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In , an electronvolt (symbol eV), also written as electron-volt and electron volt, is a unit of measurement equivalent to the amount of gained by a single accelerating through an of one in . When used as a unit of energy, the numerical value of 1 eV expressed in unit of (symbol J) is equal to the numerical value of the of an electron in (symbol C). Under the 2019 revision of the SI, this sets 1 eV equal to the exact value Historically, the electronvolt was devised as a standard unit of measure through its usefulness in electrostatic particle accelerator sciences, because a particle with q gains an energy after passing through a voltage of V.


Definition and use
An electronvolt is the amount of energy gained or lost by a single when it moves through an of one . Hence, it has a value of one , which is , multiplied by the elementary charge Therefore, one electronvolt is equal to

The electronvolt (eV) is a unit of energy, but is not an . It is a commonly used unit of energy within physics, widely used in solid state, , and physics, and high-energy astrophysics. It is commonly used with milli- (10−3), kilo- (103), mega- (106), giga- (109), tera- (1012), peta- (1015), exa- (1018), zetta- (1021), yotta- (1024), ronna- (1027), or quetta- (1030), the respective symbols being meV, keV, MeV, GeV, TeV, PeV, EeV, ZeV, YeV, ReV, and QeV. The SI unit of energy is the joule (J).

In some older documents, and in the name , the symbol BeV is used, where the B stands for . The symbol BeV is therefore equivalent to GeV, though neither is an SI unit.


Relation to other physical properties and units
In the fields of physics in which the electronvolt is used, other quantities are typically measured using units derived from it; products with fundamental constants of importance in the theory are often used.


Mass
By mass–energy equivalence, the electronvolt corresponds to a unit of . It is common in , where units of mass and energy are often interchanged, to express mass in units of eV/ c2, where c is the speed of light in vacuum (from ). It is common to informally express mass in terms of eV as a unit of mass, effectively using a system of with c set to 1. The equivalent of is:

1\; \text{eV}/c^2 = \frac{(1.602\ 176\ 634 \times 10^{-19} \, \text{C}) \times 1 \, \text{V}}{(299\ 792\ 458\; \mathrm{m/s})^2} = 1.782\ 661\ 92 \times 10^{-36}\; \text{kg}.

For example, an electron and a , each with a mass of , can to yield of energy. A has a mass of . In general, the masses of all are of the order of , which makes the GeV/ c2 a convenient unit of mass for particle physics:

The atomic mass constant ( mu), one twelfth of the mass a carbon-12 atom, is close to the mass of a proton. To convert to electronvolt mass-equivalent, use the formula:


Momentum
By dividing a particle's kinetic energy in electronvolts by the fundamental constant c (the speed of light), one can describe the particle's in units of eV/ c. In natural units in which the fundamental velocity constant c is numerically 1, the c may informally be omitted to express momentum using the unit electronvolt. The energy–momentum relation E^2 = p^2 c^2 + m_0^2 c^4 in natural units (with c=1) E^2 = p^2 + m_0^2 is a Pythagorean equation. When a relatively high energy is applied to a particle with relatively low , it can be approximated as E \simeq p in such that an applied energy with expressed in the unit eV conveniently results in a numerically approximately equivalent change of momentum when expressed with the unit eV/ c.

The dimension of momentum is . The dimension of energy is . Dividing a unit of energy (such as eV) by a fundamental constant (such as the speed of light) that has the dimension of velocity () facilitates the required conversion for using a unit of energy to quantify momentum.

For example, if the momentum p of an electron is , then the conversion to MKS system of units can be achieved by: p = 1\; \text{GeV}/c = \frac{(1 \times 10^9) \times (1.602\ 176\ 634 \times 10^{-19} \; \text{C}) \times (1 \; \text{V})}{2.99\ 792\ 458 \times 10^8\; \text{m}/\text{s}} = 5.344\ 286 \times 10^{-19}\; \text{kg} {\cdot} \text{m}/\text{s}.


