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Atomic Emission Spectroscopy: Overview01:20

Atomic Emission Spectroscopy: Overview

1.7K
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...
1.7K
Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

152
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...
152
The de Broglie Wavelength02:32

The de Broglie Wavelength

25.4K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.4K
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

582
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
582
Detection of Black Holes01:10

Detection of Black Holes

2.2K
Although black holes were theoretically postulated in the 1920s, they remained outside the domain of observational astronomy until the 1970s.
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
2.2K
Atomic Absorption Spectroscopy: Radiation and Light Sources01:13

Atomic Absorption Spectroscopy: Radiation and Light Sources

367
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...
367

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Related Experiment Video

Updated: Jun 16, 2025

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

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Experimental Search for Invisible Dark Matter Axions around 22  μeV.

Younggeun Kim1, Junu Jeong1, SungWoo Youn1

  • 1Center for Axion and Precision Physics Research, <a href="https://ror.org/00y0zf565">IBS</a>, Daejeon 34051, Republic of Korea.

Physical Review Letters
|August 19, 2024
PubMed
Summary
This summary is machine-generated.

This study searched for dark matter axions, hypothetical particles solving key physics problems. The experiment ruled out a specific axion mass range, contributing to the ongoing search for these elusive cosmic components.

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Related Experiment Videos

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Area of Science:

  • Particle Physics
  • Cosmology
  • Astroparticle Physics

Background:

  • Axions are leading candidates for dark matter and solutions to the strong CP problem.
  • Theoretical efforts suggest axion masses between 20-30 μeV.
  • Previous research has focused on constraining axion properties through various cosmological assumptions.

Purpose of the Study:

  • To experimentally search for dark matter axions within the theoretically predicted mass range of 20-30 μeV.
  • To probe the axion-photon coupling via a sensitive haloscope experiment.

Main Methods:

  • Utilized a multicell cavity haloscope immersed in a 12 Tesla magnetic field.
  • Searched for microwave signals generated by the coupling of axions to photons.
  • Focused on the mass region between 21.86 and 22.00 μeV.

Main Results:

  • Ruled out KSVZ axions as dark matter within the probed mass range (21.86–22.00 μeV) at 90% confidence level.
  • The experiment achieved high sensitivity, guided by specific theoretical predictions.
  • Provided stringent constraints on the properties of potential dark matter axions.

Conclusions:

  • The experimental search did not find evidence for KSVZ axions in the targeted mass range.
  • This result contributes to narrowing down the possible parameter space for dark matter axions.
  • Further experimental efforts are needed to explore other mass ranges and axion models.