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AlbaNova, University of Stockholm, May 13, 2014 AlbaNova, University of Stockholm, May 13, 2014

AlbaNova, University of Stockholm, May 13, 2014 - PowerPoint Presentation

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AlbaNova, University of Stockholm, May 13, 2014 - PPT Presentation

Cosmic parallax Syksy Räsänen University of Helsinki Department of Physics and The Helsinki Institute of Physics 1 arXiv13125738 AlbaNova University of Stockholm May 13 2014 Change of viewpoint ID: 360072

albanova parallax stockholm university parallax albanova university stockholm 2014 frw distance motion test intrinsic sources frame cosmological rest cmb

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Slide1

AlbaNova, University of Stockholm, May 13, 2014

Cosmic parallax

Syksy RäsänenUniversity of HelsinkiDepartment of Physics andThe Helsinki Institute of Physics

1

arXiv:1312.5738Slide2

AlbaNova, University of Stockholm, May 13, 2014

Change of viewpoint

Parallax is the change in the angular position of objects when seen from different locations.Can measure distance without knowing source properties.Problem for the heliocentric system in the 1500’s.Best current measurement by Hipparcos (1989-1993)

at 100 pc.Can be used as a cosmological test. (McCrea 1935

)

2Slide3

AlbaNova, University of Stockholm, May 13, 2014

Motion parallax

Classic definition of parallax distance: Naively, maximum δx = 2 AU.However, motion wrt. CMB frame is 78 AU/yr.

(Kardashëv 1986)

For adiabatic perturbations,

CMB

rest frame is the same as the rest frame of cosmological sources.

3Slide4

AlbaNova, University of Stockholm, May 13, 2014

Intrinsic parallax

Assume that both sources and observers move along the same timelike curves.The angle between a pair of sources is constant for all pairs and all observers at all times if and only if the spacetime is conformally stationary. (Hasse and

Perlick 1988)Dust matter:

spacetime

is

FRW

or stationary.

Same condition as vanishing CMB anisotropy.4Slide5

AlbaNova, University of Stockholm, May 13, 2014

5

Classic parallax

Observational parallaxSlide6

AlbaNova, University of Stockholm, May 13, 2014

Parallax in general

Consider a pair of sources located in directions r1 and r2. The angle φ between them is given by For observers moving along a

timelike geodesic:

6

motion parallax related to image deformation (small)

intrinsic parallax

motion parallax related to distanceSlide7

AlbaNova, University of Stockholm, May 13, 2014

Parallax distance

Classic definition of parallax distance: Suitable for a single source and spacelike separated observation points.Real observations: relative angles, timelike separated observation points.Modern definition:

(Ellis 1971)

7Slide8

AlbaNova, University of Stockholm, May 13, 2014

DP and

DA‘Parallax is angular diameter in reverse.’For DP, beam converges at the source, for DA it converges at the observer.

(No image deformation) (Rosquist

1988)

Compare (

Etherington

1933)

8Slide9

AlbaNova, University of Stockholm, May 13, 2014

Parallax in the FRW universe

In the FRW case there is no intrinsic parallax:The parallax distance is (McCrea 1935)

Solving for k, we have

9Slide10

AlbaNova, University of Stockholm, May 13, 2014

Testing the FRW

metricIf kP is not constant, universe is not FRW. (More precisely: the optical properties of the universe are not FRW.)This test of the D-D

P relation is independent of matter content or the Einstein equation.Test of

FRW

kinematics using only null geodesics. (Geometrical optics, no dynamics.)

Similar to the

D-H

relation

(Clarkson et al 2007):10Slide11

AlbaNova, University of Stockholm, May 13, 2014

Beyond FRW

Backreaction: statistical homogeneity and isotropy does not imply FRW.Parallax can be used to test specific models violating homogeity and isotropy, like large voids: real-time cosmology. (

Quercellini et al 2008)Perturbations have to be taken into account: intrinsic perturbation parallax is of the same order of magnitude as

motion

parallax.

Correct treatment of local motion requires non-linear treatment

.

11Slide12

AlbaNova, University of Stockholm, May 13, 2014

Gaia

ESA satellite launched on 19.12.2013.Will measure 3 million galaxies up to z=0.75 and 500 000 quasars up to z=5.Precision 100 μas.

Cosmological signal:

δφ

H

0

δx=H

0vδt∼10-2 μas δt/yr.Errors down by 1/(2

N

)

1/2

∼10

-3

, so feasible? (Rest frame?)

12Slide13

AlbaNova, University of Stockholm, May 13, 2014

Future

Cosmic parallax provides a powerful test of the FRW metric.Will be first probed by the Gaia satellite (some parallax data out in 2016, full data in 2022).More work needed for the cosmological analysis.

13