2012
DOI: 10.1103/physreva.85.053424
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Photoemission-time-delay measurements and calculations close to the 3s-ionization-cross-section minimum in Ar

Abstract: We present experimental measurements and theoretical calculations of photoionization time delays from the 3s and 3p shells in Ar in the photon energy range of 32-42 eV. The experimental measurements are performed by interferometry using attosecond pulse trains and the infrared laser used for their generation. The theoretical approach includes intershell correlation effects between the 3s and 3p shells within the framework of the random phase approximation with exchange (RPAE). The connection between single-pho… Show more

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Cited by 123 publications
(195 citation statements)
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“…The atomic delay difference between the 3p and 3s orbitals is ∼ 78 as at an XUV photon energy of ∼ 37 eV, which is consistent with the experimental value of 100 ± 50 presented in Ref. [4]. Figure 5: The "exact" continuum-continuum delay is determined for all outermost n shell electrons in neon and argon as τ CC ≡ τ A − τ W using Eq.…”
Section: Resultssupporting
confidence: 68%
See 1 more Smart Citation
“…The atomic delay difference between the 3p and 3s orbitals is ∼ 78 as at an XUV photon energy of ∼ 37 eV, which is consistent with the experimental value of 100 ± 50 presented in Ref. [4]. Figure 5: The "exact" continuum-continuum delay is determined for all outermost n shell electrons in neon and argon as τ CC ≡ τ A − τ W using Eq.…”
Section: Resultssupporting
confidence: 68%
“…Experimental studies have evidenced relative delays between different ionization processes of various target systems including both solid-state surfaces [1] and atomic gases [2,3,4]. This has stimulated a number of theoretical investigations concerning the role of the long-range Coulomb potential [3,5,6], many-electron screening effects [4,7,8] and electron localization [9]. The delayed response of atomic systems can be decomposed as the sum of two terms [3,10]:…”
Section: Introductionmentioning
confidence: 99%
“…Temporal characterization of attosecond pulses, which requires determination of the spectral phase of the XUV field, can be performed by laser-assisted photoionization [4,5]. More recently, this type of experiments have been used for spectral phase determination of photoelectrons from autoionizing states [6,7] and for the measurement of relative time delays in laser-assisted photoionization from different initial states in solids [8] and atoms [9][10][11]. Relative time delays have also been measured between different atomic species [12][13][14], between single and double ionization [15], between different angles of photoemission [16] and between the ion ground state and shake-up states [17].…”
Section: Introductionmentioning
confidence: 99%
“…Recent interests of such experiments [1][2][3][4][5] owe to the technology in generating attosecond single pulse [6,7] and pulse trains [8,9]. Of particular attraction are the experiments based on the interferometric metrology, namely, the reconstruction of attosecond beating by interference of two-photon transitions (RABITT) [8], in which photoelectrons emitted by a coherent XUV comb of odd harmonics (pump) driven by a tunable fundamental field subsequently absorb or emit a synchronized IR photon (probe).…”
Section: Introductionmentioning
confidence: 99%