scieee Science in your language
[en] (orig)

Causal properties of doubly warped spacetimes

Abstract

In this talk we will describe the characterization of the chronological relation on doubly warped product spacetimes of the form (a, b) × M1 × M2 with Lorentzian metric g = −dt2 + α1g1 + α2g2, and we will discuss when these spacetimes are causally continuos and causally simple. This talk is based on the first section of L. Aké, J.L. Flores and J. Herrera, Causality and c-completion of doubly warped spacetimes, available at arXiv:1709.00234.

Read accessible full text

Causal properties of doubly warped spacetimes

Author: Aké Hau, Luis; Flores Dorado, José Luis; Herrera Fernández, Jónathan
Publisher: Godel
Year: 2015
Source: https://idus.us.es/bitstreams/1357a904-cfb9-446e-b997-81b3c4831183/download
XI Encuen o Andaluz de Geome ía
IMUS (Uni e sidad de Se illa), 15 de mayo de 2015, págs. 4751
Causal p ope ies o doubly wa ped space imes
Luis Aké
•
José Luis Flo es
•
Jóna an He e a
Abs ac .
In his alk we will desc ibe he cha ac e iza ion o he ch onological
ela ion on doubly wa ped p oduc space imes o he o m
(a, b)×M1×M2
wi h Lo en zian me ic
g=−d 2+α1g1+α2g2
, and we will discuss when hese
space imes a e causally con inuos and causally simple. This alk is based on he
 s sec ion o [1], a ailable a a Xi :1709.00234.
1. In oduc ion
In he classical book on Lo en zian geome y [2] he causali y o wa ped
space imes p oduc s o he o m
((a, b)×M, −d 2+αgM)
, whe e
((a, b),−d 2)
is
a Lo en zian mani old,
(M, gM)
is a Riemannian mani old and
α:V→(0,∞)
is a smoo h unc ion, is s udied and esul s conce ning o he s ably causal,
s ongly causal and global hype bolici y o hese space imes a e ob ained, see
[2, Lemma 3.55, P op. 3.62 and Thm. 3.66]. Howe e , he s udy o he causally
con inuous and causally simple s ages o he causal hie a chy a e no included.
Ou aim in his alk is o gi e a cha ac e iza ion o he ch onological and causal
ela ions in doubly wa ped space imes and hen we will gi e condi ions o ob ain
he causally con inui y and causal simplici y o hese space imes. The s udy o
he cha ac e iza ion o he ch onological ela ion on hese space imes will be
use ul in o de o s udy he causal comple ion o hese space imes, see [1].
2. P elimina ies
A doubly wa ped space ime can be w i en as:
V:= (a, b)×M1×M2
and
g=−d 2+α1g1+α2g2.
(1)
Luis Aké,
[email p o ec ed]
Depa amen o de Álgeb a, Geome ía y Topología, Uni e sidad de Málaga
José Luis Flo es,
o [email p o ec ed]
Depa amen o de Álgeb a, Geome ía y Topología, Uni e sidad de Málaga
Jóna an He e a,
[email p o ec ed]
Depa amen o de Ma emá icas, Uni e sidad de Có doba
48 L. Aké, J.L. Flo es, J. He e a
Whe e
αi: (a, b)→(0,∞)
a e smoo h unc ions o all
i= 1,2
and
(Mi, gi)
a e
Riemannian mani olds o all
i= 1,2
.
The ch onological ela ion in hese space imes is cha ac e ized in he ollo-
wing p oposi ion (see [1]):
P oposi ion 2.1.
Le
(V, g)
be a doubly wa ped space ime as in (1), and
( o, xo),( e, xe)∈V
wi h
xo6=xe
. The ollowing condi ions a e equi alen :
(i)
( o, xo)( e, xe)
;
(ii) he e exis s ic ly posi i e cons an s
µ0
1, µ0
2>0
, wi h
µ0
1+µ0
2= 1
,
such ha
Z e
opµ0
i
αi(s) 2
X
k=1
µ0
k
αk(s)!−1/2
ds > di(xo
i, xe
i)
o
i= 1,2.
(2)
In o de o gi e a p ope cha ac e iza ion o he causal ela ion in doubly
wa ped space imes we need he ollowing deni ion:
Deni ion 2.1.
A Riemannian mani old
(N, h)
is
L
-
con ex
i any pai o poin s
p, q ∈N
wi h
dh(p, q)< L
can be joined by a minimizing geodesic.
