In particle physics, antimatter is material composed of
antiparticles, which have the same mass as particles of ordinary matter but
have opposite charge and quantum spin. Antiparticles bind with each other to
form antimatter in the same way that normal particles bind to form normal
matter. For example, a positron (the antiparticle of the electron, with symbol
e+) and an antiproton (symbol p) can form an antihydrogen atom. Furthermore,
mixing matter and antimatter can lead to the annihilation of both, in the same
way that mixing antiparticles and particles does, thus giving rise to
high-energy photons (gamma rays) or other particle–antiparticle pairs. The end
result of antimatter meeting matter is a release of energy proportional to the
mass as the mass-energy equivalence equation, E=mc2 shows.[1]
There is considerable speculation as to why the observable
universe is apparently composed almost entirely of matter (as opposed to a
mixture of matter and antimatter), whether there exist other places that are
almost entirely composed of antimatter instead, and what sorts of technology
might be possible if antimatter could be harnessed. At this time, the apparent
asymmetry of matter and antimatter in the visible universe is one of the
greatest unsolved problems in physics.[2] The process by which this asymmetry
between particles and antiparticles developed is called baryogenesis.
There are some 500 terrestrial gamma-ray flashes daily. The
red dots show those the Fermi Gamma-ray Space Telescope spotted through 2010.
Learn how scientists used the Fermi Gamma-ray Space
Telescope's gamma-ray detector to uncover bursts of antimatter from
thunderstorms.
History of the concept
The idea of negative matter appears in past theories of
matter that have now been abandoned. Using the once popular vortex theory of
gravity, the possibility of matter with negative gravity was discussed by
William Hicks in the 1880s. Between the 1880s and the 1890s, Karl Pearson
proposed the existence of "squirts" (sources) and sinks of the flow
of aether. The squirts represented normal matter and the sinks represented negative
matter. Pearson's theory required a fourth dimension for the aether to flow
from and into.[3]
The term antimatter was first used by Arthur Schuster in two
rather whimsical letters to Nature in 1898,[4] in which he coined the term. He
hypothesized antiatoms, as well as whole antimatter solar systems, and
discussed the possibility of matter and antimatter annihilating each other.
Schuster's ideas were not a serious theoretical proposal, merely speculation,
and like the previous ideas, differed from the modern concept of antimatter in
that it possessed negative gravity.[5]
The modern theory of antimatter began in 1928, with a
paper[6] by Paul Dirac. Dirac realised that his relativistic version of the
Schrödinger wave equation for electrons predicted the possibility of
antielectrons. These were discovered by Carl D. Anderson in 1932 and named
positrons (a contraction of "positive electrons"). Although Dirac did
not himself use the term antimatter, its use follows on naturally enough from
antielectrons, antiprotons, etc.[7] A complete periodic table of antimatter was
envisaged by Charles Janet in 1929.[8]
Notation
One way to denote an antiparticle is by adding a bar over
the particle's symbol. For example, the proton and antiproton are denoted as p
and p, respectively. The same rule applies if one were to address a particle by
its constituent components. A proton is made up of uud quarks, so an antiproton
must therefore be formed from uud antiquarks. Another convention is to
distinguish particles by their electric charge. Thus, the electron and positron
are denoted simply as e− and e+ respectively. However, to prevent confusion,
the two conventions are never mixed.
Origin and asymmetry
Almost all matter observable from the Earth seems to be made
of matter rather than antimatter. If antimatter-dominated regions of space
existed, the gamma rays produced in annihilation reactions along the boundary
between matter and antimatter regions would be detectable.[9]
Antiparticles are created everywhere in the universe where
high-energy particle collisions take place. High-energy cosmic rays impacting
Earth's atmosphere (or any other matter in the Solar System) produce minute
quantities of antiparticles in the resulting particle jets, which are
immediately annihilated by contact with nearby matter. They may similarly be
produced in regions like the center of the Milky Way and other galaxies, where
very energetic celestial events occur (principally the interaction of
relativistic jets with the interstellar medium). The presence of the resulting
antimatter is detectable by the two gamma rays produced every time positrons
annihilate with nearby matter. The frequency and wavelength of the gamma rays
indicate that each carries 511 keV of energy (i.e., the rest mass of an
electron multiplied by c2).
