In quantum mechanics, momentum is an operator which maps the wave function ψ(x, t) to another function. If this new function is a constant p multiplied by the original wave function ψ, then p is the eigenvalue of the momentum operator, and ψ is the eigenfunction of the momentum operator. In quantum mechanics, the set of eigenvalues of an operator are the possible results measured in an experiment. The momentum operator is an example of a differential operator, for the case of one particle in one dimension, the definition is
Contents
- Origin from De Broglie plane waves
- One dimension
- Three dimensions
- Definition position space
- Hermiticity
- Canonical commutation relation
- Fourier transform
- Derivation from infinitesimal translations
- 4 momentum operator
- References
where ħ is Planck's reduced constant, i the imaginary unit, and partial derivatives (denoted by
It is usual to think of the p-operator as "multiplying" the function, but this is not what is happening. The derivative of the function is taken.
At the time quantum mechanics was developed in the 1920s, the momentum operator was found by many theoretical physicists, including Niels Bohr, Arnold Sommerfeld, Erwin Schrödinger, and Eugene Wigner.
Origin from De Broglie plane waves
The momentum and energy operators can be constructed in the following way.
One dimension
Starting in one dimension, using the plane wave solution to Schrödinger's equation:
The first order partial derivative with respect to space is
By expressing k from the De Broglie relation:
the formula for the derivative of ψ becomes:
This suggests the operator equivalence:
so the momentum value p is a scalar factor, the momentum of the particle and the value that is measured, is the eigenvalue of the operator.
Since the partial derivative is a linear operator, the momentum operator is also linear, and because any wavefunction can be expressed as a superposition of other states, when this momentum operator acts on the entire superimposed wave, it yields the momentum eigenvalues for each plane wave component, the momenta add to the total momentum of the superimposed wave.
Three dimensions
The derivation in three dimensions is the same, except the gradient operator del is used instead of one partial derivative. In three dimensions, the plane wave solution to Schrödinger's equation is:
and the gradient is
where ex, ey and ez are the unit vectors for the three spatial dimensions, hence
This momentum operator is in position space because the partial derivatives were taken with respect to the spatial variables.
Definition (position space)
For a single particle with no electric charge and no spin, the momentum operator can be written in the position basis as:
where ∇ is the gradient operator, ħ is the reduced Planck constant, and i is the imaginary unit.
In one spatial dimension this becomes:
This is a commonly encountered form of the momentum operator, though not the most general one. For a charged particle q in an electromagnetic field, described by the scalar potential φ and vector potential A, the momentum operator must be replaced by:
where the canonical momentum operator is the above momentum operator:
This is of course true for electrically neutral particles also, since the second term vanishes if q = 0 and the original operator appears.
Hermiticity
The momentum operator is always a Hermitian operator when it acts on physical (in particular, normalizable) quantum states.
(In certain artificial situations, such as the quantum states on the semi-infinite interval [0,∞), there is no way to make the momentum operator Hermitian. This is closely related to the fact that a semi-infinite interval cannot have translational symmetry—more specifically, it does not have unitary translation operators. See below.)
Canonical commutation relation
One can easily show that by appropriately using the momentum basis and the position basis:
The Heisenberg uncertainty principle defines limits on how accurately the momentum and position of a single observable system can be known at once. In quantum mechanics, position and momentum are conjugate variables.
Fourier transform
One can show that the Fourier transform of the momentum in quantum mechanics is the position operator. The Fourier transform turns the momentum-basis into the position-basis. The following discussion uses the bra–ket notation:
Let
So momentum = h x spatial frequency, which is similar to energy = h x temporal frequency.
The same applies for the position operator in the momentum basis:
and other useful relations:
where δ stands for Dirac's delta function.
Derivation from infinitesimal translations
The translation operator is denoted T(ε), where ε represents the length of the translation. It satisfies the following identity:
that becomes
Assuming the function ψ to be analytic (i.e. differentiable in some domain of the complex plane), one may expand in a Taylor series about x:
so for infinitesimal values of ε:
As it is known from classical mechanics, the momentum is the generator of translation, so the relation between translation and momentum operators is:
thus
4-momentum operator
Inserting the 3d momentum operator above and the energy operator into the 4-momentum (as a 1-form with (+ − − −) metric signature):
obtains the 4-momentum operator;
where ∂μ is the 4-gradient, and the −iħ becomes +iħ preceding the 3-momentum operator. This operator occurs in relativistic quantum field theory, such as the Dirac equation and other relativistic wave equations, since energy and momentum combine into the 4-momentum vector above, momentum and energy operators correspond to space and time derivatives, and they need to be first order partial derivatives for Lorentz covariance.
The Dirac operator and Dirac slash of the 4-momentum is given by contracting with the gamma matrices:
If the signature was (− + + +), the operator would be
instead.