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In a relativistic theory of physics, a **Lorentz scalar** is an expression, formed from items of the theory, which evaluates to a scalar, invariant under any Lorentz transformation. A Lorentz scalar may be generated from e.g., the scalar product of vectors, or from contracting tensors of the theory. While the components of vectors and tensors are in general altered under Lorentz transformations, Lorentz scalars remain unchanged.

A Lorentz scalar is not always immediately seen to be an invariant scalar in the mathematical sense, but the resulting scalar value is invariant under any basis transformation applied to the vector space, on which the considered theory is based. A simple Lorentz scalar in Minkowski spacetime is the *spacetime distance* ("length" of their difference) of two fixed events in spacetime. While the "position"-4-vectors of the events change between different inertial frames, their spacetime distance remains invariant under the corresponding Lorentz transformation. Other examples of Lorentz scalars are the "length" of 4-velocities (see below), or the Ricci curvature in a point in spacetime from General relativity, which is a contraction of the Riemann curvature tensor there.

In special relativity the location of a particle in 4-dimensional spacetime is given by

The "length" of the vector is a Lorentz scalar and is given by

This is a time-like metric.

Often the alternate signature of the Minkowski metric is used in which the signs of the ones are reversed.

This is a space-like metric.

In the Minkowski metric the space-like interval is defined as

We use the space-like Minkowski metric in the rest of this article.

The velocity in spacetime is defined as

where

The magnitude of the 4-velocity is a Lorentz scalar,

Hence, c is a Lorentz scalar.

The 4-acceleration is given by

The 4-acceleration is always perpendicular to the 4-velocity

Therefore, we can regard acceleration in spacetime as simply a rotation of the 4-velocity. The inner product of the acceleration and the velocity is a Lorentz scalar and is zero. This rotation is simply an expression of energy conservation:

The 4-momentum of a particle is

Consider a second particle with 4-velocity and a 3-velocity . In the rest frame of the second particle the inner product of with is proportional to the energy of the first particle

Since the relationship is true in the rest frame of the second particle, it is true in any reference frame. , the energy of the first particle in the frame of the second particle, is a Lorentz scalar. Therefore,

In the rest frame of the particle the inner product of the momentum is

Therefore, the rest mass (m) is a Lorentz scalar. The relationship remains true independent of the frame in which the inner product is calculated. In many cases the rest mass is written as to avoid confusion with the relativistic mass, which is .

Note that

The square of the magnitude of the 3-momentum of the particle as measured in the frame of the second particle is a Lorentz scalar.

The 3-speed, in the frame of the second particle, can be constructed from two Lorentz scalars

Scalars may also be constructed from the tensors and vectors, from the contraction of tensors (such as ), or combinations of contractions of tensors and vectors (such as ).

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