The form of a theory has to be invariant under a transformation from one
inertial system to another.
Consider two observers, and
, in different inertial systems.
They describe the same physical event with their particular
(different) space-time coordinates.
Let the coordinates of the event be
for observer
and
for observer
.
A Lorentz change of reference is a real linear transformation of the coordinates conserving the norm of the intervals between the different points in space-time. By means of the Lorentz transformation
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(3.1) |
The real vector represents a simple translation of the
space-time axes.
In what follows, we shall treat the translations separately and give
the name Lorentz transformation to the homogeneous translations
(
).
The group formed by all Lorentz transformations including translations
is commonly called the inhomogeneous Lorentz group, or Poincaré
group.
is real (
) and depends
only on the relative velocities and spatial orientations of reference
frames.
The inverse transformation is
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(3.2) |
The distance between two space-time points is invariant
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(3.3) |
To see this
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(3.4) |
and
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(3.5) |
Therefore
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(3.6) |
which is the orthogonality relation for the Lorentz transformation.
The determinant is calculated using
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(3.7) |
Since
,
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(3.8) |
Therefore
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(3.9) |
For
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(3.10) |
we have a proper Lorentz transformation (rotations and boosts).
For
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(3.11) |
we have an improper Lorentz transformation (discrete reflection either in space or in time). Including the improper Lorentz transformation of the reflection in space into the Lorentz group gives the orthochronous Lorentz group. If time reversal is also included, it is called the complete Lorentz group.
For an infinitesimal transformation we can write
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(3.12) |
where
is infinitesimal.
Since is real,
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(3.13) |
Using the orthogonality relationship and only keeping terms to first
order in , gives
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|
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|
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||
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(3.14) |
Therefore
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|
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(3.15) |
and
is an anti-symmetric tensor.
A general Lorentz transformation thus has six parameters: three boost
parameters and three rotation parameters.