PAMELA detector

Last updated

PAMELA
PamLogo A1blu3.png
PAMELAonResurs-DK.jpg
OrganizationPAMELA group
Mission Type Cosmic Ray
Host Satellite Resurs DK1
Launch15 June 2006
Launch vehicle Soyuz-FG
Launch site Baikonur Cosmodrome
Mission duration3 years (planned),
9 years, 7 months and 23 days (achieved)
Mission end7 February 2016
Mass 470 kg
Max length1300 mm
Power consumption335 Watts
Webpage PAMELA homepage
Orbital elements (Resurs DK1)
Inclination 70 degrees
Orbit quasi-polar elliptical
Min altitude360 km
Max altitude604 km
Period94.02 min

PAMELA (Payload for Antimatter Matter Exploration and Light-nuclei Astrophysics) was a cosmic ray research module attached to an Earth orbiting satellite. PAMELA was launched on 15 June 2006 and was the first satellite-based experiment dedicated to the detection of cosmic rays, with a particular focus on their antimatter component, in the form of positrons and antiprotons. Other objectives included long-term monitoring of the solar modulation of cosmic rays, measurements of energetic particles from the Sun, high-energy particles in Earth's magnetosphere and Jovian electrons. It was also hoped that it may detect evidence of dark matter annihilation. [1] PAMELA operations were terminated in 2016, [2] as were the operations of the host-satellite Resurs-DK1. The experiment was a recognized CERN experiment (RE2B). [3] [4]

Contents

Development and launch

PAMELA was the largest device up to the time built by the Wizard collaboration, which includes Russia, Italy, Germany and Sweden and has been involved in many satellite and balloon-based cosmic ray experiments such as Fermi-GLAST. The 470 kg, US$32 million (EU€24.8 million, UK£16.8 million) instrument was originally projected to have a three-year mission. However, this durable module remained operational and made significant scientific contributions until 2016.

PAMELA is mounted on the upward-facing side of the Resurs-DK1 Russian satellite. [1] It was launched by a Soyuz rocket from Baikonur Cosmodrome on 15 June 2006. PAMELA has been put in a polar elliptical orbit at an altitude between 350 and 610 km, with an inclination of 70°.

Design

The apparatus is 1.3 m high, has a total mass of 470 kg and a power consumption of 335 W. The instrument is built around a permanent magnet spectrometer with a silicon microstrip tracker that provides rigidity and dE/dx information. At its bottom is a silicon-tungsten imaging calorimeter, a neutron detector and a shower tail scintillator to perform lepton/hadron discrimination. A Time of Flight (ToF), made of three layers of plastic scintillators, is used to measure the velocity and charge of the particle. An anticounter system made of scintillators surrounding the apparatus is used to reject false triggers and albedo particles during off-line analysis. [5]

Sensitivity [1]
ParticleEnergy Range
Antiproton flux80 MeV – 190 GeV
Positron flux50 MeV – 270 GeV
Electron fluxup to 400 GeV
Proton fluxup to 700 GeV
Electron/positron fluxup to 2 TeV
Light nuclei (up to Z=6)up to 200 GeV/n
Light isotopes (D, 3He)up to 1 GeV/n
Antinuclei searchsensitivity better than 10−7 antiHe/He

Results

Preliminary data (released August 2008, ICHEP Philadelphia) indicate an excess of positrons in the range 10–60 GeV. This is thought to be a possible sign of dark matter annihilation: [6] [7] hypothetical WIMPs colliding with and annihilating each other to form gamma rays, matter and antimatter particles. Another explanation considered for the indication mentioned above is the production of electron-positron pairs on pulsars with subsequent acceleration in the vicinity of the pulsar.

The first two years of data were released in October 2008 in three publications. [8] [9] The positron excess was confirmed and found to persist up to 90 GeV. Surprisingly, no excess of antiprotons was found. This is inconsistent with predictions from most models of dark matter sources, in which the positron and antiproton excesses are correlated.

A paper, published on 15 July 2011, confirmed earlier speculation that the Van Allen belt could confine a significant flux of antiprotons produced by the interaction of the Earth's upper atmosphere with cosmic rays. [10] The energy of the antiprotons has been measured in the range of 60–750 MeV. Cosmic rays collide with atoms in the upper atmosphere creating antineutrons, which in turn decay to produce the antiprotons. They were discovered in a part of the Van Allen belt closest to Earth. [11] When an antiproton interacts with a normal particle, both are annihilated. Data from PAMELA indicated that these annihilation events occurred a thousand times more often than would be expected in the absence of antimatter. The data that contained evidence of antimatter were gathered between July 2006 and December 2008. [12] [13]

Boron and carbon flux measurements were published in July 2014, [14] important to explaining trends in cosmic ray positron fraction. [15]

The summary document of the operations of PAMELA was published in 2017. [2]

Sources of error

Between 1 and 100 GeV, PAMELA is exposed to one hundred times as many electrons as antiprotons. At 1 GeV there are one thousand times as many protons as positrons and at 100 GeV ten thousand times as many. Therefore, to correctly determine the antimatter abundances, it is critical that PAMELA is able to reject the matter background. The PAMELA collaboration claimed in "The electron hadron separation performance of the PAMELA electromagnetic calorimeter" that less than one proton in 100,000 is able to pass the calorimeter selection and be misidentified as a positron when the energy is less than 200 GeV.

