Abstract
This article is concerned with analytic Hamiltonian dynamical systems in infinite dimension in a neighborhood of an elliptic fixed point. Given a quadratic Hamiltonian, we consider the set of its analytic higher order perturbations. We first define the subset of elements which are formally symplectically conjugated to a (formal) Birkhoff normal form. We prove that if the quadratic Hamiltonian satisfies a Diophantine-like condition and if such a perturbation is formally symplectically conjugated to the quadratic Hamiltonian, then it is also analytically symplectically conjugated to it. Of course what is an analytic symplectic change of variables depends strongly on the choice of the phase space. Here we work on periodic functions with Gevrey regularity.
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Notes
If we fix any point \(\omega _0\in \mathbb {R}^\mathbb {Z}\), then the set of Diophantine frequencies \(\omega \) such that \(|\omega -\omega ^{(0)}|_\infty <1/2\) is again typical.
A vector \(\omega \in \mathbb {R}^n\) is called diophantine when it is badly approximated by rationals, i.e. it satisfies, for some \(\gamma ,\tau >0\), \({\left| k\cdot \omega \right| } \ge \gamma {\left| k\right| }^{-\tau },\quad \forall k\in \mathbb {Z}^n\setminus {\left\{ 0\right\} }\,\).
We recall that given a complex Hilbert space H with a Hermitian product \((\cdot ,\cdot )\), its realification is a real symplectic Hilbert space with scalar product and symplectic form given by
$$\begin{aligned} \langle u,v\rangle = 2\mathrm{Re}(u,v)\,,\quad \omega (u,v)= 2\mathrm{Im}(u,v)\,. \end{aligned}$$for example if \(\chi = 15/14\) the sup on the left hand side is smaller than \(-0,2\).
A given \(h>1\) appears \({{ {\alpha }}_h + { {\beta }}_h + { {\alpha }}_{-h} + { {\beta }}_{-h}}\) times in the list \(\widehat{n}\). Thus in order to get the summand \( h {\left( { {\alpha }}_h - { {\beta }}_h - { {\alpha }}_{-h} + { {\beta }}_{-h}\right) }\) we assign to the \(\widehat{n}_l\) with \(\widehat{n}_l=h\) the sign \({\sigma }_l=+ \), \({\alpha }_h+{\beta }_{-h}\) times and the sign \({\sigma }_l=- \), \({\alpha }_{-h}+{\beta }_{h}\) times. Let us now consider the case \(h=1\). By construction, 1 appears \({{ {\alpha }}^{(1)}+ { {\beta }}^{(1)}+ { {\alpha }}_{-1} + { {\beta }}_{-1}+ {\alpha }_0 +{\beta }_0}\) times in \(\widehat{n}\). Thus in order to obtain the summand \( {\left( { {\alpha }}^{(1)}- { {\beta }}^{(1)}- { {\alpha }}_{-1} + { {\beta }}_{-1}\right) }\) we assign to the \(\widehat{n}_l\) with \(\widehat{n}_l=1\) the sign \({\sigma }_l=+ \), \({\alpha }_1+{\beta }_{-1}\) times, the sign \({\sigma }_l=- \), \({\alpha }_{-1}+{\beta }_{1}\) times and \({\sigma }_l=0\) the remaining \({\alpha }_0 +{\beta }_0\) times.
recalling that the \(x_\ell >0\) and that \( 1+(2^\theta -1)k - (k+1)^\theta \ge 0\), with \(k= n+2>1\).
Namely the solution of the equation \(\partial _t \Phi (u,t)=X(\Phi (u,t))\) with initial datum \(\Phi (u,0)=u.\)
Using that for \(x,y\ge 0\) and \(0\le c\le 1\) we get \((x+y)^c\le x^c+y^c.\)
Using that \(\ln (1+y)\le 1+\ln y\) for every \(y\ge 1.\)
Using that, for every fixed \(0<{\mathfrak C} \le 1,\) we have \({\mathfrak C} x\ge \ln x\) for every \(x\ge \frac{2}{{\mathfrak C}}\ln \frac{1}{{\mathfrak C}} .\)
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Communicated by C.Liverani.
