eta }(\bar{\varphi }) | \, |\partial _{x^i} Z^\gamma (\phi )| \, |Y^\eta (f)| \, |Y^\alpha (\varphi )|, \end{aligned}

where $$P^{\beta ,i}_{d\gamma \eta }(\bar{\varphi })$$ are multilinear forms of degree d and signature $$k \le |\beta |-1$$ satisfying $$k+|\gamma |+|\eta | \le |\beta |+1$$. Since $$|\beta | \le 9/2+3$$, we have $$|\beta |-1 \le 9/2+2 \le N-(9/2+2)$$. Thus, using the bootstrap assumption (42), all the terms in the decomposition of each of the $$P^{\beta ,i}_{d\gamma \eta }(\bar{\varphi })$$ can be bounded pointwise. Thus, we have

\begin{aligned} | I_2 | \lesssim \left( 1+\log (1+t) \right) ^{|\beta |+1}\sum _{i=1}^n \sum _{\begin{array}{c} |\gamma | \le |\beta |,\\ |\eta | \le |\beta |, \\ |\gamma |+|\eta | \le |\beta |+1 \end{array}} |\partial _{x^i} Z^\gamma (\phi )| \, |Y^\eta (f)| \, |Y^\alpha (\varphi )|. \end{aligned}

Now since $$|\gamma | \le |\beta | \le 9/2 +3$$ in the above sum, we have $$|\gamma | \le N-(9/2+1)$$ since $$N \ge 14$$ and thus, we can bound $$|\partial _{x^i} Z^\gamma (\phi )|$$ pointwise using the bootstrap assumption (40). We have thus obtained

\begin{aligned} ||I_2(t)||_{L^1({\mathbb {R}}^n_v) \times L^2({\mathbb {R}}^n_x)} \lesssim \frac{\epsilon ^{1/2}}{(1+t)^{1+\delta '}}\sum _{|\eta | \le |\beta |}|| Y^{\alpha }(\varphi )(t) Y^{\eta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }, \end{aligned}

for some $$\delta '> 0$$.

3. 3.

Conclusions of the proof of the lemma: Let

\begin{aligned} F_1(t)= & {} \sum _{|\eta | \le |\beta |}\sum _{|\alpha | \le N-1}|| Y^{\alpha }(\varphi )(t) Y^{\eta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }, \\ F_2(t)= & {} \sum _{|\eta | \le |\beta |}\sum _{i=1}^3 \sum _{|\alpha | = N-1}||Y_iY^{\alpha }(\varphi )(t) Y^{\eta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }, \\ F_3(t)= & {} \sum _{|\eta | \le |\beta |}\sum _{i=1}^3 \sum _{|\alpha | = N-1}||\partial _{x^i} Y^{\alpha }(\varphi )(t) Y^{\eta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }, \\ F= & {} F_1+F_2+F_3. \end{aligned}

Combining all the ingredients above, We have obtained that, there exists some $$\delta '> 0$$ such that

\begin{aligned} F(t) \lesssim \int _{0}^t \frac{\epsilon ^{1/2}}{(1+s)^{1+\delta '}}F(s) ds + C_\sigma \epsilon ^{3/2} t^\sigma . \end{aligned}

Applying Gronwall inequality and using the smallness of the initial data then finishes the proof.

$$\square$$

Using (8), we have similarly

### Proposition 6.3

Let $$\sigma > 0$$. Then, there exists a $$C_{\sigma }> 0$$ such that for any multi-indices $$\alpha , \beta$$, $$|\alpha | \le N-1$$, $$|\beta | \le 9/2 +3$$ and any $$\varphi \in {\mathscr {M}}$$, we have for all $$t \in [0,T]$$, and all $$1 \le i \le 3$$,

\begin{aligned}&||(1+v^2)^{\frac{\delta (\delta +3)}{2(1+\delta )}} Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^{1+\delta } \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) } \le C_{\sigma } (1+t)^{\sigma } \epsilon ,\end{aligned}
(46)
\begin{aligned}&||(1+v^2)^{\frac{\delta (\delta +3)}{2(1+\delta )}} Y_i Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^{1+\delta } \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) } \le C_{\sigma } (1+t)^{\sigma } \epsilon ,\end{aligned}
(47)
\begin{aligned}&||(1+v^2)^{\frac{\delta (\delta +3)}{2(1+\delta )}} \partial _{x^i} Y^{\alpha }(\varphi )(t) Y^{\beta }(f)(t) ||_{L^{1+\delta } \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) } \le C_{\sigma } (1+t)^{\sigma } \epsilon . \end{aligned}
(48)

### Proof

The proof is almost identical to the proof of the previous proposition and therefore left to the reader. $$\square$$

Finally, we can remove the small growth provided we consider a product of the form $$Y^\alpha \partial _x (\varphi )Y^\beta (f)$$.

