Bispinor

Template:Short description Template:Use American English In physics, and specifically in quantum field theory, a bispinor is a mathematical construction that is used to describe some of the fundamental particles of nature, including quarks and electrons. It is a specific embodiment of a spinor, specifically constructed so that it is consistent with the requirements of special relativity. Bispinors transform in a certain "spinorial" fashion under the action of the Lorentz group, which describes the symmetries of Minkowski spacetime. They occur in the relativistic [[Spin-1/2|spin-Template:Sfrac]] wave function solutions to the Dirac equation.

Bispinors are so called because they are constructed out of two simpler component spinors, the Weyl spinors. Each of the two component spinors transform differently under the two distinct complex-conjugate spin-1/2 representations of the Lorentz group. This pairing is of fundamental importance, as it allows the represented particle to have a mass, carry a charge, and represent the flow of charge as a current, and perhaps most importantly, to carry angular momentum. More precisely, the mass is a Casimir invariant of the Lorentz group (an eigenstate of the energy), while the vector combination carries momentum and current, being covariant under the action of the Lorentz group. The angular momentum is carried by the Poynting vector, suitably constructed for the spin field.

A bispinor is more or less "the same thing" as a Dirac spinor. The convention used here is that the article on the Dirac spinor presents plane-wave solutions to the Dirac equation using the Dirac convention for the gamma matrices. That is, the Dirac spinor is a bispinor in the Dirac convention. By contrast, the article below concentrates primarily on the Weyl, or chiral representation, is less focused on the Dirac equation, and more focused on the geometric structure, including the geometry of the Lorentz group. Thus, much of what is said below can be applied to the Majorana equation.

Definition

Bispinors are elements of a 4-dimensional complex vector space Template:Nowrap representation of the Lorentz group.

In the Weyl basis, a bispinor

$\psi =\left(\begin{array}{c}{\psi }_{\mathrm{L}}\\ {\psi }_{\mathrm{R}}\end{array}\right)$

consists of two (two-component) Weyl spinors ${\psi }_{\mathrm{L}}$ and ${\psi }_{\mathrm{R}}$ which transform, correspondingly, under (Template:Sfrac, 0) and (0, Template:Sfrac) representations of the $\mathrm{S}\mathrm{O}(1,3)$ group (the Lorentz group without parity transformations). Under parity transformation the Weyl spinors transform into each other.

The Dirac bispinor is connected with the Weyl bispinor by a unitary transformation to the Dirac basis,

$\psi \to \frac{1}{\sqrt{2}}\left[\begin{array}{cc}1& 1\\ -1& 1\end{array}\right]\psi =\frac{1}{\sqrt{2}}\left(\begin{array}{c}{\psi }_{\mathrm{R}}+{\psi }_{\mathrm{L}}\\ {\psi }_{\mathrm{R}}-{\psi }_{\mathrm{L}}\end{array}\right).$

The Dirac basis is the one most widely used in the literature.

Expressions for Lorentz transformations of bispinors

A bispinor field $\psi (x)$ transforms according to the rule

${\psi }^a(x)\to {{\psi }^{\prime }}^a\left(x^{\prime }\right)=S[\mathrm{\Lambda }{]}_b^a{\psi }^b\left({\mathrm{\Lambda }}^{-1}{x}^{\prime }\right)=S[\mathrm{\Lambda }{]}_b^a{\psi }^b(x)$

where $\mathrm{\Lambda }$ is a Lorentz transformation. Here the coordinates of physical points are transformed according to $x^{\prime }=\mathrm{\Lambda }x$, while $S$, a matrix, is an element of the spinor representation (for spin Template:Math) of the Lorentz group.

In the Weyl basis, explicit transformation matrices for a boost ${\mathrm{\Lambda }}_{\mathrm{b}\mathrm{o}\mathrm{o}\mathrm{s}\mathrm{t}}$ and for a rotation ${\mathrm{\Lambda }}_{\mathrm{r}\mathrm{o}\mathrm{t}}$ are the following:

$\begin{array}{cc}S[{\mathrm{\Lambda }}_{\mathrm{b}\mathrm{o}\mathrm{o}\mathrm{s}\mathrm{t}}]& =(e^{+\chi \cdot \alpha /2})\\ S[{\mathrm{\Lambda }}_{\mathrm{r}\mathrm{o}\mathrm{t}}]& =\left(\begin{array}{cc}{e}^{+i\varphi \cdot \sigma /2}& 0\\ 0& e^{+i\varphi \cdot \sigma /2}\end{array}\right)\end{array}$

Here $\chi$ is the boost parameter which is the rapidity multiplied by the normalized direction of the velocity, and ${\varphi }^i$ represents rotation around the $x^i$ axis, ${\sigma }_i$ are the Pauli matrices and $\alpha$ is the vector made of gamma matrices $\alpha ={\gamma }_t({\gamma }_x,{\gamma }_y,{\gamma }_z)$. The exponential is the exponential map, in this case the matrix exponential defined by putting the matrix into the usual power series for the exponential function.