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Appendix A. Technical Lemmata
Appendix A. Technical Lemmata
In the following, we adapt material from [BMP18] to non mass conservation situation. There are no new conceptual difficulties w.r.to [BMP18] but the proofs require a bit more care and some further case analysis. For the readers convenience, we have written also the proofs of a couple of technical lemmata from [BMP18] on which we rely.
1.1 Proof of Lemmata 3.5 and 3.6
We follow here [BMP18] [Appendix B. Proof of lemma 3.1]. For any \(H\in {{\mathcal {H}}}_{r,s}\) (we recall that this space depends on two extra parameters \(p\ge \frac{1}{2}\) and \(0<\theta \le 1\)) we define a map
by setting
where \(e_j\) is the j-th basis vector in \({\mathbb N}^\mathbb {Z}\), while the coefficient
For brevity, we set
The vector field \(Y_H\) is a majorant analytic function on \(\ell ^2\) which has the same norm as H. Since the majorant analytic functions on a given space have a natural ordering this gives us a natural criterion for immersions, as formalized in the following Lemma.
Lemma A.1
Let \(r,{r^*}>0,\,s,s'\ge 0.\) The following properties hold.
-
(1)
The norm of H can be expressed as
$$\begin{aligned} {\left\| H\right\| }_{r,s}= \sup _{|y|_{\ell ^2}\le 1}{\left| Y_H(y;r,s)\right| }_{\ell ^2} \end{aligned}$$(34) -
(2)
Given \( H^{(1)}\in {{\mathcal {H}}}_{{r^*},s'}\) and \(H^{(2)}\in {{\mathcal {H}}}_{r,s}\,, \)
such that for all \({ {\alpha }},{ {\beta }}\in {\mathbb N}^\mathbb {Z}_f\) and \(j\in \mathbb {Z}\) with \({ {\alpha }}_j+{ {\beta }}_j\ne 0\) one has
$$\begin{aligned} |H^{(1)}_{{ {\alpha }},{ {\beta }}}| c^{(j)}_{{r^*},s'}({ {\alpha }},{ {\beta }}) \le c |H^{(2)}_{{ {\alpha }},{ {\beta }}}| c^{(j)}_{r,s}({ {\alpha }},{ {\beta }}), \end{aligned}$$for some \(c>0,\) then
$$\begin{aligned} {\left\| H^{(1)}\right\| }_{{r^*},s'} \le c {\left\| H^{(2)}\right\| }_{r,s}\,. \end{aligned}$$
Proof of Lemma 3.5
Recalling (33), we have
Since \(|{ {\alpha }}|+|{ {\beta }}|-2\ge {\mathtt {d}}\), the inequality follows by Lemma A.1 with \(H^{(1)}=H^{(2)}\) and \(s=s'\). \(\square \)
In order to prove Lemma 3.6 we need some notations and results proven in [Bou05] and [CLSY].
Definition A.2
Given a vector \(v={\left( v_i\right) }_{i\in \mathbb {Z}}\in {\mathbb N}^\mathbb {Z}_f\) with \(|v|\ge 2\) we denote by \(\widehat{n}=\widehat{n}(v)\) the vector \({\left( \widehat{n}_l\right) }_{l\in I}\) (where \(I\subset {\mathbb N}\) is finite) which is the decreasing rearrangement of
Remark A.3
A good way of envisioning this list is as follows. Given an infinite set of variables \({\left( x_i\right) }_{i\in \mathbb {Z}}\) and a vector \(v={\left( v_i\right) }_{i\in \mathbb {Z}}\in {\mathbb N}^\mathbb {Z}_f\) consider the monomial \(x^v:= \prod _i x_i^{v_i}\). We can write
then \(\widehat{n}(v)\) is the decreasing rearrangement of the list \({\left( \langle j_1 \rangle ,\dots ,\langle j_{|v|} \rangle \right) }\).
