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1 Other polarimeters

• Wave plates can be used to build

polarimeters sensitive to linear or to circular polarization.

• Half-wave plate (φ=180

o

)

• Quarter-wave plate (φ=90

o

)

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

0 1 0 0

1 0 0 0

0 0 1 0

0 0 0 1 QWP

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 1 0 0

0 0 1 0

0 0 0 1 HWP

Polarimeter with HWP

⎟⎟

⎟⎟

⎜⎜

⎜⎜

=

0 0 0 0

0 0 0 0

0 0 1 1

0 0 1 1

PH

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 1 0 0

0 0 1 0

0 0 0 1 HWP

θ

source Polarizer

Intensity detector HWP

( ) ( )

{ P R HWP R } S D

W = ×

H

× − θ × × θ ×

( )

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 0

0 0

0 0 0 1

2 2

2 2

c s

s Rθ c

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= V U Q I

S D=

(

1 0 0 0

) ( )

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 0

0 0

0 0 0 1

2 2

2 2

c s

s R θ c

Polarimeter with HWP

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟

⎟⎟

⎜⎜

⎜⎜

1 0 0 0

0 0 0

0 0 0

0 0 0 1

1 0 0 0

0 0

0 0

0 0 0 1

1 0 0 0

0 1 0 0

0 0 1 0

0 0 0 1

2 2 2 2

2 2

c c c s

s c θ

source Polarizer

Intensity detector HWP

( ) ( )

{ P R HWP R } S

D

W = ×

H

× − θ × × θ ×

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟ −

⎟⎟

⎜⎜

⎜⎜

1 0 0 0

0 0 0

0 0 0

0 0 0 1

1 0 0 0

0 0 0

0 0 0

0 0 0 1

1 0 0 0

0 0

0 0

0 0 0 1

2 2 2 2 2 2 2 2

2 2

c c c c c s

s c

Polarimeter with HWP

θ

source Polarizer

Intensity detector HWP

( ) ( )

{ P R HWP R } S

D

W = ×

H

× − θ × × θ ×

⎟⎟

⎟⎟

⎜⎜

⎜⎜

=

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟ −

⎟⎟

⎜⎜

⎜⎜

0 0 0 0

0 0 0 0

0 0 1

0 0 1

1 0 0 0

0 0 0

0 0 0

0 0 0 1

0 0 0 0

0 0 0 0

0 0 1 1

0 0 1 1

2 2 2 2

2 2 2

2 c

c

c c

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎛ + +

=

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟

⎟⎟

⎜⎜

⎜⎜

0 0 0 0 0 0

0 0 0 0

0 0 1

0 0 1

2 2 2 2 2

2 2 2

Q c I

Q c I

V U Q I c c

( )

2

(

22

)

1 2 2 2 2

2 1

0 0 0 0 0

1 I cQ I Qc

Q c I

W = +

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎛ + +

=

( )

f

o

f

Q I W

4

2 cos

2

2 1

= +

= θ

Polarimeter with QWP

⎟⎟

⎟⎟

⎜⎜

⎜⎜

=

0 0 0 0

0 0 0 0

0 0 1 1

0 0 1 1

PH

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= − 0 1 0 0

1 0 0 0

0 0 1 0

0 0 0 1 QWP

θ

source Polarizer

Intensity detector QWP

( ) ( )

{ P R QWP R } S D

W = ×

H

× − θ × × θ ×

( )

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 0

0 0

0 0 0 1

2 2

2 2

c s

s Rθ c

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= V U Q I

S D=

(

1 0 0 0

) ( )

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

1 0 0 0

0 0

0 0

0 0 0 1

2 2

2 2

c s

s R θ c

Polarimeter with QWP

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟

⎟⎟

⎜⎜

⎜⎜

0 0

1 0 0 0

0 0

0 0 0 1

1 0 0 0

0 0

0 0

0 0 0 1

0 1 0 0

1 0 0 0

0 0 1 0

0 0 0 1

2 2

2 2 2

2 2 2

c s

s c c s

s c θ

source Polarizer

Intensity detector QWP

( ) ( )

{ P R HWP R } S D

W = ×

H

× − θ × × θ ×

⎟⎟

⎟⎟

⎜⎜

⎜⎜

= −

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟ −

⎟⎟

⎜⎜

⎜⎜

0 0 0 0 0 0

0 0 0 1

0 0

1 0 0 0

0 0

0 0 0 1

1 0 0 0

0 0

0 0

0 0 0 1

2 2 2 2 2

2 2 2 2 2

2 2

2 2 2 2

2 2

c s s c

s s c c

c s

s c c s

s c

(2)

2 Polarimeter with QWP

θ

source Polarizer

Intensity detector QWP

( ) ( )

{ P R HWP R } S

D

W = ×

H

× − θ × × θ ×

⎟⎟

⎟⎟

⎜⎜

⎜⎜

=

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟

⎟⎟

⎜⎜

⎜⎜

0 0 0 0

0 0 0 0 1 1

0 0 0 0 0 0

0 0 0 1

0 0 0 0

0 0 0 0

0 0 1 1

0 0 1 1

2 2 2 2 2

2 2 2 2 2

2 2 2 2 2

2 2 2 2

2 c cs s

s s c c

c s s c

s s c c

⎟⎟

⎟⎟

⎜⎜

⎜⎜

− + +

− + +

=

⎟⎟

⎟⎟

⎜⎜

⎜⎜

⎟⎟

⎟⎟

⎜⎜

⎜⎜

0 0 0

0 0 0

0 0 0 0 1 1

2 2 2 2 2

2 2 2 2 2 2

2 2 2 2

2 2 2 2 2

V s U s c Q c I

V s U s c Q c I

V U Q I s s c c

s s c c

( cos

2

2 θ cos 2 θ sin 2 θ sin 2 θ )

2

1 I Q U V

W

= + + +

fo

4 4

fo

2

fo

Modulation techniques for polarization experiments

All these techniques suffer for the need of long integration time:

One needs to point to the same sky pixel during many cycles of the analyzer. It is thus difficult to produce extended maps of the CMB polarization.

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