Properties

A bilinear form of bispinors can be reduced to five irreducible (under the Lorentz group) objects:

1. scalar, $\overline{\psi }\psi$;
2. pseudo-scalar, $\overline{\psi }{\gamma }^5\psi$;
3. vector, $\overline{\psi }{\gamma }^{\mu }\psi$;
4. pseudo-vector, $\overline{\psi }{\gamma }^{\mu }{\gamma }^5\psi$;
5. antisymmetric tensor, $\overline{\psi }({\gamma }^{\mu }{\gamma }^{\nu }-{\gamma }^{\nu }{\gamma }^{\mu })\psi$,

where $\overline{\psi }\equiv {\psi }^{†}{\gamma }^0$ and $\{{\gamma }^{\mu },{\gamma }^5\}$ are the gamma matrices. These five quantities are inter-related by the Fierz identities. Their values are used in the Lounesto spinor field classification of the different types of spinors, of which the bispinor is just one; the others being the flagpole (of which the Majorana spinor is a special case), the flag-dipole, and the Weyl spinor. The flagpole, flag-dipole and Weyl spinors all have null mass and pseudoscalar fields; the flagpole additionally has a null pseudovector field, whereas the Weyl spinors have a null antisymmetric tensor (a null "angular momentum field").

A suitable Lagrangian for the relativistic spin-Template:Sfrac field can be built out of these, and is given as

$ℒ=\frac{i}{2}(\overline{\psi }{\gamma }^{\mu }{\partial }_{\mu }\psi -{\partial }_{\mu }\overline{\psi }{\gamma }^{\mu }\psi )-m\overline{\psi }\psi .$

The Dirac equation can be derived from this Lagrangian by using the Euler–Lagrange equation.

Derivation of a bispinor representation

Introduction

This outline describes one type of bispinors as elements of a particular representation space of the (Template:Sfrac, 0) ⊕ (0, Template:Sfrac) representation of the Lorentz group. This representation space is related to, but not identical to, the Template:Nowrap representation space contained in the Clifford algebra over Minkowski spacetime as described in the article Spinors. Language and terminology is used as in Representation theory of the Lorentz group. The only property of Clifford algebras that is essential for the presentation is the defining property given in Template:EquationNote below. The [[Representation theory of the Lorentz group#Explicit formulas|basis elements of Template:Math]] are labeled Template:Math.

A representation of the Lie algebra Template:Math of the Lorentz group Template:Math will emerge among matrices that will be chosen as a basis (as a vector space) of the complex Clifford algebra over spacetime. These Template:Math matrices are then exponentiated yielding a representation of Template:Math. This representation, that turns out to be a Template:Math representation, will act on an arbitrary 4-dimensional complex vector space, which will simply be taken as Template:Math, and its elements will be bispinors.

For reference, the commutation relations of Template:Math are

with the spacetime metric Template:Math.

The gamma matrices

Let Template:Math denote a set of four 4-dimensional gamma matrices, here called the Dirac matrices. The Dirac matrices satisfy

where Template:Math is the anticommutator, Template:Math is a Template:Math unit matrix, and Template:Math is the spacetime metric with signature (+,−,−,−). This is the defining condition for a generating set of a Clifford algebra. Further basis elements Template:Math of the Clifford algebra are given by

Only six of the matrices Template:Math are linearly independent. This follows directly from their definition since Template:Math. They act on the subspace Template:Math the Template:Math span in the passive sense, according to

In Template:EquationNote, the second equality follows from property Template:EquationNote of the Clifford algebra.

Lie algebra embedding of so(3,1) in Cl₄(C)

Now define an action of Template:Math on the Template:Math, and the linear subspace Template:Math they span in Template:Math, given by

The last equality in Template:EquationRef, which follows from Template:EquationRef and the property Template:EquationRef of the gamma matrices, shows that the Template:Math constitute a representation of Template:Math since the commutation relations in Template:EquationNote are exactly those of Template:Math. The action of Template:Math can either be thought of as six-dimensional matrices Template:Math multiplying the basis vectors Template:Math, since the space in Template:Math spanned by the Template:Math is six-dimensional, or be thought of as the action by commutation on the Template:Math. In the following, Template:Math

The Template:Math and the Template:Math are both (disjoint) subsets of the basis elements of Cl₄(C), generated by the four-dimensional Dirac matrices Template:Math in four spacetime dimensions. The Lie algebra of Template:Math is thus embedded in Cl₄(C) by Template:Math as the real subspace of Cl₄(C) spanned by the Template:Math. For a full description of the remaining basis elements other than Template:Math and Template:Math of the Clifford algebra, please see the article Dirac algebra.

