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# Four-momentum

In special relativity, four-momentum is the generalization of the classical three-dimensional momentum to four-dimensional spacetime. Momentum is a vector in three dimensions; similarly four-momentum is a four-vector in spacetime. The contravariant four-momentum of a particle with three-momentum \( \vec p = (p_x, p_y, p_z) \) and energy E is

\( \mathbf{P} = \begin{pmatrix} P^0 \\ P^1 \\ P^2 \\ P^3 \end{pmatrix} = \begin{pmatrix} E/c \\ p_x \\ p_y \\ p_z \end{pmatrix} \)

The four-momentum is useful in relativistic calculations because it is a Lorentz vector. This means that it is easy to keep track of how it transforms under Lorentz transformations.

(The above definition applies under the coordinate convention that \( x^0 = ct \). Some authors use the convention \( x^0 = t \) which yields a modified definition with \( P^0 = E/c^2 \). It is also possible to define covariant four-momentum \( P_{\mu} \) where the sign of the 3 momentum is reversed.)

Minkowski norm

Calculating the Minkowski norm of the four-momentum gives a Lorentz invariant quantity equal (up to factors of the speed of light c) to the square of the particle's proper mass:

\( -||\mathbf{P}||^2 = - P^\mu P_\mu = - \eta_{\mu\nu} P^\mu P^\nu = {E^2 \over c^2} - |\vec p|^2 = m^2c^2 \)

where we use the convention that

\( \eta^{\mu\nu} = \begin{pmatrix} -1 & 0 & 0 & 0\\ 0 & 1 & 0 & 0\\ 0 & 0 & 1 & 0\\ 0 & 0 & 0 & 1 \end{pmatrix} \)

is the reciprocal of the metric tensor of special relativity. \( ||\mathbf{P}||^2\! \) is Lorentz invariant, meaning its value is not changed by Lorentz transformations/boosting into different frames of reference.

Relation to four-velocity

For a massive particle, the four-momentum is given by the particle's invariant mass m multiplied by the particle's four-velocity:

\( P^\mu = m \, U^\mu\! \)

where the four-velocity is

\( \begin{pmatrix} U^0 \\ U^1 \\ U^2 \\ U^3 \end{pmatrix} = \begin{pmatrix} \gamma c \\ \gamma v_x \\ \gamma v_y \\ \gamma v_z \end{pmatrix} \)

and \( \gamma = \frac{1}{\sqrt{1-\left(\frac{v}{c}\right)^2}} \)is the Lorentz factor and c is the speed of light.

Conservation of four-momentum

The conservation of the four-momentum yields two conservation laws for "classical" quantities:

- The total energy
*E*=*P*^{0}*c*is conserved. - The classical three-momentum \( \vec p \) is conserved.

Note that the invariant mass of a system of particles may be more than the sum of the particles' rest masses, since kinetic energy in the system center-of-mass frame and potential energy from forces between the particles contribute to the invariant mass. As an example, two particles with four-momenta (−5 GeV/*c*, 4 GeV/*c*, 0, 0) and (−5 GeV/*c*, −4 GeV/*c*, 0, 0) each have (rest) mass 3 GeV/*c*^{2} separately, but their total mass (the system mass) is 10 GeV/*c*^{2}. If these particles were to collide and stick, the mass of the composite object would be 10 GeV/*c*^{2}.

One practical application from particle physics of the conservation of the invariant mass involves combining the four-momenta **P**(*A*) and **P**(*B*) of two daughter particles produced in the decay of a heavier particle with four-momentum **P**(*C*) to find the mass of the heavier particle. Conservation of four-momentum gives *P*(*C*)^{μ} = *P*(*A*)^{μ} + *P*(*B*)^{μ}, while the mass *M* of the heavier particle is given by -||**P**(*C*)||^{2} = *M*^{2}*c*^{2}. By measuring the energies and three-momenta of the daughter particles, one can reconstruct the invariant mass of the two-particle system, which must be equal to M. This technique is used, e.g., in experimental searches for Z' bosons at high-energy particle colliders, where the Z' boson would show up as a bump in the invariant mass spectrum of electron-positron or muon-antimuon pairs.

If an object's mass does not change, the Minkowski inner product of its four-momentum and corresponding four-acceleration *A*^{μ} is zero. The four-acceleration is proportional to the proper time derivative of the four-momentum divided by the particle's mass, so

\( P^{\mu} A_{\mu} = \eta_{\mu\nu} P^{\mu} A^{\nu} = \eta_{\mu\nu} P^{\mu} \frac{d}{d\tau} \frac{P^{\nu}}{m} = \frac{1}{2m} \frac{d}{d\tau} ||\mathbf{P}||^2 = \frac{1}{2m} \frac{d}{d\tau} (-m^2c^2) = 0 . \)

Canonical momentum in the presence of an electromagnetic potential

For applications in relativistic quantum mechanics, it is useful to define a "canonical" momentum four-vector, Q^\mu , which is the sum of the four-momentum and the product of the electric charge with the electromagnetic four-potential:

\( Q^{\mu} = P^{\mu} + q A^{\mu} \! \)

where the four-vector potential is a result of combining the scalar potential and the vector potential:

\( \begin{pmatrix} A^0 \\ A^1 \\ A^2 \\ A^3 \end{pmatrix} = \begin{pmatrix} \phi / c \\ A_x \\ A_y \\ A_z \end{pmatrix} \)

This allows the potential energy from the charged particle in an electrostatic potential and the Lorentz force on the charged particle moving in a magnetic field to be incorporated in a compact way into the Schrödinger equation.

See also

Momentum

Four-force

Four-vector

Special relativity

References

Rindler, Wolfgang (1991). Introduction to Special Relativity (2nd). Oxford: Oxford University Press. ISBN 0-19-853952-5.

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