Detecting Supernova Neutrinos at Neutrino Experiments Shaomin Chen
- Slides: 45
Detecting Supernova Neutrinos at Neutrino Experiments Shaomin Chen (陈少敏) Center for High Energy Physics (高能物理研究中心) Department of Engineering Physics( 程物理系) Tsinghua University (北京清华大学) 2013年兩岸粒子物理與宇宙學研討會 2020/10/7 1
Outline n Introduction n Supernova Neutrino Signal ØSN Burst neutrinos ØSN Relic Neutrinos n SN Neutrino Interactions at Targets n Typical Neutrino Detection Methods ØIn Water and In Liquid Scintillator ØBackground sources n Status & Outlook 2020/10/7 2
INTRODUCTION 2020/10/7 3
SN 1987 a Before February 23, 1987 After February 23, 1987 First observation came from optical instruments. 2020/10/7 4
SN 1987 a Neutrino Detections 2140 -ton pure water Time accuracy 1 s Threshold: 5 Me. V 6800 -ton pure water Time accuracy 50 ms Threshold 5 Me. V w/ ¼ PMT HV off 200 -ton LS Time accuracy +2/-54 s Later confirmed by the neutrino experiments. 2020/10/7 5
2002 Nobel Prize in Physics "for pioneering contributions to astrophysics, in particular for the detection of cosmic neutrinos" 2020/10/7 6
Puzzles in Measurements “One puzzling feature of the SN 1987 a data is that the neutrinos detected by the IMB detector were seemingly more energetic than those detected by the Kam-II detector, which were clustered at low energies. ” Phys. Rev. D 76 (2007) 083007 2020/10/7 7
Classification of SN Neutrinos John Beacom, TAUP 2011 DSNB=Diffuse Supernova Neutrino Background But we prefer to call them Supernova Relic Neutrinos 2020/10/7 8
SUPERNOVA NEUTRINO SIGNAL 2020/10/7 9
Model for Core-Collapse SN Stage 3, 4, 5 are expected to be distinguished by the SN neutrino time spectra. 2020/10/7 10
SN Neutrino Time Spectra 2020/10/7 11
Time Structures in N and <E> T. Totani, K. Sato, H. E. Dalhed and J. R. Wilson, Ap. J. 496, 216(1998) 1. Model based on SN 1987 a. 2. Special time structure. 2020/10/7 12
SN Neutrinos As Probes of MH The original flavor at emission arriving at a detector on Earth depends on the neutrino mass hierarchy. C. D. Ott, et al. , ar. Xiv: 1212. 4250 2020/10/7 13
Expected SN Rate per Century SN burst neutrinos expected from Type Ib, Ic and Type II SNe. 2020/10/7 14
Galactic SN Distance Mirizzi, et al. astro-ph/0604300 If a detector is sensitive up to 20 kpc, it covers 97% of our galaxy. Core collapse type Type Ia 0 7% probability < 3. 16 kpc 2020/10/7 10 kpc 16% probability < 5 kpc mean: 10. 7 kpc r. m. s. : 4. 9 kpc 20 kpc 3% probability > 20 kpc 15
Candidate SN Close to Us Eta Carinae: 2. 3 kpc to the Earth (SN 1987 a为 52± 5 kpc), with a mass equivalent to 100 -150 Suns. Near the same bright as normal SNs, predicted to be the next SN or Hyper SN. Betelgeuse: 0. 2 kpc to the earth, with a Mass equivalent to 18 -19 Suns. The brightest one in the sky if our eyes can see all the wavelength. 2020/10/7 SN 1987 a 16
Supernova Relic Neutrinos 2020/10/7 17
SRN @ SK 2020/10/7 18
SN NEUTRINO INTERACTIONS AT TARGETS 2020/10/7 19
SN Neutrino Interactions in Use 1. Inverse Beta Decay 2. Elastic Scattering On Electrons 3. CC and NC Interactions With Nuclei 4. Coherent Elastic Neutrino-Nucleus Scattering 2020/10/7 20
