KNOWPIA
WELCOME TO KNOWPIA

In quantum field theory, the **Dirac spinor** is the spinor that describes all known fundamental particles that are fermions, with the possible exception of neutrinos. It appears in the plane-wave solution to the Dirac equation, and is a certain combination of two Weyl spinors, specifically, a bispinor that transforms "spinorially" under the action of the Lorentz group.

Dirac spinors are important and interesting in numerous ways. Foremost, they are important as they do describe all of the known fundamental particle fermions in nature; this includes the electron and the quarks. Algebraically they behave, in a certain sense, as the "square root" of a vector. This is not readily apparent from direct examination, but it has slowly become clear over the last 60 years that spinorial representations are fundamental to geometry. For example, effectively all Riemannian manifolds can have spinors and spin connections built upon them, via the Clifford algebra.^{[1]} The Dirac spinor is specific to that of Minkowski spacetime and Lorentz transformations; the general case is quite similar.

This article is devoted to the Dirac spinor in the **Dirac representation**. This corresponds to a specific representation of the gamma matrices, and is best suited for demonstrating the positive and negative energy solutions of the Dirac equation. There are other representations, most notably the chiral representation, which is better suited for demonstrating the chiral symmetry of the solutions to the Dirac equation. The chiral spinors may be written as linear combinations of the Dirac spinors presented below; thus, nothing is lost or gained, other than a change in perspective with regards to the discrete symmetries of the solutions.

The remainder of this article is laid out in a pedagogical fashion, using notations and conventions specific to the standard presentation of the Dirac spinor in textbooks on quantum field theory. It focuses primarily on the algebra of the plane-wave solutions. The manner in which the Dirac spinor transforms under the action of the Lorentz group is discussed in the article on bispinors.

The **Dirac spinor** is the bispinor in the plane-wave solution

of the free Dirac equation,

where (in the units )

- is a relativistic spin-1/2 field,
- is the Dirac spinor related to a plane-wave with wave-vector ,
- ,
- is the four-wave-vector of the plane wave, where is arbitrary,
- are the four-coordinates in a given inertial frame of reference.

The Dirac spinor for the positive-frequency solution can be written as

where

- is an arbitrary two-spinor,
- is the Pauli vector,
- is the positive square root

In natural units, when *m*^{2} is added to *p*^{2} or when *m* is added to , *m* means *mc* in ordinary units; when *m* is added to *E*, *m* means *mc*^{2} in ordinary units. When *m* is added to or to it means (which is called the *inverse reduced Compton wavelength*) in ordinary units.

The Dirac equation has the form

In order to derive an expression for the four-spinor ω, the matrices α and β must be given in concrete form. The precise form that they take is representation-dependent. For the entirety of this article, the Dirac representation is used. In this representation, the matrices are

These two 4×4 matrices are related to the Dirac gamma matrices. Note that **0** and **I** are 2×2 matrices here.

The next step is to look for solutions of the form

- ,

while at the same time splitting ω into two two-spinors:

- .

Using all of the above information to plug into the Dirac equation results in

- .

This matrix equation is really two coupled equations:

Solve the 2nd equation for χ and one obtains

- .

Note that this solution needs to have in order for the solution to be valid in a frame where the particle has .

Derivation of the sign of the energy in this case. We consider the potentially problematic term .

- If , clearly as .
- On the other hand, let , with a unit vector, and let .

Hence the negative solution clearly has to be omitted, and . End derivation.

Assembling these pieces, the full **positive energy solution** is conventionally written as

The above introduces a normalization factor derived in the next section.

Solving instead the 1st equation for a different set of solutions are found:

- .

In this case, one needs to enforce that for this solution to be valid in a frame where the particle has . The proof follows analogously to the previous case. This is the so-called **negative energy solution**. It can sometimes become confusing to carry around an explicitly negative energy, and so it is conventional to flip the sign on both the energy and the momentum, and to write this as

In further development, the -type solutions are referred to as the particle solutions, describing a positive-mass spin-1/2 particle carrying positive energy, and the -type solutions are referred to as the antiparticle solutions, again describing a positive-mass spin-1/2 particle, again carrying positive energy. In the laboratory frame, both are considered to have positive mass and positive energy, although they are still very much dual to each other, with the flipped sign on the antiparticle plane-wave suggesting that it is "travelling backwards in time". The interpretation of "backwards-time" is a bit subjective and imprecise, amounting to hand-waving when one's only evidence are these solutions. It does gain stronger evidence when considering the quantized Dirac field. A more precise meaning for these two sets of solutions being "opposite to each other" is given in the section on charge conjugation, below.