Bispinors introduced

Now introduce any 4-dimensional complex vector space U where the γ^μ act by matrix multiplication. Here Template:Math will do nicely. Let Template:Math be a Lorentz transformation and define the action of the Lorentz group on U to be

$u\to S(\mathrm{\Lambda })u=e^{i\pi ({\omega }_{\mu \nu }{M}^{\mu \nu })}u;u^{\alpha }\to [e^{{\omega }_{\mu \nu }{\sigma }^{\mu \nu }}{]}^{\alpha }{}_{\beta }{u}^{\beta }.$

Since the Template:Math according to Template:EquationNote constitute a representation of Template:Math, the induced map

according to general theory either is a representation or a projective representation of Template:Math. It will turn out to be a projective representation. The elements of U, when endowed with the transformation rule given by S, are called bispinors or simply spinors.

A choice of Dirac matrices

It remains to choose a set of Dirac matrices Template:Math in order to obtain the spin representation Template:Mvar. One such choice, appropriate for the ultrarelativistic limit, is

where the Template:Math are the Pauli matrices. In this representation of the Clifford algebra generators, the Template:Math become

This representation is manifestly not irreducible, since the matrices are all block diagonal. But by irreducibility of the Pauli matrices, the representation cannot be further reduced. Since it is a 4-dimensional, the only possibility is that it is a Template:Math representation, i.e. a bispinor representation. Now using the recipe of exponentiation of the Lie algebra representation to obtain a representation of Template:Math,

a projective 2-valued representation is obtained. Here Template:Math is a vector of rotation parameters with Template:Math, and Template:Math is a vector of boost parameters. With the conventions used here one may write

for a bispinor field. Here, the upper component corresponds to a right Weyl spinor. To include space parity inversion in this formalism, one sets Template:NumBlk

as representative for Template:Math. It is seen that the representation is irreducible when space parity inversion is included.

An example

Let Template:Math so that Template:Mvar generates a rotation around the z-axis by an angle of Template:Math. Then Template:Math but Template:Math. Here, Template:Mvar denotes the identity element. If Template:Math is chosen instead, then still Template:Math, but now Template:Math.

This illustrates the double-valued nature of a spin representation. The identity in Template:Math gets mapped into either Template:Math or Template:Math depending on the choice of Lie algebra element to represent it. In the first case, one can speculate that a rotation of an angle Template:Math negates a bispinor, and that it requires a Template:Math rotation to rotate a bispinor back into itself. What really happens is that the identity in Template:Math is mapped to Template:Math in Template:Math with an unfortunate choice of Template:Mvar.

It is impossible to continuously choose Template:Mvar for all Template:Math so that Template:Mvar is a continuous representation. Suppose that one defines Template:Mvar along a loop in Template:Math such that Template:Math. This is a closed loop in Template:Math, i.e. rotations ranging from 0 to Template:Math around the z-axis under the exponential mapping, but it is only "half" a loop in Template:Math, ending at Template:Math. In addition, the value of Template:Math is ambiguous, since Template:Math and Template:Math gives different values for Template:Math.

The Dirac algebra

The representation Template:Mvar on bispinors will induce a representation of Template:Math on Template:Math, the set of linear operators on U. This space corresponds to the Clifford algebra itself so that all linear operators on U are elements of the latter. This representation, and how it decomposes as a direct sum of irreducible Template:Math representations, is described in the article on Dirac algebra. One of the consequences is the decomposition of the bilinear forms on Template:Math. This decomposition hints how to couple any bispinor field with other fields in a Lagrangian to yield Lorentz scalars.

Bispinors and the Dirac algebra

The Dirac matrices are a set of four 4×4 matrices forming the Dirac algebra, and are used to intertwine the spin direction with the local reference frame (the local coordinate frame of spacetime), as well as to define charge (C-symmetry), parity and time reversal operators.

Conventions

There are several choices of signature and representation that are in common use in the physics literature. The Dirac matrices are typically written as ${\gamma }^{\mu }$ where $\mu$ runs from 0 to 3. In this notation, 0 corresponds to time, and 1 through 3 correspond to x, y, and z.

The Template:Nowrap signature is sometimes called the west coast metric, while the Template:Nowrap is the east coast metric. At this time the Template:Nowrap signature is in more common use, and our example will use this signature. To switch from one example to the other, multiply all ${\gamma }^{\mu }$ by $i$.

After choosing the signature, there are many ways of constructing a representation in the 4×4 matrices, and many are in common use. In order to make this example as general as possible we will not specify a representation until the final step. At that time we will substitute in the "chiral" or Weyl representation.

