Detecting dark matter through line emission a suggestion

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Detecting dark matter through line emission a suggestion for the Chinese space station Guoming

Detecting dark matter through line emission a suggestion for the Chinese space station Guoming Chen IHEP, CAS Sep. 23, 2008 2021/12/31 Guoming CHEN 1

What to detect in space? • Charged particles: AMS • Gamma ray: GLAST 2021/12/31

What to detect in space? • Charged particles: AMS • Gamma ray: GLAST 2021/12/31 Guoming CHEN 2

γray from neutralino annihilation smoke gun evidence Mχ=1. 5 Te. V Line emission: •

γray from neutralino annihilation smoke gun evidence Mχ=1. 5 Te. V Line emission: • large acceptance • excellent energy resolution 2021/12/31 Guoming CHEN 3

Where to detect? advantage disadvantage Galactic Center large statistics Sub-halo Satellite background free large

Where to detect? advantage disadvantage Galactic Center large statistics Sub-halo Satellite background free large No. of subs low background Background foreground low statistics per subhalo Extra galactic good statistics 2021/12/31 Guoming CHEN low statistics background Jan Conrad 4

Strategy • To detect dark matter through line emission • To scan the full

Strategy • To detect dark matter through line emission • To scan the full sky, mostly depending on sub-halos • Different from normal gamma ray detector, this one emphasizes on acceptance, energy resolution and particle ID. 2021/12/31 Guoming CHEN 5

Detector concept design (High Energy Gamma Ray detector, HEGARD) Tungsten 1000*3. 5 mm 3

Detector concept design (High Energy Gamma Ray detector, HEGARD) Tungsten 1000*3. 5 mm 3 Scintillator fiber 5*5*1000 mm 3 50 mm thick plastic rubber 20 radiation lengths Lithium Glass 20*20*5 mm 3 2021/12/31 Plastic Scintillator 10*10*1200 mm 3 Guoming CHEN 6

One layer of the ECAL One layer = one radiation length, 20 layers in

One layer of the ECAL One layer = one radiation length, 20 layers in total 2021/12/31 Guoming CHEN 7

Weight and Acceptance ECAL size m 2 naked detector support kg kg area m

Weight and Acceptance ECAL size m 2 naked detector support kg kg area m 2 geo. factor m 2 sr 0. 71 x 0. 71 854 85 0. 5 1. 00 x 1. 00 1707 154 1 3 1. 40 x 1. 40 3414 2 6 1. 73 x 1. 73 5121 276 393 3 9 take 1 m 2 scenario as an example 2021/12/31 Guoming CHEN 8

MC simulation Hits level 2021/12/31 Guoming CHEN 9

MC simulation Hits level 2021/12/31 Guoming CHEN 9

Energy measurement From 30 Ge. V to 4 Te. V , energy resolution better

Energy measurement From 30 Ge. V to 4 Te. V , energy resolution better than 2% (leakage corrected) scale energy resolution deviation from linearity 2021/12/31 Guoming CHEN 10

Shower shape difference on γ/p 2021/12/31 Guoming CHEN 11

Shower shape difference on γ/p 2021/12/31 Guoming CHEN 11

2021/12/31 Guoming CHEN 12

2021/12/31 Guoming CHEN 12

Boost decision tree output 2021/12/31 Guoming CHEN 13

Boost decision tree output 2021/12/31 Guoming CHEN 13

γeff. vs. p eff. 2021/12/31 Guoming CHEN 14

γeff. vs. p eff. 2021/12/31 Guoming CHEN 14

γ/e separation • Veto efficiency 0. 9999, i. e. , only 10 -4 electron

γ/e separation • Veto efficiency 0. 9999, i. e. , only 10 -4 electron can contaminate gamma • The problem is gamma efficiency 2021/12/31 Guoming CHEN 15

Backlash 2021/12/31 Guoming CHEN 16

Backlash 2021/12/31 Guoming CHEN 16

backlash property • Back scattering particles include both electrons and gammas, gammas dominate •

backlash property • Back scattering particles include both electrons and gammas, gammas dominate • Energy mostly less than 2 Me. V 2021/12/31 energy of backlash gamma Guoming CHEN 17

Backlash identification Using plastic rubber to absorb electrons in the backlash For the gammas:

Backlash identification Using plastic rubber to absorb electrons in the backlash For the gammas: 1)ID with position 2)ID with energy y xx gamma efficiency: 92% at 200 Ge. V, Ex>1 Me. V, Ey>1 Me. V 光子效率:〉95% 2021/12/31 Guoming CHEN 18

HEGARD concept • • • size 112 x 40 cm 3 weight 2000 kg

HEGARD concept • • • size 112 x 40 cm 3 weight 2000 kg power consumption 500 W time resolution 1 ns area 1 m 2 geometry factor 3 m 2 sr gamma energy measurement 30 Ge. V— 4 Te. V energy resolution 2% angular resolution 0. 5 o proton rejection 10 -7 electron rejection 10 -4 2021/12/31 Guoming CHEN 19

ISS orbit simulation 2021/12/31 Guoming CHEN 20

ISS orbit simulation 2021/12/31 Guoming CHEN 20

effective time in one year survey 2021/12/31 Guoming CHEN 21

effective time in one year survey 2021/12/31 Guoming CHEN 21

backgrounds astroph/05107 14 v 2 1996 A&A. . 120 C. 465 M 2021/12/31 Guoming

backgrounds astroph/05107 14 v 2 1996 A&A. . 120 C. 465 M 2021/12/31 Guoming CHEN 22

Theoretical calculation bu X. J. Bi 416 Ge. V 2021/12/31 Guoming CHEN 23

Theoretical calculation bu X. J. Bi 416 Ge. V 2021/12/31 Guoming CHEN 23

One year sensitivity HEGARD 2021/12/31 Guoming CHEN 24

One year sensitivity HEGARD 2021/12/31 Guoming CHEN 24

Conclusion The proposed detector has large acceptance, excellent energy resolution and excellent particle ID.

Conclusion The proposed detector has large acceptance, excellent energy resolution and excellent particle ID. It is able to detect dark matte through line emission 2021/12/31 Guoming CHEN 25

Thank you You are welcome to give any criticism, comments, and improvements of the

Thank you You are welcome to give any criticism, comments, and improvements of the design. And you more than welcome to offer collaboration. 2021/12/31 Guoming CHEN 26

backup 2021/12/31 Guoming CHEN 27

backup 2021/12/31 Guoming CHEN 27

电磁量能器事例数 能量 (Ge. V) 50 100 200 500 1000 2000 4000 总和 电子 10

电磁量能器事例数 能量 (Ge. V) 50 100 200 500 1000 2000 4000 总和 电子 10 k 5 k 50 k 光子 10 k 5 k 5 k 5 k 45 k 质子 300 k 298 k 227 k 170 k 163 k 1. 498 M 2021/12/31 Guoming CHEN 28