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Relativity & Cosmology-II

Oleg RUCHAYSKIY

April 15, 2014

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Reminder: Friedmann equations

Friedmann equations

H (t) ≡

a(t)a(t)˙

H

2

(t) + κ

a

2

= 8πG

3 ρ(t) κ = 0, +1, −1 (1)

∂ρ

∂t + 3H (t)(ρ + p) = 0 (2)

¨ a

a = − 4πG

3 (ρ + 3p) (3)

Einstein’s Λ-term: ρ(t) = −p(t) = const

Matter: ρ(t)a

3

(t) = const, p(t) = 0

Hubble equation — interplay between kinetic energy E

k

=

a˙22

and potential energy E

p

= −

GMa(t)

:

˙ a

2

2 − G

3

ρ(t)a

3

(t)

a(t) = − κ

2

(3)

Reminder: redshift

Universe stretches:

1 + z ≡ λ

observed

λ

emitted

= a(t

obs

) a(t

emit

)

Doppler effect:

a galaxy is receding

1 + z ≡ λ

observed

λ

emitted

=

s

1 + v/c 1 − v/c

where Hubble velocity

v = H

0

× distance

(4)

Luminosity distance

Consider a source (star/galaxy) at redshift z > 0. Let it has intrinsic luminosity L ( energy emitted per unit time, measured in ergs/sec )

In the flat non-expanding “absolute” space we would measure a flux ( energy received per unit time per unit area, measured in ergs/sec/cm

2

):

F = L

4πr

2

non-expanding Universe!

What changes with expansion?

1. Photons change their energy: a photon, emitted with energy E

emit

= ~ ω is detected with the energy E

obs

= ~ ω/(1 + z )

2. Time interval changes as δt

emit

a(t

emit

) = δt

obs

a(t

obs

)

3. Sphere of the area 4πr

2

= 4πr

2

a

2

(t

obs

)

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Luminosity distance

Therefore the flux received from a source at redshift z is given by F = L

4πr

2

→ F = L

4π r

2

a

2

(t

obs

)(1 + z)

2

| {z }

≡d2

L

and the luminosity distance is defined as

d

L

= ra(t

obs

)(1 + z ) = r a

2

(t

obs

) a(t

emit

)

when z 1 one has

z = H0dL Check!

(6)

Cepheids

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Hubble constant measurement

0806.3018

../images/0806_3018_fig1-eps-converted-to.pdf

µ – distance modulus – difference between absolute and apparent magnitude of an object

d = 10

0.2µ−5

Mpc

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Hubble constant history

https://www.cfa.harvard.edu/˜dfabricant/huchra/hubble

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Surface of zero velocity

0811.4610

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Surface of zero velocity

../images/0811_4610_fig1-eps-converted-to.pdf

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Content of the Universe

Friedmann equation ( for spatially flat Universe! ) H

2

(z) = H

02

Λ

+ Ω

mat

(1 + z )

3

+ Ω

rad

(1 + z )

4

( z

today

= 0, z increases into the past )

Ω is a fraction of a given substance in the total energy balance of the Universe today

Relative importance of components changes with time (redshift)

WMAP

website

(12)

Primordial plasma

H

2

(z ) = H

02

Λ

+ Ω

mat

(1 + z)

3

+ Ω

rad

(1 + z )

4

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Primordial plasma

../images/Lambda_matter_radiation-eps-converted-to.pdf

(14)

Primordial plasma

Λ-dominated universe and cosmologyL. M. Krauss R. J. Scherrer “The End of Cosmology?” Scientific American (2008)

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Classification of Friedmann models

../images/Solution_Friedmann_equation-eps-converted-to.pdf

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Classification of Friedmann models

Re-write Friedmann equations selecting out Λ term:

H

2

(t) + κ

a

2

= 8πG

3 ρ(t) + Λ

3 κ = 0, +1, −1 (4)

∂ρ

∂t + 3H (t)(ρ + p) = 0 (5)

¨ a

a = Λ

3 − 4πG

3 (ρ + 3p) (6)

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