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Related Concept Videos

Atomic Emission Spectroscopy: Overview01:20

Atomic Emission Spectroscopy: Overview

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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...
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Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

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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....
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Emission Spectra02:39

Emission Spectra

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When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
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Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

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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...
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High-Resolution Mass Spectrometry (HRMS)01:15

High-Resolution Mass Spectrometry (HRMS)

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The resolution of a mass spectrometer depends on the efficiency of separating ions with different ion masses. The mass of an atom is approximated to the sum of the masses of protons and neutrons inside, considering the masses of protons and neutrons as equal. However, the masses of the proton (1.6726 × 10−24 g) and neutron (1.6749 × 10−24 g) are not truly equal. There is a minor error in the expression of atomic masses relative to the simplest atom of hydrogen. For...
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Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

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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.
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Updated: Jun 5, 2025

Applying X-ray Imaging Crystal Spectroscopy for Use as a High Temperature Plasma Diagnostic
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High-Statistics Measurement of the Cosmic-Ray Electron Spectrum with H.E.S.S.

F Aharonian1,2,3, F Ait Benkhali4, J Aschersleben5

  • 1Dublin Institute for Advanced Studies, 31 Fitzwilliam Place, Dublin 2, Ireland.

Physical Review Letters
|December 13, 2024
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Summary
This summary is machine-generated.

High-energy cosmic-ray electrons and positrons (CRe) were measured up to 40 TeV. The spectrum shows a break around 1 TeV, providing constraints on nearby accelerators and dark matter.

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Area of Science:

  • Astrophysics
  • Particle Physics
  • Cosmic Ray Physics

Background:

  • Cosmic-ray electrons and positrons (CRe) at very high energies are crucial for probing local accelerators.
  • Their rapid cooling limits propagation, making them sensitive probes of nearby sources and exotic physics like dark matter annihilation.
  • Understanding the CRe spectrum provides insights into astrophysical processes and fundamental physics.

Purpose of the Study:

  • To present a high-statistics measurement of the cosmic-ray electron and positron spectrum from 0.3 to 40 TeV.
  • To search for spectral features that could indicate nearby CRe accelerators or exotic production mechanisms.
  • To constrain models of CRe propagation and potential dark matter signals.

Main Methods:

  • Utilized the High Energy Stereoscopic System (H.E.S.S.) for data collection.
  • Achieved a proton rejection power exceeding 10^4.
  • Analyzed the CRe spectrum over two orders of magnitude in energy.

Main Results:

  • The measured CRe spectrum from 0.3 to 40 TeV is well-described by a broken power law.
  • A spectral break was observed around 1 TeV, with the spectral index changing from 3.25±0.02(stat)±0.2(sys) to 4.49±0.04(stat)±0.2(sys).
  • No other distinct spectral features were found at multi-TeV energies.

Conclusions:

  • The observed spectral break provides information about the energy spectrum of local cosmic-ray sources.
  • The absence of additional features constrains the existence of nearby CRe accelerators and exotic propagation models.
  • The results place limits on dark matter annihilation scenarios contributing to the local CRe flux.