an event generator for supernova neutrinos in argon
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An event generator for supernova neutrinos in argon Steven Gardiner Emilija Pantjc Robert Svoboda University of California, Davis Christopher Grant Boston University Weak Interactjons and Neutrinos 21 June 2017 1 Outline Motjvatjon


  1. An event generator for supernova neutrinos in argon Steven Gardiner Emilija Pantjc Robert Svoboda University of California, Davis Christopher Grant Boston University Weak Interactjons and Neutrinos 21 June 2017 1

  2. Outline ● Motjvatjon for argon-based supernova neutrino detectors ● Event reconstructjon challenges (why is this hard?) ● MARLEY : M odel of A rgon R eactjon L ow E nergy Y ields – Ingredients in our model – Example simulatjon results ● Current studies and future prospects 2

  3. Water- and argon-based neutrino detectors have complementary sensitjvitjes to SN neutrinos 3

  4. Supernova neutrino detectjon with water Cherenkov detectors ● Inverse beta decay is the dominant reactjon ● Number of detected photons gives a positron energy measurement ● From there, reconstructjng the antjneutrino energy is straightgorward inverse beta decay 4

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  6. The need for a supernova neutrino simulatjon tool ● Simulatjons are needed to understand LArTPC response to SN neutrinos ● A number of neutrino event generators exist, but the emphasis is on high-energy physics ● In the low tens-of-MeV regime, nuclear structure details become quite important! ● We have developed a new generator to help us understand the response of 40 Ar to SN neutrinos – Nuclear data measurements (levels, gammas, matrix elements) can help us 6

  7. ● Event generator for supernova neutrinos on 40 Ar ● Current version does CC (dominant channel) ● Framework allows adding new reactjons, target nuclei, etc. M odel of A rgon R eactjon L ow E nergy Y ields ● In use by DUNE for SN Bob Marley illustration by Zero Anixter simulatjons ● Also has users from several other liquid argon experiments 7

  8. MARLEY event generatjon fmowchart Transmission coeffjcient model 8

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  11. World’s B(GT) data for 40 Ar ● Measurements using (p,n) scatuering vs. 40 Ti beta decay show signifjcant disagreements ● Hard to calculate and hard to measure! ● Karakoç, et al. Phys. Rev. C 89, 064313 (2014) refers to a third measurement that remains unpublished ● Must be supplemented by theory at higher energies 11

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  13. MARLEY’s cross sectjon agrees with similar calculatjons over much of the relevant energy range - * 4 0 4 0 T o t a l c r o s s s e c t i o n f o r + A r K + e ) ν → e 2 3 8 m − 1 0 c ( n o i t c e 3 9 − 1 0 s s s o r c 4 0 − 1 0 4 1 1 0 − 4 2 − 1 0 M A R L E Y 4 3 − 1 0 4 4 1 0 − 0 2 0 4 0 6 0 8 0 1 0 0 n e u t r i n o e n e r g y ( M e V ) ● Low energies = forbidden transitjons make a small contributjon below MARLEY’s hard cutof ● High energies = forbidden transitjons start to dominate near 100 MeV 13

  14. MARLEY transmission coeffjcient model ● Unbound states in MARLEY de-excite according to the Hauser-Feshbach model – W. Hauser and H. Feshbach, Physical Review 87 , 366 (1952) – Successfully used for many years to describe nuclear cross sectjons – Work contjnues to refjne the input parameters (e.g., RIPL-3) – Used in many SN neutrino theory papers (in combinatjon with RPA, QRPA, etc.) – Two key assumptjons: 1. compound nucleus 2. reciprocity theorem (tjme-reversal invariance) ● Final states are sampled using decay widths 14

  15. MARLEY transmission coeffjcient model ● Nuclear potentjal from Koning & Delaroche global optjcal model A. J. Koning and J. P. Delaroche, Nuclear Physics A 713 3-4 (2003) Solve radial Schrödinger equatjon numerically in matching region ● Match to asymptotjc solutjon, extract transmission coeffjcient ● Transmission coeffjcient represents the probability of 15 penetratjng the nuclear surface

  16. L i v e r m o r e s u p e r n o v a s p e c t r u m 3 0 0 0 0 2 5 0 0 0 2 0 0 0 0 1 5 0 0 0 1 0 0 0 0 5 0 0 0 0 0 1 0 2 0 3 0 4 0 5 0 6 0 83.7% 14.6% 1.5% 16

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  23. Current studies and future prospects ● MARLEY development is ongoing – Interfaces to other codes (e.g., LArSofu) – Physics improvements – Preparatjon of data for other reactjon channels ● A variety of reconstructjon topics are beginning to be addressed using MARLEY events M odel of A rgon R eactjon L ow E nergy Y ields De-excitatjon vs. bremsstrahlung γ – Nucleon emission tagging – – Event t0 determinatjon SN triggering – – MC-based smearing matrix for SNOwGLoBES ● ACED : A rgon C apture E xperiment at D ANCE Measurement of 40 Ar thermal neutron capture cross – sectjon and event-by-event gammas Addresses key uncertaintjes in liquid argon response to – low energy neutrons The D etector for A dvanced N eutron C apture E xperiments at Los Alamos – First data this fall 23

  24. Conclusion ● Nuclear efects greatly complicate supernova neutrino event reconstructjon in argon ● MARLEY is a new generator specifjcally targetjng supernova neutrinos in 40 Ar ● Studies are underway to learn how to reconstruct these events in DUNE ● A direct measurement of these cross sectjons M odel of A rgon R eactjon L ow E nergy Y ields would be very valuable! – See C. McGrew’s CAPTAIN talk for one proposed experiment ● Want to become a MARLEY user or developer? Email me at support@marleygen.org for more 24 informatjon

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