The ratio of matter to antimatter in cosmic rays of energy less than 10 GeV that reach PAMELA from outside the Solar System depends on solar activity and in particular on the point in the 11 year solar cycle. The PAMELA team has invoked this effect to explain the discrepancy between their low energy results and those obtained by CAPRICE, HEAT and AMS-01 , which were collected during that half of the cycle when the solar magnetic field had the opposite polarity. It is important to note that these results are consistent with the series of positron / electron measurements obtain by AESOP, which has spanned coverage over both polarities. Also the PAMELA experiment has contradicted an earlier claim by the HEAT experiment of anomalous positrons in the 6 GeV to 10 GeV range.

See also

Related Research Articles

<span class="mw-page-title-main">Antimatter</span> Material composed of antiparticles of the corresponding particles of ordinary matter

In modern physics, antimatter is defined as matter composed of the antiparticles of the corresponding particles in "ordinary" matter, and can be thought of as matter with reversed charge, parity, and time, known as CPT reversal. Antimatter occurs in natural processes like cosmic ray collisions and some types of radioactive decay, but only a tiny fraction of these have successfully been bound together in experiments to form antiatoms. Minuscule numbers of antiparticles can be generated at particle accelerators; however, total artificial production has been only a few nanograms. No macroscopic amount of antimatter has ever been assembled due to the extreme cost and difficulty of production and handling. Nonetheless, antimatter is an essential component of widely-available applications related to beta decay, such as positron emission tomography, radiation therapy, and industrial imaging.

<span class="mw-page-title-main">Antiparticle</span> Particle with opposite charges

In particle physics, every type of particle is associated with an antiparticle with the same mass but with opposite physical charges. For example, the antiparticle of the electron is the positron. While the electron has a negative electric charge, the positron has a positive electric charge, and is produced naturally in certain types of radioactive decay. The opposite is also true: the antiparticle of the positron is the electron.

<span class="mw-page-title-main">Neutrino</span> Elementary particle with extremely low mass

A neutrino is a fermion that interacts only via the weak interaction and gravity. The neutrino is so named because it is electrically neutral and because its rest mass is so small (-ino) that it was long thought to be zero. The rest mass of the neutrino is much smaller than that of the other known elementary particles. The weak force has a very short range, the gravitational interaction is extremely weak due to the very small mass of the neutrino, and neutrinos do not participate in the electromagnetic interaction or the strong interaction. Thus, neutrinos typically pass through normal matter unimpeded and undetected.

<span class="mw-page-title-main">Positron</span> Anti-particle to the electron

The positron or antielectron is the particle with an electric charge of +1e, a spin of 1/2, and the same mass as an electron. It is the antiparticle of the electron. When a positron collides with an electron, annihilation occurs. If this collision occurs at low energies, it results in the production of two or more photons.

<span class="mw-page-title-main">Cosmic ray</span> High-energy particle, mainly originating outside the Solar system

Cosmic rays or astroparticles are high-energy particles or clusters of particles that move through space at nearly the speed of light. They originate from the Sun, from outside of the Solar System in our own galaxy, and from distant galaxies. Upon impact with Earth's atmosphere, cosmic rays produce showers of secondary particles, some of which reach the surface, although the bulk are deflected off into space by the magnetosphere or the heliosphere.

<span class="mw-page-title-main">Antihydrogen</span> Exotic particle made of an antiproton and positron

Antihydrogen is the antimatter counterpart of hydrogen. Whereas the common hydrogen atom is composed of an electron and proton, the antihydrogen atom is made up of a positron and antiproton. Scientists hope that studying antihydrogen may shed light on the question of why there is more matter than antimatter in the observable universe, known as the baryon asymmetry problem. Antihydrogen is produced artificially in particle accelerators.

<span class="mw-page-title-main">Antiproton</span> Subatomic particle

The antiproton,
p
, is the antiparticle of the proton. Antiprotons are stable, but they are typically short-lived, since any collision with a proton will cause both particles to be annihilated in a burst of energy.