Recent observations by the European Space Agency's INTEGRAL
satellite may explain the origin of a giant cloud of antimatter surrounding the
galactic center. The observations show that the cloud is asymmetrical and
matches the pattern of X-ray binaries (binary star systems containing black
holes or neutron stars), mostly on one side of the galactic center. While the
mechanism is not fully understood, it is likely to involve the production of
electron–positron pairs, as ordinary matter gains tremendous energy while
falling into a stellar remnant.[10][11]
Antimatter may exist in relatively large amounts in far-away
galaxies due to cosmic inflation in the primordial time of the universe.
Antimatter galaxies, if they exist, are expected to have the same chemistry and
absorption and emission spectra as normal-matter galaxies, and their
astronomical objects would be observationally identical, making them difficult
to distinguish.[12] NASA is trying to determine if such galaxies exist by
looking for X-ray and gamma-ray signatures of annihilation events in colliding superclusters.[13]
Natural production
Positrons are produced naturally in β+ decays of naturally
occurring radioactive isotopes (for example, potassium-40) and in interactions
of gamma quanta (emitted by radioactive nuclei) with matter. Antineutrinos are another
kind of antiparticle created by natural radioactivity (β− decay). Many
different kinds of antiparticles are also produced by (and contained in) cosmic
rays. Recent (as of January 2011) research by the American Astronomical Society
has discovered antimatter (positrons) originating above thunderstorm clouds;
positrons are produced in gamma-ray flashes created by electrons accelerated by
strong electric fields in the clouds.[14] Antiprotons have also been found to
exist in the Van Allen Belts around the Earth by the PAMELA module.[15][16]
Artificial production
Antiparticles are also produced in any environment with a
sufficiently high temperature (mean particle energy greater than the pair
production threshold). During the period of baryogenesis, when the universe was
extremely hot and dense, matter and antimatter were continually produced and
annihilated. The presence of remaining matter, and absence of detectable
remaining antimatter,[17] also called baryon asymmetry, is attributed to
violation of the CP-symmetry relating matter to antimatter. The exact mechanism
of this violation during baryogenesis remains a mystery.
Positrons can also be produced by radioactive β+ decay, but
this mechanism can occur both naturally and artificially.
Positrons
Main article: Positron
Positrons were reported[18] in November 2008 to have been
generated by Lawrence Livermore National Laboratory in larger numbers than by
any previous synthetic process. A laser drove electrons through a
millimeter-radius gold target's nuclei, which caused the incoming electrons to
emit energy quanta that decayed into both matter and antimatter. Positrons were
detected at a higher rate and in greater density than ever previously detected
in a laboratory. Previous experiments made smaller quantities of positrons
using lasers and paper-thin targets; however, new simulations showed that
short, ultra-intense lasers and millimeter-thick gold are a far more effective
source.[19]
Antiprotons, antineutrons, and antinuclei
Main articles: Antiproton and Antineutron
The existence of the antiproton was experimentally confirmed
in 1955 by University of California, Berkeley physicists Emilio Segrè and Owen
Chamberlain, for which they were awarded the 1959 Nobel Prize in Physics.[20]
An antiproton consists of two up antiquarks and one down antiquark (uud). The
properties of the antiproton that have been measured all match the
corresponding properties of the proton, with the exception of the antiproton
having opposite electric charge and magnetic moment from the proton. Shortly
afterwards, in 1956, the antineutron was discovered in proton–proton collisions
at the Bevatron (Lawrence Berkeley National Laboratory) by Bruce Cork and
colleagues.[21]
In addition to antibaryons, anti-nuclei consisting of
multiple bound antiprotons and antineutrons have been created. These are
typically produced at energies far too high to form antimatter atoms (with
bound positrons in place of electrons). In 1965, a group of researchers led by
Antonino Zichichi reported production of nuclei of antideuterium at the Proton
Synchrotron at CERN.[22] At roughly the same time, observations of
antideuterium nuclei were reported by a group of American physicists at the
Alternating Gradient Synchrotron at Brookhaven National Laboratory.[23]
Antihydrogen atoms
Main article: Antihydrogen
In 1995, CERN announced that it had successfully brought
into existence nine antihydrogen atoms by implementing the SLAC/Fermilab
concept during the PS210 experiment. The experiment was performed using the Low
Energy Antiproton Ring (LEAR), and was led by Walter Oelert and Mario
Macri[citation needed]. Fermilab soon confirmed the CERN findings by producing
approximately 100 antihydrogen atoms at their facilities. The antihydrogen
atoms created during PS210 and subsequent experiments (at both CERN and
Fermilab) were extremely energetic ("hot") and were not well suited
to study. To resolve this hurdle, and to gain a better understanding of
antihydrogen, two collaborations were formed in the late 1990s, namely, ATHENA
and ATRAP. In 2005, ATHENA disbanded and some of the former members (along with
others) formed the ALPHA Collaboration, which is also based at CERN. The
primary goal of these collaborations is the creation of less energetic
("cold") antihydrogen, better suited to study[citation needed].
