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In physics, the electron volt (symbol eV; also written electronvolt^{[1]}^{[2]}) is a unit of energy equal to approximately 1.6×10^{Template:Val/delimitnum/gaps11} joule (symbol J). By definition, it is the amount of energy gained (or lost) by the charge of a single electron moved across an electric potential difference of one volt. Thus it is 1 volt (1 joule per coulomb, 1 J/C) multiplied by the elementary charge (e, or 1.602176565(35)×10^{Template:Val/delimitnum/gaps11} C). Therefore, one electron volt is equal to 1.602176565(35)×10^{Template:Val/delimitnum/gaps11} J.^{[3]} Historically, the electron volt was devised as a standard unit of measure through its usefulness in electrostatic particle accelerator sciences because a particle with charge q has an energy E = qV after passing through the potential V; if q is quoted in integer units of the elementary charge and the terminal bias in volts, one gets an energy in eV.
The electron volt is not an SI unit, and thus its value in SI units must be obtained experimentally.^{[4]} Like the elementary charge on which it is based, it is not an independent quantity but is equal to 1 Template:Sfrac √2hα / μ_{0}c_{0}. It is a common unit of energy within physics, widely used in solid state, atomic, nuclear, and particle physics. It is commonly used with the SI prefixes milli, kilo, mega, giga, tera, peta or exa (meV, keV, MeV, GeV, TeV, PeV and EeV respectively). Thus meV stands for millielectron volt.
In some older documents, and in the name Bevatron, the symbol BeV is used, which stands for billion electron volts; it is equivalent to the GeV.
Measurement 
Unit 
SI value of unit

