Home Square function inequality for a class of Fourier integral operators satisfying cinematic curvature conditions
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Square function inequality for a class of Fourier integral operators satisfying cinematic curvature conditions

  • Chuanwei Gao , Changxing Miao EMAIL logo and Jianwei-Urbain Yang
Published/Copyright: July 16, 2020

Abstract

In this paper, we establish an improved variable coefficient version of the square function inequality, by which the local smoothing estimate LαpLp for the Fourier integral operators satisfying cinematic curvature condition is further improved. In particular, we establish almost sharp results for 2<p3 and push forward the estimate for the critical point p=4. As a consequence, the local smoothing estimate for the wave equation on the manifold is refined. We generalize the results in [S. Lee and A. Vargas, On the cone multiplier in 3, J. Funct. Anal. 263 2012, 4, 925–940; J. Lee, A trilinear approach to square function and local smoothing estimates for the wave operator, preprint 2018, https://arxiv.org/abs/1607.08426v5] to its variable coefficient counterpart. The main ingredients in the argument includes multilinear oscillatory integral estimate [J. Bennett, A. Carbery and T. Tao, On the multilinear restriction and Kakeya conjectures, Acta Math. 196 2006, 2, 261–302] and decoupling inequality [D. Beltran, J. Hickman and C. D. Sogge, Variable coefficient Wolff-type inequalities and sharp local smoothing estimates for wave equations on manifolds, Anal. PDE 13 2020, 2, 403–433].

MSC 2010: 35S30; 35L05

Communicated by Christopher D. Sogge


Award Identifier / Grant number: 8206300279

Award Identifier / Grant number: 11831004

Award Identifier / Grant number: 11901032

Funding statement: C. Gao was supported by Chinese Postdoc Foundation grant 8206300279. C. Miao was supported by NSFC Grant 11831004. J. Yang was supported by NSFC grant 11901032, and Beijing Institute of Technology Research Fund Program for Young Scholars.

A Appendix

In this section, we will prove Lemma 5.4.

Proof of Lemma 5.4.

Due to the fast decay of the weight wR away from |z|R12+ε4, it suffices to consider

(ν𝟏{|x|R12+ε4}(Ez¯νf)L2(wBR)12)12.

Freeze time t0, and note that

(A.1)Ez¯νf(x,t0)=eix,ηχz¯,ν(η)(Ez¯f)(η,t0)dη,

where

Ez¯f(x,t0)=2ei(x,η+t0hz¯(η))a2,z¯(η)f(η)dη,χz¯,ν(η)=χν(Ψλ(z¯,η)).

We further decompose

(A.2)Ez¯f(,t0)=𝟏{|x|R12+ε2}()Ez¯f(,t0)+𝟏{|x|>R12+ε2}()Ez¯f(,t0).

It remains to estimate

eix,ηχz¯,ν(η)(𝟏{|x|R12+ε2}()Ezkf(,t0))(η)dη.

In fact, for |x~|R12+ε4, the contribution of the second term in (A.2) to (A.1) equals

χ^z¯,ν(x~-y)𝟏{|x|>R12+ε2}(y)Ez¯f(y,t0)dyR-εNfL2.

Now, unfreezing t0, by Plancherel’s theorem, we have

(νeix,ηχz¯,ν(η)(𝟏{|x|R12+ε2}()Ez¯f(,t))(η)dηL2(wBR)2)12Ez¯fL2(wBR).

This completes the proof of Lemma 5.4. ∎

Acknowledgements

The authors would like to thank David Beltran and Christopher Sogge for their helpful discussion and suggestions. The authors are also deeply grateful to the anonymous referees for their invaluable comments which helped improve the paper greatly.

References

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Received: 2020-03-06
Revised: 2020-05-31
Published Online: 2020-07-16
Published in Print: 2020-11-01

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