### Proposition 6.4

For any multi-indices $$\alpha , \beta$$, $$|\alpha | \le N-1$$, $$|\beta | \le 9/2 +3$$ and any $$\varphi \in {\mathscr {M}}$$, we have for all $$t \in [0,T]$$ and all $$1 \le j \le 3$$,

\begin{aligned} || Y^{\alpha }(\partial _{x^j}\varphi )(t) Y^{\beta }(f)(t) ||_{L^1 \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) }\lesssim & {} \epsilon ,\\ \end{aligned}

as well as

\begin{aligned} ||(1+v^2)^{\frac{\delta (\delta +3)}{2(1+\delta )}} Y^{\alpha }(\partial _{x^j}\varphi )(t) Y^{\beta }(f)(t) ||_{L^{1+\delta } \left( {\mathbb {R}}_x \times {\mathbb {R}}_v \right) } \lesssim \epsilon . \end{aligned}

### Proof

First note that the previous arguments used in the proof of Proposition 6.2 still apply and that we may only focus on the terms leading to the $$t^\sigma$$ growth in the proof of Proposition 6.2, which were contained in the error term $$I_{1,2}$$. More precisely, the term leading to the $$t^\sigma$$ growth is the first one on the right-hand side of (45), i.e. the term $$t Z^\alpha \partial _{x^i} Z(\phi )$$. In our case, this term should be replaced by

\begin{aligned} t Z^\alpha \partial _{x^i} \partial _{x^j}Z(\phi ), \end{aligned}

with $$|\alpha | \le N-1$$. Commuting the $$\partial _{x}$$ and $$Z^\alpha$$, we have

\begin{aligned} |t Z^\alpha \partial _{x^i} \partial _{x^j}Z(\phi )| \le t \sum _{|\eta | \le N} |\partial _x^2 Z^\eta \phi |. \end{aligned}

We can then repeat the previous arguments (i.e. use Hölder inequality and the bootstrap assumption (39)), except that we have gained a 1 / t factor. This gain now means that the resulting error will decay like $$1/t^{2-\sigma }$$, which is integrable in t and therefore does not lead to any growth. The $$L^{1+\delta }_{x,v}$$ weighted estimates can be treated similarly. $$\square$$

### Improving the Bootstrap Assumptions

We are now in a position to improve each of the bootstrap assumptions.

#### Improving the Estimates on $$Z^\alpha (\phi )$$

Similarly to Lemma 5.2, we can improve assumption (39) to

### Lemma 6.7

For all $$0 < \delta ' \le \delta$$, there exists a $$C_{\delta '} > 0$$ such that for all multi-index $$\alpha$$ with $$|\alpha | \le N$$,

\begin{aligned} ||\nabla ^2 Z^\alpha \phi (t) ||_{L^{1+\delta '}} \le C_{\delta '} \epsilon . \end{aligned}
(49)

Applying the Gagliardo-Nirenberg inequality, we deduce that for all $$t\in [0,T]$$,

\begin{aligned} ||\nabla Z^\alpha \phi (t) ||_{L^q({\mathbb {R}}^n)} \lesssim \epsilon , \end{aligned}

for all $$3/2< q < \frac{3(1+\delta )}{2-\delta }$$.

### Proof

Using the commuted equation (32) for $$Z^\alpha \phi$$, we have

\begin{aligned} || \Delta Z^\alpha (\phi )||_{L^{1+\delta '}} \lesssim J_1 +J_2 \end{aligned}

where

\begin{aligned} J_1=\sum _{j=1}^{|\alpha |} \sum _{d=1}^{|\alpha |+1} \sum _{|\beta | \le |\alpha | } \frac{1}{t^j} || \rho \left( P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) \right) ||_{L^{1+\delta '}}, \end{aligned}

where the $$P^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ are multilinear forms of degree d and signature less than k satisfying

\begin{aligned} k \le |\alpha |, \quad k+|\beta | \le |\alpha |, \end{aligned}

and, in view of Lemma 6.4, such that when $$|\alpha |=N$$ the only top order terms in $$P^{\alpha ,j}_{d\beta }(\bar{\varphi })$$ are of the form $$Y_i Y^\beta (\varphi )$$ or $$\partial _{x^i} Y^\beta (\varphi )$$ with $$|\beta |=N-1$$, so that we can apply Propositions 6.2 and 6.3,