Example A.4
Let us set
Hence, 1 is repeated 6 times, 3 is repeated 1 time, and 4 is repeated 2 times :
Given \({ {\alpha }},{ {\beta }}\in {\mathbb N}^\mathbb {Z}_f\) with \( |{ {\alpha }}|+|{ {\beta }}|\ge 2\) from now on we define
which is the cardinality of \(\widehat{n}.\) We observe that, \(N\ge 2\) and since
there exists a choice of \({\sigma }_i = \pm 1, 0\) such thatFootnote 5
with \(\sigma _l \ne 0\) if \(\widehat{n}_l \ne 1\). Hence,
Indeed, if \(\sigma _1 = \pm 1\), the inequality follows directly from (36); if \(\sigma _1 = 0\), then \(\widehat{n}_1=1\) and consequently \(\widehat{n}_l = 1\, \forall l\). Since \(|{\alpha }|+|{\beta }|\ge 2\), the list \(\widehat{n}\) has at least two elements, so the inequality is achieved.
Lemma A.5
Given \({ {\alpha }},{ {\beta }}\) such that \(\sum _i i ({ {\alpha }}_i-{ {\beta }}_i)=0\), and \(|{\alpha }|+|{\beta }|\ge 2\), we have that setting \(\widehat{n}=\widehat{n}({ {\alpha }}+{ {\beta }})\)
Proof
The lemma above was proved in [Bou05] for \(\theta =\frac{1}{2}\) and for general \(0<\theta <1\) in [CLSY][Lemma 2.1], in the case of zero mass and momentum. Below we give a proof, using only momentum conservation.
We start by noticing that if \(|{\alpha }|+|{\beta }|= 2\) then \(\widehat{n}\) has cardinality equal to two and (38) becomes \(\widehat{n}_1+\widehat{n}_2 \ge 2\widehat{n}_1\). Now, by (37), momentum conservation implies that \(\widehat{n}_1=\widehat{n}_2\) and hence (38).
If \(|{\alpha }|+|{\beta }|\ge 3\) we write
since the cardinality of \(\widehat{n}\) is at least three we may write
Now setting, for \(x_i\ge 1\), \(i=2,\ldots , N\),
Hence, we have \(\partial _{x_2} f\ge 0\) for \(x_2\ge x_3\ge 1\). Then
Now we set
so that \(f(x_2,\dots ,x_N)\ge f_3(x_3,\dots ,x_N)\). Assume inductively that for some \(3\le n<N\), one has \(f(x_2,\dots ,x_N)\ge f_3(x_3,\dots ,x_N) \ge \dots \ge f_{n}(x_n,\dots ,x_N)\). By direct computationFootnote 6
so that the minimum is attained in \(x_n= x_{n+1}\) and \(f(x_2,\dots ,x_N) \ge f_{n+1}(x_{n+1},\dots ,x_N)\). In conclusion
where the last inequality follows by recalling that \( 1+(2^\theta -1)k - (k+1)^\theta \ge 0\) for \(k\ge 1\).
\(\square \)
The Lemma proved above, is fundamental in discussing the properties of \({{\mathcal {H}}}_{r}({\mathtt {h}}_{p,s,a})\) with \(s>0\), indeed it implies
for all \({ {\alpha }},{ {\beta }}\) such that \({ {\alpha }}_j+{ {\beta }}_j\ne 0\). Indeed, this follows from the fact that \(\langle j \rangle \le \widehat{n}_1\).
Proof of Lemma 3.6
In all that follows we shall use systematically the fact that our Hamiltonians are momentum preserving, are zero at the origin and have no linear term so that \({\left| { {\alpha }}\right| } +{\left| { {\beta }}\right| } \ge 2\).
We need to show that
The first identity comes form (33), while the last inequality follows by (39) of Lemma A.5\(\square \)
1.2 Proof of Lemma 3.7
This is a rather classical result, the proof we give is taken from [BMP18], where it is stated under the extra hypothesis of mass conservation, which is not used in the proof.
Lemma A.6
Let \(0<r_1<r.\) Let E be a Banach space endowed with the norm \(|\cdot |_E\). Let \(X:B_r \rightarrow E\) a vector field satisfying
Then the flow \(\Phi (u,t)\) of the vector fieldFootnote 7 is well defined for every
and \(u\in B_{r_1}\) with estimate
Proof of Lemma 3.7
The estimate for the Poisson bracket is proven in [BBP13]. In order to prove the other estimates we use Lemma A.6, with \(E\rightarrow {\mathtt {h}}_{s}\), \(X\rightarrow X_S\), \(\delta _0\rightarrow (r+\rho ) |S|_{r+\rho },\) \(r\rightarrow r+\rho ,\) \(r_1\rightarrow r,\) \(T\rightarrow 8e.\) finally we do not write the dependence on s which is fixed.