Construction of Dirac spinor with a given spin direction and charge

First we choose a spin direction for our electron or positron. As with the example of the Pauli algebra discussed above, the spin direction is defined by a unit vector in 3 dimensions, (a, b, c). Following the convention of Peskin & Schroeder, the spin operator for spin in the (a, b, c) direction is defined as the dot product of (a, b, c) with the vector

$\begin{array}{cc}(i{\gamma }^2{\gamma }^3,i{\gamma }^3{\gamma }^1,i{\gamma }^1{\gamma }^2)& =-({\gamma }^1,{\gamma }^2,{\gamma }^3)i{\gamma }^1{\gamma }^2{\gamma }^3\\ {\sigma }_{(a,b,c)}& =ia{\gamma }^2{\gamma }^3+ib{\gamma }^3{\gamma }^1+ic{\gamma }^1{\gamma }^2\end{array}$

Note that the above is a root of unity, that is, it squares to 1. Consequently, we can make a projection operator from it that projects out the sub-algebra of the Dirac algebra that has spin oriented in the (a, b, c) direction:

$P_{(a,b,c)}=\frac{1}{2}(1+{\sigma }_{(a,b,c)})$

Now we must choose a charge, +1 (positron) or −1 (electron). Following the conventions of Peskin & Schroeder, the operator for charge is $Q=-{\gamma }^0$, that is, electron states will take an eigenvalue of −1 with respect to this operator while positron states will take an eigenvalue of +1.

Note that $Q$ is also a square root of unity. Furthermore, $Q$ commutes with ${\sigma }_{(a,b,c)}$. They form a complete set of commuting operators for the Dirac algebra. Continuing with our example, we look for a representation of an electron with spin in the Template:Nowrap direction. Turning $Q$ into a projection operator for charge = −1, we have

$P_{-Q}=\frac{1}{2}(1-Q)=\frac{1}{2}(1+{\gamma }^0)$

The projection operator for the spinor we seek is therefore the product of the two projection operators we've found:

$P_{(a,b,c)}{P}_{-Q}$

The above projection operator, when applied to any spinor, will give that part of the spinor that corresponds to the electron state we seek. So we can apply it to a spinor with the value 1 in one of its components, and 0 in the others, which gives a column of the matrix. Continuing the example, we put (a, b, c) = (0, 0, 1) and have

$P_{(0,0,1)}=\frac{1}{2}(1+i{\gamma }_1{\gamma }_2)$

and so our desired projection operator is

$P=\frac{1}{2}(1+i{\gamma }^1{\gamma }^2)\cdot \frac{1}{2}(1+{\gamma }^0)=\frac{1}{4}(1+{\gamma }^0+i{\gamma }^1{\gamma }^2+i{\gamma }^0{\gamma }^1{\gamma }^2)$

The 4×4 gamma matrices used in the Weyl representation are

$\begin{array}{cc}{\gamma }_0& =\left[\begin{array}{cc}0& 1\\ 1& 0\end{array}\right]\\ {\gamma }_k& =\left[\begin{array}{cc}0& {\sigma }^k\\ -{\sigma }^k& 0\end{array}\right]\end{array}$

for k = 1, 2, 3 and where ${\sigma }^i$ are the usual 2×2 Pauli matrices. Substituting these in for P gives

$P=\frac{1}{4}\left[\begin{array}{cc}1+{\sigma }^3& 1+{\sigma }^3\\ 1+{\sigma }^3& 1+{\sigma }^3\end{array}\right]=\frac{1}{2}\left[\begin{array}{cccc}1& 0& 1& 0\\ 0& 0& 0& 0\\ 1& 0& 1& 0\\ 0& 0& 0& 0\end{array}\right]$

Our answer is any non-zero column of the above matrix. The division by two is just a normalization. The first and third columns give the same result:

$|e^{-},+\frac{1}{2}⟩=\left[\begin{array}{c}1\\ 0\\ 1\\ 0\end{array}\right]$

More generally, for electrons and positrons with spin oriented in the (a, b, c) direction, the projection operator is

$\frac{1}{4}\left[\begin{array}{cccc}1+c& a-ib& \pm (1+c)& \pm (a-ib)\\ a+ib& 1-c& \pm (a+ib)& \pm (1-c)\\ \pm (1+c)& \pm (a-ib)& 1+c& a-ib\\ \pm (a+ib)& \pm (1-c)& a+ib& 1-c\end{array}\right]$

where the upper signs are for the electron and the lower signs are for the positron. The corresponding spinor can be taken as any non zero column. Since $a^2+b^2+c^2=1$ the different columns are multiples of the same spinor. The representation of the resulting spinor in the Dirac basis can be obtained using the rule given in the bispinor article.

See also

• Dirac spinor
• Spin(3,1), the double cover of SO(3,1) by a spin group
• Rarita–Schwinger equation

References

• Template:Cite journal
• Template:Citation.