and where

\begin{aligned} J_2= \sum _{d=0}^{|\alpha |}\sum _{|\beta | \le |\alpha | } || \rho \left( Q^{\alpha }_{d\beta }(\partial _x \bar{\varphi }) Y^\beta (g) \right) ||_{L^{1+\delta '}}, \end{aligned}

where the $$Q^{\alpha }_{d\beta }(\partial _x\bar{\varphi })$$ are multilinear forms of degree d of the form (33) and signature less than $$k'$$ satisfying

\begin{aligned} k' \le |\alpha |-1, \quad k'+|\beta | \le |\alpha |. \end{aligned}

Following the strategy of the proof of Lemma 5.2, we see that it is sufficient to prove $$L^p_x$$ bounds on $$\rho (J_1)$$ and $$\rho (J_2)$$. With this in mind, recall that, for $$i=1,2$$,

\begin{aligned} ||\rho (J_i) ||_{L^p_x}=\left| \left| \int _v J_i dv\right| \right| _{L^p_x} \lesssim \left( \int _{v} \chi (v)^{-1} dv \right) ^{1/q} \left| \left| \chi (v)^{1/q} J_i \right| \right| _{L^p_{x,v}}, \end{aligned}

for any weight function $$\chi (v)$$. Choosing $$\chi (v)$$, p and q as in the proof of 5.2, we only need to prove the v-weighted $$L^p_{x,v}$$ bounds for $$J_1$$ and $$J_2$$.

1. 1.

Estimates on $$J_1$$. Since $$k \le |\alpha |$$, there can be at most one term in the decomposition of each of the $$P^{\alpha ,j}_{d\beta }$$ for which we do not have access to pointwise estimates. Thus, we have

\begin{aligned} | P^{\alpha ,j}_{d\beta }(\bar{\varphi }) Y^\beta (g) | \le (1+(\log (1+t))^{d-1} \sum _{|\eta |+|\beta | \le |\alpha |}\sum _{\varphi \in \gamma _m} |Y^{\eta }(\varphi )| \, |Y^\beta (g) |. \end{aligned}

Now in the above sum, either $$|\eta | > N-(9/2+2)$$, in which case $$|\beta | \le 9/2+3$$ and we apply the product estimates of Proposition 6.3, or $$|\eta | \le N-(9/2+2)$$, in which case we can still estimate $$|Y^{\eta }(\varphi )|$$ pointwise. In this case, we use the v-weighted bounds on $$Y^\beta (f)$$ contained in the norm $$E_N$$, see (20). In both case, we can absorb the t-growth thanks to the t weights in the definition of $$J_1$$.

2. 2.

Estimates on $$J_2$$. These are obtained similarly, using Proposition 6.4 instead of 6.3, since there is no t weight in $$J_2$$ to absorb any t growth.$$\square$$

The preceding lemma improves the bootstrap assumption (39).

Similarly to Lemma 5.3 and Corollary 5.2, the pointwise estimates on $$\rho \left( |Y^\beta (f)| \right)$$ can be transformed into pointwise estimates for $$\nabla Z^\alpha \phi$$.

### Lemma 6.8

For all multi-index $$\alpha$$ such that $$|\alpha | \le N-3$$

\begin{aligned} ||\nabla Z^\alpha \phi ||_{L^2({\mathbb {R}}^n)} \lesssim \frac{\epsilon }{t^{1/2}}, \end{aligned}

and for any multi-index $$|\alpha | \le N-(9/2+1)$$ and $$Z^\alpha \in \Gamma _{s}^{|\alpha |}$$, we have for all $$t \in [0,T],$$

\begin{aligned} \left| \nabla Z^\alpha \phi \right| \lesssim \frac{\epsilon }{(1+|x|+t)^{3/2}t^{1/2}}. \end{aligned}
(50)

