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Above-threshold multiphoton detachment from the H- ion by 10.6-m radiation : Angular distributions and partial widths. / Telnov, Dmitry A.; Chu, Shih I.

In: Physical Review A, Vol. 50, No. 5, 01.01.1994, p. 4099-4108.

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@article{22c510a2404d42eca89e039a416aa340,
title = "Above-threshold multiphoton detachment from the H- ion by 10.6-m radiation: Angular distributions and partial widths",
abstract = "We present a general procedure for accurate nonperturbative treatment of the angular distribution and partial widths for multiphoton above-threshold detachment (ATD) of atoms or negative ions in intense laser fields. The procedure consists of the following two steps: (1) The resonance wave function is determined by means of the non-Hermitian Floquet Hamiltonian method. The Floquet Hamiltonian is discretized by the complex scaling generalized pseudospectral method recently developed by Yao and Chu [Chem. Phys. Lett. 204, 381 (1993)]. No computation of potential matrix elements is required, and the kinetic-energy matrix elements can be evaluated analytically. (2) The angular distribution and partial rates are calculated, based on an exact differential expression, and a procedure is developed for the backrotation of the total complex resonance wave function to the real axis. The method is applied to the study of multiphoton ATD of H- in strong fields at 10.6 m. An accurate one-electron model potential [Laughlin and Chu, Phys. Rev. A 48, 4654 (1993)], which reproduces the known H- binding energy and the low-energy e-H(1s) elastic scattering phase shifts, is employed. At this low frequency, the resonance wave functions can be obtained efficiently and rather accurately by means of a nonperturbative adiabatic approach recently developed by Telnov [J. Phys. B 24, 2967 (1991)]. This adiabatic theory is also valid in the limit of weak fields, and its validation is justified by its agreement with the exact perturbation calculations for the seven- and eight-photon detachment of H-. Detailed results for the angular distribution and partial widths for multiphoton ATD of H- are presented for the moderately strong laser intensity regime (10101011 W/cm2) at 10.6 m.",
author = "Telnov, {Dmitry A.} and Chu, {Shih I.}",
year = "1994",
month = jan,
day = "1",
doi = "10.1103/PhysRevA.50.4099",
language = "English",
volume = "50",
pages = "4099--4108",
journal = "Physical Review A - Atomic, Molecular, and Optical Physics",
issn = "1050-2947",
publisher = "American Physical Society",
number = "5",

}

RIS

TY - JOUR

T1 - Above-threshold multiphoton detachment from the H- ion by 10.6-m radiation

T2 - Angular distributions and partial widths

AU - Telnov, Dmitry A.

AU - Chu, Shih I.

PY - 1994/1/1

Y1 - 1994/1/1

N2 - We present a general procedure for accurate nonperturbative treatment of the angular distribution and partial widths for multiphoton above-threshold detachment (ATD) of atoms or negative ions in intense laser fields. The procedure consists of the following two steps: (1) The resonance wave function is determined by means of the non-Hermitian Floquet Hamiltonian method. The Floquet Hamiltonian is discretized by the complex scaling generalized pseudospectral method recently developed by Yao and Chu [Chem. Phys. Lett. 204, 381 (1993)]. No computation of potential matrix elements is required, and the kinetic-energy matrix elements can be evaluated analytically. (2) The angular distribution and partial rates are calculated, based on an exact differential expression, and a procedure is developed for the backrotation of the total complex resonance wave function to the real axis. The method is applied to the study of multiphoton ATD of H- in strong fields at 10.6 m. An accurate one-electron model potential [Laughlin and Chu, Phys. Rev. A 48, 4654 (1993)], which reproduces the known H- binding energy and the low-energy e-H(1s) elastic scattering phase shifts, is employed. At this low frequency, the resonance wave functions can be obtained efficiently and rather accurately by means of a nonperturbative adiabatic approach recently developed by Telnov [J. Phys. B 24, 2967 (1991)]. This adiabatic theory is also valid in the limit of weak fields, and its validation is justified by its agreement with the exact perturbation calculations for the seven- and eight-photon detachment of H-. Detailed results for the angular distribution and partial widths for multiphoton ATD of H- are presented for the moderately strong laser intensity regime (10101011 W/cm2) at 10.6 m.

AB - We present a general procedure for accurate nonperturbative treatment of the angular distribution and partial widths for multiphoton above-threshold detachment (ATD) of atoms or negative ions in intense laser fields. The procedure consists of the following two steps: (1) The resonance wave function is determined by means of the non-Hermitian Floquet Hamiltonian method. The Floquet Hamiltonian is discretized by the complex scaling generalized pseudospectral method recently developed by Yao and Chu [Chem. Phys. Lett. 204, 381 (1993)]. No computation of potential matrix elements is required, and the kinetic-energy matrix elements can be evaluated analytically. (2) The angular distribution and partial rates are calculated, based on an exact differential expression, and a procedure is developed for the backrotation of the total complex resonance wave function to the real axis. The method is applied to the study of multiphoton ATD of H- in strong fields at 10.6 m. An accurate one-electron model potential [Laughlin and Chu, Phys. Rev. A 48, 4654 (1993)], which reproduces the known H- binding energy and the low-energy e-H(1s) elastic scattering phase shifts, is employed. At this low frequency, the resonance wave functions can be obtained efficiently and rather accurately by means of a nonperturbative adiabatic approach recently developed by Telnov [J. Phys. B 24, 2967 (1991)]. This adiabatic theory is also valid in the limit of weak fields, and its validation is justified by its agreement with the exact perturbation calculations for the seven- and eight-photon detachment of H-. Detailed results for the angular distribution and partial widths for multiphoton ATD of H- are presented for the moderately strong laser intensity regime (10101011 W/cm2) at 10.6 m.

UR - http://www.scopus.com/inward/record.url?scp=0000389265&partnerID=8YFLogxK

U2 - 10.1103/PhysRevA.50.4099

DO - 10.1103/PhysRevA.50.4099

M3 - Article

AN - SCOPUS:0000389265

VL - 50

SP - 4099

EP - 4108

JO - Physical Review A - Atomic, Molecular, and Optical Physics

JF - Physical Review A - Atomic, Molecular, and Optical Physics

SN - 1050-2947

IS - 5

ER -

ID: 28840940