Now, we can es ablish he announced cha ac e iza ion abou he causal e-
la ion (see [3, Thm. 2(2)])
P oposi ion 2.2.
Le
(V, g)
be a doubly wa ped space ime as in (1) whose be s
(Mi, gi)
a e
Li
-con ex o
i= 1,2
. Conside wo poin s
( o, xo
1, xo
2),( e, xe
1, xe
2)∈
V
, wi h
o≤ e
, sa is ying
d(xo
i, xe
i)< Li
,
i= 1,2
. Then, he ollowing condi-
ions a e equi alen :
(i) he poin s a e causally ela ed,
( o, xo
1, xo
2)≤( e, xe
1, xe
2)
;
(ii) he e exis s a causal geodesic joining
( o, xo
1, xo
2)
wi h
( e, xe
1, xe
2)
;
(iii) he e exis cons an s
µ0
1, µ0
2≥0
,
µ0
1+µ0
2= 1
,
such ha
Z e
opµ0
i
αi(s) 2
X
k=1
µ0
k
αk(s)!−1/2
ds ≥di(xo
i, xe
i)
o
i= 1,2.
(3)
Mo eo e , i he equali ies hold in (3), hen he e is a ligh like and no imelike
geodesic joining he poin s.
Wi h he cha ac e iza ion o he ch onological ela ion and causali y ela ion,
he las unde
L−
weakly con ex condi ion, we a e eady o s udy he causally
con inui y and causally simplici y o doubly wa ped space imes.
Causali y on doubly wa ped space imes 49
Causal hie a chy on doubly wa ped space imes
Nex we a e going o p o e ha double wa ped space imes a e causally
con inuous, and, causally simple i and only i each
(Mi, gi)
sa is y a no ion o
L−
con exi y. Fi s we ecall he ollowing deni ions on he causal hie a chy o
space imes, see [5] o a comple e lis :
Deni ion 2.2.
A space ime
(V, g)
is
Causal
i i does no con ain closed causal cu es.
Dis inguishing
i whene e
I+(p) = I+(q)
and
I−(p) = I−(q)
, necessa ily
p=q
.
Causally con inuous
i i is dis inguishing and he se alued unc ions
I+(·)
and
I−(·)
a e ou e con inuous (say,
I+(·)
is
ou e con inuous a
some
p∈V
i , o any compac subse
K⊂I+(p)
he e exis s an open
neighbo hood
U3p
such ha
K⊂I+(q)
o all
q∈U
). This is equi alen
o being dis inguishing and
eec ing
, i.e. o any pai o e en s
p, q ∈V
,
I+(q)⊂I+(p)
i and only i
I−(p)⊂I−(q)
.
Causally simple
i i is causal and
J±(p)
a e closed se s o any
p∈V
.
P op. 2.1 allow us o p o e ha all doubly wa ped space imes a e causally
con inuous:
Theo em 2.1.
Any doubly wa ped space ime
(V, g)
as in (1) is causally con i-
nuous.
Idea o he p oo :
Since
(V, g)
is s ably causal, i is also dis inguishing. So, i
suces o show ha
(V, g)
is eec ing. Le
( o, xo
1, xo
2),( e, xe
1, xe
2)∈V
be such
ha
I+(( e, xe
1, xe
2)) ⊂I+(( o, xo
1, xo
2))
, and le us p o e ha
I−(( o, xo
1, xo
2)) ⊂I−(( e, xe
1, xe
2))
( he con e se is analogous). Conside he se-
quence
{( e+ 1/n, xe
1, xe
2)}n⊂I+(( e, xe
1, xe
2))
and no e ha , by he hypo hesis,
his sequence also belongs o
I+(( o, xo
1, xo
2))
. The e o e, om P op. 2.1, he e
exis cons an s
µn
1, µn
2>0
, wi h
µn
1+µn
2= 1
, sa is ying he ollowing inequali-
ies:
Z e+1/n
opµn
i
αi(s) 2
X
k=1
µn
k
αk(s)!−1/2
ds > di(xo
i, xe
i)
o
i= 1,2.
(4)
Up o a subsequence, we can assume ha
{µn
i}n
con e ges o
µi
, o all
i
, wi h
0≤µ1, µ2≤1
and
µ1+µ2= 1
. Using a gumen s ela ed o con e gence o
50 L. Aké, J.L. Flo es, J. He e a
unc ions we deduce ha :
Z e
o
õi
αi(s) 2
X
k=1
µk
αk(s)!−1/2
ds ≥di(xo
i, xe
i),
o
i= 1,2
.
I we conside
( o−1/n, xo
1, xo
2)
, and modi y sligh ly
(µ1, µ2)
, by con inui y we
ob ain new coecien s
(µ0
1, µ0
2)
, wi h
µ0
1, µ0
2>0
and
µ0
1+µ0
2= 1
and p e-
ious inequali ies a e s ic . Again om P op. 2.1, we ha e
( o−1/n, xo
1, xo
2)
( e, xe
1, xe
2)
o all
n
. So, aking in o accoun ha
I−(( o, xo
1, xo
2)) = ∪n∈NI−(( o−
1/n, xo
1, xo
2))
, we deduce he inclusion
I−(( o, xo
1, xo
2)) ⊂I−(( e, xe
1, xe
2))
, as e-
qui ed.