Distance
In , a system of natural units in which the speed of light in vacuum c and the ħ are dimensionless and equal to unity is widely used: . 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 using a unit of inverse particle mass.

Outside this system of units, the conversion factors between electronvolt, second, and nanometer are the following: \hbar = 1.054\ 571\ 817\ 646\times 10^{-34}\ \mathrm{J{\cdot}s} = 6.582\ 119\ 569\ 509\times 10^{-16}\ \mathrm{eV{\cdot}s}.

The above relations also allow expressing the τ of an unstable particle (in seconds) in terms of its Γ (in eV) via . For example, the has a lifetime of 1.530(9) , mean decay length is , or a decay width of .

Conversely, the tiny meson mass differences responsible for meson oscillations are often expressed in the more convenient inverse picoseconds.

Energy in electronvolts is sometimes expressed through the wavelength of light with photons of the same energy: \frac{1\; \text{eV}}{hc} = \frac{1.602\ 176\ 634 \times 10^{-19} \; \text{J}}{(6.62\ 607\ 015 \times 10^{-34}\; \text{J} {\cdot} \text{s}) \times (2.99\ 792\ 458 \times 10^{11}\; \text{mm}/\text{s})} \thickapprox 806.55439 \; \text{mm}^{-1}.


Temperature
In certain fields, such as , it is convenient to use the electronvolt to express temperature. The electronvolt is divided by the Boltzmann constant to convert to the : {1 \,\mathrm{eV} / k_{\text{B}}} = {1.602\ 176\ 634 \times 10^{-19} \text{ J} \over 1.380\ 649 \times 10^{-23} \text{ J/K}} = 11\ 604.518\ 12 \text{ K}, where kB is the Boltzmann constant.

The kB is assumed when using the electronvolt to express temperature, for example, a typical magnetic confinement fusion plasma is (kiloelectronvolt), which corresponds to 174 MK (megakelvin).

As an approximation: at a temperature of , kB T is about (≈ ).


Wavelength
The energy E, frequency ν, and wavelength λ of a photon are related by E = h\nu = \frac{hc}{\lambda} = \frac{\mathrm{4.135\ 667\ 696 \times 10^{-15}\;eV/Hz} \times \mathrm{299\, 792\, 458\;m/s}}{\lambda} where h is the , c is the speed of light. This reduces to \begin{align} E &= 4.135\ 667\ 696 \times 10^{-15}\;\mathrm{eV/Hz}\times\nu \\4pt &=\frac{1\ 239.841\ 98\;\mathrm{eV{\cdot}nm}}{\lambda}. \end{align} A photon with a wavelength of (green light) would have an energy of approximately . Similarly, would correspond to an infrared photon of wavelength or frequency .


Scattering experiments
In a low-energy 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 is measured in phe/keVee ( per keV electron-equivalent 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
varies only with the frequency of the photon, related by the speed of light. This contrasts with a massive particle of which the energy depends on its velocity and .
HF:
MF:
LF:
VLF: very low freq.
ULF: ultra-low freq.
SLF: super low freq.
ELF: extremely low freq.
]]

approximate grand unification energy
the highest-energy neutrino detected by the neutrino telescope in Antarctica
designed proton center-of-mass collision energy at the Large Hadron Collider (operated at 3.5 TeV since its start on 30 March 2010, reached 13 TeV in May 2015)
rest mass energy of the , as measured by two separate detectors at the LHC to a certainty better than 5 sigma
rest mass energy of a
rest mass energy of an electron
energy required to ; are on the order of to per bond
range of (\tfrac{hc}{\lambda}) of from to violet
average kinetic energy, , of one gas molecule at
, , at the cosmic microwave background radiation temperature of ~2.7 


Molar energy
One mole of particles given 1 eV of energy each has approximately 96.5 kJ of energy – this corresponds to the ( F ≈ ), where the energy in joules of n moles of particles each with energy E eV is equal to E· F· n.


See also
  • Orders of magnitude (energy)


External links

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