In the Dirac representation, the most convenient definitions for the two-spinors are:

and

The Pauli matrices are

Using these, one obtains what is sometimes called the **Pauli vector**:

The Dirac spinors provide a complete and orthogonal set of solutions to the Dirac equation.^{[2]}^{[3]} This is most easily demonstrated by writing the spinors in the rest frame, where this becomes obvious, and then boosting to an arbitrary Lorentz coordinate frame. In the rest frame, where the three-momentum vanishes: one may define four spinors

Introducing the Feynman slash notation

the boosted spinors can be written as

and

The conjugate spinors are defined as which may be shown to solve the conjugate Dirac equation

with the derivative understood to be acting towards the left. The conjugate spinors are then

and

The normalization chosen here is such that the scalar invariant really is invariant in all Lorentz frames. Specifically, this means

The four rest-frame spinors indicate that there are four distinct, real, linearly independent solutions to the Dirac equation. That they are indeed solutions can be made clear by observing that, when written in momentum space, the Dirac equation has the form

and

This follows because

which in turn follows from the anti-commutation relations for the gamma matrices:

with the metric tensor in flat space (in curved space, the gamma matrices can be viewed as being a kind of vielbein, although this is beyond the scope of the current article). It is perhaps useful to note that the Dirac equation, written in the rest frame, takes the form

and

so that the rest-frame spinors can correctly be interpreted as solutions to the Dirac equation. There are four equations here, not eight. Although 4-spinors are written as four complex numbers, thus suggesting 8 real variables, only four of them have dynamical independence; the other four have no significance and can always be parameterized away. That is, one could take each of the four vectors and multiply each by a distinct global phase This phase changes nothing; it can be interpreted as a kind of global gauge freedom. This is not to say that "phases don't matter", as of course they do; the Dirac equation must be written in complex form, and the phases couple to electromagnetism. Phases even have a physical significance, as the Bohm-Aharonov effect implies: the Dirac field, coupled to electromagnetism, is a U(1) fiber bundle (the circle bundle), and the Bohm-Aharonov effect demonstrates the holonomy of that bundle. All this has no direct impact on the counting of the number of distinct components of the Dirac field. In any setting, there are only four real, distinct components.

With an appropriate choice of the gamma matrices, it is possible to write the Dirac equation in a purely real form, having only real solutions: this is the Majorana equation. However, it has only two linearly independent solutions. These solutions do *not* couple to electromagnetism; they describe a massive, electrically neutral spin-1/2 particle. Apparently, coupling to electromagnetism doubles the number of solutions. But of course, this makes sense: coupling to electromagnetism requires taking a real field, and making it complex. With some effort, the Dirac equation can be interpreted as the "complexified" Majorana equation. This is most easily demonstrated in a generic geometrical setting, outside the scope of this article.

It is conventional to define a pair of projection matrices and , that project out the positive and negative energy eigenstates. Given a fixed Lorentz coordinate frame (i.e. a fixed momentum), these are

These are a pair of 4×4 matrices. They sum to the identity matrix:

are orthogonal

and are idempotent

It is convenient to notice their trace:

Note that the trace, and the orthonormality properties hold independent of the Lorentz frame; these are Lorentz covariants.

Charge conjugation transforms the positive-energy spinor into the negative-energy spinor. Charge conjugation is a mapping (an involution) having the explicit form

where denotes the transpose, is a 4×4 matrix, and is an arbitrary phase factor, The article on charge conjugation derives the above form, and demonstrates why the word "charge" is the appropriate word to use: it can be interpreted as the electrical charge. In the Dirac representation for the gamma matrices, the matrix can be written as

Thus, a positive-energy solution (dropping the spin superscript to avoid notational overload)

is carried to its charge conjugate

Note the stray complex conjugates. These can be consolidated with the identity

to obtain

with the 2-spinor being

As this has precisely the form of the negative energy solution, it becomes clear that charge conjugation exchanges the particle and anti-particle solutions. Note that not only is the energy reversed, but the momentum is reversed as well. Spin-up is transmuted to spin-down. It can be shown that the parity is also flipped. Charge conjugation is very much a pairing of Dirac spinor to its "exact opposite".

- Dirac equation
- Weyl equation
- Majorana equation
- Helicity basis
- Spin(1,3), the double cover of SO(1,3) by a spin group

**^**Jurgen Jost, (2002) "Riemannian Geometry and Geometric Analysis (3rd edition)", Springer.*See Chapter 1, section 1.8.***^**James D. Bjorken, Sidney D. Drell, (1964) "Relativistic Quantum Mechanics", McGraw-Hill*(See Chapter 3)***^**Claude Itzykson and Jean-Bernard Zuber, (1980) "Quantum Field Theory", MacGraw-Hill*(See Chapter 2)*

- Aitchison, I.J.R.; A.J.G. Hey (September 2002).
*Gauge Theories in Particle Physics (3rd ed.)*. Institute of Physics Publishing. ISBN 0-7503-0864-8. - Miller, David (2008). "Relativistic Quantum Mechanics (RQM)" (PDF). pp. 26–37.