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Status of XMASS experiment. Cygnus 2013@Toyama 2013/06/05 Nagoya univ . H.Uchida for XMASS collaboration. XMASS-II. XMASS-I. Overview. XMASS-1.5. 835 kg, 100 kg Fiducial volume (FV) φ80 cm, 642 PMTs. 5 ton, 1 ton FV φ1.5 m, ~1000 PMTs. 25 ton, 10 ton FV φ2.5 m
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Status of XMASS experiment Cygnus 2013@Toyama 2013/06/05 Nagoya univ. H.Uchida for XMASS collaboration
XMASS-II XMASS-I Overview XMASS-1.5 835 kg, 100 kgFiducial volume (FV) φ80 cm, 642 PMTs 5 ton,1 ton FV φ1.5 m, ~1000 PMTs 25 ton, 10 ton FV φ2.5 m ・ Dark matter ・ pp solar neutrino ・ 0n2b decay ・ Dark matter search Y. Suzuki, hep-ph/0008296 • A purpose of XMASS-I and 1.5 experiment is dark matter search. • Commissioning data was taken with XMASS-I at the Kamioka Observatory in Japan between Nov. 2010 and May. 2012. And now refurbishment work is on going. • XMASS-II has multi purpose of dark matter, pp solar neutrino and 0ν2β decay.
800kg detector • XMASS is a single phase detector with ultra pure liquid xenon. • Background is reduced by a self-shielding of liquid xenon. • This detector has high light yield (~14p.e./keV) & low energy threshold (~0.3keVee). • This detector is sensitivefor electromagnetic signals.
Detector configuration There is a this detector at Kamioka observatory. Elec. hut OFHC copper vessel Water tank Refrigerator 11m 835kg liq. xenon 642 PMTs ~ 1.2m 10m 700L reservoir 72 20inch PMTs (veto)
Source calibration • Calibration sources are used for checking detector response. • The sources can be moved along the vertical axis in the detector. Stepping motor Linear and rotary motion feed-through Gate valve (*1) Ka X-rays from the copper used for housing. (*2) Ka X-rays from the tungsten used for housing. ~5m 0.21mmf for 57Co source 4mmf Top photo tube Source rod with a dummy source • We can use one of five sources. • Right hand animation shows a procedure of calibration data taking. First, installation of a source to a calibration rod, opening the top PMT, and insertion of the rod. 5
Calibration data • Calibration dataでreal dataを 57Co calibration data (122keV) Real data MC 40 30 40 40 30 30 20 20 z [cm] 10 10 0 0 -10 -10 -20 -20 -30 -30 -40 -40 -10 10 0 -20 20 10 0 -20 20 -10 y [cm] y [cm]
Background • Background level of XMASS-I is a fewevent/day/keV/kg [dru] without fiducualization. • It is similar level with DAMA and CoGeNT. • The origin of BG for more than 5 keV were almost identified(lower figure). Also for less than 5 keV, Gore-Tex may explain the events. • Events originate at the inner surface must explain major part of the observed events.. PMT写真と アルミの位置の 説明 ● Black line: Real data ● Colored histogram: BG (MC) Surface Cu 210Pb PMT Al 235U-231Pa 210Pb 232Th 238U-230Th PMT gamma Gore-Tex 210Pb Gore-Tex 14C Full volume dru[/day/keVee/kg] 7 5 20 10 15
Light mass WIMP search • Full volume (835 kg) analysis • 6.70 days×835kg in 2012 Feb. • 0.3 keVee threshold 5 4 3 Counts/day/kg/keVee 2 1 0 0 0.5 2 1.5 1 Energy [keVee]
solar axionsearch • Axion is a hypothetical particle to solve the strong CP problem • Produced in the Sun and detected in the detector • XMASS is suitable to search because of a large mass and low BG Bremsstrahlung and Compton effect Axio-electric effect gaee gaee ma= Our data Max allowed 50 keV
WIMP-Xe129 inelastic scattering 他の非弾性散乱実験についての言及。 I127を使った(DAMA、PICORON)? 論文があるか見ておくこと。 Inelasticの図
Cross section of DM100GeV Event Event/keV Scaled energy(13.9PE/keV) Reconstructed R (cm) # of events of no cut in DM100GeV MC are 82625. If these events occur in 55.6days, (explanation of this function in backup slide) Calculation of cross section DM100GeV: 82625/835/0.264/55.6 = 6.74 event/kg(Xe129)/day NA of Xe129 = 3.758×10-37×6.74×100/0.3 = 8.4×10‐34cm2 (8.4×102pb) When cross section is 8.4×102pb, inelastic events by DM100GeV occur 82625 events in 55.6days.
Cross section of DM200GeV Event Event/keV Scaled energy(13.9PE/keV) Reconstructed R (cm) # of events of no cut in DM200GeV MC are 82640. If these events occur in 55.6days, (explanation of this function in backup slide) Calculation of cross section DM200GeV: 82640/835/0.264/55.6 = 6.74 event/kg(Xe129)/day NA of Xe129 = 3.758×10-37×6.74×200/0.5 = 1.0×10‐33cm2 (1.0×103pb) When cross section is 1.0×103pb, inelastic events by DM200GeV occur 82640 events in 55.6days.
Cross section of DM400GeV Event Event/keV Scaled energy(13.9PE/keV) Reconstructed R (cm) # of events of no cut in DM400GeV MC are 82175. If these events occur in 55.6days, (explanation of this function in backup slide) Calculation of cross section DM200GeV: 82175/835/0.264/55.6 = 6.70 event/kg(Xe129)/day NA of Xe129 = 3.758×10-37×6.70×400/0.53 = 1.9×10‐33cm2 (1.9×103pb) When cross section is 1.9×103pb, inelastic events by DM400GeV occur 82175 events in 55.6days.
Reduction of best parameter set Live time: 55 days # of events Energy(keV) Signal region # of events Reconstructed R
Origin of BG in XMASS-I Main BG source (≧5keV) Al seal BG candidate (< 5keV) • In refurbishment, Al seal will be covered • by copper rings and GORE-TEX will be • removed • In XMASS-1.5, Al seal will be replaced • with ultra pure one 24