ATHENA, also known as the AD-1 experiment, was an antimatter research project at the Antiproton Decelerator at CERN, Geneva. In August 2002, it was the first experiment to produce 50,000 low-energy antihydrogen atoms, as reported in Nature. In 2005, ATHENA was disbanded and many of the former members of the research team worked on the subsequent ALPHA experiment and AEgIS experiment.

<span class="mw-page-title-main">Protonium</span> Bound state of a proton and antiprotron

Protonium, also known as antiprotonic hydrogen, is a type of exotic atom in which a proton and an antiproton orbit each other. Since protonium is a bound system of a particle and its corresponding antiparticle, it is an example of a type of exotic atom called an onium.

<span class="mw-page-title-main">Alpha Magnetic Spectrometer</span> Particle detector on the International Space Station

The Alpha Magnetic Spectrometer (AMS-02) is a particle physics experiment module that is mounted on the International Space Station (ISS). The experiment is a recognized CERN experiment (RE1). The module is a detector that measures antimatter in cosmic rays; this information is needed to understand the formation of the Universe and search for evidence of dark matter.

<span class="mw-page-title-main">Gravitational interaction of antimatter</span> Theory of gravity on antimatter

The gravitational interaction of antimatter with matter or antimatter has been observed by physicists. As was the consensus among physicists previously, it was experimentally confirmed that gravity attracts both matter and antimatter at the same rate within experimental error.

<span class="mw-page-title-main">LHCf experiment</span>

The LHCf is a special-purpose Large Hadron Collider experiment for astroparticle physics, and one of nine detectors in the LHC accelerator at CERN. LHCf is designed to study the particles generated in the forward region of collisions, those almost directly in line with the colliding proton beams.

<span class="mw-page-title-main">Antiproton Decelerator</span> Particle storage ring at CERN, Switzerland

The Antiproton Decelerator (AD) is a storage ring at the CERN laboratory near Geneva. It was built from the Antiproton Collector (AC) to be a successor to the Low Energy Antiproton Ring (LEAR) and started operation in the year 2000. Antiprotons are created by impinging a proton beam from the Proton Synchrotron on a metal target. The AD decelerates the resultant antiprotons to an energy of 5.3 MeV, which are then ejected to one of several connected experiments.

<span class="mw-page-title-main">Cosmic-ray observatory</span> Installation built to detect high-energy-particles coming from space

A cosmic-ray observatory is a scientific installation built to detect high-energy-particles coming from space called cosmic rays. This typically includes photons, electrons, protons, and some heavier nuclei, as well as antimatter particles. About 90% of cosmic rays are protons, 9% are alpha particles, and the remaining ~1% are other particles.

Atomic Spectroscopy and Collisions Using Slow Antiprotons (ASACUSA), AD-3, is an experiment at the Antiproton Decelerator (AD) at CERN. The experiment was proposed in 1997, started collecting data in 2002 by using the antiprotons beams from the AD, and will continue in future under the AD and ELENA decelerator facility.

High-precision experiments could reveal small previously unseen differences between the behavior of matter and antimatter. This prospect is appealing to physicists because it may show that nature is not Lorentz symmetric.

<span class="mw-page-title-main">Breit–Wheeler process</span> Electron-positron production from two photons

The Breit–Wheeler process or Breit–Wheeler pair production is a proposed physical process in which a positron–electron pair is created from the collision of two photons. It is the simplest mechanism by which pure light can be potentially transformed into matter. The process can take the form γ γ′ → e+ e where γ and γ′ are two light quanta.

<span class="mw-page-title-main">Calorimetric Electron Telescope</span> 2015 Japanese space observatory

The CALorimetric Electron Telescope (CALET) is a space telescope being mainly used to perform high precision observations of electrons and gamma rays. It tracks the trajectory of electrons, protons, nuclei, and gamma rays and measures their direction, charge and energy, which may help understand the nature of dark matter or nearby sources of high-energy particle acceleration.

AEgIS, AD-6, is an experiment at the Antiproton Decelerator facility at CERN. Its primary goal is to measure directly the effect of Earth's gravitational field on antihydrogen atoms with significant precision. Indirect bounds that assume the validity of, for example, the universality of free fall, the Weak Equivalence Principle or CPT symmetry also in the case of antimatter constrain an anomalous gravitational behavior to a level where only precision measurements can provide answers. Vice versa, antimatter experiments with sufficient precision are essential to validate these fundamental assumptions. AEgIS was originally proposed in 2007. Construction of the main apparatus was completed in 2012. Since 2014, two laser systems with tunable wavelengths and synchronized to the nanosecond for specific atomic excitation have been successfully commissioned.

