On the molecular information revealed by photoelectron angular distributions of isotropic samples

TL;DR

This paper introduces a new approach to analyze photoelectron angular distributions from isotropic samples, revealing molecular information through the $b_{l,m}$ coefficients without explicit partial wave expansion.

Contribution

It presents a vector field-based method to interpret PADs, linking molecular rotational invariants to experimental setup parameters, applicable to one- and two-photon ionization.

Findings

$b_{0,0}$ depends on the magnitude of $oldsymbol{D}(oldsymbol{k})$

$b_{1,0}$ is sensitive to the perpendicular components of $oldsymbol{D}(oldsymbol{k})$ in chiral molecules

$b_{2,0}$ relates to the component of $oldsymbol{D}(oldsymbol{k})$ along $oldsymbol{k}$

Abstract

We propose an alternative approach to the description and analysis of photoelectron angular distributions (PADs) resulting from isotropic samples in the case of few-photon absorption via electric fields of arbitrary polarization. As we demonstrate for the one- and two-photon cases, this approach reveals the molecular frame information encoded in the $b_{l,m}$ expansion coefficients of the PAD in a particularly clear way. Our approach does not rely on explicit partial wave expansions of the scattering wave function and the expressions we obtain are therefore interpreted in terms of the vector field structure of the photoionization dipole $\vec{D}(\vec{k})$ as a function of the photoelectron momentum $\vec{k}$. This provides very compact expressions that reveal how molecular rotational invariants couple to the setup (electric field polarization and detectors) rotational invariants. We rely heavily on this approach in a companion paper on tensorial chiral setups. Here we apply this approach to one-photon ionization and find that while $b_{0,0}$ depends only on the magnitude of $\vec{D}(\vec{k})$, $b_{1,0}$ (non-zero for chiral molecules) is sensitive only to the components of $\vec{D}(\vec{k})$ perpendicular to $\vec{k}$ encoded in the propensity field $\vec{B}(\vec{k})\equiv i\vec{D}^{*}(\vec{k})\times\vec{D}(\vec{k})$, and $b_{2,0}$ is sensitive only to the the component of $\vec{D}(\vec{k})$ along $\vec{k}$. We also analyze the resonantly enhanced two-photon case where we show that $b_{0,0}$ and $b_{1,0}$ can be written in terms of an effectively stretched $\vec{D}(\vec{k})$, and that $b_{1,0}$ and $b_{3,0}$ reveal structural information of the field $\vec{B}(\vec{k})$ encoded in three of its vector spherical harmonic expansion coefficients.