### Proof

We use again the commutation formula (32). Apart from the top order terms, we can estimate all the quantities on the right-hand side using the pointwise estimates (42) on $$Y^\rho (\varphi )$$ for $$|\rho | \le N-(9/2+2)$$, (43) on $$Y^\rho (\partial \varphi )$$ for $$|\rho | \le N-(9/2+3)$$ and Proposition 6.1. Once we have access to pointwise estimates, we can just follow the strategy of the proof of 5.3. Thus, the only difficult term are those containing top order terms in $$Y^\rho (\varphi )$$. Those coming from the P multilinear forms are of the type

\begin{aligned} \frac{1}{t} \rho \left( Y^\rho (\varphi ) f \right) \end{aligned}

with $$|\rho |$$ the largest integer such that $$|\rho | \le N-(9/2+1)$$, i.e. $$|\rho |=N-6$$. Now, since $$|\rho | \le N-6$$, we can consider $$Y^\beta (Y^\rho (\varphi ) f)$$ for $$|\beta | \le 3$$. Thus, we may apply Proposition 6.1 directly to the product $$Y^\rho (\varphi ) f$$ and we find

\begin{aligned} \left| \frac{1}{t} \rho \left( Y^\rho (\varphi ) f \right) \right| \lesssim \frac{\epsilon }{ t^{1-\sigma }\left( 1+t+|x|\right) ^3}, \end{aligned}

where we have used Proposition 6.2 to bound the norms appearing on the right-hand side after applications of Proposition 6.1. Choosing $$\sigma < 1$$, these terms therefore decay better than what is needed for the statement of the Lemma.

The top order terms coming from the Q forms are of type

\begin{aligned} \rho \left( Y^\rho (\partial _{x^i} \varphi ) f \right) , \end{aligned}

with $$|\rho | \le N-(9/2+2)$$, i.e. $$|\rho | \le N-5$$. We can then proceed similarly. Since we have no extra t decay in front of the Q forms, it is important not to lose any t decay here and thus we use the improvements of Proposition 6.4. The rest of the proof is identical to that of Lemma 5.3 and therefore omitted. $$\square$$

The preceeding lemma improves (40). To improve (41) is then suffices to use Lemma 6.6 as well as the pointwise bounds on $$Y^{\alpha }(\varphi )$$ (42). Thus, it remains only to improve (38), (42) and (43).

We have

### Lemma 6.9

For all $$t \in [0,T]$$,

\begin{aligned} E_{N,\delta }[f(t)] \le 3/2 \epsilon , \end{aligned}

which improves (38).

### Proof

Using the commutation formula (30), we have

\begin{aligned}{}[T_\phi ,Y^\alpha ](f)= \sum _{d=0}^{|\alpha |+1}\sum _{i=1}^n \sum _{\begin{array}{c} |\gamma | \le |\alpha |,\\ |\beta | \le |\alpha | \end{array}} P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\beta (f), \end{aligned}

where the $$P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi })$$ are multilinear forms of degree d and signature less than k such that $$k \le |\alpha |-1 \le N-1$$ and $$k+|\gamma |+|\beta | \le |\alpha |+1 \le N+1$$. When $$k \le N- (9/2+2)$$, we can bound $$P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi })$$ by a polynomial power of $$1+\log (1+t)$$ using the bootstrap assumption (42). The product $$\partial _{x^i} Z^\gamma (\phi ) Y^\beta (f)$$ can be treated as in Section 5.3.1, either $$|\gamma | \le N-(9/2+1)$$ and we can apply (50) to bound $$|\partial _{x^i} Z^\gamma (\phi )|$$ or $$|\beta | \le N-3$$ in which case, we use Hölder inequality first and then Lemma 6.7 to estimate $$||\nabla Z^\gamma (\phi )||_{L^q_x}$$ and the pointwise estimate on $$\rho \left( \left| Y^\beta (f)\right| \right)$$ to estimate $$|| \rho \left( \left| Y^\beta (f)\right| \right) ||_{L^p_x}$$.

Otherwise $$k > N- (9/2+2)$$ and thus $$|\beta | \le 9/2+3$$ and we can use the estimates on products of Proposition 6.2. As in Section 5.3, it follows that all terms are integrable in $$L^1\left( {\mathbb {R}}_t; L^1( {\mathbb {R}}^n_x \times {\mathbb {R}}_v^n )\right)$$ and the lemma follows from Lemma 2.9$$\square$$

#### Improving the Pointwise Bounds on $$Y^\alpha (\varphi )$$ and $$Y^\alpha (\partial _{x^i} \varphi )$$

Finally, we conclude the proof of the 3d case by improving (42) and (43).