Energy 
eV 
1.602176565(35)×10^{Template:Val/delimitnum/gaps11} J

Mass 
eV/c^{2} 
1.782662×10^{Template:Val/delimitnum/gaps11} kg

Momentum 
eV/c 
5.344286×10^{Template:Val/delimitnum/gaps11} kg⋅m/s

Temperature 
eV/k_{B} 
11604.505(20) K

Time 
ħ/eV 
6.582119×10^{Template:Val/delimitnum/gaps11} s

Distance 
ħc/eV 
1.97327×10^{Template:Val/delimitnum/gaps11} m

Mass
By mass–energy equivalence, the electronvolt is also a unit of mass. It is common in particle physics, where mass and energy are often interchanged, to express mass in units of eV/c^{2}, where c is the speed of light in vacuum (from E = mc^{2}). It is common to simply express mass in terms of "eV" as a unit of mass, effectively using a system of natural units with c set to 1.
The Mass equivalent of 1 eV is 1.783×10^{Template:Val/delimitnum/gaps11} kg.
For example, an electron and a positron, each with a mass of 0.511 MeV/c^{2}, can annihilate to yield 1.022 MeV of energy. The proton has a mass of 0.938 GeV/c^{2}. In general, the masses of all hadrons are of the order of 1 GeV/c^{2}, which makes the GeV (gigaelectronvolt) a convenient unit of mass for particle physics:
 1 GeV/c^{2} = 1.783×10^{Template:Val/delimitnum/gaps11} kg
The atomic mass unit, 1 gram divided by Avogadro's number, is almost the mass of a hydrogen atom, which is mostly the mass of the proton. To convert to megaelectronvolts, use the formula:^{[3]}
 1 amu = 931.4941 MeV/c^{2} = 0.9314941 GeV/c^{2}
Momentum
In highenergy physics, the electron volt is often used as a unit of momentum. A potential difference of 1 volt causes an electron to gain an amount of energy (i.e., 1 eV). This gives rise to usage of eV (and keV, MeV, GeV or TeV) as units of momentum, for the energy supplied results in acceleration of the particle.
The dimensions of momentum units are Template:Dimanalysis. The dimensions of energy units are Template:Dimanalysis. Then, dividing the units of energy (such as eV) by a fundamental constant that has units of velocity (Template:Dimanalysis), facilitates the required conversion of using energy units to describe momentum. In the field of highenergy particle physics, the fundamental velocity unit is the speed of light in vacuum c. Thus, dividing energy in eV by the speed of light, one can describe the momentum of an electron in units of eV/c.^{[5]}
^{[6]}
The fundamental velocity constant c is often dropped from the units of momentum by way of defining units of length such that the value of c is unity. For example, if the momentum p of an electron is said to be 1 GeV, then the conversion to MKS can be achieved by:
 $p\; =\; 1\backslash ;\; \backslash text\{GeV\}/c\; =\; \backslash frac\{(1\; \backslash times\; 10^\{9\})\; \backslash cdot\; (1.60217646\; \backslash times\; 10^\{19\}\; \backslash ;\; \backslash text\{C\})\; \backslash cdot\; \backslash text\{V\}\}\{(2.99792458\; \backslash times\; 10^\{8\}\backslash ;\; \backslash text\{m\}/\backslash text\{s\})\}\; =\; 5.344286\; \backslash times\; 10^\{19\}\backslash ;\; \backslash text\{kg\}\{\backslash cdot\}\backslash text\{m\}/\backslash text\{s\}$
Distance
In particle physics, a system of "natural units" in which the speed of light in vacuum c and the reduced Planck constant ħ are dimensionless and equal to unity is widely used: c = ħ = 1. In these units, both distances and times are expressed in inverse energy units (while energy and mass are expressed in the same units, see mass–energy equivalence). In particular, particle scattering lengths are often presented in units of inverse particle masses.
Outside this system of units, the conversion factors between electronvolt, second, and nanometer are the following:^{[3]}
 $\backslash hbar\; =\; =\; 1.054\backslash \; 571\backslash \; 726(47)\backslash times\; 10^\{34\}\backslash \; \backslash mbox\{J\; s\}\; =\; 6.582\backslash \; 119\backslash \; 28(15)\backslash times\; 10^\{16\}\backslash \; \backslash mbox\{eV\; s\}.$
The above relations also allow expressing the mean lifetime τ of an unstable particle (in seconds) in terms of its decay width Γ (in eV) via Γ = ħ/τ. For example, the B^{0} meson has a lifetime of 1.530(9) picoseconds, mean decay length is cτ = 459.7 µm, or a decay width of (4.302±25)×10^{Template:Val/delimitnum/gaps11} eV.
Conversely, the tiny meson mass differences responsible for meson oscillations are often expressed in the more convenient inverse picoseconds.
Temperature
In certain fields, such as plasma physics, it is convenient to use the electronvolt as a unit of temperature. The conversion to kelvin is defined by using k_{B}, the Boltzmann constant:
 $\{1\; \backslash over\; k\_\{\backslash text\{B\}\}\}\; =\; \{1.602\backslash ,176\backslash ,53(14)\; \backslash times\; 10^\{19\}\; \backslash text\{\; J/eV\}\; \backslash over\; 1.380\backslash ,6505(24)\; \backslash times\; 10^\{23\}\; \backslash text\{\; J/K\}\}\; =\; 11\backslash ,604.505(20)\; \backslash text\{\; K/eV\}.$
For example, a typical magnetic confinement fusion plasma is 15 keV, or 170 megakelvin.
As an approximation: k_{B}T is about 0.025 eV (≈ Template:Sfrac) at a temperature of 20 °C.
Properties
The energy E, frequency v, and wavelength λ of a photon are related by
 $E=h\backslash nu=\backslash frac\{hc\}\{\backslash lambda\}=\backslash frac\{(4.135\; 667\; 33\backslash times\; 10^\{15\}\backslash ,\backslash mbox\{eV\}\backslash ,\backslash mbox\{s\})(299\backslash ,792\backslash ,458\backslash ,\backslash mbox\{m/s\})\}\{\backslash lambda\}$
where h is the Planck constant, c is the speed of light. This reduces to
 $E\backslash mbox\{(eV)\}=\backslash frac\{1239.84187\backslash ,\backslash mbox\{eV\}\backslash ,\backslash mbox\{nm\}\}\{\backslash lambda\backslash \; \backslash mbox\{(nm)\}\}$
A photon with a wavelength of 532 nm (green light) would have an energy of approximately 2.33 eV. Similarly, 1 eV would correspond to an infrared photon of wavelength 1240 nm, and so on.
Scattering experiments
In a lowenergy nuclear scattering experiment, it is conventional to refer to the nuclear recoil energy in units of eVr, keVr, etc. This distinguishes the nuclear recoil energy from the "electron equivalent" recoil energy (eVee, keVee, etc.) measured by scintillation light. For example, the yield of a phototube is measured in phe/keVee (photoelectrons per keV electronequivalent energy). The relationship between eV, eVr, and eVee depends on the medium the scattering takes place in, and must be established empirically for each material.
Energy comparisons
 5.25×10^{32} eV: total energy released from a 20 kt nuclear fission device
 ~624 EeV (6.24×10^{20} eV): energy consumed by a single 100watt light bulb in one second (100 W = 100 J/s ≈ 6.24×10^{20} eV/s)
 300 EeV (3×10^{20} eV = ~50 J):^{[7]} the socalled OhMyGod particle (the most energetic cosmic ray particle ever observed)
 1 PeV: one petaelectronvolt, the amount of energy measured in each of two different cosmic neutrino candidates detected by the IceCube neutrino telescope in Antarctica^{[8]}
 14 TeV: the designed proton collision energy at the Large Hadron Collider (which has operated at half of this energy since 30 March 2010^{[update]})
 1 TeV: a trillion electronvolts, or 1.602×10^{Template:Val/delimitnum/gaps11} J, about the kinetic energy of a flying mosquito^{[9]}
 125.3±0.6 GeV: the energy emitted by the decay of the Higgs Boson, as measured by two separate detectors at the LHC to a certainty of 5 sigma^{[10]}
 210 MeV: the average energy released in fission of one Pu239 atom
 200 MeV: the average energy released in nuclear fission of one U235 atom
 17.6 MeV: the average energy released in the fusion of deuterium and tritium to form He4; this is 0.41 PJ per kilogram of product produced
 1 MeV (1.602×10^{Template:Val/delimitnum/gaps11} J): about twice the rest energy of an electron
 13.6 eV: the energy required to ionize atomic hydrogen; molecular bond energies are on the order of 1 eV to 10 eV per bond
 1.6 eV to 3.4 eV: the photon energy of visible light
 25 meV: the thermal energy k_{B}T at room temperature; one air molecule has an average kinetic energy 38 meV
 230 µeV: the thermal energy k_{B}T of the cosmic microwave background
See also
Notes and references
External links
 BIPM's definition of the electronvolt
 http://physics.nist.gov/cuu/Constants physical constants reference; CODATA data
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