Abstract
We examine the asymptotics of the spectral counting function of a compact Riemannian manifold by Avakumovic (Math Z 65:327–344, [1]) and Hörmander (Acta Math 121:193–218, [15]) and show that for the scale of orthogonal and unitary groups \(\mathbf{SO}(N)\), \(\mathbf{SU}(N)\), \(\mathbf{U}(N)\) and \(\mathbf{Spin}(N)\) it is not sharp. While for negative sectional curvature improvements are possible and known, cf. e.g., Duistermaat and Guillemin (Invent Math 29:39–79, [7]), here, we give sharp and contrasting examples in the positive Ricci curvature case [non-negative for \(\mathbf{U}(N)\)]. Furthermore here the improvements are sharp and quantitative relating to the dimension and rank of the group. We discuss the implications of these results on the closely related problem of closed geodesics and the length spectrum.
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Notes
In the sequel when the choice of \(M^d\) is clear from the context, or when there is no danger of confusion, we suppress the dependence on \(M^d\) and simply write \(\mathscr {N}=\mathscr {N}(\lambda )\).
In fact the Liouville measure of the set of periodic orbits of the geodesics flow in the co-tangent bundle \(T^\star \mathbf{SO}(N)\) is zero for \(N \ge 4\) (see [24] for more).
Therefore in the \(\mathbf {SO}(2n+1)\) case, in contrast to \(\mathbf {SO}(2n)\), we have \(b_n\in {\mathbb N}_0\).
This is a consequence of the identities \(\widehat{f(\cdot +h)}(\xi ) = \widehat{f}(\xi ) e^{2\pi i h \cdot \xi }\), \(|\widehat{f(\cdot +h)}(\xi )| = |\widehat{f}(\xi )|\).
Below we shall be using the notation of \(\mathscr {A}_\rho = \mathscr {A} + \rho \).
It can be easily checked that the Weyl group W maps \(\mathscr {A}_{\rho }\) to itself since for each \(w \in W\) we have that \(w\cdot \rho = \rho - \alpha \) for some \(\alpha \in \mathfrak {R}\subset \mathscr {A}\). Then as \(W \cdot \mathscr {A} = \mathscr {A}\) we clearly have that for any \(w\in W\), \(w\cdot (\mu + \rho ) \in \mathscr {A}_{\rho }\).
For more on approximation results of this nature the reader is referred to ([9] pp. 187–192).
The remainder term here accounts for \(j=0\) which is \(t^{m+1}D(t) = O(t^{m+1}\ln t)\) since \(D(t)=O(\ln t)\), however, in what follows we show that \(H(t),L(t)=O(t^{m+3/2})\) and therefore we can omit this additional remainder as it will be adsorbed into this asymptotics.
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Communicated by Hartmut Führ.
Asymptotics of Weighted Integrals Involving Bessel Functions
Asymptotics of Weighted Integrals Involving Bessel Functions
In this appendix we present the proof of an estimate used earlier in the paper. This is concerned with the asymptotics of Bessel functions and their weighted integrals.
Proposition 6.1
Let \(\alpha \ge 2\) and \(\beta >-1/2\). Then there exist constants \(M>0\) and \(c>0\) such that for any \(z \ge M\) we have
Proof
Using the identity established in Lemma 6.1 below we can write
Next in virtue of the asymptotic decay of Bessel function at infinity (see, e.g., Stein and Weiss [30]) it follows that there exists \(M>0\) such that \(J_{\beta +1}(z) \le {cz^{-\frac{1}{2}}}\) for \(z>M\). Hence we can write
from which the conclusion follows at once. \(\square \)
Lemma 6.1
Let \(\alpha \ge 2\) and \(\beta >-1/2\) with \(z \in {\mathbb R}\).Then the following identity holds
Proof
Starting from the following weighted integral identity for Bessel functions (cf., e.g., Grafakos [11] Appendix B.3)
we can write
Now integrating the term on the right gives
and so the conclusion follows by simple manipulation of the above. \(\square \)
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Morris, C., Taheri, A. On Weyl’s Asymptotics and Remainder Term for the Orthogonal and Unitary Groups. J Fourier Anal Appl 24, 184–209 (2018). https://doi.org/10.1007/s00041-017-9522-1
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DOI: https://doi.org/10.1007/s00041-017-9522-1