Then the fact that the time 1-Hamiltonian flow \(\Phi ^1_S: B_r({\mathtt {h}}_{s}) \rightarrow B_{r + \rho }({\mathtt {h}}_{s})\) is well defined, analytic, symplectic follows, since
Regarding the estimate (22), again by Lemma A.6 (choosing \(t=1\)), we get
Estimates (23), (24), (25) directly follow by (26) with \(h=0,1,2,\) respectively and \(c_k=1/k!\), recalling that by Lie series
where \( H^{(i)} := \mathrm{ad}_S^i (H)= \mathrm{ad}_S ( H^{(i-1)}) \), \( H^{(0)}:=H \).
Let us prove (26). Fix \(k\in {\mathbb N},\) \(k>0\) and set
Note that, by the immersion properties of the norm in Lemma 3.5,
Noting that
by using k times (20) we have
Then, using \( k^k\le e^k k!, \) we get
Finally, if S and H satisfy momentum conservation so does each \( \mathrm{ad}_S^k H \), \( k \ge 1 \), hence \( H \circ \Phi ^1_S \) too. \(\square \)
1.3 Proof of lemma 3.8
Here we strongly use the fact that \(\omega _j \sim j^2\). As we said in the introduction, it would not be hard to modify the proof in order to deal with \(\omega _j\sim j^\alpha \) with \(\alpha >1\), by adapting the proof of Lemmata A.9–A.10.
By Lemma A.1 (2), we have
where
Therefore proving (27) amounts to showing that
We divide in two cases regarding whether the inequality
holds or not. We remark that
indeed denoting \(\omega _j = j^2 + \xi _j \) with \({\left| \xi _j\right| }\le \frac{1}{2}\),
Of course if \({\left| \omega \cdot {\left( { {\alpha }}-{ {\beta }}\right) }\right| }\ge 1\), by (39) and (40) we get
and the bound (43) is trivially achieved.
Otherwise, to deal with the case in which (44) holds, we need some notation. Given \(u\in \mathbb {Z}^\mathbb {Z}_f\), consider the set
where \(D(u)<\infty \) is its cardinality. Define the vector \(m=m(u)\) as the reordering of the elements of the set above such that \(|m_1|\ge |m_2|\ge \dots \ge |m_D|\ge 1.\)
Given \({ {\alpha }}\ne { {\beta }}\in {\mathbb N}^\mathbb {Z}_f\) with \(|{ {\alpha }}|+|{ {\beta }}|\ge 3\) we consider \(m=m({ {\alpha }}-{ {\beta }})\) and \(\widehat{n}=\widehat{n}({ {\alpha }}+{ {\beta }}).\) If we denote by D the cardinality of m and N the one of \(\widehat{n}\) we have
and
Example A.7
Let set \(v={\alpha }+\beta \) and \(u={\alpha }-\beta \) with
Therefore, we have \(D(u)+\alpha _0+\beta _0=8\le 13=N({\hat{n}}(v))\). Hence, (46) holds.
Furthermore, \((6,4, 3, 3, 2, 2, 1,1,1,1,1,1,1)\le {\hat{n}}(v)\), that is (47).
Lemma A.8
(Lemma C.3 of [BMP18]). Assume that g defined on \(\mathbb {Z}\) is non negative, even and not decreasing on \({\mathbb N}.\) Then, if \({ {\alpha }}\ne { {\beta }}\),
Proof
By definition of \(m({\alpha }-{\beta })\) and setting \( {\sigma }_l= \mathrm{sign}({ {\alpha }}_{m_l}-{ {\beta }}_{m_l})\,, \) we have
Hence
and (48) follows by (46) and (47). \(\square \)
By (49)
and
Analogously
Finally note that
Lemma A.9
Given \({ {\alpha }}\ne { {\beta }}\in {\mathbb N}^\mathbb {Z}_f,\) such that \(\pi ({ {\alpha }}-{ {\beta }})=0\), \(N\ge 3,D\ge 1 \) and satisfying (44), we have
Proof
The case \(D=1\) is not compatible with momentum conservation. Let us now consider the case \(D=2\), i.e.