### Lemma 6.10

For all $$\varphi \in {\mathscr {M}}$$ and for all $$t \in [0,T]$$,

1. 1.

for all multi-index $$\alpha$$ with $$|\alpha |\le N-(9/2+2)$$,

\begin{aligned} \left| Y^\alpha ( \varphi )\right| \lesssim \epsilon \left( 1+\log (1+t) \right) , \end{aligned}
(51)
2. 2.

for all multi-index $$\alpha$$ with $$|\alpha |\le N-(9/2+3)$$ and all $$1 \le i \le n$$,

\begin{aligned} \left| Y^\alpha (\partial _{x^i} \varphi )\right| \lesssim \epsilon . \end{aligned}
(52)

### Proof

Using the commutation formula (30), we have

\begin{aligned}{}[T_\phi ,Y^\alpha ](\varphi )= \sum _{d=0}^{|\alpha |+1}\sum _{i=1}^n \sum _{\begin{array}{c} |\gamma | \le |\alpha |,\\ |\beta | \le |\alpha | \end{array}} P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi }) \partial _{x^i} Z^\gamma (\phi ) Y^\beta (\varphi ), \end{aligned}

where the $$P^{\alpha ,i}_{d \gamma \beta }(\bar{\varphi })$$ are multilinear forms of degree d and signature less than k such that $$k \le |\alpha |-1 \le N-1$$ and $$k+|\gamma |+|\beta | \le |\alpha |+1 \le N+1$$. Given the range of the indices, we can estimates all terms on the right-hand side pointwise and find that

\begin{aligned} \left| [T_\phi ,Y^\alpha ](\varphi ) \right| \lesssim \frac{\left( 1+\log (1+t) \right) ^{|\alpha |+2} \epsilon }{t^2}, \end{aligned}

which is integrable in t. On the other hand, we have $$Y^\alpha T_\phi (\varphi )=Y^\alpha t \nabla Z(\phi ).$$ Using Lemma 6.6, it follows that

\begin{aligned} Y^\alpha T_\phi (\varphi )=t Z^\alpha \nabla Z \phi +\sum _{d=1}^{|\alpha |} P^\alpha _{d\beta } ( \bar{\varphi } ) Z^\beta \nabla Z \phi , \end{aligned}

where the second term is integrable in t, while the first term satisfied only the weak bound, for all

\begin{aligned} | t Z^\alpha \nabla Z \phi | \lesssim \frac{\epsilon }{1+t}. \end{aligned}

Since any solution to $$T_\phi (g)=h$$ with 0 initial data satisfies, for all $$t > 0$$, and for all $$x,v \in {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v$$,

\begin{aligned} |g|(t,x,v) \lesssim \int _0^t \sup _{(x',v')\in {\mathbb {R}}^n_x \times {\mathbb {R}}^n_v} |h(s,x,v)|ds, \end{aligned}

(51) follows. (52) can be obtained similarly, using that

\begin{aligned} | t Z^\alpha \nabla Z \partial _{x^i} \phi | \lesssim \frac{\epsilon }{t^2}. \end{aligned}

since $$\partial _{x^i} \phi = \frac{1}{t} \left( t \partial _{x^i} \right) (\phi )$$ with $$t \partial _{x^i} \in \Gamma$$$$\square$$

## Some Open Problems

We end this paper with a description of some open problems, where the methods developed in this paper could find further applications.

### Small Data Solutions of the Einstein-Vlasov and Vlasov-Maxwell Systems

One of our original motivations for the present work came from the so-called Einstein-Vlasov system, which is the general relativistic generalization of the (gravitational) Vlasov-Poisson system. We refer to the recent bookFootnote 17 [27] for a thorough introduction to this system. The small data theory around the Minkowski space is still incomplete for the Einstein-Vlasov system. The spherically symmetric cases in dimension $$(3+1)$$ have been treated in [25, 26] for the massive case and in [4] for the massless case with compactly supported initial data. A proof of stability for the massless case without spherical symmetry but with compact support in both x and v has recently been obtained in [31]. As in [4], the compact support assumptions and the fact that the particles are massless are important as they allow to reduce the proof to that of the vacuum case outside from a strip going to null infinity. Interestingly, the argument in [31] is quite geometric, relying for instance on the double null foliation, in the spirit of [13], as well as several structures associated with the tangent bundle of the tangent bundle of the base manifold. The case of massive particles introduces however several extra difficulties, some of them already present in the case of the Einstein-massive scalar field system, for which a small data global existence result was only obtained very recently [14, 32].

An important open problem is thus to prove the stability of the Minkowski space for the Einstein-Vlasov system with massive particles. We believe that vector field type methods are well suited to address this problem. For instance, obtaining improved decay for derivatives, which is typically crucial for quasilinear wave equations, follows easily from vector fields type arguments, as highlighted by the present article. To this end, a vector field approach for relativistic kinetic equations has already been developed in [7].

