Skip to content
DraconiticResearch
Search Sources API
186,541 studies31 sourcesUpdated 9 min ago
PreprintCC BY 4.0arXiv

Time delay in nonadiabatic tunneling ionization

Abstract

The under-the-barrier recollision pathway during the tunneling ionization of an atom, despite its minuscule amplitude, leaves its signature on the observable photoelectron momentum distribution due to a phase shift relative to the direct ionization path, that can be interpreted as a tunneling time delay. We investigate how this time delay is modified in the nonadiabatic regime, where the tunneling barrier evolves dynamically during the ionization process. Our analysis is based on a simple model of a one-dimensional short-range potential driven by a strong laser pulse which remains amenable to a systematic analytical treatment with the strong field approximation (SFA). We show a significant contribution of the high-order SFA corrections, which describes the recollision channel with recombination and further ionization, and is additional to the rescattering. Whereas the recombination channel dominates over the rescattering for the tunneling time delay in the quasistatic regime at relatively large laser fields, their contributions are reversed in weak fields.

Related

  1. Time-Dependent Tunneling in the Thin-Barrier Limit
    Tanmay Vachaspati, Frank Wilczek, Zara Yu
    arXivPreprintCC BY 4.0Full textCondensed matterHigh-energy & particle physicsarXiv
  2. A combined segmented anode gas ionization chamber and time-of-flight detector for heavy ion elastic recoil detection analysis
    Petter Ström, Per Petersson, Marek Rubel +1
    arXivPreprintarXiv licenceFull textApplied physics & instrumentationCondensed matterarXiv
  3. Multimode Angle-Compensated Interferometer with Long Time-Bin Delay Using a Multi-Pass Herriott Cell
    Ramy Tannous, Stéphane Vinet, Kaylee Sherk +2
    arXivPreprintCC BY 4.0Full textOptics & photonicsQuantum physics & quantum informationarXiv
  4. Optoelectronic Reservoir Computing with an On-Chip True-Time-Delay Element
    Ahmad Murad, Shadad Watad, Alina Karabchevsky
    arXivPreprintarXiv licenceFull textOptics & photonicsarXiv
  5. Gravitational-wave responses and noise correlations in geometric time-delay interferometry
    Rui Luo, Pan-Pan Wang, Lin-Lin Yang +2
    arXivPreprintCC BY 4.0Full textInstrumentation & methodsGravitation & general relativityarXiv
BibTeX
@misc{klaiber2026time,
  title = {{Time delay in nonadiabatic tunneling ionization}},
  author = {Michael Klaiber and Karen Z. Hatsagortsyan and Christoph H. Keitel},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.08609},
  eprint = {2610.08609},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.08609},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Time delay in nonadiabatic tunneling ionization
AU  - Michael Klaiber
AU  - Karen Z. Hatsagortsyan
AU  - Christoph H. Keitel
PY  - 2026
DA  - 2026/10/06
PB  - arXiv
DO  - 10.48550/arxiv.2610.08609
UR  - https://arxiv.org/abs/2610.08609
AB  - The under-the-barrier recollision pathway during the tunneling ionization of an atom, despite its minuscule amplitude, leaves its signature on the observable photoelectron momentum distribution due to a phase shift relative to the direct ionization path, that can be interpreted as a tunneling time delay. We investigate how this time delay is modified in the nonadiabatic regime, where the tunneling barrier evolves dynamically during the ionization process. Our analysis is based on a simple model of a one-dimensional short-range potential driven by a strong laser pulse which remains amenable to a systematic analytical treatment with the strong field approximation (SFA). We show a significant contribution of the high-order SFA corrections, which describes the recollision channel with recombination and further ionization, and is additional to the rescattering. Whereas the recombination channel dominates over the rescattering for the tunneling time delay in the quasistatic regime at relatively large laser fields, their contributions are reversed in weak fields.
ER  -