Dirac adjoint
Encyclopedia
In quantum field theory
, the Dirac adjoint of a Dirac spinor is defined to be the dual spinor
, where is the time-like gamma matrix. Possibly to avoid confusion with the usual Hermitian adjoint
, some textbooks do not give a name to the Dirac adjoint, simply calling it "psi-bar".
, and is not even Hermitian
. One source of trouble is that if is the spinor representation
of a Lorentz transformation
, so that
then
Since the Lorentz group
of special relativity
is not compact
, will not be unitary
, so . Using fixes this problem, in that it transforms as
density for a spin-1/2 particle field
where is the probability density and j the probability current 3-density can be written as
where c is the speed of light. Taking and using the relation for Gamma matrices
the probability density becomes
.
Quantum field theory
Quantum field theory provides a theoretical framework for constructing quantum mechanical models of systems classically parametrized by an infinite number of dynamical degrees of freedom, that is, fields and many-body systems. It is the natural and quantitative language of particle physics and...
, the Dirac adjoint of a Dirac spinor is defined to be the dual spinor
Spinor
In mathematics and physics, in particular in the theory of the orthogonal groups , spinors are elements of a complex vector space introduced to expand the notion of spatial vector. Unlike tensors, the space of spinors cannot be built up in a unique and natural way from spatial vectors...
, where is the time-like gamma matrix. Possibly to avoid confusion with the usual Hermitian adjoint
Hermitian adjoint
In mathematics, specifically in functional analysis, each linear operator on a Hilbert space has a corresponding adjoint operator.Adjoints of operators generalize conjugate transposes of square matrices to infinite-dimensional situations...
, some textbooks do not give a name to the Dirac adjoint, simply calling it "psi-bar".
Motivation
The Dirac adjoint is motivated by the need to form well-behaved, measurable quantities out of Dirac spinors. For example, is not a Lorentz scalarLorentz scalar
In physics, a Lorentz scalar is a scalar which is invariant under a Lorentz transformation. A Lorentz scalar may be generated from multiplication of vectors or tensors...
, and is not even Hermitian
Self-adjoint operator
In mathematics, on a finite-dimensional inner product space, a self-adjoint operator is an operator that is its own adjoint, or, equivalently, one whose matrix is Hermitian, where a Hermitian matrix is one which is equal to its own conjugate transpose...
. One source of trouble is that if is the spinor representation
Representations of the Lorentz group
The Lorentz group of theoretical physics has a variety of representations, corresponding to particles with integer and half-integer spins in quantum field theory. These representations are normally constructed out of spinors....
of a Lorentz transformation
Lorentz transformation
In physics, the Lorentz transformation or Lorentz-Fitzgerald transformation describes how, according to the theory of special relativity, two observers' varying measurements of space and time can be converted into each other's frames of reference. It is named after the Dutch physicist Hendrik...
, so that
then
Since the Lorentz group
Lorentz group
In physics , the Lorentz group is the group of all Lorentz transformations of Minkowski spacetime, the classical setting for all physical phenomena...
of special relativity
Special relativity
Special relativity is the physical theory of measurement in an inertial frame of reference proposed in 1905 by Albert Einstein in the paper "On the Electrodynamics of Moving Bodies".It generalizes Galileo's...
is not compact
Compact space
In mathematics, specifically general topology and metric topology, a compact space is an abstract mathematical space whose topology has the compactness property, which has many important implications not valid in general spaces...
, will not be unitary
Unitary operator
In functional analysis, a branch of mathematics, a unitary operator is a bounded linear operator U : H → H on a Hilbert space H satisfyingU^*U=UU^*=I...
, so . Using fixes this problem, in that it transforms as
Usage
Using the Dirac adjoint, the conserved probability four-currentFour-current
In special and general relativity, the four-current is the Lorentz covariant four-vector that replaces the electromagnetic current density, or indeed any conventional charge current density...
density for a spin-1/2 particle field
where is the probability density and j the probability current 3-density can be written as
where c is the speed of light. Taking and using the relation for Gamma matrices
the probability density becomes
.