A similar (easier) open problem would be to obtain sharp asymptotics (in particular optimal decay of derivatives) for the Vlasov-Maxwell system, which the current small data results [8, 29] do not provide.

### Stability of Stationary Solutions and Multiplier Estimates

While there are now satisfying results concerning the question of orbital stability of stationary solutions (see for instance [9, 15]), there are still very few results describing the precise asymptotic behaviour near orbitally stable stationary solutions, even in symmetric cases. A first step in this direction is to prove quantitative decay estimates for the linear problem. In the case of quasilinear wave equations with a non-trivial background geometry, the standard approach is based on multiplier estimates (in the style of Morawetz [19]). For solutions f to the classical free transport equation, one can easily derive a multiplier estimate of the form

\begin{aligned} \int _{{\mathbb {R}}_t} \int _{{\mathbb {R}}^3_x \times {\mathbb {R}}^3_v} f(t,x,v) \frac{|v|^2}{r^{1+\epsilon }} dv dx dt \lesssim \int _{{\mathbb {R}}_x^3 \times {\mathbb {R}}^3_v} f(0,x,v) dxdv. \end{aligned}

This leads to a natural question: does there exist a multiplier estimate approach to the question of linear and non-linear stability of stationary solutions to the Vlasov-Poisson equation?

### The 2-d Vlasov-Poisson and Vlasov-Yukawa Systems

If we try to repeat the analysis of this paper in dimension 2, several extra difficulties arise. The most important oneFootnote 18 is due to the slow time decay of the force field: for f a regular solution to the free transport operator (with $$(x,v) \in {\mathbb {R}}^2_x \times {\mathbb {R}}^2_v$$) and $$\phi$$ solution to $$\Delta \phi = \rho (f)$$, one only has in general $$| \nabla \phi | \lesssim 1/t$$. Since this decay rate is not integrable, the best one can hope using the methods of this paper is a proof of almost global existence, i.e. a control of the solution for times of size $$\exp \left( \frac{1}{\epsilon ^p} \right)$$, for some $$p > 0$$ and data of size $$\epsilon > 0$$. On the other hand, the methods of this paper should extend naturally to the Yukawa caseFootnote 19, in which the Poisson equation is replaced by

\begin{aligned} (\Delta - 1) \phi = \rho (f), \end{aligned}

as the extra $$L^2$$ control on $$\phi$$ gives stronger than integrable decay for $$\nabla \phi$$ even in the 2d case.

## Notes

1. 1.

A third ingredient not needed in the present case is that of modulation theory, see for instance [15] for an application of modulation theory in the context of the Vlasov-Poisson system.

2. 2.

In case of perbutations around a non-flat solution with metric g, the operator $$\square$$ would naturally be replaced by $$\square _g$$, the wave operator of the metric g.

3. 3.

More recently, a mix of microlocal and vector field methods have also been successfully developed, in particular to handle complex geometries involving trapped trajectories, see for instance [6] for an application of these tools.

4. 4.

See Section 4.1 for a precise definition of the norms. The $$\delta$$ encodes some additional integrability properties of the solutions.

5. 5.

Under some mild conditions on the initial data, global existence is already guaranteed from the works [18, 24], so the main points of the theorem, apart from providing an illustration of our new method, are the propagation of the global bounds and the optimal space and time decay estimates for the solutions.

6. 6.

See for instance [10] for some stability results using the linearization approach in the case of the spherically-symmetric King model.

7. 7.

Recall that these vector fields are the generators of the Gallilean transformations of the form $$x \in {\mathbb {R}}^n \rightarrow x+tv_i$$, where $$v_i^k=\delta _i^k$$.

8. 8.

Instead of simply considering v weights, we could also consider generalized moments, in particular adding as weights functions of $$v^i$$ and $$x^i -v^i t$$. This can be used for instance to obtain improved decay estimates in spatially bounded regions. Those will however not be needed for the present applications.

9. 9.

For instance, one can assume that $$\phi$$ is a smooth function on $$[0,T] \times {\mathbb {R}}^n_x$$ with compact support in x.

10. 10.

For instance, assume first that f has compact support in (xv) with a uniform bound on the support of f in (xv) for $$t \in [0,T]$$. For all $$\epsilon > 0$$, consider the function $$f_\epsilon =\sqrt{\epsilon ^2+f^2}\chi (x,v)$$, where $$\chi (x,v)$$ is a smooth cut-off function which is 1 on the support of f and vanishes for large x and v. Apply then the previous estimates to $$f_\epsilon$$ and take the limit $$\epsilon \rightarrow 0$$. A standard density argument deals with the case of non-compact support.

