Attoclock revisited on electron tunnelling time
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The last decade has seen an intense renewed debate on tunnelling time, both from a theoretical and an experimental perspective. Here, we review recent developments and new insights in the field of strong-field tunnel ionization related to tunnelling time, and apply these findings to the interpretation of the attoclock experiment Landsman et al. [<i>Optica</i> <b>2014</b>, <i>1</i>, 343]. We conclude that models including finite tunnelling time are consistent with recent experimental measurements. <b>Abbreviations</b>: A: adiabatic; ADK: Ammosov, Delone and Krainov model (<i>1, 2</i>); CEO: carrier-envelope-offset phase ϕCEO; CoM: centre of mass; CTMC: classical trajectory monte carlo simulation; FWHM: full width half maximum; IR: infrared; KR: Keldysh-Rutherford model; NA: non-adiabatic; PMD: photoelectron momentum distribution; PPT: Perelomov, Popov and Terent'ev model (<i>3, 4</i>); SAE: single active electron approximation; SCT: singleclassical trajectory; SFA: strong field approximation; TDSE: time-dependent Schrödinger equation
提供机构:
Taylor & Francis
创建时间:
2019-04-25