In 1999, CERN activated the Antiproton Decelerator, a device
capable of decelerating antiprotons from 3.5 GeV to 5.3 MeV — still too
"hot" to produce study-effective antihydrogen, but a huge leap
forward. In late 2002 the ATHENA project announced that they had created the
world's first "cold" antihydrogen.[24] The ATRAP project released
similar results very shortly thereafter.[25] The antiprotons used in these
experiments were cooled by decelerating them with the Antiproton Decelerator,
passing them through a thin sheet of foil, and finally capturing them in a
Penning-Malmberg trap.[26] The overall cooling process is workable, but highly
inefficient; approximately 25 million antiprotons leave the Antiproton
Decelerator and roughly 25,000 make it to the Penning-Malmberg trap, which is
about 1⁄1000 or 0.1% of the original amount.
The antiprotons are still hot when initially trapped. To
cool them further, they are mixed into an electron plasma. The electrons in
this plasma cool via cyclotron radiation, and then sympathetically cool the
antiprotons via Coulomb collisions. Eventually, the electrons are removed by
the application of short-duration electric fields, leaving the antiprotons with
energies less than 100 meV.[27] While the antiprotons are being cooled in the
first trap, a small cloud of positrons is captured from radioactive sodium in a
Surko-style positron accumulator.[28] This cloud is then recaptured in a second
trap near the antiprotons. Manipulations of the trap electrodes then tip the
antiprotons into the positron plasma, where some combine with antiprotons to
form antihydrogen. This neutral antihydrogen is unaffected by the electric and
magnetic fields used to trap the charged positrons and antiprotons, and within
a few microseconds the antihydrogen hits the trap walls, where it annihilates.
Some hundreds of millions of antihydrogen atoms have been made in this fashion.
Most of the sought-after high-precision tests of the
properties of antihydrogen could only be performed if the antihydrogen were
trapped, that is, held in place for a relatively long time. While antihydrogen
atoms are electrically neutral, the spins of their component particles produce
a magnetic moment. These magnetic moments can interact with an inhomogeneous
magnetic field; some of the antihydrogen atoms can be attracted to a magnetic
minimum. Such a minimum can be created by a combination of mirror and multipole
fields.[29] Antihydrogen can be trapped in such a magnetic minimum (minimum-B)
trap; in November 2010, the ALPHA collaboration announced that they had so
trapped 38 antihydrogen atoms for about a sixth of a second.[30][31] This was
the first time that neutral antimatter had been trapped.
On 26 April 2011, ALPHA announced that they had trapped 309
antihydrogen atoms, some for as long as 1,000 seconds (about 17 minutes). This
was longer than neutral antimatter had ever been trapped before.[32][33]
The biggest limiting factor in the large-scale production of
antimatter is the availability of antiprotons. Recent data released by CERN
states that, when fully operational, their facilities are capable of producing
ten million antiprotons per minute.[34] Assuming a 100% conversion of
antiprotons to antihydrogen, it would take 100 billion years to produce 1 gram
or 1 mole of antihydrogen (approximately 6.02×1023 atoms of antihydrogen).
