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Published on: July 27, 2018
Conservation laws for electron vortices in strong-field ionisation
Yuxin Kang1, Emilio Pisanty2,3, Marcelo Ciappina3,4,5
1Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT UK.
We studied twisted electrons ionized by strong laser fields. Our new theory explains how their orbital angular momentum (OAM) is conserved and linked to initial states and laser properties.
Area of Science:
- Atomic, Molecular, and Optical Physics
- Quantum Mechanics
- Strong Field Physics
Background:
- Electrons with orbital angular momentum (OAM) are crucial in various physical phenomena.
- Strong laser fields can ionize atoms, leading to complex electron dynamics.
- Understanding electron OAM during ionization is key to controlling quantum states.
Purpose of the Study:
- To develop a theoretical framework for understanding the OAM of twisted electrons during strong field ionization.
- To derive conservation laws for electron OAM under different laser polarizations.
- To provide a new interpretation for above-threshold ionization (ATI) peaks using OAM principles.
Main Methods:
- Formulation of a novel variant of the strong field approximation (SFA).
- Derivation of conservation laws for angular momenta in linearly and circularly polarized fields.
- Analysis of the dependence of photoelectron OAM spectra on laser pulse parameters (e.g., duration, polarization).
Main Results:
- Orbital angular momentum of twisted electrons in linear fields is determined by the magnetic quantum number of the initial state.
- A selection rule for circularly polarized fields is related to ATI peaks, offering a new interpretation.
- Photoelectron OAM spectra are sensitive to laser pulse duration and the parity of laser cycles.
Conclusions:
- The study establishes a theoretical foundation for electron OAM in strong field ionization.
- The findings offer insights into controlling and interpreting electron OAM based on laser properties and initial states.
- This work paves the way for advanced control over electron quantum states in laser-matter interactions.
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