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1 229-ThTES
2 α = e 2 /2ε 0 hc (John D. Barrow 2005) Radiationdominated era Matterdominated era Dark energy era Time (years) Time 2
3 α = e 2 /2ε 0 hc (John D. Barrow 2005) Radiationdominated era Matterdominated era Dark energy era Time (years) Time 3
4 α = e 2 /2ε 0 hc (John D. Barrow 2005) Radiationdominated era Matterdominated era Dark energy era Time (years) Time 4
5 α = e 2 /2ε 0 hc α α = (6.40 ± 1.35) yr 1 (M.Murphy+, 2003) α =( 0.3 ± 2.0) yr 1 (E.Peik+ 2004) ω ω = V c α V c [ ω ] α [ ω ] 10 5 (Xiao+ 2008) 5
6 229Th 9.5 ev< E( 229m Th) <18.3 ev 233U (τ 1/2 =16) α-decay 0.3 % 229Th TES-thorium project(2015~) kev ~10 % 0 kev ~10 ev ~ 90 % E( 229m Th) 6
7 TES ΔT~E/C~1 mk log R ~ mk r C ~ 100 mω log T E T T E 2 ev 100 mk C 1pJ/K 1/2 1/
8 29 kevtes Soft X-ray band Hard X-ray band E (kev) ΔE=2.8 ev@5.9 kev (ISAS+ 2009) ΔE=27 ev@103 kev E sat CT log R ΔR ΔT log T 8
9 TES 4TES Au 3.6 μm 6 mm 300 μm Al TES(Ti/Au) Esat (kev) ΔE (ev) 10 21@26 kev 2 (pj/k) Tc =164 mk 0 (mk) Temperature (mk) Resistance (mω) CH2 CH3 9
10 229Th異性体準位の測定試験 233U線源を使用可能な環境であるJAEAで試験を実施した 動作は1素子 低温ステージを温度90mKまで希釈冷凍機を使用し冷却 233U,133Ba,241Am線源を用いて試験 26 kevに対する分解能は41 ev U線源の強度 26 MBq 測定日数 18日間 希釈冷凍機 低温ステージ TES素子 10
11 233U Th Lα Th Lβ Th Lγ Ag Kβ 26 kev Cs Kα1,2 normalized counts s 1 kev 1 Cs Kβ Au Lα escape 59 kev Energy(keV) kev 811 counts kev 24 counts (data model)/error Energy (kev) 11
12 233U Th Lα Th Lβ Th Lγ Ag Kβ 26 kev Cs Kα1,2 Cs Kβ Au Lα escape 59 kev Energy(keV) AgK β1 E kev AgK β2 Cs Kβ1 Cs Kβ2 CsK β1 CsK β2 E (35,36) E kev doublet E35 E kev 43.4 kev Au Lβ escape Au L β1,2,3,4 escape Au L α1,2 escape Au Lα escape E kev 59 kev 59 kev Energy (kev) PI (kev)
13 229Th (kev) 97.1 E13 E E24 (kev) (keV) E 13 = E 0 (35, 36) = E 0 (35, 36) = E 35 E 12 = E 24 = E 0 (45, 46) = b 42 E( 229m Th) E 0 (45, 46) = E 46 + b 29 E( 229m Th) E( 229m Th) = (E 13 + E 0 (35, 36)) (E 12 + E 24 + E 0 (45, 46)) 1 b 29 b 42 E b 29 =1/13, b 42 =1/50 (Beck+2007,2009) E35 E45 0 E46 E( 229m Th) E( 229m Th) = ± 9.5 (ev) : = 1-b 42 : b 42 : = b 29 1-b 29 13
14 JAEA 14
15 TES TES ΔE=18 ± 4 ev CH2 CH1 CH3 CH4 normalized counts s 1 kev (data model)/error Energy (kev) 15
16 29.19 kev E( 229m Th)=9.5 ev E( 229m Th)=18.3 ev normalized counts s 1 kev normalized counts s 1 kev (data model)/error 5 0 (data model)/error Energy (kev) Energy (kev) 16
17 29.19 kev 1 error (ev) ev 0.5 ev E 1 E 1 E 2 =9.5 ev E 2 = 18.3 ev 45 k 2 k Total Counts 30 k 17
18 E( 229m Th) = ± (ev) ΔE=18 ev 18
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