the physics of inflation and dark energy 1.3 dark energy: some evidence (short list) ages of glob....

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The physics of inflation and dark energy 1.3 Dark energy: some evidence (short list) •Ages of glob. clusters/galaxies at z~2-3: m 0.6 •SN Ia: - m 0.3 •CMB: + m 1.0 Large scale motions: 0.15 m 0.4 •Cluster mass function: m 0.3 Bottom line: many indep. hints that m 0.35 0.65

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The physics of inflation and dark energy

1.3 Dark energy: some evidence (short list)

•Ages of glob. clusters/galaxies at z~2-3: m 0.6

•SN Ia: - m 0.3

•CMB: + m 1.0

•Large scale motions: 0.15 m 0.4

•Cluster mass function: m 0.3

Bottom line: many indep. hints that m 0.35

0.65

0.0)

The physics of inflation and dark energy 2. How to achieve acceleration

•Newtonian physics ?DENIED

...only mass is a source for gravity in Newtonian physics

•Einstein’s theory ?

APPROVED...energy density and pressure are components of a tensor (the stress-energy

tensor Tab) and both are sources for gravity

2.1 Physical basis

=> gravity is always attractive...

=> gravity can be “repulsive” (cosmologically) if pressure is sufficiently negative !

The physics of inflation and dark energy

2.2 Einstein, Friedman, de Sitter...

22

2

2222

1)( dr

Kr

drtadtdsFRW geometry:

a

a

abab TGG 8

jiji pTT

00

p<-/3: acceleration

p>-/3: decceleration

22

a

aH 23

8

a

KG

)3(3

4p

G

Friedman equations:

The physics of inflation and dark energy

2.3 Can pressure ever be negative?

0 v:Dust pc

31 :like-Vacuum p

31 v:Radiation pc

General equation of state: pX = wXXwXwX t

The physics of inflation and dark energy

2.4 Pressure and energy density conservation

dVpdE

dE )( Vd dVdV 0)(

dVpdV 0)(1

pdt

dV

Vdt

d

Energy conservation law in FRW: 0)(3

XXX pa

a

)(3 taV

0)w1(3

XXX a

a

wX constant:

)w1(3

00

X

a

aX

)w1(3

2

00

X

t

taa

If X is dominant:

wRad = 1/3wDust = 0w= -1wX = ...

The physics of inflation and dark energy

2.5 Life in an accelerating spacetime

s

00

t

taa

v = c

v = c

v = c

v = c

31- w 1s

:onAccelerati

Horizon:Rhorizon = H-1