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<title>
special relativity in nLab
</title>
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nLab
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special relativity
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<h3 id="context">
Context
</h3>
<h4 id="physics">
Physics
</h4>
<div class="hide">
<div>
<p>
<strong>
<a class="existingWikiWord">
physics
</a>
</strong>
,
<a class="existingWikiWord">
mathematical physics
</a>
,
<a class="existingWikiWord">
philosophy of physics
</a>
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<h2 class="context_menu" id="surveys_textbooks_and_lecture_notes">
Surveys, textbooks and lecture notes
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<p>
<em>
<a class="existingWikiWord">
(higher) category theory and physics
</a>
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<p>
<em>
<a class="existingWikiWord">
geometry of physics
</a>
</em>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
books and reviews
</a>
,
<a class="existingWikiWord">
physics resources
</a>
</p>
</li>
</ul>
<hr>
<p>
<a class="existingWikiWord">
theory (physics)
</a>
,
<a class="existingWikiWord">
model (physics)
</a>
</p>
<p>
<a class="existingWikiWord">
experiment
</a>
,
<a class="existingWikiWord">
measurement
</a>
,
<a class="existingWikiWord">
computable physics
</a>
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<p>
<strong>
<a class="existingWikiWord">
mechanics
</a>
</strong>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
mass
</a>
,
<a class="existingWikiWord">
charge
</a>
,
<a class="existingWikiWord">
momentum
</a>
,
<a class="existingWikiWord">
angular momentum
</a>
,
<a class="existingWikiWord">
moment of inertia
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
dynamics on Lie groups
</a>
</p>
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<li>
<a class="existingWikiWord">
rigid body dynamics
</a>
</li>
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</li>
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</li>
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<p>
<a class="existingWikiWord">
field (physics)
</a>
</p>
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<p>
<a class="existingWikiWord">
Lagrangian mechanics
</a>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
configuration space
</a>
,
<a class="existingWikiWord">
state
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
action functional
</a>
,
<a class="existingWikiWord">
Lagrangian
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
covariant phase space
</a>
,
<a class="existingWikiWord">
Euler-Lagrange equations
</a>
</p>
</li>
</ul>
</li>
<li>
<p>
<a class="existingWikiWord">
Hamiltonian mechanics
</a>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
phase space
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
symplectic geometry
</a>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
Poisson manifold
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
symplectic manifold
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
symplectic groupoid
</a>
</p>
</li>
</ul>
</li>
<li>
<p>
<a class="existingWikiWord">
multisymplectic geometry
</a>
</p>
<ul>
<li>
<a class="existingWikiWord">
n-symplectic manifold
</a>
</li>
</ul>
</li>
</ul>
</li>
<li>
<p>
<a class="existingWikiWord">
spacetime
</a>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
smooth Lorentzian manifold
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
special relativity
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
general relativity
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
gravity
</a>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
supergravity
</a>
,
<a class="existingWikiWord">
dilaton gravity
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
black hole
</a>
</p>
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</ul>
</li>
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<p>
<strong>
<a class="existingWikiWord">
Classical field theory
</a>
</strong>
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<a class="existingWikiWord">
classical physics
</a>
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<a class="existingWikiWord">
classical mechanics
</a>
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<a class="existingWikiWord">
waves
</a>
and
<a class="existingWikiWord">
optics
</a>
</li>
<li>
<a class="existingWikiWord">
thermodynamics
</a>
</li>
</ul>
</li>
</ul>
</li>
<li>
<p>
<strong>
<a class="existingWikiWord">
Quantum Mechanics
</a>
</strong>
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
in terms of &infin;-compact categories
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
quantum information
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
Hamiltonian operator
</a>
</p>
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<p>
<a class="existingWikiWord">
density matrix
</a>
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<h1 id="contents">
Contents
</h1>
<div class="maruku_toc">
<ul>
<li>
<a>
1. Idea
</a>
</li>
<li>
<a>
2. Related concepts
</a>
</li>
<li>
<a>
3. References
</a>
</li>
</ul>
</div>
<h2 id="idea">
1. Idea
</h2>
<p>
In
<a class="existingWikiWord">
physics
</a>
the
<a class="existingWikiWord">
theory
</a>
of
<em>
special relativity
</em>
describes dynamics in
<a class="existingWikiWord">
physical
</a>
<a class="existingWikiWord">
spacetime
</a>
in absence of a field of
<a class="existingWikiWord">
gravity
</a>
.
