2016
DOI: 10.1103/physreva.93.051401
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Nonadiabatic dynamics and multiphoton resonances in strong-field molecular ionization with few-cycle laser pulses

Abstract: We study strong field molecular ionization using few-(four to ten) cycle laser pulses. Employing a supercontinuum light source, we are able to tune the optical laser wavelength (photon energy) over a range of about ∼200 nm (500 meV). We measure the photoelectron spectrum for a series of different molecules as a function of laser intensity, frequency, and bandwidth and illustrate how the ionization dynamics vary with these parameters. We find that multiphoton resonances and nonadiabatic dynamics (internal conve… Show more

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Cited by 25 publications
(27 citation statements)
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“…"# ratio is again near unity. However, at intermediate UP, where non-adiabatic ionization strongly contributes to the ionization yield [64][65][66][67][68] all three gases exhibit an enhancement in ionization for counter-rotating laser fields. Note that the low UP behavior in argon differs from helium and krypton.…”
Section: Iiia Experimental Resultsmentioning
confidence: 99%
“…"# ratio is again near unity. However, at intermediate UP, where non-adiabatic ionization strongly contributes to the ionization yield [64][65][66][67][68] all three gases exhibit an enhancement in ionization for counter-rotating laser fields. Note that the low UP behavior in argon differs from helium and krypton.…”
Section: Iiia Experimental Resultsmentioning
confidence: 99%
“…For example, optical spectroscopies, such as transient absorption [24][25][26][27][28], can provide high time resolution with a compact apparatus but require detailed knowledge of the potential energy surfaces (electronic energies as a function of nuclear coordinates) and transition dipole moments along the reaction coordinate in order to be interpreted. Time-resolved ionization spectroscopies [23,[29][30][31][32][33][34][35][36] offer the advantage over optical spectroscopies that it is always possible to ionize, regardless of the character of the excited-state, and if one measures the energy of the photoelectrons as a function of pump-probe delay, then one can extract information about the distribution of energy within the molecule as a function of time. UED [37][38][39][40][41][42][43] holds the promise of providing direct structural information as a function of time, but it suffers from orientational averaging over the sample, repulsion between the electrons in a short pulse, and the group velocity mismatch between electrons and light.…”
Section: Introductionmentioning
confidence: 99%
“…The ponderomotive potential is estimated to be approximately 0.5-0.7 eV based on previous work [24,29]. …”
Section: Resultsmentioning
confidence: 99%
“…Pulses with octave-spanning bandwidth (400-900 nm at the tails) are produced through supercontinuum generation in argon gas [29,36]. To compress the pulses and produce durations of less than 10 fs, we use an AOMbased pulse shaper in a 4f geometry [34,37] and perform a multiphoton intrapulse interference phase scan (MIIPS) to retrieve the optical phase [38][39][40][41][42].…”
Section: Experimental Apparatusmentioning
confidence: 99%
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