monoenergetic neutrino beam for long baseline experiments

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Monoenergetic Neutrino Beam for Long Baseline Experiment s Joe Sato (Saitama & TUM) hep-ph/0503144 Joe Sato hep-ph/05????? Mark Rolinec , Joe Sato

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Monoenergetic Neutrino Beam for Long Baseline Experiments. Joe Sato (Saitama & TUM) hep-ph/0503144 Joe Sato hep-ph/05????? Mark Rolinec , Joe Sato. Introduction. Precision Measurement Precise Energy Determination for Neutrino. New Idea to determine Neutrino Energy at a Detector ?. - PowerPoint PPT Presentation

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Page 1: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Monoenergetic Neutrino Beamfor

Long Baseline Experiments

Joe Sato (Saitama & TUM)

hep-ph/0503144 Joe Satohep-ph/05????? Mark Rolinec , Joe Sato

Page 2: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Introduction

Precision Measurement  Precise Energy Determination for Neutrino

New Idea to determine Neutrino Energy at a Detector ?

Page 3: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Basic Idea

Electron Capture

Neutrino Energy at Rest : Definite

Boosting Mother Nuclei by

Control Neutrino Energy and Get Monoenergetic Neutrino Beam

Page 4: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Experimental SetupConcept

Neutral

Ionized

RemoveInjection

Page 5: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Condition on (and )

Highest Energy

Neutrino Energy in Lab

(Which Energy Range ?)

Assuming a beam pointing to a detector: At first glance

determines

Page 6: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Neutrinos “fly”

Larger Preferable

to get higher intensity beam

Lower

better

Inverse of “Quality Factor” (Zucchelli)

Baseline in rest frame

Page 7: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

However, Lower

Longer lifetime

Constraint from “our (experiment)” lifetime

Upper bound for

Find a nuclei with lower and

shorter

for mother nucleus

: At most several years

“Lower bound” for

Page 8: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Theoretical AspectsCase (i) : Purely monoenergetic neutrino

4.11 hour

Mass difference Excited Energy Binding Energy

No positron emission

Consider

Neutrino Energy in rest frame

Page 9: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Acceleration of

Baseline in the rest frame

  L independent

   (Q dependent)

Page 10: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

For

“All/2”

hit a detector with diameter D=176m! Detector

Rest frame of2D (= 176+176)m

Baseline length in the rest frame

Lifetime in lab

176m

Oscillation maximum is covered

Page 11: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Compare0.01% (nufact) ,1% (beta beam) neutrinos are used

Comparable with

Very Preliminary

NO optimization, rough estimate

Page 12: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Neutrino Energy as a function of R

For a detector size D

For example

Very wide range of neutrino energy

Detector position from beam center

Page 13: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

For the position resolution

Energy resolution

~ 30 cm for SK

Much better than others

Energy uncertainty is related with δR

Detection Position = Neutrino Energy !!

Page 14: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

In a solid angle

the number of neutrinos distribute uniformly

neutrino beam uniformly distributed in its energy

Energy Distribution

in rest frame

The solid angle is related with detector position

Optimum , baseline ? How large detector ?

Under consideration

Page 15: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Candidate Nucleus

Up to A=114

Page 16: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Case (ii) : Monoenergetic and Continuous energy neutrino

Both Electron capture and Positron Emission occur

If

Still Lower Q Nucleus

Energy distribution in rest frame

Page 17: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

is high

is small

At a detector, neutrinos from EC are monoenergetic

By varying

we can survey oscillation with definite energy resolution

EC dominates in decay of

Optimum combination of ‘s ?

Page 18: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

EC and Emission almost half and half

Can we make use of

both line spectrum and continuum spectrum ?

Appropriate

?

First maximum ?

Second maximum ?

Page 19: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Summary and Discussion

Electron Capture :Definite Neutrino Energy at rest frameControl Neutrino Energy at lab by boosting mother nuclei

For very low

Very large

If large enough, almost all neutrinos hit a detector

Very efficient use of neutrinosVery good “quality factor”

Summary

Page 20: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

Furthermore we can survey very wide range of neutrino energy simultaneously and energy is extremely “measured” by the detector position

Neutrino energy as a function of detector position

Simultaneous experiment with definite energy

Position is determined very precisely

Can we remove backgrounds more efficiently !?

Page 21: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

For not low

Monoenergetic Neutrino at a detector due to lower

By varying

we can survey oscillation with definite energy resolution

EC and Emission almost half and half Efficien

t ?

Both Electron capture and Positron Emission occur

EC dominates in decay of

Making use of both continuous and line spectrum?

Page 22: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

1. Even under a usual beta beam context,

Is better candidate than ?

Lower Q value by 6

Less nuclei by 40

633 KeV ( positron emission) 3935 KeV

Demerit : longer life ... But,

If we can circulate nuclei during one month or more,

Merit 2: much easier to create

Even a medical doctor can create

will be better source

Merit 1: lower Q

Discussion

Page 23: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

2. Other Problems

Otherwise

How to create anti-neutrino beam ?

Rely on parameter fitting?

How to create muon-neutrino beam ?

CP/T conjugate channels?

Very Preliminary

No optimization

Some of Correlation resolved

Page 24: Monoenergetic  Neutrino Beam for  Long Baseline Experiments

ありがとうございました(Arigatou Gozaimashita)

Vielen Danke