</p>
<p>
Specifically, it models
</p>
<ul>
<li>
<p>
<a class="existingWikiWord">
spacetime
</a>
as a flat time-oriented
<a class="existingWikiWord">
pseudo-Riemannian manifold
</a>
:
</p>
<p>
<a class="existingWikiWord">
Minkowski space
</a>
;
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
trajectories
</a>
of point
<a class="existingWikiWord">
particles
</a>
as timelike
<a class="existingWikiWord">
curves
</a>
in Minkowski space.
</p>
</li>
<li>
<p>
the
<a class="existingWikiWord">
electromagnetic field
</a>
as a closed 2-
<a class="existingWikiWord">
form
</a>
on Minkowski space.
</p>
</li>
<li>
<p>
the
<a class="existingWikiWord">
Lorentz force
</a>
exerted by the electromagnetic field on a charged particle as the contraction of that 2-form with the tangent vector of the trajectory of the particle.
</p>
</li>
</ul>
<p>
If instead of restricting to Minkowski space, spacetime is allowed to be an arbitrary
<a class="existingWikiWord">
pseudo-Riemannian manifold
</a>
one speaks of the resulting framework as the theory of
<em>
<a class="existingWikiWord">
general relativity
</a>
</em>
.
</p>
<p>
Mathematically, special relativity is essentially the theory of
<a class="existingWikiWord">
Minkowski space
</a>
as a
<a class="existingWikiWord">
pseudo-Riemannian manifold
</a>
, hence equipped with the constant
<a class="existingWikiWord">
metric
</a>
<a class="existingWikiWord">
tensor
</a>
which at each point is the
<a class="existingWikiWord">
bilinear form
</a>
with
<a class="existingWikiWord">
signature
</a>
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(
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&minus;
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,
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+
</mo>
<mo>
,
</mo>
<mi>
&ctdot;
</mi>
<mo>
,
</mo>
<mo lspace="verythinmathspace" rspace="0em">
+
</mo>
<mo stretchy="false">
)
</mo>
</mrow>
<annotation encoding="application/x-tex">
(-,+, \cdots, +)
</annotation>
</semantics>
</math>
or else
<math class="maruku-mathml" display="inline" xmlns="">
<semantics>
<mrow>
<mo stretchy="false">
(
</mo>
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+
</mo>
<mo>
,
</mo>
<mo lspace="verythinmathspace" rspace="0em">
&minus;
</mo>
<mo>
,
</mo>
<mi>
&ctdot;
</mi>
<mo>
,
</mo>
<mo lspace="verythinmathspace" rspace="0em">
&minus;
</mo>
<mo stretchy="false">
)
</mo>
</mrow>
<annotation encoding="application/x-tex">
(+,-,\cdots, -)
</annotation>
</semantics>
</math>
(depending on convention). The null-vectors in this metric characterize the
<a class="existingWikiWord">
speed of light
</a>
. The linear
<a class="existingWikiWord">
isometries
</a>
of this metric are the
<a class="existingWikiWord">
Lorentz transformations
</a>
and the fact that with the Minkowski metric these also preserve, hence, null rays is the mathematical model for the famous
<a class="existingWikiWord">
phenomenological
</a>
observation that &ldquo;the speed of light is the same in all reference systems&rdquo;.
</p>
<h2 id="related_concepts">
2. Related concepts
</h2>
<ul>
<li>
<p>
<a class="existingWikiWord">
speed of light
</a>
</p>
<p>
<a class="existingWikiWord">
Michelson-Morley experiment
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
theory (physics)
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
electromagnetism
</a>
</p>
</li>
<li>
<p>
<a class="existingWikiWord">
general relativity
</a>
,
<a class="existingWikiWord">
gravity
</a>
</p>
</li>
</ul>
<h2 id="references">
3. References
</h2>
<ul>
<li>
Wikipedia,
<em>
<a>
Special relativity
</a>
</em>
</li>
</ul>
</body>
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<p>
Last revised on January 26, 2019 at 11:38:24.
See the
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