Minkowski Space

(redirected from Minkowskian)

Minkowski Space

 

a four-dimensional space, combining the physical three-dimensional space and time; introduced by H. Minkowski in 1907–08. Points in Minkowski space correspond to “events” of the special theory of relativity.

The position of an event in Minkowski space is specified by four coordinates—three space coordinates and one time coordinate. The coordinates that are usually used are x = x, x2 = y, x3 = z, where x, y, and z are rectangular Cartesian coordinates of the event in a given inertial frame of reference, and the coordinate xθ = ct, where t is the time of the event and c is the velocity of light. The imaginary time coordinate x4 = ix0 = ict can be introduced instead of X0.

It follows from the special theory of relativity that space and time are not independent. In passing from one inertial frame of reference to another, the space coordinates and the time are transformed through each other by Lorentz transformations. The introduction of Minkowski space permits the Lorentz transformation to be represented as the transformation of the coordinates x1, x2, x3, x4 of an event in a rotation of the four-dimensional coordinate system in this space.

The chief invariant of Minkowski space is the square of the length of the four-dimensional vector that connects two points—events—and that remains invariant in rotations in Minkowski space and equal in magnitude (but opposite in sign) to the square of the four-dimensional interval (sAB2) of the special theory of relativity:

(x1Ax1B)2 + (x2Ax2B)2 + (x3Ax3B)2 + (x4Ax4B)2 = (xAxB)2 + (yAyB)2 + (zAzB)2 + c2(tAtB)2 = −sAB2

where the subscripts A and B indicate the space coordinates and time of events A and B, respectively. The uniqueness of the geometry of Minkowski space is that this expression contains the squares of the components of a four-dimensional vector along the time and space axes with different signs (such a geometry is said to be pseudo-Euclidean, in contrast to Euclidean geometry in which the square of the distance between two points is determined by the sum of the squares of the components, on the corresponding axes, of the vector that joins the points). As a result, a four-dimensional vector with nonzero components can have zero length. This is the case for the vector that joins two events connected by a light signal:

(xAxB)2 + (yAyB)2 + (zAzB)2 + c2(tAtB)2 = c2(tA - tB)

The geometry of Minkowski space makes it possible to give a lucid interpretation of the kinematic effects of the special theory of relativity (for example, the variation in length and rate of passage of time in passing over from one inertial frame of reference to another). It also serves as the basis for the modern mathematical apparatus of the theory of relativity.

G. A. ZISMAN

References in periodicals archive ?
Rehren and the PI is the basis to set up the operator-algebraic, Minkowskian description of phase boundary, relating to the tensor categorical, Euclidean description by J.
Later chapters take a closer look at the photon source domain and field propagators, the photon vacuum and light quanta in Minkowskian space, and two-photon entanglement associated with the biphoton in space-time.
These differences in symmetries can be empirically measured, strongly favouring a Minkowskian space-time over a Galilean space-time.
Sets of basis vectors, also labeled by a binary index, with signature 0 and any (necessarily even) number of dimensions can thus be built up recursively from the basis vectors (one space-like and one time-like) of the Minkowskian plane.
K is of constant Minkowskian width if all its affine diameters have equal lengths measured in the respective norm; see [7] and the survey [13].
Busemann, The foundations of Minkowskian geometry, Comment.
with the first four components denoting a Minkowskian space-time vector in Cartesian coordinates:
He surveys some of its recent triumphs--such as dissolving the dichotomy between Einsteinian and Minkowskian relativity--and emphasizes the interdisciplinary collaborations required to further develop the mathematical innovation and its applications.
In the first place, much depends upon which interpretation of SR is adopted: the Einsteinian relativity interpretation (which is a theoretical construct rather than an ontology or depiction of reality, leading to a denial of any objective frame of reference and simultaneity and affirming a pluralist ontology) or the Minkowskian spacetime interpretation (in which a shared, objective unified reality exists independently of observers or reference frames).
Measor says that "the four-dimensional 'space-time worms' which inhabit, say, Minkowskian space-time, are one and the same as the enduring things with which we are familiar.
This demand--equivalent to the demand that space-time be Minkowskian (in the formulation of theories)--is not merely a methodological principle for, as we have seen, it has substantial physics in it.
If the Universe began with a state of maximum entropy than we can very well assume that space-time was not Minkowskian even locally.