14
Conserved Quantities in General Relativity A story about asymptotic flatness

Conserved Quantities in General Relativity A story about asymptotic flatness

Embed Size (px)

Citation preview

Page 1: Conserved Quantities in General Relativity A story about asymptotic flatness

Conserved Quantities in General Relativity

A story about asymptotic flatness

Page 2: Conserved Quantities in General Relativity A story about asymptotic flatness

Conserved quantities in physics

Charge Mass Energy Momentum Parity Lepton Number

Page 3: Conserved Quantities in General Relativity A story about asymptotic flatness

Conserved quantities in physics

Energy– Time translation

Momentum– Linear translation

Parity– Inversion

Charge– Phase of the gauge field

Page 4: Conserved Quantities in General Relativity A story about asymptotic flatness

Measurement

Direct– Scales, meter sticks

Indirect– Fields due to the conserved quantity

Page 5: Conserved Quantities in General Relativity A story about asymptotic flatness

Measurement

Direct Indirect

– Fields due to the conserved quantity

dAnM

dAnEQ

ˆ4

1

ˆ0

Page 6: Conserved Quantities in General Relativity A story about asymptotic flatness

Extension to General Relativity

Komar Mass, requires existence of Killing vector

ADM Mass, hab is the expansion of gab around Minkowski

S

dcabcdM 8

1

dAnEQ ˆ0

dAnhhM b

S aababa )(161

Page 7: Conserved Quantities in General Relativity A story about asymptotic flatness

Extension to General Relativity

Komar Mass, requires existence of Killing vector

ADM Mass, hab is the expansion of gab around Minkowski

S

dcabcdM 8

1

dAnEQ ˆ0

dAnhhM b

S aababa )(161

Small note: These definitions hold in anAsymptotically flat spacetime

Page 8: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Intuitively,

4

3

2

1

1

1

Rabdc

Rabc

Rab

ababab

h

h

h

hg

Page 9: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Intuitively, Problems:– Expansion might not be

possible for a general metric

– Exchanging limits and derivatives causes issues

4

3

2

1

1

1

Rabdc

Rabc

Rab

ababab

h

h

h

hg

Page 10: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Better: Conformal mapping to put “infinity” in a finite place

22222 drdrdtds

Vv

Uu

rtv

rtu

tan

tan

2222

2 )(sin4coscos4

1 dUVdUdV

VUds

Page 11: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Better: Conformal mapping to put “infinity” in a finite place

UVR

VUT

gVUg

2)coscos2(~

2222

2 )(sin4coscos4

1 dUVdUdV

VUds

22222 sin dRdRdTds

Page 12: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Einstein Universe– i0 “spacelike infinity” R=, T=0– i+ “future timelike infinity” R=0, T=– “future null infinity” T=– R

We’ve thus taken infinity and placed it in our extended spacetime

22222 sin dRdRdTds

Page 13: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

Asymptotically simple:– (M,gab) is an open submanifold of (M,gab) with

smooth boundary– There exists a smooth scalar field such that

( ) = 0 d( ) not 0gab=2 gab

– Every null geodesic in M begins and ends on– Asymptotically flat:

Asymptotically simple Rab=0 in the neighbourhood of

Page 14: Conserved Quantities in General Relativity A story about asymptotic flatness

“Asymptotically Flat?”

What is asymptotically flat:– Minkowski– Schwarzchild– Kerr

What is not:– De Sitter universe (no matter, positive

cosmological constant)– Schwarzschild-de Sitter lambdavacuum– Friedmann – Lemaître – Robertson – Walker

Homogenous, isotropically expanding (or contracting)