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Related Concept Videos

Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...
Atomic Emission Spectroscopy: Overview01:20

Atomic Emission Spectroscopy: Overview

Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
Atomic Spectroscopy: Absorption, Emission, and Fluorescence01:23

Atomic Spectroscopy: Absorption, Emission, and Fluorescence

Atomic spectroscopy is a vital tool in elemental analysis, both qualitatively and quantitatively. It can be broadly divided into optical spectroscopy, mass spectroscopy, and X-ray spectroscopy methods. The optical spectroscopic methods are atomic absorption spectroscopy (AAS), atomic emission spectroscopy (AES), and atomic fluorescence spectroscopy (AFS). The first step in all three methods is atomization, where the solid, liquid, or solution-phase samples are converted into gas-phase atoms and...
Atomic Absorption Spectroscopy: Radiation and Light Sources01:13

Atomic Absorption Spectroscopy: Radiation and Light Sources

Atomic absorption spectroscopy (AAS) relies on the Beer-Lambert law, which requires that the radiation source emits a narrow range of wavelengths to match the absorption characteristics of the analyte atom. The primary criteria for choosing an appropriate radiation source in AAS is to provide a precise and intense emission at specific wavelengths that will allow accurate detection of the analyte.
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
Atomic Fluorescence Spectroscopy01:29

Atomic Fluorescence Spectroscopy

Atomic fluorescence spectroscopy (AFS) is an analytical technique that involves the electronic transitions of atoms in a flame, furnace, or plasma being excited by electromagnetic (EM) radiation. When these atoms absorb energy, they become excited and subsequently release energy as they return to their original state. This emitted light, or "fluorescence," is observed at a right angle to the incident beam. Both absorption and emission processes transpire at distinct wavelengths, which are...

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Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
06:53

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Published on: July 27, 2018

Laser-induced electron diffraction for probing rare gas atoms.

Junliang Xu1, Cosmin I Blaga, Anthony D DiChiara

  • 1J.R. Macdonald Laboratory, Physics Department, Kansas State University, Manhattan, Kansas 66506-2604, USA.

Physical Review Letters
|February 2, 2013
PubMed
Summary

Laser-induced electron diffraction (LIED) captures molecular vibrations on femtosecond timescales. This study extracts atomic electron-ion differential cross sections, a crucial step for advancing LIED imaging techniques.

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Last Updated: May 14, 2026

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
06:53

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

Published on: July 27, 2018

Synthesis and Microdiffraction at Extreme Pressures and Temperatures
07:26

Synthesis and Microdiffraction at Extreme Pressures and Temperatures

Published on: October 7, 2013

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
08:22

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization

Published on: August 6, 2018

Area of Science:

  • Atomic, Molecular, and Optical Physics
  • Ultrafast Science
  • Chemical Physics

Background:

  • Femtosecond time-resolved molecular imaging is a key goal in ultrafast science.
  • Laser-induced electron diffraction (LIED) has emerged as a promising technique for capturing molecular dynamics.
  • Previous studies demonstrated LIED for molecular snapshots, necessitating a deeper understanding of the underlying atomic processes.

Purpose of the Study:

  • To provide a comprehensive treatment of the atomic laser-induced electron diffraction (LIED) response.
  • To extract electron-ion differential cross sections (DCSs) for rare gas atoms.
  • To establish the foundational elements for generalizing LIED to complex molecular imaging.

Main Methods:

  • Utilizing intense midinfrared lasers to generate high-energy electron momentum distributions from rare gas atoms.
  • Measuring angular-resolved electron momentum distributions following strong-field ionization.
  • Extracting electron-ion differential cross sections (DCSs) from the measured distributions.

Main Results:

  • High-energy electrons arise from elastic rescattering of field-driven wave packets with parent ions.
  • Extracted DCSs for neutral atoms and ions were indistinguishable at recollision energies ≥100 eV, confirming close collision dynamics.
  • The measured DCSs demonstrated independence from laser parameters, aligning with theoretical predictions.

Conclusions:

  • The study successfully extracts atomic electron-ion differential cross sections, validating the LIED mechanism.
  • The findings confirm the close collision nature of electron-ion interactions in LIED.
  • This work lays the groundwork for applying LIED to achieve femtosecond molecular imaging.