2016
DOI: 10.1103/physreva.94.013423
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Relativistic calculations of angle-dependent photoemission time delay

Abstract: Angular dependence of photoemission time delay for the valence np 3/2 and np 1/2 subshells of Ar, Kr and Xe is studied in the dipole relativistic random phase approximation. Strong angular anisotropy of the time delay is reproduced near respective Cooper minima while the spin-orbit splitting affects the time delay near threshold.

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Cited by 32 publications
(39 citation statements)
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“…The C parameter is converted to the atomic time delay τ a by (8) and analyzed as a function of the photoelectron direction relative to the polarization axis. The angular dependence of τ a is compared with the analogous dependence of the Wigner time delay τ W [21]. The time delay difference τ a − τ W in the zero angle direction is compared with the hydrogenic CC correction τ CC [22].…”
Section: A Solution Of Tdsementioning
confidence: 99%
“…The C parameter is converted to the atomic time delay τ a by (8) and analyzed as a function of the photoelectron direction relative to the polarization axis. The angular dependence of τ a is compared with the analogous dependence of the Wigner time delay τ W [21]. The time delay difference τ a − τ W in the zero angle direction is compared with the hydrogenic CC correction τ CC [22].…”
Section: A Solution Of Tdsementioning
confidence: 99%
“…As shown in earlier work [21,22], the interplay between two different angular components may give rise to an anisotropic time delay τ W (also known as Wigner time delay [23]) of the photoelectron wave packet, which is generated by the absorption of one XUV photon. The relativistic case involves a more complex analysis of several spin-orbit split channels [24]. So far, the angular dependence of group delays was exclusively studied theoretically, and in the context of the ionization from a nonsymmetric orbital [21,25].…”
Section: Introductionmentioning
confidence: 99%
“…The relativistic formalism of the angular dependent WTD is presented in [26]. Briefly, the electric dipole transition amplitude from an initial state a, (ljm), to the final statesā, (ljm), for linearly polarized photons in thê z direction is, to within an overall real multiplicative factor,…”
Section: Methodsmentioning
confidence: 99%
“…Here χ ν is a two-component spinor and C is a Clebsch-Gordan coefficient. We combine the reduced electric dipole matrix element ā Q (1) 1 a defined in [26] with the phase factors and introduce…”
Section: Methodsmentioning
confidence: 99%
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