Also, he cha ac e iza ion o he causal ela ion gi en in P op. 2.2 allow us
o gi e a cha ac e iza ion o he causally simple doubly wa ped p oduc s:
Theo em 2.2.
A doubly wa ped space ime
(V, g)
as in (1) is causally simple i
and only i
(Mi, gi)
is
Li
-con ex o
Li=Rb
a
1
√αi(s)ds
, o all
i= 1,2
.
Main idea:
Fo he implica ion o he igh . Le
xo
1
and
xe
1
wi h
0< d1(xo
1, xe
1)< L1=Zb
a
ds
pα1(s),
hen, he e exis s some
c1
and
c2
wi h
a<c1< c2< b
and
d1(xo
1, xe
1)<
Rc2
c1
ds
√α1(s)
ake some poin
x2=x0
2=xe
2
in
M2
and conside he ollowing
poin s
(c1, xo
1, x2)
and
(c2, xe
1, x2)
, hen, by P op. 2.1 we ha e ha
(c2, xe
1, x2)∈
I+((c1, xo
1, x2))
. Since
(c1, xe
1, x2)6∈ I+((c1, xo
1, x2))
, he e exis s a poin
( e, xe
1, x2)) ∈∂I+((c1, xo
1, x2)) = J+((c1, xo
1, x2)) I+((c1, xo
1, x2)),
(because
(V, g)
is causally simple), so, he e exis s a null geodesic be ween hese
poin s. The p ojec ion o his geodesic on
M1
will be a minimizing geodesic
be ween
xo
1
and
xe
1
, he e o e
(M1, g1)
is
L1
-con ex, he same easoning gi es
he esul o
(M2, g2)
.
Fo he implica ion o he le , we ha e o show ha
J±(( o, xo
1, xo
2)) = J±(( o, xo
1, xo
2)),
o all
( o, xo
1, xo
2)∈V
. Reasoning o he u u e case, le
( e, xe
1, xe
2)∈J+(( o, xo
1, xo
2)),
Causali y on doubly wa ped space imes 51
and conside a sequence
{( e+ 1/n, xe
1, xe
2)}n⊂I+(( o, xo
1, xo
2))
, using P op. 2.1
and con e gence o unc ions we show ha
di(xo
i, xe
i)<Zb
a
õi
αi(s) 2
X
k=1
µk
αk(s)!−1/2
ds ≤Zb
a
1
pαi(s)ds =Li,
and, since
(Mi, gi)
is
Li
-con ex we ha e ha P op. 2.2 implies ha
( e, xe
1, xe
2)∈
J+(( o, xo
1, xo
2))
. The pas case is analogous.

Acknowledgmen s
The au ho s a e pa ially suppo ed by he Spanish G an MTM2016-78807-
C2-2-P (MINECO and FEDER unds). L. Aké also acknowledges a g an unded
by he Consejo Nacional de Ciencia y Tecnología (CONACyT), México.
Re e ences
[1] L. Aké, J.L. Flo es and J. He e a,
Causali y and c-comple ion o doubly
wa ped space imes
, a Xi :1709.00234.
[2] J.K. Beem, P.E. Eh lich and K.L. Easley,
Global Lo en zian Geome y
.
Monog aphs Tex books Pu e Appl. Ma h.
202
, Dekke Inc., New Yo k
(1996).
[3] J.L. Flo es and M. Sánchez,
Geodesic connec edness o mul iwa ped spa-
ce imes.
J. Die en ial Equa ions,
186
(1):1-30, 2002.
[4] J.L. Flo es and M. Sánchez,
The causal bounda y o wa e- ype space imes
.
J. High. Ene gy Phys., (3):036,
43
, 2008.
[5] E. Minguzzi and M. Sánchez,
The causal hie a chy o space imes
. Zu ich:
Eu . Ma h. Soc. Publ. House, ol. H. Baum, D. Aleksee sky (eds.), Recen
de elopmen s in Pseudo-Riemannian geome y o ESI Lec . Ma h. Phys.,
299358 (2008).
[6] Volke Pe lick.
G a i a ional lensing om a space ime pe spec i e
. Li ing
Re iews in Rela i i y,
7
(1):9 2004.