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Reactor & Accelerator Thanks to Bob McKeown for many of the slides

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Reactor & Accelerator . Thanks to Bob McKeown for many of the slides. Outline. Reactor Neutrinos The neutrinos Past experiments What we know and what we want to learn Accelerator Neutrinos The neutrinos Past experiments What we know and what we want to learn. n e Disappearance. - PowerPoint PPT Presentation

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Page 1: Reactor & Accelerator

Reactor & Accelerator

Thanks to Bob McKeown for many of the slides

Page 2: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 2

Outline

• Reactor NeutrinosThe neutrinosPast experimentsWhat we know and what we want to learn

• Accelerator NeutrinosThe neutrinosPast experimentsWhat we know and what we want to learn

Page 3: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 3

Distance (m)

P(ee)

Pee ≈1− cos4 θ13 1− sin2θ12 sin2 Δm122L

4Eν

⎝ ⎜

⎠ ⎟

⎣ ⎢

⎦ ⎥

Dominant 12 Oscillation

Pee ≈1− sin2 2θ13 sin2 Δm312L

4Eν+ Δm21

2L4Eν

⎝ ⎜

⎠ ⎟cos4 θ13 sin2 2θ12

Subdominant 13 Oscillation

e Disappearance

Page 4: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 4

13

90, 95, 99% CL

hep-

ph/0

3091

30

m232 from SK

atmospheric

Chooz

Solar

122

134

122

134

NCCC sinsinsincos/ ≈+≈ΦΦ

Page 5: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 5

Neutrino Oscillation Studies with Nuclear Reactors

• e from n-rich fission products

• detection via inverse beta decay (e+pe++n)

• Measure flux and energy spectrum

• Improve detectors, reduce background

• Variety of distances L= 10m-250km

Page 6: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 6

Detection Signal

Coincidence signal: detect• Prompt: e+ annihilation EEprompt+En+0.8 MeV• Delayed: n capture 180 s capture time

p+e

511keV

511keV 2.2 MeV

d

n

Page 7: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 7

Page 8: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 8

KamLAND usesthe entire Japanese

nuclear powerindustry as a

long baseline source

Kashiwazaki

Takahama

Ohi

Page 9: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 9

Page 10: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 10

Solar : m2 = 5.5x10-5 eV2

sin2 2 = 0.833

G.Fogli et al., PR D66, 010001-406,(2002)

Ratio of Measured and Expected e Flux from Reactor Neutrino Experiments

Page 11: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 11

Measurement of Energy Spectrum

Page 12: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 12

KamLAND best fit : m2 = 7.9 x 10-5 eV2

tan2 = 0.45

KamLAND fixes massSolar fixes angle

Page 13: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 13

New Reactor Proposals

Braidwood, Il

Daya Bay, China

Chooz, France• ~1.5 km baseline• Deeper/bigger• Near/Far

Page 14: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 14

Detector Design Studies

horizontal cylinder

horizontal cylinder

spherical

Page 15: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 15

Oscillation Formulae for Long-Baseline Neutrinos

For anti-neutrinos, the Jcp terms change sign.

Page 16: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 16

Long Baseline Physics Goals

• Definitive observation of oscillatory behavior in disappearance mode and precise determination of m2

23 and 23.• Detection of oscillation e in appearance

mode and measurement of 13.• Observe matter effects, hence sign of m2

23.• Measure cp

Page 17: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 17

CP violation and matter effects

hep-

ph/0

3062

21

Page 18: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 18

T2K

Phase I0.75 MW +SKPhase II4 MW + HyperK

Page 19: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 19

HyperK

Page 20: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 20

NOAUse the NUMI beam line from FermiLab.Far detector uses alternate vertical planes of active scintillator with passive wood absorber.

Page 21: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 21

Off-Axis Beam• For pions decaying in

flight, most neutrinos are forward directed

• Neutrino energy is proportional to E

• Neutrino energy flattens with angle, however. Allowing one to “choose” an energy by choosing the angle.

Page 22: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 22

Far Detector810 km from target10-14 km off axis

Page 23: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 23

LONG baseline 2500-3000 km

Page 24: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 24

The LSND Puzzle and MiniBOONE

30 meters

e etectorNeutrios e , , a

Protobea

Pios

Coer bea sto

Muos a electros

Watertaret

Page 25: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 25

The Evidence for Neutrino Oscillations

Page 26: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 26

Requires a 3rd m2

Page 27: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 27

Page 28: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 28

Page 29: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 29

Measurement of Oscillation Parameters

Page 30: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 30

Typical Muon-Neutrino Event

Page 31: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 31

Typical Michel Electron Event

Page 32: Reactor & Accelerator

June 2005 Steve Elliott, NPSS 2005 32

Resources

• Bob Mckeown APS April 2005 (Tampa)• APS neutrino study on reactors and

long baseline experiments.• BNL, T2K and NOA Letters of Intent• Bill Louis Talks