First Results from an Axion Haloscope at CAPP around 10.7 μeV
Ohjoon Kwon1, Doyu Lee1, Woohyun Chung1
1Center for Axion and Precision Physics Research (CAPP), IBS, Daejeon 34051, Republic of Korea.
Physical Review Letters
|May 28, 2021
Summary
Researchers searched for axion dark matter using ultralow temperature microwave resonators. This study excludes specific axion mass ranges, marking a first for these ranges and resonator temperatures below 40 mK.
Area of Science:
- Particle Physics
- Cosmology
- Astrophysics
Background:
- Dark matter constitutes a significant portion of the universe's mass.
- Axions are hypothetical elementary particles proposed as a dark matter candidate.
- Ultralow temperature microwave resonators offer a sensitive method for detecting axions.
Purpose of the Study:
- To search for axion dark matter within specific mass ranges.
- To establish new exclusion limits for axion properties.
- To demonstrate the efficacy of ultralow temperature resonators in axion detection.
Main Methods:
- Utilizing the Center for Axion and Precision Physics Research's experimental setup.
- Employing ultralow temperature microwave resonators operating below 40 mK.
- Analyzing data to exclude axion mass ranges with specific coupling sensitivities.
Main Results:
- Exclusion of the axion mass range 10.7126–10.7186 μeV with near Kim-Shifman-Vainshtein-Zakharov (KSVZ) coupling sensitivity.
- Exclusion of the axion mass range 10.16–11.37 μeV with approximately 9 times larger coupling at 90% confidence level.
- Achieved the lowest resonator physical temperature for an axion search to date.
Conclusions:
- The study provides the first axion search results in the reported mass ranges.
- The experiment demonstrates significant progress in axion detection sensitivity and temperature thresholds.
- These findings contribute to narrowing down the parameter space for axion dark matter.
Related Concept Videos
Atomic Nuclei: Larmor Precession Frequency
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession, and the angular frequency...
Thomson's e/m Experiment
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
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...
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
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: 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 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...


