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In modern physics (especially general relativity) spacetime is represented by a Lorentzian manifold. The causal relations between points in the manifold are interpreted as describing which events in spacetime can influence which other events.
The causal structure of an arbitrary (possibly curved) Lorentzian manifold is made more complicated by the presence of curvature. Discussions of the causal structure for such manifolds must be phrased in terms of smoothcurves joining pairs of points. Conditions on the tangent vectors of the curves then define the causal relationships.
Tangent vectors
Subdivision of Minkowski spacetime with respect to a point in four disjoint sets. The light cone, the causal future, the causal past, and elsewhere. The terminology is defined in this article.
If $\,(M,g)$ is a Lorentzian manifold (for metric$g$ on manifold$M$) then the tangent vectors at each point in the manifold can be classified into three disjoint types.
A tangent vector $X$ is:
timelike if $\,g(X,X)<0$
null or lightlike if $\,g(X,X)=0$
spacelike if $\,g(X,X)>0$
Here we use the $(-,+,+,+,\cdots )$metric signature. We say that a tangent vector is non-spacelike if it is null or timelike.
The canonical Lorentzian manifold is Minkowski spacetime, where $M=\mathbb {R} ^{4}$ and $g$ is the flatMinkowski metric. The names for the tangent vectors come from the physics of this model. The causal relationships between points in Minkowski spacetime take a particularly simple form because the tangent space is also $\mathbb {R} ^{4}$ and hence the tangent vectors may be identified with points in the space. The four-dimensional vector $X=(t,r)$ is classified according to the sign of $g(X,X)=c^{2}t^{2}-\|r\|^{2}$, where $r\in \mathbb {R} ^{3}$ is a Cartesian coordinate in 3-dimensional space, $c$ is the constant representing the universal speed limit, and $t$ is time. The classification of any vector in the space will be the same in all frames of reference that are related by a Lorentz transformation (but not by a general Poincaré transformation because the origin may then be displaced) because of the invariance of the metric.
Time-orientability
At each point in $M$ the timelike tangent vectors in the point's tangent space can be divided into two classes. To do this we first define an equivalence relation on pairs of timelike tangent vectors.
If $X$ and $Y$ are two timelike tangent vectors at a point we say that $X$ and $Y$ are equivalent (written $X\sim Y$) if $\,g(X,Y)<0$.
There are then two equivalence classes which between them contain all timelike tangent vectors at the point.
We can (arbitrarily) call one of these equivalence classes future-directed and call the other past-directed. Physically this designation of the two classes of future- and past-directed timelike vectors corresponds to a choice of an arrow of time at the point. The future- and past-directed designations can be extended to null vectors at a point by continuity.
A Lorentzian manifold is time-orientable^{[1]} if a continuous designation of future-directed and past-directed for non-spacelike vectors can be made over the entire manifold.
Curves
A path in $M$ is a continuous map $\mu :\Sigma \to M$ where $\Sigma$ is a nondegenerate interval (i.e., a connected set containing more than one point) in $\mathbb {R}$. A smooth path has $\mu$ differentiable an appropriate number of times (typically $C^{\infty }$), and a regular path has nonvanishing derivative.
A curve in $M$ is the image of a path or, more properly, an equivalence class of path-images related by re-parametrisation, i.e. homeomorphisms or diffeomorphisms of $\Sigma$. When $M$ is time-orientable, the curve is oriented if the parameter change is required to be monotonic.
Smooth regular curves (or paths) in $M$ can be classified depending on their tangent vectors. Such a curve is
chronological (or timelike) if the tangent vector is timelike at all points in the curve. Also called a world line.^{[2]}
null if the tangent vector is null at all points in the curve.
spacelike if the tangent vector is spacelike at all points in the curve.
causal (or non-spacelike) if the tangent vector is timelike or null at all points in the curve.
The requirements of regularity and nondegeneracy of $\Sigma$ ensure that closed causal curves (such as those consisting of a single point) are not automatically admitted by all spacetimes.
If the manifold is time-orientable then the non-spacelike curves can further be classified depending on their orientation with respect to time.
A chronological, null or causal curve in $M$ is
future-directed if, for every point in the curve, the tangent vector is future-directed.
past-directed if, for every point in the curve, the tangent vector is past-directed.
These definitions only apply to causal (chronological or null) curves because only timelike or null tangent vectors can be assigned an orientation with respect to time.
A closed timelike curve is a closed curve which is everywhere future-directed timelike (or everywhere past-directed timelike).
A closed null curve is a closed curve which is everywhere future-directed null (or everywhere past-directed null).
The holonomy of the ratio of the rate of change of the affine parameter around a closed null geodesic is the redshift factor.
Causal relations
There are two types of causal relations between points $x$ and $y$ in the manifold $M$.
$x$chronologically precedes$y$ (often denoted $\,x\ll y$) if there exists a future-directed chronological (timelike) curve from $x$ to $y$.
$x$strictly causally precedes$y$ (often denoted $x<y$) if there exists a future-directed causal (non-spacelike) curve from $x$ to $y$.
$x$causally precedes$y$ (often denoted $x\prec y$ or $x\leq y$) if $x$ strictly causally precedes $y$ or $x=y$.