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TYPICAL NEUTRINO DETECTION METHOD 2020/10/7 22
Detection in Water ne n p e+ 2020/10/7 p Gd g g 23
Particle ID at SK If +/ – is fully contained in the inner tank Cone vertex and # of PMT and total charge collected used for measuring Evis 2020/10/7 If e+/e– is fully contained in the inner tank Ring pattern diff. used for PID 24
Detection in Liquid Scintillator e n e t e+ n 2020/10/7 Ø A prompt event correlated with a delayed event Ø Isotropic scintillation light Ø Typical a 8 Me. V gamma cascade and a 2. 2 Me. V gamma 25
Summary of SN Experiments 2020/10/7 26
Background in SN Burst Neutrinos Signal 2020/10/7 Background 27
Spallation Background 2020/10/7 28
Background Sources in SRN 2020/10/7 29
STATUS AND OUTLOOK 2020/10/7 30
Expected SN Neutrino Events Kamioande 参宿四 (0. 2 kpc) Daya Bay 海山二 (2. 3 kpc) 1987 a (51. 4 kpc) 31 2020/10/7
Super. Nova Early Warning System Individual SN-sensitive experiments send burst datagram to SNEWS coincidence computer at BNL to alert astronomers if coincidence in 10 s Participating experiments: Super. Kamiokande (Japan) 2020/10/7 Large Volume Detector (Italy) AMANDA/ Ice. Cube (South Pole) SNO (Canada) until end of 2006 32
Approaches @ SK ne Forced Trigger n p p g n+p→d + g 2. 2 Me. V g-ray DT = ~ 200 sec # of hit PMT’s ~ 6 e+ Gd (S. Chen and Z. Deng) g Nucl. Phys. Proc. Suppl. 166: 252, 2006 GADZOOKS! n+Gd →~8 Me. V g’s DT = ~30 sec Add 0. 2% Gd. Cl 3 in (J. Beacom and M. Vagins) water Phys. Rev. Lett. 93: 171101, 2004 2020/10/7 ne can be identified by delayed coincidence. 33
Water with 0. 2% Gd. Cl 3 Solution 5 cm Am/Be α + 9 Be → 12 C* + n 12 C* → 12 C + (4. 4 Me. V) n + p → …… → n + Gd → Gd + (totally 8 Me. V) 2020/10/7 34
The 8 Me. V Gamma Cascade @SK Efficiency ~ 67% Background probability ~ 2 x 10 -4 Distance to positron [cm] 2020/10/7 35
The 2. 2 Me. V Gamma @ SK 2020/10/7 36
Efficiency & BKG Prob. Efficiency ~ 18% Background probability ~ 1 x 10 -2 2020/10/7 37
2. 2 Me. V Gamma in Neutrino Data 2020/10/7 38
A First Look Into SK-IV Data SK-I Kam. Land SK-IV SK-I+II+III 2020/10/7 39
Prospect of SRN at SK Assuming invisible muon B. G. can be reduced by a factor of 5 by neutron tagging. Assuming ~70% efficiency. By 10 yrs SK data, Signal: 33, B. G. 27 (Evis =10 -30 Me. V) 2020/10/7 40
SN Burst Neutrinos @Daya. Bay 4 x(20+20)+2 x(20+20)+ 2 x(20+20)=320 tons Three-hall configuration can significantly reduce false SN alarming by the spallation background 2020/10/7 41
SN Neutrinos at Daya. Bay-II DYB 2020/10/7 DYB II 20 k ton LS 42
Status Power 阳江 Under construction 17. 4 GW 台山 Under construction 18. 4 GW 43 2020/10/7
Outlook u Many Physics in SN Neutrinos ü Dynamics of Core-Collapse SN, Mass Hierarchy ü Star Formation History, … u Rare SN burst neutrinos but copious SRNs u Need large volume of target mass with advanced detection technologies u A more realistic outlook ü SK with Gd+H and Daya Bay II 2020/10/7 44
THANKS! 2020/10/7 45
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