Abstract
We consider the second-order elliptic operator
\(a>0\), \(b,\ c \in \mathbb {R}\) and we prove gradient estimates for the heat kernel.
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Appendix
Appendix
1.1 Radial and Angular Derivatives
In this section, we study further properties about the spherical harmonics and the Laplace–Beltrami operator \(\Delta _0\) on the sphere. For \(x\in \mathbb {R}^N\), we use spherical coordinates to write \(x=r\omega \), where \(r:=|x|\), \(\omega :=\frac{x}{|x|}\in S^{N-1}\). For every \(u\in C^2(\mathbb {R}^n)\), we denote by \(D_r u\), \(D_{rr} u\) the radial derivatives of u and by \(\nabla _{\tau }u\) the tangential component of its gradient. They are defined through the formulas
We recall that in spherical coordinates, we have the following relation between the Laplace operator and \(\Delta _0\):
The operator \(A:=rD_r\) is the Euler operator \(\sum _{i=1}^nx_iD_i\) and, for a given function u, the Euler’s theorem implies that u is \(\alpha \)-homogeneous if and only if \(Au=\alpha u\).
For \(i,j=1,\dots ,N\) we introduce, moreover, the angular operators \(S_{ij}\) defined as
They are first-order differential operators and have a central role in the analysis on the sphere since they allow to decompose the Laplace–Beltrami operator into a sum of second-order angular derivatives. Obviously, \(S_{ii}=0\) and \(S_{ij}=-S_{ji}\) so it is sufficient to consider \(S_{ij}\) for \(i<j\).
We collect in the next proposition some basic properties about the angular derivatives \(S_{ij}\).
Proposition 4.1
Denote by \(\left[ A,B\right] =AB-BA\) the commutator of A, B and by \(\delta _i^j\) the Kronecker delta. The following properties hold.
- (i)
For every \(i<j\) and \(h<k\) we have
$$\begin{aligned} \left[ S_{ij},S_{hk}\right] =-\delta _i^hS_{jk}+\delta _i^kS_{jh}+\delta _j^hS_{ik}-\delta _j^kS_{ih}. \end{aligned}$$In particular, \(S_{ij}\) and \( S_{hk}\) commute if and only if \((i,j)=(h,k)\) or \(\left\{ i,j\right\} \cap \left\{ h,k\right\} =\emptyset \).
- (ii)
For every radial function \(u=u(r)\), with \(u\in C^2(\mathbb {R}^N)\) and for every \(v\in C^2(\mathbb {R}^N)\) , we have \(S_{ij}u=0\) and \(S_{ij}(uv)=u S_{ij}v\).
- (iii)
For every radial differential operator \(E=\sum _{k=0}^n a_k(r)\frac{d^k}{dr^k}\), we have \(S_{ij}E=ES_{ij}\).
- (iv)
\(\Delta \,S_{ij}=S_{ij}\,\Delta \) and \(\Delta _0\,S_{ij}=S_{ij}\,\Delta _0\).
Proof
(i) easily follows by a straightforward computation.
Let \(u,v\in C^2(\mathbb {R}^N)\) with \(u=u(r)\); we have \(S_{ij}u=x_iu'(r)\frac{x_j}{r}-x_ju'(r)\frac{x_i}{r}=0\). Moreover, \(S_{ij}(uv)=uS_{ij}v+(S_{ij}u)v=uS_{ij}v\) that proves (ii).
To prove (iii), we observe that for \(E=a(r)D_r\) we have, using (ii),
On the other hand,
Comparing the last expressions, we have \(S_{ij}E=ES_{ij}\); the general case follows easily by induction.
Finally, to prove (iv), let us suppose, without losing generality, \(i=1,\,j=2\). We have
and so, \(S_{12}\) commutes with \(\Delta \).
Using property (ii), we have also
Since \(r^2\Delta =r^2D_{rr}+(N-1)rD_r+\Delta _0\), it follows immediately from property (iii) and the fact that \(S_{12}\) commutes with \(r^2\Delta \), that \(\Delta _0\,S_{ij}=S_{ij}\,\Delta _0\).
\(\square \)
Before stating the main results, it is worth noting that every function \(f\in C^2(S^{N-1})\) is extendible on a neighbourhood of \(S^{N-1}\) preserving the same degree of regularity; therefore, in what follows, we can always suppose f defined on an open set of \(\mathbb {R}^N\) containing \(S^{N-1}\). In particular, \(\nabla f\), \(\Delta f\) and \(S_{ij}f\) are well defined. For instance, if we define \(\tilde{f}\) on \(\mathbb {R}^N{\setminus }\{0\}\) by \(\tilde{f}(y):=f(\frac{y}{|y|})\), being \(\tilde{f}\) constant along every radial direction, it follows immediately by the decomposition of \(\nabla \) and \(\Delta \) that
Let now \(\omega \in S^{N-1}\) and \(v\in T_\omega (S^{N-1})\); the tangential derivative of f in \(\omega \) in the direction v is given by
Setting \(\omega =(\omega _1,\ldots ,\omega _N)\in S^{N-1}\), let us define for \(i<j\)
i.e. the vector which has \(-\omega _j\) and \(\omega _i\) as, respectively, the ith and the jth components and zeros in the other entries. \(\left( \omega _{ij}\right) _{1\le i<j\le N}\) is, by construction, a system of generators of \(T_\omega (S^{N-1})\).