Indirect detection of dark matter is a method of searching for dark matter that focuses on looking for the products of dark matter interactions rather than the dark matter itself. Contrastingly, direct detection of dark matter looks for interactions of dark matter directly with atoms. There are experiments aiming to produce dark matter particles using colliders. Indirect searches use various methods to detect the expected annihilation cross sections for weakly interacting massive particles (WIMPs). It is generally assumed that dark matter is stable, that dark matter interacts with Standard Model particles, that there is no production of dark matter post-freeze-out, and that the universe is currently matter-dominated, while the early universe was radiation-dominated. Searches for the products of dark matter interactions are profitable because there is an extensive amount of dark matter present in the universe, and presumably, a lot of dark matter interactions and products of those interactions ; and many currently operational telescopes can be used to search for these products. Indirect searches help to constrain the annihilation cross section the lifetime of dark matter , as well as the annihilation rate.

References

  1. 1 2 3 Vincenzo Buttaro (ed.). "The Space Mission PAMELA" . Retrieved 4 September 2009.
  2. 1 2 Adriani, O; et al. (PAMELA Collaboration) (2018). "Ten Years of PAMELA in Space". Rivista del Nuovo Cimento. 10 (2017): 473–522. arXiv: 1801.10310 . Bibcode:2018arXiv180110310A. doi:10.1393/ncr/i2017-10140-x. S2CID   119078426.
  3. "Recognized Experiments at CERN". The CERN Scientific Committees. CERN. Retrieved 20 January 2020.
  4. "RE2B/PAMELA : A Payload for Antimatter Matter Exploration and Light-nuclei Astrophysics". CERN. Retrieved 20 January 2020.
  5. Casolino, M; et al. (2008). "Launch of the Space experiment PAMELA". Advances in Space Research. 42 (3): 455–466. arXiv: 0708.1808 . Bibcode:2008AdSpR..42..455C. doi:10.1016/j.asr.2007.07.023. S2CID   119608020.
  6. Brumfiel, Geoff (14 August 2008). "Physicists await dark-matter confirmation". Nature. 454 (7206): 808–809. doi: 10.1038/454808b . PMID   18704050.
  7. Cholis, Ilias; Finkbeiner, Douglas P; Goodenough, Lisa; Weiner, Neal (2009). "The PAMELA Positron Excess from Annihilations into a Light Boson". Journal of Cosmology and Astroparticle Physics. 2009 (12): 007. arXiv: 0810.5344 . Bibcode:2009JCAP...12..007C. doi:10.1088/1475-7516/2009/12/007. S2CID   73574983.
  8. Casolino, M; et al. (2008). "Two years of flight of the Pamela experiment: Results and perspectives". Journal of the Physical Society of Japan. 78: 35–40. arXiv: 0810.4980 . Bibcode:2009JPSJ...78S..35C. doi:10.1143/JPSJS.78SA.35. S2CID   119187767.
  9. Adriani, O; et al. (2009). "Observation of an anomalous positron abundance in the cosmic radiation". Nature. 458 (7238): 607–609. arXiv: 0810.4995 . Bibcode:2009Natur.458..607A. doi:10.1038/nature07942. PMID   19340076. S2CID   11675154.
  10. Adriani, O.; et al. (2011). "The Discovery of Geomagnetically Trapped Cosmic-Ray Antiprotons". The Astrophysical Journal Letters. 737 (2): L29. arXiv: 1107.4882 . Bibcode:2011ApJ...737L..29A. doi:10.1088/2041-8205/737/2/L29.
  11. Than, Ker (10 August 2011). "Antimatter Found Orbiting Earth—A First". National Geographic Society. Archived from the original on 10 October 2011. Retrieved 12 August 2011.
  12. Cowen, Ron (9 August 2011). "Antimatter Belt Found Circling Earth". Science . Archived from the original on 24 October 2011. Retrieved 12 August 2011.
  13. Chung, Emily (8 August 2011). "Antimatter belt surrounds Earth". CBC News . Retrieved 12 August 2011.
  14. Adriani, O; et al. (31 July 2014). "Measurement of Boron and Carbon Fluxes in Cosmic Rays with the Pamela Experiment". Astrophysical Journal. 791 (2): 93. arXiv: 1407.1657 . Bibcode:2014ApJ...791...93A. doi:10.1088/0004-637X/791/2/93. S2CID   53002540.
  15. Cholis, Ilias; Hooper, Dan (24 February 2014). "Constraining the origin of the rising cosmic ray positron fraction with the boron-to-carbon ratio". Physical Review D. 89 (4): 043013. arXiv: 1312.2952 . Bibcode:2014PhRvD..89d3013C. doi:10.1103/PhysRevD.89.043013. S2CID   96470471.