Abstract

Using the strong-field approximation we systematically investigate the selection rules for high-order harmonic generation and the symmetry properties of the angle-resolved photoelectron spectra for various atomic and molecular targets exposed to one-component and two-component laser fields. These include bicircular fields and orthogonally polarized two-color fields. The selection rules are derived directly from the dynamical symmetries of the driving field. Alternatively, we demonstrate that they can be obtained using the conservation of the projection of the total angular momentum on the quantization axis. We discuss how the harmonic spectra of atomic targets depend on the type of the ground state or, for molecular targets, on the pertinent molecular orbital. In addition, we briefly discuss some properties of the high-order harmonic spectra generated by a few-cycle laser field. The symmetry properties of the angle-resolved photoelectron momentum distribution are also determined by the dynamical symmetry of the driving field. We consider the first two terms in a Born series expansion of the T matrix, which describe the direct and the rescattered electrons. Dynamical symmetries involving time translation generate rotational symmetries obeyed by both terms. However, those that involve time reversal generate reflection symmetries that are only observed by the direct electrons. Finally, we explain how the symmetry properties, imposed by the dynamical symmetry of the driving field, are altered for molecular targets.

Highlights

  • Symmetry is one of the most prominent concepts in physics, chemistry, and biology [1].Symmetries allow one to simplify a problem and predict a solution without solving it

  • In [24] it was shown how the selection rules for high-order harmonic generation (HHG) of atomic targets exposed to a bicircular field are related to the dynamical symmetry of the field and, alternatively, how they can be derived using conservation of the projection of the angular momentum on the quantization axis

  • Above-threshold ionization of atomic and molecular targets exposed to various laser fields has been analyzed in detail during the past decades

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Summary

Introduction

Symmetry is one of the most prominent concepts in physics, chemistry, and biology [1]. In [24] it was shown how the selection rules for HHG of atomic targets exposed to a bicircular field are related to the dynamical symmetry of the field and, alternatively, how they can be derived using conservation of the projection of the angular momentum on the quantization axis. Above-threshold ionization of atomic and molecular targets exposed to various laser fields has been analyzed in detail during the past decades (see [11,33,34,35,36,37,38] and references therein) In this case, the experimental features where symmetries become manifest include the shape and the spatial symmetries (reflection or rotation) of the angle-resolved spectrum of the liberated electron.

HHG Theory
HATI Theory
Laser Fields and Dynamical Symmetries
Selection Rules for HHG
Derivation of the Selection Rules
Illustration of the Selection Rules
Symmetry Properties of the Photoelectron Momentum Distribution
Symmetries of the Direct and Rescattered Photoelectron Momentum Spectra
Symmetries of the Direct Photoelectron Momentum Spectra
Conclusions
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