11. 11.

Recall that, while the general $$W^{k,p}({\mathbb {R}}^n) \hookrightarrow L^\infty ({\mathbb {R}}^n)$$ embedding requires $$k > \frac{n}{p}$$, the special case $$p=1$$ only needs $$k \ge n$$.

12. 12.

In that case, the decay estimates are worse near the cone $$t=|x|$$, as for the wave equation, see again [7].

13. 13.

Note that however, quantities such as $$\rho \left( \left| \partial _{x} f \right| \right)$$ do not typically enjoy any additional decay.

14. 14.

Once again, in all the formulae of this section, we assume that $$\phi$$ is a sufficiently regular function of (tx) defined on $$[0,T] \times {\mathbb {R}}^3$$ and we will eventually control the regularity of $$\phi$$ through a bootstrap argument.

15. 15.

Recall also that commuting with the vector fields containing t-derivatives is not necessary to prove Theorem 4.1 and is only useful if one wants to obtain improved decay of t-derivatives.

16. 16.

Note that these difficulties arise only at the top order $$|\alpha |=N$$. An alternative to the approach taken here would be to allow for the top order estimates to grow slightly in t.

17. 17.

Apart from a general introduction to the Einstein-Vlasov system, the main purpose of this book is to present a proof of stability of certain exponentially expanding spacetimes for the Einstein-Vlasov system, see [27].

18. 18.

Another difficulty comes from the slow radial decay of the solutions to the Poisson equation which forbids the use of norms such as $$||\nabla \phi ||_{L^2}$$ for the potential. This can however be solved by using other $$L^p$$ norms.

19. 19.

See [2] for an analysis of the small data theory based on the approach originally developed in [11].

## References

1. 1.

Bardos, C., Degond, P.: Global existence for the Vlasov-Poisson equation in 3 space variables with small initial data. Ann. Inst. H. Poincaré Anal. Non Linéaire 2(2), 101–118 (1985)

2. 2.

Choi, S.-H., Ha, S.-Y., Lee, H.: Dispersion estimates for the two-dimensional Vlasov-Yukawa system with small data. J. Differ. Equ. 250(1), 515–550 (2011)

3. 3.

Christodoulou, D., Klainerman, S.: The Global Nonlinear Stability of the Minkowski Space, vol. 41 of Princeton Mathematical Series. Princeton University Press, Princeton (1993)

4. 4.

Dafermos, M.: A note on the collapse of small data self-gravitating massless collisionless matter. J. Hyperbolic Differ. Equ. 3(4), 589–598 (2006)

5. 5.

Dafermos, M., Rodnianski, I.: A new physical-space approach to decay for the wave equation with applications to black hole spacetimes. In: XVIth International Congress on Mathematical Physics, pp. 421-432. World Scientific Publishing, Hackensack (2010)

6. 6.

Dafermos, M., Rodnianski, I., Shlapentokh-Rothman, Y.: Decay for solutions of the wave equation on kerr exterior spacetimes. iii: The full subextremal case. arXiv:1402.7034 (2014)

7. 7.

Fajman, D., Joudioux, J., Smulevici, J.: A vector field method for relativistic transport equations with applications. arXiv:1510.04939 (2015)

8. 8.

Glassey, R.T., Strauss, W.A.: Absence of shocks in an initially dilute collisionless plasma. Commun. Math. Phys. 113(2), 191–208 (1987)

9. 9.

Guo, Y., Lin, Z.: Unstable and stable galaxy models. Commun. Math. Phys. 279(3), 789–813 (2008)

10. 10.

Guo, Y., Rein, G.: A non-variational approach to nonlinear stability in stellar dynamics applied to the King model. Commun. Math. Phys. 271(2), 489–509 (2007)

11. 11.

Hwang, H., Rendall, A., Velázquez, J.: Optimal gradient estimates and asymptotic behaviour for the Vlasov-Poisson system with small initial data. Arch. Ration. Mech. Anal. 200(1), 313–360 (2011)

12. 12.

Klainerman, S.: Uniform decay estimates and the Lorentz invariance of the classical wave equation. Commun. Pure Appl. Math. 38(3), 321–332 (1985)

13. 13.

Klainerman, S., Nicolò, F.: The Evolution Problem in General Relativity, vol. 25 of Progress in Mathematical Physics. Birkhäuser Boston Inc., Boston (2003)

14. 14.

