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• W2000794253 abstract "Using numerical solutions of the time-dependent Schrodinger equation for a hydrogen and a helium atom in a linearly polarized laser field, we calculate the photoelectron signal ${P}_{+}$, ${P}_{ensuremath{-}}$ measured by two opposing detectors placed along the laser polarization vector, with laser focus in the center. Our calculations show a significant sensitivity of the normalized asymmetry coefficient $a=({P}_{+}ensuremath{-}{P}_{ensuremath{-}})∕({P}_{+}+{P}_{ensuremath{-}})$ to the carrier-envelope (CE) phase for few-cycle laser pulses. We find a very simple dependence of this coefficient on the CE phase $ensuremath{phi}$ and on pulse duration for laser intensities slightly below the tunneling regime, i.e., for the intensities range between the perturbative-multiphoton and tunneling regime, for laser pulses shorter than two laser cycles. In particular, we find that in this intensity regime, the asymmetry is zero for a fixed, particular value of $ensuremath{phi}={ensuremath{phi}}_{0}ensuremath{simeq}ensuremath{-}0.3ensuremath{pi}$ and is maximum for $ensuremath{phi}={ensuremath{phi}}_{M}={ensuremath{phi}}_{0}+ensuremath{pi}∕2$. These regularities would allow one to measure the CE phase. In particular, the condition of zero asymmetry for few-cycle pulses can be useful for stabilizing the CE phase." @default.
• W2000794253 created "2016-06-24" @default.
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• W2000794253 date "2004-07-29" @default.
• W2000794253 modified "2023-09-30" @default.
• W2000794253 title "Phase-dependent asymmetries in strong-field photoionization by few-cycle laser pulses" @default.
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• W2000794253 doi "https://doi.org/10.1103/physreva.70.013815" @default.
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