SNS Spallation Neutrino Source 1 SNS layout Stripping

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SNS Spallation Neutrino Source 1

SNS Spallation Neutrino Source 1

SNS layout Stripping foil 1. 0 Ge. V proton linear accelerator Main target Accumulator

SNS layout Stripping foil 1. 0 Ge. V proton linear accelerator Main target Accumulator ring 2

SNS Parameters Proton beam energy – 1. 0 - 1. 4 Ge. V Intensity

SNS Parameters Proton beam energy – 1. 0 - 1. 4 Ge. V Intensity - 9. 6 1015 protons/sec Pulse duration - 380 ns(FWHM) Repetition rate - 60 Hz Total power – 1. 0 3 MW Liquid Mercury target 3

Target building Proton Beam m 0 6 ~ 4

Target building Proton Beam m 0 6 ~ 4

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Mercury target 21 cm Mercury Inventory – 20 t Flow rate 340 kg/sec Vmax

Mercury target 21 cm Mercury Inventory – 20 t Flow rate 340 kg/sec Vmax 3. 5 m/sec Tin 600 C Tout 900 C Mercury lasts the entire 40 year lifetime of SNS no change is required 6 Stainless steel vessel should be replaced periodically

Some Details of Interaction in the Target Average interaction energy is ~1. 1 Ge.

Some Details of Interaction in the Target Average interaction energy is ~1. 1 Ge. V Average interaction depth ~11 cm Proton interacts near the front part of the target 7

DIF vs. DAR Pion Spectra 200 Me. V/c pions range in mercury is ~

DIF vs. DAR Pion Spectra 200 Me. V/c pions range in mercury is ~ 5 cm Very few pions have a chance to decay before coming to the rest Because of the bulk Mercury target, SNS is a Decay At Rest facility !! 8

Neutrino Production + Hg 0. 13 + e e+ 0. 09 p 1. 3

Neutrino Production + Hg 0. 13 + e e+ 0. 09 p 1. 3 Ge. V - 99. 6% At the first approximation: N +/proton = 0. 14*E(Ge. V)-0. 05 For E~0. 8 -1. 5 Ge. V ISIS, LANSCE SNS 9

Actual spectra of neutrinos from SNS Neutrino spectra well defined in SM Energy e

Actual spectra of neutrinos from SNS Neutrino spectra well defined in SM Energy e and are in the different time intervals Time 10

Neutrino Rates Number of protons on the target for 1. 1 m. A at

Neutrino Rates Number of protons on the target for 1. 1 m. A at 1. 3 Ge. V is 0. 687· 1016 sec-1 Number of each flavor neutrino produced by one proton is 0. 13 SNS live time is 2/3 of the year Number of each flavor of neutrinos produced at SNS is 1. 9· 1022 year-1 Caveat: There is larger flux of antineutrinos from decay of radioactivity in the target However, heir energy is a few Me. V and almost continues in time. We did a few attempted to calculate those, but all grad students failed to deliver robust result. It would be nice to finish this. . 11

Cross Sections Integrated over SNS spectra. Reaction Integrated Cross Section ee - ee e

Cross Sections Integrated over SNS spectra. Reaction Integrated Cross Section ee - ee e - e e 12 C 12 Ngs e e 12 C* 12 C* e 56 Fe 56 Co e- 0. 297 10 -43 cm 2 0. 050 10 -43 cm 2 0. 92 10 -41 cm 2 0. 45 10 -41 cm 2 0. 27 10 -41 cm 2 ~2. 5 10 -40 cm 2 SNS delivers ~ 1. 9· 1022 neutrinos per year 12

Necessary detector mass KARMEN LSND

Necessary detector mass KARMEN LSND

SNS Beam Info Mode: Target Power on Target: 1003. 24 k. W Charge to

SNS Beam Info Mode: Target Power on Target: 1003. 24 k. W Charge to Target: 18. 5 E-6 C Proton Energy: 910. 0 Me. V Ring Frequency: 1. 041 MHz Beam Rate: 59. 9 Hz MPS Mode: 1 m. Sec SNS status 14

SNS Status Long Term 15

SNS Status Long Term 15

SNS Calendar 16

SNS Calendar 16

Cosmic rays BG estimation Lets assume shielded bunker with area of 25 m 2

Cosmic rays BG estimation Lets assume shielded bunker with area of 25 m 2 on the surface SNS duty factor is 4 10 -4 This effectively reduce flux to 105 muons and ~600 neutrons per day entering enclosure We need one meter of steel overburden to reduce hadronic component of atmospheric showers and hermetic veto with efficiency of 99% Our estimations shows that expected number of untagged neutrons events in the detector is a few per day. This is below expected neutrino event rates Extra factor can be expected from PID in detectors. 17

SNS induced BG Most dangerous B. G. is from SNS neutrons Analysis is complicated

SNS induced BG Most dangerous B. G. is from SNS neutrons Analysis is complicated because many uncertainties still exist. We know for sure that environment is OK for humans. However neutrinos detectors are much more sensitive then humans! 6. 3 m 1. 7 m We considered three major sources: Space 1. 7 m Allocated For Neutrinos 4 m From the tunnel From the neutron instruments th i l o on t. M e g 18. 3 m Tar Proton Beam Target 18

Target Neutrons Full 3 D MSNPX calculations were performed till ~2 m Coupling tool

Target Neutrons Full 3 D MSNPX calculations were performed till ~2 m Coupling tool MTD was used to couple to 2 D DORT code to propagate further. Instrumental floor was modeled up to distance of 30 m 19

Neutrons from the Target 20

Neutrons from the Target 20

Neutrons from the Tunnel Similar Calculations were done taking into account beam losses Beam

Neutrons from the Tunnel Similar Calculations were done taking into account beam losses Beam losses ~ 1 W/m (Linear source) 21

Neutrons from the Tunnel 22

Neutrons from the Tunnel 22

SNS induced neutron flux High energy neutrons at 20 meters can be eliminated using

SNS induced neutron flux High energy neutrons at 20 meters can be eliminated using time cut To reduce low energy neutrons (neutron gas), extra shielding and neutron absorbers are required Just moving out without erecting extra shielding: • Front side (target) 1/R 2 • Right side (instruments) required detailed study • Left side (tunnel) 1/R