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

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supernovae. Measurements on Ba and Ta are possible and would provide meaningful constraints<br />

on the theoretical rates used in models thus far.<br />

Observations of the abundance of boron in stars as a function of metallicity do not show the<br />

strictly quadratic dependence that is expected from secondary production mechanisms, like<br />

cosmic-ray spallation, that operate after the galaxy has been enriched with metals. This implies<br />

[58] that primary mechanisms that operate early in the history of our galaxy, such as neutrino<br />

nucleosynthesis, also contribute significantly. According to current supernova nucleosynthesis<br />

models, neutrino nucleosynthesis in supernovae favors the production of 11 B over 10 B. <strong>The</strong>se two<br />

isotopes are produced through the following spallation channels:<br />

12<br />

12<br />

' 11<br />

C( ν<br />

x<br />

, ν<br />

x<br />

p)<br />

B<br />

' 11 +<br />

C( ν<br />

x<br />

, ν<br />

xn)<br />

C(<br />

e ν<br />

e<br />

)<br />

12<br />

'<br />

C d 10<br />

( ν<br />

x<br />

, ν<br />

x<br />

) B<br />

12<br />

' 10<br />

C( ν , ν pn)<br />

B ,<br />

x<br />

which need laboratory calibration. Neutrino spallation measurements, used in conjunction with<br />

future Hubble Space Telescope observations discriminating between 10 B and 11 B, would be<br />

invaluable in resolving this controversy and supporting (or refuting) the suggestion that neutrino<br />

nucleosynthesis in supernovae is an important source of 11 B in the galaxy [59].<br />

It has been suggested [60] that the final abundance of 19 F produced in a supernova can serve as a<br />

“supernova thermometer” because the ratio of [ 19 F/ 20 Ne]/[ 19 F/ 20 Ne] <br />

(the denominator is the<br />

measured ratio in our sun) is a measure of the µ and τ neutrinosphere temperatures (provided the<br />

abundance of 19 F produced in the supernova is due to neutrino nucleosynthesis). 19 F is produced<br />

through the following spallation channels:<br />

20<br />

x<br />

11<br />

' 19 +<br />

Ne( ν<br />

x<br />

, ν<br />

xn)<br />

Ne(<br />

e , ν<br />

e<br />

)<br />

20<br />

' 19<br />

Ne(<br />

ν , p)<br />

F.<br />

x<br />

ν<br />

x<br />

Recent models [57], using improved neutrino nucleus reaction rates, show marked decreases in<br />

the production of 19 F, casting some doubt on the possibility that 19 F is made in supernovae.<br />

Laboratory measurements of the relevant rates are clearly necessary to resolve this.<br />

Experiments to directly measure the cross sections for these reactions are extremely<br />

challenging and are not the goal of the initial suite of experiments at the ν-<strong>SNS</strong> facility.<br />

However, they are worthy of future consideration, since they provide direct insight into the<br />

productions sites of these rare isotopes and shed light on the conditions within these sites.<br />

3.3.3 <strong>Nu</strong>cleosynthesis in the Neutrino-Driven Wind<br />

Neutrino interactions may aid or prevent the r-process in a neutrino driven wind.<br />

<strong>The</strong> astrophysical r-process is responsible for roughly half of the Solar System’s supply of<br />

elements heavier than iron, with the remainder originating from the s-process occurring in<br />

Asymptotic Giant Branch stars. While the nuclear conditions necessary to produce the r-process<br />

are well established (see, e.g., [61]), the astrophysical site remains uncertain. <strong>The</strong> leading<br />

candidate is the neutrino-driven wind emanating from the proto-neutron star after a core collapse<br />

B<br />

19<br />

F<br />

ν-<strong>SNS</strong> Proposal 28 8/4/2005

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