The next propositions clarify the role and the interaction among the operators introduced so far. We begin by a geometric Lemma.
Lemma 4.2
Let \(\omega \in S^{N-1}\) and \(x,y\in \omega ^\perp \). Then
Proof
Since \((\omega _{ij},x)=\omega _ix_j-\omega _jx_i,\; (\omega _{ij},y)=\omega _iy_j-\omega _jy_i\), we have
Adding and subtracting, in the last formula, the term \(\sum _{i=1}^N\omega _i^2x_iy_i\), we obtain
Choosing \(x=y\), we get \(\sum _{i<j}|(x,\omega _{ij})|^2=|x|^2\). \(\square \)
Proposition 4.3
Let f, g be \(C^1\) functions defined on a neighbourhood of \(S^{N-1}\). The following properties hold.
- (i)
\(S_{ij}f(\omega )\) is the tangential derivative of f in \(\omega \) in the direction \(\omega _{ij}\), i.e.
$$\begin{aligned} S_{ij}f(\omega )= (\nabla f(\omega ),\omega _{ij})=(\nabla _\tau f(\omega ),\omega _{ij}). \end{aligned}$$ - (ii)
The jth component of \(\nabla _{\tau } f\) satisfies
$$\begin{aligned} (\nabla _{\tau } f(\omega ))_j=\sum _{i\ne j}\omega _i \,S_{ij}f(\omega ),\quad \omega \in S^{N-1}. \end{aligned}$$ - (iii)
For every \(\omega \in S^{N-1}\)
$$\begin{aligned} (\nabla _{\tau } f(\omega ),\nabla _{\tau } g(\omega ))=\sum _{i<j}S_{ij}f(\omega )S_{ij}g(\omega ),\quad |\nabla _{\tau } f(\omega )|^2=\sum _{i<j}|S_{ij}f(\omega )|^2. \end{aligned}$$
Proof
The first assertion is an immediate consequence of the definition of \(S_{ij}\). For the second sentence, we observe that for \(\omega \in S^{N-1}\) it follows from (27) that
(iii) is an immediate consequence of (i) and (28). \(\square \)
We can now show the announced decomposition of the Laplace–Beltrami operator as a sum of second-order angular derivatives.
Proposition 4.4
where using the spherical coordinates \(x=r\omega \), \(\Delta _0f(r\omega )\) acts on the \(\omega \)-variable.
In particular, on \(S^{N-1}\) we have the decomposition \({\sum _{i<j}S_{ij}^2=\Delta _0}\).
Proof
We observe preliminary that
and
Summing over \(i<j\) the last expression and using (29) we obtain
Recalling that \(r^2\Delta =r^2D_{rr}+(N-1)rD_r+\Delta _0\) we get the conclusion. \(\square \)
Next we have the following integration by parts formula.
Proposition 4.5
For every \(i<j\) and for every \(u,v\in C^1(S^{N-1})\)
Proof
Let \(i<j\) and \(u,v\in C^1(S^{N-1})\). We have obviously \(S_{ij}(uv)=S_{ij}u\,v+u\,S_{ij}v\) and so
Using the Gauss–Green theorem, the claim immediately follows by observing that
\(\square \)
Let \(\mathcal {H}_n\) be the set of the spherical harmonics of order n. We recall that from [9, Proposition 2.1 (iii)], we have
The following proposition shows that \(\mathcal {H}_n\) is preserved by \(S_{ij}\).
Proposition 4.6
Let \(\phi \in \mathcal {H}_n\). Then, for every \(i<j\), \(S_{ij}\phi \in \mathcal {H}_n\). Moreover, if \(-\lambda _n=-n(n+N-2)\) is the eigenvalue associated with \(\phi \), then
Proof
Let \(p(x)=r^n\phi (\omega )\); p is a homogeneous harmonic polynomial by construction and \(S_{ij}p\) is a polynomial of the same degree by the definition of \(S_{ij}\). Moreover, using (iv) of Proposition 4.1, we have
and so \(S_{ij}p\) is harmonic since from (ii) of Proposition 4.1 \(S_{ij}P(r\omega )=r^nS_{ij}\phi (\omega )\), we have \(S_{ij}\phi \in \mathcal {H}_n\). In particular,
and
Now, using propositions 4.5 and 4.4,
The last inequality implies
which, combined with (32), yields (30). Finally, applying (28) and (30), it follows for every \(\omega \in S^{N-1}\)
which proves (31). \(\square \)
Corollary 4.7
The tangential derivative of the zonal harmonics \(\mathbb {Z}^{(n)}\) satisfies
In particular, for a constant \(C=C(N)\) we have
Proof
The first property is an immediate consequence of (31) and of the estimate
To prove the second inequality it is sufficient to recall the asymptotic behaviours \(\mathrm{{dim}}\mathcal H_n\approx n^{N-2}\), \(\lambda _n\approx n^2\) for \(n\rightarrow \infty \). \(\square \)
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Metafune, G., Negro, L. & Spina, C. Gradient Estimates for Elliptic Operators with Second-Order Discontinuous Coefficients. Mediterr. J. Math. 16, 138 (2019). https://doi.org/10.1007/s00009-019-1415-x
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DOI: https://doi.org/10.1007/s00009-019-1415-x