1997
DOI: 10.1103/physrevlett.79.2018
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Ionization of Na Rydberg Atoms by Subpicosecond Quarter-Cycle Circularly Polarized Pulses

Abstract: We report the first observation of ionization of Rydberg atoms by subpicosecond, circularly polarized THz radiation. The field amplitude in these pulses is non-negligible for only one-quarter of an optical cycle. The experiment is performed in the short-pulse regime, where the duration of the ionizing pulse is shorter than the classical Kepler period of the Rydberg electron. We find that the ionization probability for these atoms is remarkably insensitive to the time-varying polarization of the THz field.Over … Show more

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Cited by 38 publications
(26 citation statements)
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“…[8][9][10][11] One of the most important but least studied aspects of the THz-TDS system is the polarization state of the emitted radiation. Several recent measurements have exploited the polarization properties of the THz radiation, 12,13 and others have noted the polarization dependence of the transmittance or reflectance of optical elements. 14,15 In most cases the emission from THz di-pole antennas has been described with the approximation of an ideal dipole, 7 producing linearly polarized radiation.…”
Section: Introductionmentioning
confidence: 99%
“…[8][9][10][11] One of the most important but least studied aspects of the THz-TDS system is the polarization state of the emitted radiation. Several recent measurements have exploited the polarization properties of the THz radiation, 12,13 and others have noted the polarization dependence of the transmittance or reflectance of optical elements. 14,15 In most cases the emission from THz di-pole antennas has been described with the approximation of an ideal dipole, 7 producing linearly polarized radiation.…”
Section: Introductionmentioning
confidence: 99%
“…Such a situation has already been experimentally realized with a very fine control of the time delay τ between the pulses. 18 Following the same considerations as for the calculation of the total dipole moment one derives the following expression for the induced current…”
Section: Excitation Of Carriers In Single-channel Ballistic Ring By Hcpsmentioning
confidence: 99%
“…For time delays between the pulses such that τ 2π/ω 0 (a condition that holds in the time domain of our interest since 2π/ω 0 ≈ 13 ns) and for the relatively weak pulses considered here, the behavior of the current as a function of τ is mainly dominated by the sine oscillations with nodes at τ = 2πk/(Nω 0 ) [see Eqs. (17), (18), and (25)] with k being a positive integer. Thus the sign of the peak current can be controlled not only by the polarity of the pulses but also by choosing the appropriate value of τ .…”
Section: Excitation Of Carriers In Single-channel Ballistic Ring By Hcpsmentioning
confidence: 99%
“…40,41 Half cycle pulses (HCPs) with the peak field of up to several hundreds of kV/cm and duration in the femtosecond regimes can be experimentally generated. [42][43][44][45][46] Ultrashort pulses create non-stationary superposition, or wave packet, in the multilevel medium. This wave packet oscillates with a characteristic time that corresponds to the quantum beat period between the excited states.…”
Section: Introductionmentioning
confidence: 99%