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宇宙のトポロジーを決定するための天体分 布を用いた新手法

宇宙のトポロジーを決定するための天体分 布を用いた新手法

宇宙のトポロジーを決定するための天体分 布を用いた新手法

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()<br />

<br />

Λ-CDM (e.g., Ω tot =<br />

1.0050 +0.0060<br />

−0.0061<br />

, Hinshaw et al. 2009)<br />

() ()<br />

2 Λ-CDM <br />

3 <br />

<br />

18 (Nowacki 1934, 1 )<br />

<br />

1 <br />

<br />

<br />

(CMB) <br />

(LSS) (≃ 14Gpc) <br />

LSS 1 <br />

WMAP <br />

(Cornish et al. 2004; Key et al. 2007; Roukema et al.<br />

2008; Aurich 2008; Bielewicz & Banday 2011)<br />

<br />

1 17 <br />

3 (3-torus, chimney space, slab space) <br />

(Mota et al. 2010) 14 “”<br />

<br />

<br />

<br />

(Fujii & Yoshii 2011a,<br />

Fujii 2011) CMB 3 <br />

180 ◦ <br />

:<br />

γ: (X, Y, Z) ↦−→ (−X, −Y, Z + L) (1)<br />

1


1: 17 3 (<br />

)<br />

Jeffrey Weeks <br />

<br />

1 <br />

L 2 <br />

(Fujii & Yoshii 2011a)2<br />

⃗X 1 , ⃗X 2 γ “” ⃗X<br />

1 ′, ⃗X<br />

2 ′ <br />

X 2 ′ − X′ 1 = −(X 2 − X 1 ), (2)<br />

Y 2 ′ − Y′ 1 = −(Y 2 − Y 1 ), (3)<br />

Z 2 ′ − Z′ 1 = Z 2 − Z 1 . (4)<br />

<br />

(X, Y, Z) <br />

( 180 ◦ ) <br />

(x, y, z) γ <br />

<br />

⎛<br />

⎞ ⎛<br />

1 0 0 0<br />

0 -1 0 0<br />

γ = U<br />

U −1 +<br />

0 0 -1 0<br />

⎜⎝<br />

⎟⎠ ⎜⎝<br />

0 0 0 1<br />

⎞<br />

1 0 0 0<br />

L 1 0 0 0<br />

,<br />

L 2 0 0 0<br />

⎟⎠<br />

L 3 0 0 0<br />

2


U <br />

(2),(3),(4) (x, y, z) <br />

CMB <br />

<br />

(Fujii 2011) 2 ⃗x 1 , ⃗x 2 ⃗x ′ 1 , ⃗x′ 2 <br />

3 : <br />

(⃗x 2 − ⃗x 1 ) + (⃗x<br />

2 ′ − ⃗x′ 1<br />

) ( 2)<br />

2: 4 ⃗n pec ∝ ⃗a + ⃗b <br />

2 ⃗n pec <br />

4 ⃗n pec ∝ ⃗a +⃗b <br />

<br />

<br />

3 <br />

“” (X, Y, Z) 30 ◦ z <br />

<br />

<br />

1<br />

1<br />

0.5<br />

0.5<br />

0<br />

0<br />

-0.5<br />

-0.5<br />

-1 -0.5 0 0.5 1 -1<br />

-1 -0.5 0 0.5 1 -1<br />

3: <br />

<br />

3 2dF SDSS<br />

<br />

<br />

3


4

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