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Related Concept Videos

Atomic Absorption Spectroscopy: Interference01:25

Atomic Absorption Spectroscopy: Interference

Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
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 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.
Interference and Diffraction02:18

Interference and Diffraction

Interference is a characteristic phenomenon exhibited by waves. When two electromagnetic waves interact with their peaks and troughs coinciding, a resulting wave with enhanced amplitude is produced. This is known as constructive interference. In this case, the two waves interacting are in phase with each other.
Atomic Absorption Spectroscopy: Atomization Methods01:25

Atomic Absorption Spectroscopy: Atomization Methods

Atomic Absorption Spectroscopy (AAS) atomizes samples through flame atomization or electrothermal atomization. Flame atomization typically involves a nebulizer and spray chamber assembly to combine the sample with a fuel–oxidant mixture, creating a fine aerosol mist that enters a burner. Typically, the fuel and oxidant are combined in an approximately stoichiometric ratio. However, for atoms that are easily oxidized, a fuel-rich mixture may be more advantageous. Only about 5% of the aerosol...
Atomic Emission Spectroscopy: Interference01:30

Atomic Emission Spectroscopy: Interference

In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...

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Related Experiment Video

Updated: Jun 19, 2026

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
12:14

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry

Published on: August 12, 2013

A prototype differential atom interferometer for fundamental physics.

C F A Baynham1, R Hobson1, O Buchmüller2

  • 1Department of Physics, Imperial College London, London, UK.

Nature
|June 17, 2026
PubMed
Summary
This summary is machine-generated.

Researchers developed a prototype differential atom interferometer using strontium-87 atoms. This device demonstrates noise-immune operation, crucial for detecting gravitational waves and ultralight dark matter with future long-baseline atom interferometers.

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Implementation of a Reference Interferometer for Nanodetection
16:11

Implementation of a Reference Interferometer for Nanodetection

Published on: April 26, 2014

Related Experiment Videos

Last Updated: Jun 19, 2026

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
12:14

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry

Published on: August 12, 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

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Implementation of a Reference Interferometer for Nanodetection

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Area of Science:

  • Fundamental Physics
  • Quantum Sensing
  • Astrophysics

Background:

  • Gravitational waves and ultralight dark matter are key research areas in fundamental physics.
  • Very-long-baseline atom interferometers are proposed for detecting signals at frequencies where other interferometers are less sensitive.
  • Laser phase noise is a critical noise source that challenges the performance of these atom interferometers.

Purpose of the Study:

  • To experimentally validate noise rejection techniques for very-long-baseline atom interferometers.
  • To demonstrate a prototype differential atom interferometer capable of operating at the quantum limit.
  • To advance the development of next-generation quantum sensors for gravitational-wave detection and dark matter searches.

Main Methods:

  • Demonstrated a prototype differential atom interferometer using the single-photon clock transition of fermionic strontium-87.
  • Configured the instrument as a gradiometer suitable for kilometer-scale and space-baseline operations.
  • Artificially injected significant laser phase noise to emulate conditions in very-long-baseline atom interferometers.

Main Results:

  • The interferometer operated at the standard quantum limit with no excess noise beyond atom shot noise.
  • Quantum-limited sensitivity was maintained despite several radians of injected laser phase noise.
  • Coherent oscillatory signals were recovered across a broad frequency range under phase-randomized conditions.

Conclusions:

  • Experimental validation of the noise-immune measurement principle for very-long-baseline atom interferometers was achieved.
  • The prototype demonstrates a significant step towards next-generation quantum sensors.
  • This technology holds promise for gravitational-wave detection and ultralight dark matter searches.