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5.4 Energy Conditions
T__ satis_es the dominant energy condition if for all future-directed timelike vector _elds
v, the vector _eld
j(v) _ v_T _
_ @_ (5.48)
is future-directed non-spacelike, or zero.
All physically reasonable matter satis_es this condition, e.g. for massless
scalar _eld _ (with T__ = @__@__ 1
2g__(@_)2):
j_(v) = v _ @_@__ +
1
2
v_(@_)2 (5.49)
j2(v) =
1
4
v2
(@_)2_2
| {z }
_0
_ 0 if v2 < 0 (5.50)
so j(v) is timelike or null if v is timelike. Since v is assumed future-directed,
j(v) will be too if v _ j > 0. Allowing for j = 0 means that we have to
prove that v _ j _ 0. Now
v _ j = (v _ @_)2
1
2
v2(@_)2 (5.51)
=
1
2
(v _ @_)2 +
1
2
v2__
@_
v(v _ @_)
v2
_2
(5.52)
But (v _ @_)2 _ 0 and v2 > 0 for timelike v, so we have to prove that
_
@_
v(v _ @_)
v2
_2
_ 0 (5.53)
i.e. that
_
@_ v(v_@_)
v2
_
is spacelike or zero. This follows from
v _
_
@_
v(v _ @_)
v2
_
= 0 (5.54)
99
since v _V < 0 for any non-zero timelike or null vector for timelike v (choose
coordinates s.t. v = (1;~0)). So if v _V = 0 then V cannot be timelike or null.
Since v _ j = v_v_T__ , the dominant energy condition implies that
v_v_T__ _ 0 for all timelike v. By continuity it also implies the
Weak energy condition
v_v_T__ _ 0 8 non-spacelike v (5.55)
There is also the
Strong energy condition
v_v_
_
T__
1
2
g__T
_
_ 0 8 non-spacelike v (5.56)
Note, Dominant 6, Strong.
The strong energy condition is needed to prove the singularity theorems,
but the dominant energy condition is the physically important one. (An
inationary universe violates the strong energy condition). For example it
is needed for the
Positive Energy Theorem (Shoen & Yau, Witten)
The ADM energy of an asymptotically-at spacetime satisfying G__ =
8_GT__ is positive semi-de_nite, and vanishes only for Minkowski spacetime
with T__ = 0, provided that
i) 9 an initially non-singular Cauchy surface (otherwiseM < 0 Schwarzschild
would be a counter-example).
ii) T__ satis_es the dominant energy condition (clearly, some condition
on T__ is necessary).
iii) Some other technical assumptions which we ignore here.
100
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