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The Nu-SNS proposal - ORNL Physics Division - Oak Ridge ...

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56<br />

'<br />

Fe( ν , ν xn)<br />

x<br />

55<br />

Fe<br />

dominates.<br />

For lead, cross sections for the following neutral- and charged-current channels are desirable:<br />

'<br />

Pb(<br />

ν<br />

x,<br />

ν<br />

xn)<br />

'<br />

Pb(<br />

ν<br />

x,<br />

ν<br />

x<br />

2n)<br />

−<br />

Pb(<br />

ν , e n)<br />

A A−1<br />

A A−2<br />

A A−1<br />

e<br />

Since they are a both a necessary calibration for future supernova neutrino experiments and are<br />

important to nucleosynthesis simulations, iron and lead cross section measurements are a very<br />

high priority.<br />

3.4.3 Deuterium<br />

Neutrino experiments that use heavy water, like SNO, can detect supernova neutrinos via four<br />

main channels:<br />

− ' −<br />

e ( ν<br />

x<br />

, ν<br />

x<br />

) e<br />

'<br />

d(<br />

ν n x<br />

, ν<br />

x<br />

) p<br />

−<br />

d(<br />

ν e<br />

, e p)<br />

p<br />

d ( _ +<br />

ν e , e n)<br />

n<br />

Measurement of the reaction d(ν e ,e - p)p, which has been suggested as a calibration for the<br />

reaction p(e + ,ν e )d (part of the pp chain of reactions powering the Sun), would also provide a<br />

calibration for heavy water neutrino detectors. Monte Carlo studies suggest that for the source<br />

brightness predicted for the <strong>SNS</strong>, two years of data in approximately fifteen fiducial tons of<br />

D 2 O would yield a cross section measurement with an accuracy of a few percent [84], which<br />

in turn may enable a more accurate interpretation of SNO data. This measurement would<br />

also serve as an important test case for the effective field theory approach to neutrino-nucleus<br />

interactions (see [85] and references therein).<br />

Pb<br />

Pb<br />

Bi<br />

3.4.4 Carbon<br />

Large neutrino detectors that use liquid scintillator, such as KamLAND and MiniBoone, are<br />

+<br />

ideally suited to detect antineutrinos from a supernova collapse via ν<br />

e<br />

+ p → e + n . In addition,<br />

a significant number of neutral- and charged-current interactions could be detected [88] via:<br />

C(<br />

ν , e )<br />

12 − 12<br />

e<br />

N gs<br />

12 − 12 *<br />

C( ν e<br />

, e ) N<br />

12<br />

' 12 *<br />

C( ν<br />

x,<br />

ν<br />

x<br />

) C<br />

It is clear that every recorded neutrino interaction from the next galactic supernova will be<br />

extremely important. Detailed measurements of neutrino interactions in multiple channels will<br />

help untangle intensities and temperature of individual neutrino species. Although ν+Carbon<br />

interactions have been measured by LSND and KARMEN, ν-<strong>SNS</strong> measurements of double<br />

ν-<strong>SNS</strong> Proposal 32 8/4/2005

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