Antihelium
Antihelium-3 nuclei (3He) were first observed in the 1970s
in proton-nucleus collision experiments[35] and later created in
nucleus-nucleus collision experiments.[36] Nucleus-nucleus collisions produce
antinuclei through the coalescense of antiprotons and antineutrons created in
these reactions. In 2011, the STAR detector reported the observation of
Antihelium-4 nuclei (4He).[37]
Preservation
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Antimatter cannot be stored in a container made of ordinary
matter because antimatter reacts with any matter it touches, annihilating
itself and an equal amount of the container. Antimatter in the form of charged
particles can be contained by a combination of electric and magnetic fields, in
a device called a Penning trap. This device cannot, however, contain antimatter
that consists of uncharged particles, for which atomic traps are used. In
particular, such a trap may use the dipole moment (electric or magnetic) of the
trapped particles. At high vacuum, the matter or antimatter particles can be
trapped and cooled with slightly off-resonant laser radiation using a
magneto-optical trap or magnetic trap. Small particles can also be suspended with
optical tweezers, using a highly focused laser beam.[citation needed]
Cost
Scientists claim that antimatter is the costliest material
to make.[38] In 2006, Gerald Smith estimated $250 million could produce 10
milligrams of positrons[39] (equivalent to $25 billion per gram); in 1999, NASA
gave a figure of $62.5 trillion per gram of antihydrogen.[38] This is because
production is difficult (only very few antiprotons are produced in reactions in
particle accelerators), and because there is higher demand for other uses of
particle accelerators. According to CERN, it has cost a few hundred million
Swiss Francs to produce about 1 billionth of a gram (the amount used so far for
particle/antiparticle collisions).[40]
Several studies funded by the NASA Institute for Advanced
Concepts are exploring whether it might be possible to use magnetic scoops to
collect the antimatter that occurs naturally in the Van Allen belt of the
Earth, and ultimately, the belts of gas giants, like Jupiter, hopefully at a
lower cost per gram.[41]
Uses
Medical
Matter-antimatter reactions have practical applications in
medical imaging, such as positron emission tomography (PET). In positive beta
decay, a nuclide loses surplus positive charge by emitting a positron (in the
same event, a proton becomes a neutron, and a neutrino is also emitted).
Nuclides with surplus positive charge are easily made in a cyclotron and are
widely generated for medical use. Antiprotons have also been shown within
laboratory experiments to have the potential to treat certain cancers, in a
similar method currently used for ion (proton) therapy.[42]
Fuel
The scarcity of antimatter means that it is not readily
available for use as fuel. Any antimatter propulsion would require engine
construction so as to prevent the annihilation of all the fuel simultaneously.
Anti-matter could be used as a fuel for interplanetary travel or interstellar
travel[43] as part of a antimatter catalyzed nuclear pulse propulsion or other
antimatter rocketry, such as the redshift rocket. Since the energy density of
antimatter is higher than that of conventional fuels, an antimatter-fueled
spacecraft would have a higher thrust-to-weight ratio than a conventional
spacecraft.
In matter-antimatter collisions resulting in photon
emission, the entire rest mass of the particles is converted to kinetic energy.
The energy per unit mass (9×1016 J/kg) is about 10 orders of magnitude greater
than typical chemical energies,[44] and about 3 orders of magnitude greater
than the nuclear potential energy that can be liberated, today, using nuclear
fission (about 200 MeV per atomic nucleus that undergoes nuclear fission,[45]
or 8×1013 J/kg), and about 2 orders of magnitude greater than the best possible
results expected from fusion (about 6.3×1014 J/kg for the proton-proton chain).
The reaction of 1 kg of antimatter with 1 kg of matter would produce 1.8×1017 J
(180 petajoules) of energy (by the mass-energy equivalence formula, E = mc2),
or the rough equivalent of 43 megatons of TNT – slightly less than the yield of
the 27,000kg Tsar Bomb, the largest thermonuclear weapon ever detonated.
Not all of that energy can be utilized by any realistic
propulsion technology because, while electron-positron reactions result in
gamma ray photons, in reactions between protons and antiprotons, their energy
is converted into relativistic neutral and charged pions. While the neutral
pions decay into high-energy photons, the charged pions decay into a
combination of neutrinos (carrying about 22% of the energy of the charged
pions) and unstable charged muons (carrying about 78% of the charged pion
energy), with the muons then decaying into a combination of electrons,
positrons and neutrinos (cf. muon decay; the neutrinos from this decay carry
about 2/3 of the energy of the muons, meaning that from the original charged
pions, the total fraction of their energy converted to neutrinos by one route
or another would be about 0.22 + (2/3)*0.78 = 0.74). Gamma radiation can be
largely absorbed and converted into heat energy, though some is bound to be
lost. Neutrinos very rarely interact with any form of matter, so for all
intents and purposes, the energy converted into neutrinos can be considered
lost.[46]

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