$x$horismos$y$^{[3]} (often denoted $x\to y$ or $x\nearrow y$) if $x=y$ or there exists a future-directed null curve from $x$ to $y$^{[4]} (or equivalently, $x\prec y$ and $x\not \ll y$).
and satisfy^{[5]}
$x\ll y$ implies $x\prec y$ (this follows trivially from the definition)
For a point $x$ in the manifold $M$ we define^{[5]}
The chronological future of $x$, denoted $\,I^{+}(x)$, as the set of all points $y$ in $M$ such that $x$ chronologically precedes $y$:
$\,I^{+}(x)=\{y\in M|x\ll y\}$
The chronological past of $x$, denoted $\,I^{-}(x)$, as the set of all points $y$ in $M$ such that $y$ chronologically precedes $x$:
$\,I^{-}(x)=\{y\in M|y\ll x\}$
We similarly define
The causal future (also called the absolute future) of $x$, denoted $\,J^{+}(x)$, as the set of all points $y$ in $M$ such that $x$ causally precedes $y$:
$\,J^{+}(x)=\{y\in M|x\prec y\}$
The causal past (also called the absolute past) of $x$, denoted $\,J^{-}(x)$, as the set of all points $y$ in $M$ such that $y$ causally precedes $x$:
$\,J^{-}(x)=\{y\in M|y\prec x\}$
The future null cone of $x$ as the set of all points $y$ in $M$ such that $x\to y$.
The past null cone of $x$ as the set of all points $y$ in $M$ such that $y\to x$.
The light cone of $x$ as the future and past null cones of $x$ together.^{[6]}
elsewhere as points not in the light cone, causal future, or causal past.^{[6]}
Points contained in $\,I^{+}(x)$, for example, can be reached from $x$ by a future-directed timelike curve.
The point $x$ can be reached, for example, from points contained in $\,J^{-}(x)$ by a future-directed non-spacelike curve.
In Minkowski spacetime the set $\,I^{+}(x)$ is the interior of the future light cone at $x$. The set $\,J^{+}(x)$ is the full future light cone at $x$, including the cone itself.
These sets $\,I^{+}(x),I^{-}(x),J^{+}(x),J^{-}(x)$
defined for all $x$ in $M$, are collectively called the causal structure of $M$.
The chronological future of $S$ relative to $T$, $I^{+}(S;T)$, is the chronological future of $S$ considered as a submanifold of $T$. Note that this is quite a different concept from $I^{+}(S)\cap T$ which gives the set of points in $T$ which can be reached by future-directed timelike curves starting from $S$. In the first case the curves must lie in $T$ in the second case they do not. See Hawking and Ellis.
The causal future of $S$ relative to $T$, $J^{+}(S;T)$, is the causal future of $S$ considered as a submanifold of $T$. Note that this is quite a different concept from $J^{+}(S)\cap T$ which gives the set of points in $T$ which can be reached by future-directed causal curves starting from $S$. In the first case the curves must lie in $T$ in the second case they do not. See Hawking and Ellis.
A future set is a set closed under chronological future.
A past set is a set closed under chronological past.
An indecomposable past set (IP) is a past set which isn't the union of two different open past proper subsets.
$I^{-}(x)$ is a proper indecomposable past set (PIP).
A terminal indecomposable past set (TIP) is an IP which isn't a PIP.
The future Cauchy development of $S$, $D^{+}(S)$ is the set of all points $x$ for which every past directed inextendible causal curve through $x$ intersects $S$ at least once. Similarly for the past Cauchy development. The Cauchy development is the union of the future and past Cauchy developments. Cauchy developments are important for the study of determinism.
A subset $S\subset M$ is achronal if there do not exist $q,r\in S$ such that $r\in I^{+}(q)$, or equivalently, if $S$ is disjoint from $I^{+}(S)$.
A Cauchy surface is a closed achronal set whose Cauchy development is $M$.
A metric is globally hyperbolic if it can be foliated by Cauchy surfaces.
The chronology violating set is the set of points through which closed timelike curves pass.
The causality violating set is the set of points through which closed causal curves pass.
For a causal curve $\gamma$, the causal diamond is $J^{+}(\gamma )\cap J^{-}(\gamma )$ (here we are using the looser definition of 'curve' whereon it is just a set of points). In words: the causal diamond of a particle's world-line $\gamma$ is the set of all events that lie in both the past of some point in $\gamma$ and the future of some point in $\gamma$.
Properties
See Penrose (1972), p13.
A point $x$ is in $\,I^{-}(y)$ if and only if $y$ is in $\,I^{+}(x)$.
$I^{\pm }[S]$ is open for all subsets $S\subset M$.
$I^{\pm }[S]=I^{\pm }[{\overline {S}}]$ for all subsets $S\subset M$. Here ${\overline {S}}$ is the closure of a subset $S$.
$I^{\pm }[S]\subset {\overline {J^{\pm }[S]}}$
Conformal geometry
Two metrics $\,g$ and ${\hat {g}}$ are conformally related^{[7]} if ${\hat {g}}=\Omega ^{2}g$ for some real function $\Omega$ called the conformal factor. (See conformal map).
Looking at the definitions of which tangent vectors are timelike, null and spacelike we see they remain unchanged if we use $\,g$ or ${\hat {g}}.$ As an example suppose $X$ is a timelike tangent vector with respect to the $\,g$ metric. This means that $\,g(X,X)<0$. We then have that ${\hat {g}}(X,X)=\Omega ^{2}g(X,X)<0$ so $X$ is a timelike tangent vector with respect to the ${\hat {g}}$ too.
It follows from this that the causal structure of a Lorentzian manifold is unaffected by a conformal transformation.
^Galloway, Gregory J. "Notes on Lorentzian causality"(PDF). ESI-EMS-IAMP Summer School on Mathematical Relativity. University of Miami. p. 4. Retrieved 2021.
A.V. Levichev; Prescribing the conformal geometry of a lorentz manifold by means of its causal structure; Soviet Math. Dokl. 35:452-455, (1987); (Geometry, Causal Structure)
R.D. Sorkin, E. Woolgar; A Causal Order for Spacetimes with C^0 Lorentzian Metrics: Proof of Compactness of the Space of Causal Curves; Classical & Quantum Gravity 13: 1971-1994 (1996); arXiv:gr-qc/9508018 (Causal Structure)