LeFloch, P., Ma, Y.: The global nonlinear stability of minkowski space for self-gravitating massive fields. arXiv:1511.03324 (2015)

15. 15.

Lemou, M., Méhats, F., Raphaël, P.: Orbital stability of spherical galactic models. Invent. Math. 187(1), 145–194 (2012)

16. 16.

Lieb, E.H., Loss, M.: Analysis, 2nd edn, vol. 14 of Graduate Studies in Mathematics. American Mathematical Society, Providence (2001)

17. 17.

Lindblad, H., Rodnianski, I.: The global stability of Minkowski space-time in harmonic gauge. Ann. Math. 171(3), 1401–1477 (2010)

18. 18.

Lions, P.-L., Perthame, B.: Propagation of moments and regularity for the 3-dimensional Vlasov-Poisson system. Invent. Math. 105(2), 415–430 (1991)

19. 19.

Morawetz, C.S.: The decay of solutions of the exterior initial-boundary value problem for the wave equation. Commun. Pure Appl. Math. 14, 561–568 (1961)

20. 20.

Morawetz, C.S.: The limiting amplitude principle. Commun. Pure Appl. Math. 15, 349–361 (1962)

21. 21.

Morawetz, C.S.: Time decay for the nonlinear Klein-Gordon equations. Proc. R. Soc. Ser. A 306, 291–296 (1968)

22. 22.

Mouhot, C.: Stabilité orbitale pour le système de Vlasov-Poisson gravitationnel (d’après Lemou-Méhats-Raphaël, Guo, Lin, Rein et al.). Astérisque, 352 (2013), Exp. No. 1044, vii, 35–82. Séminaire Bourbaki. Vol. 2011/2012. Exposés 1043–1058

23. 23.

Mouhot, C., Villani, C.: On Landau damping. Acta Math. 207(1), 29–201 (2011)

24. 24.

Pfaffelmoser, K.: Global classical solutions of the Vlasov-Poisson system in three dimensions for general initial data. J. Differ. Equ. 95(2), 281–303 (1992)

25. 25.

Rein, G., Rendall, A.D.: Global existence of classical solutions to the Vlasov-Poisson system in a three-dimensional, cosmological setting. Arch. Ration. Mech. Anal. 126(2), 183–201 (1994)

26. 26.

Rein, G., Rendall, A.D.: Erratum: Global existence of solutions of the spherically symmetric Vlasov-Einstein system with small initial data” [Commun. Math. Phys. 150 (1992), no. 3, 561–583; MR1204320 (94c:83028)]. Commun. Math. Phys. 176(2), 475–478 (1996)

27. 27.

Ringström, H.: On the Topology and Future Stability of the Universe. Oxford Mathematical Monographs. Oxford University Press, Oxford (2013)

28. 28.

Sarbach, O., Zannias, T.: Tangent bundle formulation of a charged gas. In: American Institute of Physics Conference Series (January 2014), vol. 1577 of American Institute of Physics Conference Series, pp. 192–207. arXiv:1311.3532 (2014)

29. 29.

Schaeffer, J.: A small data theorem for collisionless plasma that includes high velocity particles. Indiana Univ. Math. J. 53(1), 1–34 (2004)

30. 30.

Sogge, C.D.: Lectures on Nonlinear Wave Equations. II. Monographs in Analysis. International Press, Boston (1995)

31. 31.

Taylor, M.: The global nonlinear stability of the Minkowski space for the massless Einstein-Vlasov system. arXiv:1602.02611 (2016)

32. 32.

Wang, J., Wang, Q.: Global existence for the einstein equations with massive scalar fields. Talk Given at the Conference General Relativity: A Celebration of the 100th Anniversary, Institut Henri Poincaré, Nov 2011. (2015)

## Acknowledgments

This project was motivated by my joint work with David Fajman and Jérémie Joudioux on relativistic transport equations. I would like to thank both of them, as well as Christophe Pallard and Frédéric Rousset for many interesting discussions on these topics. I would also like to thank Pierre Raphaël for an extremely stimulating conversation which took place during the conference “Asymptotic analysis of dispersive partial differential equations” held in October 2014 at Pienza, Italy. Some of this research was done during this conference. Finally, I would like to acknowledge partial funding from the Agence Nationale de la Recherche ANR-12-BS01-012-01 (AARG) and ANR SIMI-1-003-01.

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Smulevici, J. Small Data Solutions of the Vlasov-Poisson System and the Vector Field Method. Ann. PDE 2, 11 (2016). https://doi.org/10.1007/s40818-016-0016-2