Matrix elements of Fourier Integral Operator

Author(s):  
Steve Zelditch
2004 ◽  
Vol 76 (1) ◽  
pp. 1-22 ◽  
Author(s):  
Terence Tao

AbstractLet T be a Fourier integral operator on Rn of order–(n–1)/2. Seeger, Sogge, and Stein showed (among other things) that T maps the Hardy space H1 to L1. In this note we show that T is also of weak-type (1, 1). The main ideas are a decomposition of T into non-degenerate and degenerate components, and a factorization of the non-degenerate portion.


2000 ◽  
Vol 52 (5) ◽  
pp. 897-919
Author(s):  
T. J. Christiansen ◽  
M. S. Joshi

AbstractWe develop a scattering theory for perturbations of powers of the Laplacian on asymptotically Euclidean manifolds. The (absolute) scattering matrix is shown to be a Fourier integral operator associated to the geodesic flow at time π on the boundary. Furthermore, it is shown that on n the asymptotics of certain short-range perturbations of Δk can be recovered from the scattering matrix at a finite number of energies.


2001 ◽  
Vol 59 (2) ◽  
pp. 269-300 ◽  
Author(s):  
Eric Leichtnam ◽  
Ryszard Nest ◽  
Boris Tsygan

2001 ◽  
Vol 13 (07) ◽  
pp. 891-920 ◽  
Author(s):  
KENJI YAJIMA

We show that the asymptotic behavior at infinity of the fundamental solution of the initial value problem for the free Schrödinger equation or of the harmonic oscillator at non-resonant time is stable under subquadratic perturbations. We also show that the same is true for the phase and the amplitude of the Fourier integral operator representing the propagator.


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