Particle detector

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In experimental and applied particle physics, nuclear physics, and nuclear engineering, a particle detector, also known as a radiation detector, is a device used to detect, track, and/or identify ionizing particles, such as those produced by nuclear decay, cosmic radiation, or reactions in a particle accelerator. Detectors can measure the particle energy and other attributes such as momentum, spin, charge, particle type, in addition to merely registering the presence of the particle.

Contents

Examples and types

Summary of particle detector types Detectors summary 3.png
Summary of particle detector types

Many of the detectors invented and used so far are ionization detectors (of which gaseous ionization detectors and semiconductor detectors are most typical) and scintillation detectors; but other, completely different principles have also been applied, like Čerenkov light and transition radiation.

Cloud chambers visualize particles by creating a supersaturated layer of vapor. Particles passing through this region create cloud tracks similar to condensation trails of planes Alpha radiation in a cloud chamber.jpg
Cloud chambers visualize particles by creating a supersaturated layer of vapor. Particles passing through this region create cloud tracks similar to condensation trails of planes
Recording of a bubble chamber at CERN Recording bubble chamber.jpg
Recording of a bubble chamber at CERN

Historical examples

Detectors for radiation protection

The following types of particle detector are widely used for radiation protection, and are commercially produced in large quantities for general use within the nuclear, medical, and environmental fields.

Commonly used detectors for particle and nuclear physics

Modern detectors

Modern detectors in particle physics combine several of the above elements in layers much like an onion.

Research particle detectors

Detectors designed for modern accelerators are huge, both in size and in cost. The term counter is often used instead of detector when the detector counts the particles but does not resolve its energy or ionization. Particle detectors can also usually track ionizing radiation (high energy photons or even visible light). If their main purpose is radiation measurement, they are called radiation detectors, but as photons are also (massless) particles, the term particle detector is still correct.

At colliders

Under construction

Without colliders

On spacecraft

Theoretical Models of Particle Detectors

Beyond their experimental implementations, theoretical models of particle detectors are also of great importance to theoretical physics. These models consider localized non-relativistic quantum systems coupled to a quantum field. [1] They receive the name of particle detectors because when the non-relativistic quantum system is measured in an excited state, one can claim to have detected a particle. [2] [3] The first instance of particle detector models in the literature dates from the 80's, where a particle in a box was introduced by W. G. Unruh in order to probe a quantum field around a black hole. [2] Shortly after, Bryce DeWitt proposed a simplification of the model, [4] giving rise to the Unruh-DeWitt detector model.

Beyond their applications to theoretical physics, particle detector models are related to experimental fields such as quantum optics, where atoms can be used as detectors for the quantum electromagnetic field via the light-matter interaction. From a conceptual side, particle detectors also allow one to formally define the concept of particles without relying on asymptotic states, or representations of a quantum field theory. As M. Scully puts it, from an operational viewpoint one can state that "a particle is what a particle detector detects", [5] which in essence defines a particle as the detection of excitations of a quantum field.

See also

Related Research Articles

<span class="mw-page-title-main">Geiger counter</span> Instrument used for measuring ionizing radiation

A Geiger counter is an electronic instrument used for detecting and measuring ionizing radiation. It is widely used in applications such as radiation dosimetry, radiological protection, experimental physics and the nuclear industry.

<span class="mw-page-title-main">Scintillation counter</span> Instrument for measuring ionizing radiation

A scintillation counter is an instrument for detecting and measuring ionizing radiation by using the excitation effect of incident radiation on a scintillating material, and detecting the resultant light pulses.

<span class="mw-page-title-main">Scintillator</span> Material which glows when excited by ionizing radiation

A scintillator is a material that exhibits scintillation, the property of luminescence, when excited by ionizing radiation. Luminescent materials, when struck by an incoming particle, absorb its energy and scintillate. Sometimes, the excited state is metastable, so the relaxation back down from the excited state to lower states is delayed. The process then corresponds to one of two phenomena: delayed fluorescence or phosphorescence. The correspondence depends on the type of transition and hence the wavelength of the emitted optical photon.

