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Anisotropic Orientations of Polarisations from quasar light

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A

NISOTROPIC

O

RIENTATIONS

OF

P

OLARISATIONS FROM

Q

UASAR

L

IGHT

_

V

INCENT

P

ELGRIMS

in collaboration with J.-R. Cudell

_

IFPA, AGO Dept.

GRAPPA A

NISOTROPY

W

ORKSHOP

Sept. 2013

,

A

MSTERDAM

(2)

Introduction

The large-scale coherent orientations of quasar

polarisation vectors

Probability of uniformity ~

6 10

-5

[Hutsemékers, D. 1998]

[Hutsemékers, D., Lamy, H. 2001]; [Jain et al. 2004]; [Cabanac et al. 2005]; [Hutsemékers et al. 2005];

Full sample : 355 quasars

Orientation correlations up to ~1 Gpc

at z ≈ 1-2

(3)

Significance Level coordinate system

i =1,2,3,4=0 1,2 ,3,4=

{

0, 90, 0, 90

}

°

Introduction

(4)

A Coordinate-Invariant Method

Need for a

coordinate-invariant

statistical test

that keeps

physical information

and that can be used for

non-uniformly

dispersed

sources

(5)

The Polarisation Space

1 data point = 1 line of sight + 1 polarisation angle in the orthogonal plane

Physical information: electric field oscillation direction in

3D

(6)

The Polarisation Space

1 data point = 1 line of sight + 1 polarisation angle in the orthogonal plane

Physical information: electric field oscillation direction in

3D

(7)

The Polarisation Space

The polarisation space = unit 2-sphere

Polarisation “vectors„ regarded as points on the polarisation space

(8)

The Polarisation Space

Polarisation “vectors„: spherical data

Configuration density of polarisation points with spherical caps of equal area

(half aperture angle )

Polarisation space for the A3 region from [Hutsemékers et al. 2005]

(9)

The Polarisation Space

How to distinguish unexpected densities of polarisation points from

“natural

ones, i.e, drawn from a uniform distribution?

Polarisation space for the A3 region from [Hutsemékers et al. 2005]

(10)

The Polarisation Space

How to distinguish unexpected densities of polarisation points from

“natural

ones, i.e, drawn from a uniform distribution?

Cone Algorithm

Polarisation “vectors“: spherical data

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The Cone Algorithm

1)

Cones of fixed half aperture angle

2)

Analytical individual probability

p

ia

p

ia

=

arc−length

ia

(12)

The Cone Algorithm

3) Recursive algorithm gives

probability distribution

P

na

1)

Cones of fixed half aperture angle

(13)

Polarisation Map

Expected Background

(14)

Polarisation Map

Observations v.s. Expected Background

At least 3 deviation in number of polarisation points At least 2 deviation in number of polarisation points

(15)

Polarisation Map

Observations v.s. Expected Background

2

3

Polarisation space for the A3 region from [Hutsemékers et al. 2005]

p-value :

~ 0,14%

p-value :

(16)

At least 3 deviation in number of polarisation points

(17)

Polarisation space for the A1 and A3 regions from [Hutsemékers et al. 2005]

(355 quasars)

(29 quasars) (56 quasars)

(18)
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Conclusion

a coordinate-invariant method

confirmation of anisotropies on polarisation orientations

objective cuts on physical parameters (RA, dec, z, p_lin)

preferred axis definition

probe the geometry of the signal

DIRECT PROBE OF PHYSICS STANDING BEHIND THE

ANISOTROPIC ORIENTATIONS OF LINEAR

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References

Hutsemékers, D. 1998, A&A, 332,410

Hutsemékers, D., Lamy, H. 2001, A&A, 367, 381

Hutsemékers et al., 2005, A&A, 441, 915

Jain, P., Narain, G., Sarala, S. 2004, MNRAS, 347, 394

Cabanac et al., 2005, ASP Conf. Series

(22)

Radio Sources

CMB Polarisation (Planck)

...

Annex

(23)

Annex

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Annex

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Annex

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Annex

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Annex

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