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Non-Accelerator Physics with the Homestake “Megaton Array” 1) Nucleon Decay P o + e + , & P K + + e (improved PMTs may permit spatial & time recognition of K + + e ) 2) Prompt SN neutrinos – our Galaxy and nearby galaxies 3) Relic SN neutrinos (greater depth provides critical C.R. muon background reduction) 4) Low background shield (Used Hank Sobel talk-Korea 2005 & Ed Kearns talk -NNN07)
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Non-Accelerator Physics with the Homestake “Megaton Array”

Dec 30, 2015

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Kristen Wong

Non-Accelerator Physics with the Homestake “Megaton Array”. 1) Nucleon Decay P   o + e + , & P  K + + e (improved PMTs may permit spatial & time recognition of K + + e ) 2) Prompt SN neutrinos – our Galaxy and nearby galaxies - PowerPoint PPT Presentation
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Page 1: Non-Accelerator Physics with the Homestake “Megaton Array”

Non-Accelerator Physics with the Homestake “Megaton Array”

• 1) Nucleon Decay P o + e+, & P K+ +e

(improved PMTs may permit spatial & time recognition of K+ +e)

• 2) Prompt SN neutrinos – our Galaxy and nearby galaxies

• 3) Relic SN neutrinos (greater depth provides critical C.R. muon background reduction)

• 4) Low background shield

• (Used Hank Sobel talk-Korea 2005 & Ed Kearns talk -NNN07)

Page 2: Non-Accelerator Physics with the Homestake “Megaton Array”

Various Detection Techniques

%Free Protons

% Nuclei Features

Water 11% 89% Cerenkov radiation

Liquid ScintillatorCould insert into center of 100 kton water detector

~10% ~90% Signal from slow particles

Liquid Argon 0% 100% Tracking

Page 3: Non-Accelerator Physics with the Homestake “Megaton Array”

Detector Location Constraints

• 1) Depth

• 2) Distance from Power Reactors –

• Lead, SD is ~ 500 km from “nearby” U.S. power reactors – factor 30 (1/r2) better than Kamioka location

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Vertex Reconstruction of Vertex Reconstruction of EventsEventsN16

PMT times used to reconstruct event position

Resolution ~15 cm

UNTAGGEDUNTAGGED

TAGGEDTAGGED

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8 inch 10 inch13 inch

20 inch

13 inch PMT is very low profiledespite its diameter.

Large Format PMTsLarge Format PMTs

Applications:Neutrino Experiment

For Better Detection EfficiencyFor Better Detection Efficiency

Trial for High QE

R7081R7081R5912R5912

R8055R8055

R3600R3600

Page 12: Non-Accelerator Physics with the Homestake “Megaton Array”

Hamamatsu PMT Characteristics

PMT Dia. Quantum Efficiency

Rise Time

Transit time jitter

3600 20” 20% 10 ns 5.5 ns

7081 10.5” >35% 4.3 ns 2.9 ns

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Bialkali QE ComparisonBialkali QE Comparison

0

10

20

30

40

50

200 300 400 500 600 700Wavelength [nm]

Qu

an

tum

Effi

cien

cy [

%] Example Data for

UBA : R7600-200SBA : R7600-100STD : R7600

UBA:43%

SBA:35%

STD:26%

x1.3

x1.6

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0

5

10

15

20

25

30

35

40

200 300 400 500 600 700 800

Wavelength [nm]

Qu

an

tum

Effi

cie

ncy [

%]

Example data R7081 (10 Example data R7081 (10 inch)inch)

StandardStandard26% at 380 nm26% at 380 nm

High QE TypeHigh QE TypeChampion DataChampion Data35% at 380 nm35% at 380 nm

0

2

4

6

8

10

12

~28 ~30 ~32 ~34 ~36QE at 380 nm (%)

Samples:22 pcsAverage:31.6%

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