The Unruh effect is a theoretical prediction in quantum field theory that states that an observer who is uniformly accelerating through empty space will perceive a thermal bath. This means that even in the absence of any external heat sources, an accelerating observer will detect particles and experience a temperature. In contrast, an inertial observer in the same region of spacetime would observe no temperature.

A semiconductor detector in ionizing radiation detection physics is a device that uses a semiconductor to measure the effect of incident charged particles or photons.

<span class="mw-page-title-main">Proportional counter</span>

The proportional counter is a type of gaseous ionization detector device used to measure particles of ionizing radiation. The key feature is its ability to measure the energy of incident radiation, by producing a detector output pulse that is proportional to the radiation energy absorbed by the detector due to an ionizing event; hence the detector's name. It is widely used where energy levels of incident radiation must be known, such as in the discrimination between alpha and beta particles, or accurate measurement of X-ray radiation dose.

A wire chamber or multi-wire proportional chamber is a type of proportional counter that detects charged particles and photons and can give positional information on their trajectory, by tracking the trails of gaseous ionization.

<span class="mw-page-title-main">Photodetector</span> Sensors of light or other electromagnetic energy

Photodetectors, also called photosensors, are sensors of light or other electromagnetic radiation. There are a wide variety of photodetectors which may be classified by mechanism of detection, such as photoelectric or photochemical effects, or by various performance metrics, such as spectral response. Semiconductor-based photodetectors typically use a p–n junction that converts photons into charge. The absorbed photons make electron–hole pairs in the depletion region. Photodiodes and photo transistors are a few examples of photo detectors. Solar cells convert some of the light energy absorbed into electrical energy.

<span class="mw-page-title-main">Time projection chamber</span>

In physics, a time projection chamber (TPC) is a type of particle detector that uses a combination of electric fields and magnetic fields together with a sensitive volume of gas or liquid to perform a three-dimensional reconstruction of a particle trajectory or interaction.

The ionization chamber is the simplest type of gaseous ionisation detector, and is widely used for the detection and measurement of many types of ionizing radiation, including X-rays, gamma rays, alpha particles and beta particles. Conventionally, the term "ionization chamber" refers exclusively to those detectors which collect all the charges created by direct ionization within the gas through the application of an electric field. It uses the discrete charges created by each interaction between the incident radiation and the gas to produce an output in the form of a small direct current. This means individual ionising events cannot be measured, so the energy of different types of radiation cannot be differentiated, but it gives a very good measurement of overall ionising effect.

<span class="mw-page-title-main">Gamma spectroscopy</span> Quantitative study of the energy spectra of gamma-ray sources

Gamma-ray spectroscopy is the qualitative study of the energy spectra of gamma-ray sources, such as in the nuclear industry, geochemical investigation, and astrophysics. Gamma-ray spectrometry, on the other hand, is the method used to acquire a quantitative spectrum measurement.

<span class="mw-page-title-main">Gaseous ionization detector</span> Radiation detector

Gaseous ionization detectors are radiation detection instruments used in particle physics to detect the presence of ionizing particles, and in radiation protection applications to measure ionizing radiation.

<span class="mw-page-title-main">ALICE experiment</span> Detector experiments at the Large Hadron Collider

ALICE is one of nine detector experiments at the Large Hadron Collider at CERN. The other eight are: ATLAS, CMS, TOTEM, LHCb, LHCf, MoEDAL, FASER and SND@LHC.

The XENON dark matter research project, operated at the Italian Gran Sasso National Laboratory, is a deep underground detector facility featuring increasingly ambitious experiments aiming to detect hypothetical dark matter particles. The experiments aim to detect particles in the form of weakly interacting massive particles (WIMPs) by looking for rare nuclear recoil interactions in a liquid xenon target chamber. The current detector consists of a dual phase time projection chamber (TPC).

