Dirac Equation

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Dirac equation

[di′rak i′kwā·zhən]
(quantum mechanics)
A relativistic wave equation for an electron in an electromagnetic field, in which the wave function has four components corresponding to four internal states specified by a two-valued spin coordinate and an energy coordinate which can have a positive or negative value.
McGraw-Hill Dictionary of Scientific & Technical Terms, 6E, Copyright © 2003 by The McGraw-Hill Companies, Inc.
The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.

Dirac Equation


a quantum equation for the motion of an electron, meeting the requirements of the theory of relativity; established by Dirac in 1928. It follows from the Dirac equation that an electron has a characteristic mechanical moment of angular momentum—spin—equal to ħ/2 and a characteristic magnetic moment equal to the Bohr magneton /2mc, which were previously (1925) discovered experimentally (e and m are the charge and mass of the electron, c is the velocity of light, and ħ is Planck’s constant). The Dirac equation has made it possible to obtain a more accurate formula of the energy levels of hydrogen and hydrogen-like atoms, which includes the fine structure of the levels; it has also helped explain the Zeeman effect. With the Dirac equation as the basis, formulas have been obtained for the probabilities of scattering photons by free electrons (Compton effect) and radiation emitted by a decelerating electron (bremstrahlung); these formulas have been experimentally confirmed. However, a systematic relativistic description of the motion of an electron is provided by quantum electro-dynamics.

A characteristic feature of the Dirac equation is that its solutions include those that correspond to negative values of energy for the free motion of a particle (corresponding to the negative mass of a particle). This presented a difficulty for the theory, since all the mechanical laws for a particle in such states would be incorrect, although transitions in such states are possible in quantum theory. The real physical sense of transitions to a negative energy level were elucidated later, when the possibility of particle interconversion was proved. It followed from the Dirac equation that a new particle must exist (an antiparticle with respect to the electron) with the mass of an electron and a positive charge: in 1932 such a particle was actually discovered by C. D. Anderson and called the positron. This was a great success for the Dirac theory of the electron. The passage of an electron from a state of negative energy to one of positive energy and the reverse are interpreted as the process of the formation of an electron-positron pair and the annihilation of such a pair.

The Dirac equation is also valid for particles with spin ½ (in ħ units)—mu-mesons and the neutrino. With the proton and neutron, which also have spin ½, it leads to incorrect values of the magnetic moments. The magnetic moment for the Dirac proton should be equal to the nuclear magneton /2Mc (m is the mass of the proton) and that of the neutron to zero since it is uncharged. Experiments show that the magnetic moment of the proton is about 2.8 mangetons and the magnetic moment of the neutron is negative, with an absolute value equal to about two-thirds of the magnetic moment of a proton. The anomalous magnetic moments of these particles are due to their strong interactions.


Broglie, L. de. Magnitnyi elektron. Kharkov, 1936. (Translated from French.)
The Great Soviet Encyclopedia, 3rd Edition (1970-1979). © 2010 The Gale Group, Inc. All rights reserved.
References in periodicals archive ?
Dirac's equation is shown to be an eigenvector equation associated with an interaction field endomorphism.
The light and colored pentads of Clifford's set of such rank contain in threes 2-diagonal matrices, corresponding to 3 space coordinates in accordance with Dirac's equation. Hence, a space of these events is 3-dimensional.
The same strategy was adopted by Herman Wyel in 1929using Dirac's equation. At that time a known particle with zero mass was only the Photon, a Boson, with tsh spin but he reduced mass of a fermion or an electron in Dirac's equation and got a pair of particles with zero mass and therefore with no electric charge because if a particle has no rest mass but spin half of tsh then we are forced to assign it, zero electric charge.
Dirac's equation forced him to confront apparently absurd phenomena that he interpreted, after a few false starts, as evidence for the existence of the electron's antiparticle.
But although Dirac's equation is Lorentz-covariant, his state-function is a 4x1 matrix which behaves, not like a 4-vector, but like a spinor whose transformation is fixed by a change of frame only to within a factor of [+ or -]1.
The DO has attracted a lot of interests both because it provides one of the examples of the Dirac's equation exact solvability and because of its numerous physical applications [22-27].
4 x 1-Marix Functions and Dirac's Equation, Progress in Physics, 2009, v.
This equation is a generalization of the Dirac's equation with gauge fields [[THETA].sub.k] ([x.sub.k]) and [Y.sub.k] ([x.sub.k]) and with eight mass members.
It is known that Dirac's equation contains four anticommutive complex 4 x 4 matrices.
Dirac's equations for the spinor field y and its adjoint [bar.[psi]] are obtained from the Lagrangian (19) such that the Euler-Lagrange equations of [psi] and [bar.[psi]] are, respectively,
For inclusion of the spin effects one should employ the related Dirac's equations (Dirac, 1978).
Therefore, unessential restrictions on 4X1 matrix functions give Dirac's equations, and it seems that some gluon and gravity phenomena can be explained with the help of these equations.