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Related Concept Videos

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.
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
There are three main types of inductively coupled plasma atomic emission spectroscopy  (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
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 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...

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Updated: Jun 5, 2026

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

Route to attosecond nonlinear spectroscopy.

F Reiter1, U Graf, E E Serebryannikov

  • 1Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, D-85748 Garching, Germany.

Physical Review Letters
|January 15, 2011
PubMed
Summary
This summary is machine-generated.

Researchers generated deep and vacuum ultraviolet supercontinua using laser pulses. This breakthrough promises powerful subfemtosecond pulses for studying ultrafast phenomena in matter.

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Area of Science:

  • Quantum optics
  • Ultrafast science
  • Atomic, molecular, and optical physics

Background:

  • Generation of coherent light in the deep and vacuum ultraviolet (UV) spectral regions is crucial for advanced spectroscopy.
  • Existing methods often face limitations in terms of pulse energy, coherence, or spectral range.

Purpose of the Study:

  • To demonstrate the generation of microjoule-scale, low-order harmonic supercontinua in the deep and vacuum UV (4-9 eV).
  • To explore the underlying nonlinear physics enabling this process.
  • To pave the way for novel spectroscopic techniques probing ultrafast dynamics.

Main Methods:

  • Nonlinear transformation of near-single-cycle laser pulses within a gas cell.
  • Theoretical modeling to understand the novel nonlinear regime responsible for supercontinuum formation.

Main Results:

  • Successful generation of coherent microjoule-scale supercontinua in the 4-9 eV range.
  • Identification of a novel nonlinear regime governing the supercontinuum generation process.
  • Theoretical validation of the experimental observations.

Conclusions:

  • The demonstrated method enables efficient generation of powerful deep-UV and vacuum UV subfemtosecond pulses.
  • This capability opens new avenues for pump-probe spectroscopy of subfemtosecond-scale valence-shell phenomena.
  • The findings have broad implications for studying ultrafast processes in atoms, molecules, and condensed matter.