2014
DOI: 10.1103/physrevlett.113.223002
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Nonlinear Dichroism in Back-to-Back Double Ionization of He by an Intense Elliptically Polarized Few-Cycle Extreme Ultraviolet Pulse

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Cited by 33 publications
(31 citation statements)
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References 51 publications
(63 reference statements)
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“…2(a)], the energy distributions [see Fig. 3(a)], and the angular distributions (not shown) from either a TDSE calculation or by using the PT formula (24) are in excellent quantitative agreement. According to our discussion following PT formula (18), for time delays τ equal to or longer than the total pulse duration T , the TDP reduces to the following form:…”
Section: A Two-photon Single Ionization By Two Identical Time-delaymentioning
confidence: 76%
See 1 more Smart Citation
“…2(a)], the energy distributions [see Fig. 3(a)], and the angular distributions (not shown) from either a TDSE calculation or by using the PT formula (24) are in excellent quantitative agreement. According to our discussion following PT formula (18), for time delays τ equal to or longer than the total pulse duration T , the TDP reduces to the following form:…”
Section: A Two-photon Single Ionization By Two Identical Time-delaymentioning
confidence: 76%
“…To obtain the wave packet (r 1 ,r 2 ,t) solution of the TDSE (1), we use the methods developed previously for either an arbitrarily polarized attosecond single pulse [24] or a pair of pulses [8]. In brief, we adopt the time-dependent closecoupling expansion [25,26] of the wave packet (r 1 ,r 2 ,t) onto the orthonormal basis functions of bipolar spherical harmonics…”
Section: Methodsmentioning
confidence: 99%
“…This corresponds to a spectral width [6] Δω ≃ 1.44ω=n p ≈ 17 eV, and a FWHM in the intensity of 0.36T, or 1.1 cycles. Such single-cycle attosecond pulses (having linear polarization) have been achieved experimentally [7][8][9], albeit with much lower intensity.…”
mentioning
confidence: 99%
“…We obtain the wave packet ΨðtÞ by solving the six-dimensional two-electron TDSE for the He atom interacting with two circularly polarized attosecond pulses using methods developed previously [6] for a single arbitrarily polarized attosecond pulse. Our method uses the finite-element discrete-variable representation combined with the real-space-product algorithm [10] as well as Wigner rotation transformations at each time step from the laboratory frame to the frame of the instantaneous electric field [11,12].…”
mentioning
confidence: 99%
“…However, there is great interest in developing efficient schemes for production of short, coherent xuv pulses with tunable polarizations . This interest is motivated by the numerous applications of chiral-sensitive (dichroic) light-matter interactions, such as in photoionization circular dichroism investigations of chiral molecules [36][37][38], in x-ray magnetic circular dichroism investigations of magnetic materials [39][40][41][42], and in nonlinear elliptic dichroism investigations of double-photoionization processes [43].…”
Section: Introductionmentioning
confidence: 99%