If \({\sigma }_1{\sigma }_2=-1\), momentum conservation imposes \(m_1=m_2\) but this contradicts (53). In the case \({\sigma }_1{\sigma }_2=1,\) by momentum conservation we have \(m_1= -m_2\). Then conditions (44) and (52) imply that
since \(\widehat{n}_l\ge 1\).
Let us now consider the case \(D \ge 3\). By (44), (51) and (52)
since (recall \(N\ge 3\)) \( 2 N\le 6(N-2) \le 6\sum _{l=3}^N \widehat{n}_l^2\).
If \(\sigma _1\sigma _2 = 1\) then
If \({\sigma }_1{\sigma }_2 = -1\)
Now, if \({\left| m_1\right| }\ne {\left| m_2\right| }\) then
Conversely, if \({\left| m_1\right| } = {\left| m_2\right| }\), by (53), \(m_1\ne m_2\), hence \(m_1 = - m_2\). By substituting this relation into (50), we have
concluding the proof. \(\square \)
Lemma A.10
Consider \({ {\alpha }},{ {\beta }}\in {{\mathcal {M}}}\) with \({\alpha }\ne {\beta }\) and \( |{\alpha }|+|{\beta }| \ge 3\). If (44) holds then
for all j such that \({ {\alpha }}_j+{ {\beta }}_j\ne 0\) one has
Proof
Let us first consider the case \(D=0\), this means that \({\alpha }-{\beta }= ({\alpha }_0-{\beta }_0)\mathbf{e}_0\) and the left hand side of (55) reads \( |{\alpha }_0-{\beta }_0|\). By (39) and \(N\ge 3\) the right hand side of (55) is at least \(2-2^\theta \), so if \(|{\alpha }_0-{\beta }_0| \le 7 \) the result is trivial. Otherwise we have two cases, if \(j=0\)
Otherwise we remark that if \(j\ne 0\), \({\alpha }_j+{\beta }_j\ne 0\) and \({\alpha }_j-{\beta }_j=0\), then \({\alpha }_j+{\beta }_j \ge 2\), then
Now we consider indices \({\alpha },{\beta }\) such that \(N\ge 3,D\ge 1 \). Here we apply Lemma A.9 Given \({ {\alpha }},{ {\beta }}\in {\mathbb N}^\mathbb {Z}_f,\) as above we consider \(m=m({ {\alpha }}-{ {\beta }})\) and \(\widehat{n}=\widehat{n}({ {\alpha }}+{ {\beta }}).\)
We haveFootnote 8
Then by Lemma A.5 and (56) we get
proving (55). \(\square \)
Conclusion of the proof of Lemma 3.8 By applying Lemma A.10, since \(\omega \in {\mathtt {D}_\gamma }\) we get:
where, for \(0<{\sigma }\le 1\), \(i\in \mathbb {Z}\) and \(x\ge 0\), we defined
\(\square \)
Finally, we have
Lemma A.11
(Lemma 7.2 of [BMP18]) Setting
we get
for every \(\ell \in \mathbb {Z}^\mathbb {Z}_f\).
Proof
First of all we note that
since \(f_i(0)=0.\) We have thatFootnote 9
Now,
where
since the maximum is achieved for \(x=1\) if \(\langle i \rangle \ge i_0\) and \(x=\frac{2C_* }{{\sigma }\langle i \rangle ^{\theta /2}}\) if \(\langle i \rangle < i_0\). Note that \(i_0\ge e.\) Then we get
We immediately have that
Moreover, in the case \(\langle i \rangle \ge i_0\ge e,\)
where
We have thatFootnote 10
Note that
Therefore
In conclusion we get
\(\square \)
The inequality (27) follows from plugging (58) into (57) and evaluating the constant. \(\square \)
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Procesi, M., Stolovitch, L. About Linearization of Infinite-Dimensional Hamiltonian Systems. Commun. Math. Phys. 394, 39–72 (2022). https://doi.org/10.1007/s00220-022-04398-7
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DOI: https://doi.org/10.1007/s00220-022-04398-7