<span class="mw-page-title-main">Neutron detection</span>

Neutron detection is the effective detection of neutrons entering a well-positioned detector. There are two key aspects to effective neutron detection: hardware and software. Detection hardware refers to the kind of neutron detector used and to the electronics used in the detection setup. Further, the hardware setup also defines key experimental parameters, such as source-detector distance, solid angle and detector shielding. Detection software consists of analysis tools that perform tasks such as graphical analysis to measure the number and energies of neutrons striking the detector.

Nuclear MASINT is one of the six major subdisciplines generally accepted to make up Measurement and Signature Intelligence (MASINT), which covers measurement and characterization of information derived from nuclear radiation and other physical phenomena associated with nuclear weapons, reactors, processes, materials, devices, and facilities. Nuclear monitoring can be done remotely or during onsite inspections of nuclear facilities. Data exploitation results in characterization of nuclear weapons, reactors, and materials. A number of systems detect and monitor the world for nuclear explosions, as well as nuclear materials production.

R. Clark Jones was an American physicist working in the field of optics. He studied at Harvard University and received his PhD in 1941. Until 1944 he worked at Bell Labs, later until 1982 with the Polaroid Corporation. In a sequence of publications between 1941 and 1956 he demonstrated a mathematical model to describe the polarization of coherent light, the Jones calculus.

<span class="mw-page-title-main">X-ray detector</span> Instrument that can measure properties of X-rays

X-ray detectors are devices used to measure the flux, spatial distribution, spectrum, and/or other properties of X-rays.

<span class="mw-page-title-main">LZ experiment</span> Experiment in South Dakota, United States

The LUX-ZEPLIN (LZ) Experiment is a next-generation dark matter direct detection experiment hoping to observe weakly interacting massive particles (WIMP) scatters on nuclei. It was formed in 2012 by combining the LUX and ZEPLIN groups. It is currently a collaboration of 30 institutes in the US, UK, Portugal and South Korea. The experiment is located at the Sanford Underground Research Facility (SURF) in South Dakota, and is managed by the United States Department of Energy's (DOE) Lawrence Berkeley National Lab.

References

  1. Martín-Martínez, Eduardo; Montero, Miguel; del Rey, Marco (2013-03-25). "Wavepacket detection with the Unruh-DeWitt model". Physical Review D. 87 (6): 064038. arXiv: 1207.3248 . Bibcode:2013PhRvD..87f4038M. doi:10.1103/PhysRevD.87.064038. S2CID   19334396.
  2. 1 2 Unruh, W. G. (1976-08-15). "Notes on black-hole evaporation". Physical Review D. 14 (4): 870–892. Bibcode:1976PhRvD..14..870U. doi:10.1103/PhysRevD.14.870.
  3. Unruh, William G.; Wald, Robert M. (1984-03-15). "What happens when an accelerating observer detects a Rindler particle". Physical Review D. 29 (6): 1047–1056. Bibcode:1984PhRvD..29.1047U. doi:10.1103/PhysRevD.29.1047.
  4. Irvine, J M (May 1980). "General Relativity – An Einstein Centenary Survey". Physics Bulletin. 31 (4): 140. doi:10.1088/0031-9112/31/4/029. ISSN   0031-9112.
  5. Scully, Marlan O. (2009), Muga, Gonzalo; Ruschhaupt, Andreas; del Campo, Adolfo (eds.), "The Time-Dependent Schrödinger Equation Revisited: Quantum Optical and Classical Maxwell Routes to Schrödinger's Wave Equation", Time in Quantum Mechanics - Vol. 2, Lecture Notes in Physics, Berlin, Heidelberg: Springer, vol. 789, pp. 15–24, doi:10.1007/978-3-642-03174-8_2, ISBN   978-3-642-03174-8 , retrieved 2022-08-19

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