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Direct search of a dark matter with NaI: current status and possible perspective Dzhonrid Abdurashitov Institute for nuclear research, Moscow 25.07.2013 International conference DARK MATTER, DARK ENERGY and THEIR DETECTION Novosibirsk State University Novosibirsk, Russia July 22-26, 2013
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Topics Modulation is a main result of the DAMA experiment Other NaI(Tl) experiments (ANAIS, NAIAD, ELEGANT, DM-Ice) Pure NaI at LN2: - possibility to reduce the threshold Some technical aspects
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Bernabei et al, Eur. Phys. J. C 56 (2008) 2-6 keV, А=[0.0114 ± 0.0013] cpd/keV/kg2-6 кэВ, Rate ~1 cpd/keV/kg DAMA/NaI/LIBRA 25 detectors NaI(Tl) each 10 kg
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NaI ELEGANT V Fushimi et al, Astrop. Phys. 12 (1999) DAMA/LIBRA: 2-6 кэВ, А=[0.0114 ± 0.0013] cpd/keV/kg 30 detectors NaI(Tl) Each of 20 kg (Total 600 kg) Time of data acqisition ~1 year
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Sarsa et al, Phys. Rev. D56 4 (1997) 10-20 keV, no modulationDAMA, 2-6 keV, Rate ~1 cpd/keV/kg ANAIS 3 detectors NaI(Tl) ea 10 kg Time of acq < 2 years Window 10-30 keV
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NAIAD В.Ahmed et al, Astrop. Phys. 19 (2003) G.Alner et al, arXiv:hep-ex/0504031v1 7 detectors NaI(Tl), total 55 kg Time of acq < 2 years Window 4-10 keV
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Radiopurity Kim et al, New J. of Phys. 12 (2010) SD WIMP-proton SI WIMP-proton
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DAMA: 238 U - 0.5-10 ppt (in equlibrium) 232 Th - 0.5-7.5 ppt (in equlibrium) 40 K - < 2 ppt GEANT best fit: 238 U - 40 ppt (in equlibrium) 232 Th - 20 ppt (in equlibrium) 40 K - 20 ppt BUT: equilibrium is broken GEANT simulation of DAMA bkg V.A. Kudryavtsev et al., "The expected background spectrum in NaI dark matter detectors", Astroparticle Physics 33 (2010) 91–96
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DAMA experimental spectrum
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DAMA modulation spectrum
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To decrease a threshold … pure NaI at LN2 temperature scintillates 2 times more intensively… … dark rate of PMT at LN2 may be drastically decreased … one needs to increase light yield But both are questionnable
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Pure NaI at LN2 temperature D.E.Persyk et al., "Research on pure sodium iodide as a practical scintillator“, IEEE Trans.Nucl.Sci, NS-27:168-171 (1980) LY at LN2 increased twice to that of RT: from 40 to 80 photon/keV M.Moszynski et al., "Study of Pure NaI at Room and Liquid Nitrogen Temperatures", IEEE Trans.Nucl.Sci, v.50, n.4, (2003) Emission at 310 nm Timing ~10 µs LY is ~80 phot/keV But not all samples
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Pure NaI at LN2 temperature M.Moszynski et al., "A Comparative Study of Undoped NaI Scintillators With Different Purity",IEEE Trans.Nucl.Sci, v.56, n.3, Jun 2009 DAMA threshold, Phase 1: apparatus 6.7 ph.e. = 1 keV software 2 keV Phase 2: software 2 keV ============== At the same conditions: Qeff - 30% Light collection - 60% 6.7 ph.e. = 0.5 keV
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PMT single electron noise at low T H.O. Meyer. "Spontaneous electron emission from a cold surface." Europhysics Letters, 89 (2010) 58001 DAMA individual PMT noise: ~0.1 kHz at T=270 K one may expect ~0.02 kHz Physics is unknown yet But at low T the electrons are emitted in bursts
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Some technical aspects Stability at LN2 temp +-0.5 K – no problem see XENON10, LUX etc More complicated than DAMA but … Much easier in comparison to He temp Many aspects are similar to DAMA: background sources, light collection, DAQ system etc.
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Conclusion Pure NaI at LN2 is promising LY =80 phot/keV Cooled PMT may reveal high rate of bursts R@D is required The threshold of 0.5 keV in NaI is possible
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KIMS - CsI Lee et al, Phys. Rev. Lett. 99 091301 (2007) 4 кристалла CsI(Tl), 35 кг всего ~3 мес набора Окно 3-10 кэВ Reconstructed NR events 137 Cs – на уровне 10-100 мБк/кг
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CaF 2 (Eu) Y. Shimizu et al, Phys.Lett.B633 (2006) 1 кристалл CaF 2 (Eu), 310 г Время набора < 3 мес Окно 2-10 кэВ Eu – основной источник U/Th
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Орбитальная скорость Солнца V ~230 км/с Орбитальная скорость Земли V ~30 км/с Угол наклона δ~31° Скорость движения Земли вокруг гало ω =2 π /365 [1/сут], t 0 = 2 июня V max =245 км/с, V min =215 км/с ЯДРА ОТДАЧИ: СПЕКТР, ГОДОВАЯ МОДУЛЯЦИЯ DAMA/LIBRA, 2-6 кэВ, А~[0.01 ± 0.01] отсч/кг/сут 23 Na 127 I Sarsa Ph.Rev. D56 4 (1997) G.Jungman et al, Ph.Rep. 267 (1996) Форма спектра ядер отдачи 73 Ge σ 0 =4x10 -36 см 2
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