Coincidence charged-current neutrino-induced deuteron disintegration

Deuteron disintegration by charged-current neutrino (CCν) scattering offers the possibility to determine the energy of the incident neutrino by measuring in coincidence two of the three resulting particles: a charged lepton (usually a muon) and two protons, where we show that this channel can be iso...

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Bibliographic Details
Main Authors: Van Orden, J. W (Author), Ford, W. P (Author), Moreno Diaz, Oscar (Contributor), Donnelly, T. William (Contributor)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor), Massachusetts Institute of Technology. Laboratory for Nuclear Science (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2015-09-16T12:23:05Z.
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Online Access:Get fulltext
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100 1 0 |a Van Orden, J. W.  |e author 
100 1 0 |a Massachusetts Institute of Technology. Center for Theoretical Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Laboratory for Nuclear Science  |e contributor 
100 1 0 |a Moreno Diaz, Oscar  |e contributor 
100 1 0 |a Donnelly, T. William  |e contributor 
700 1 0 |a Ford, W. P.  |e author 
700 1 0 |a Moreno Diaz, Oscar  |e author 
700 1 0 |a Donnelly, T. William  |e author 
245 0 0 |a Coincidence charged-current neutrino-induced deuteron disintegration 
260 |b American Physical Society,   |c 2015-09-16T12:23:05Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/98528 
520 |a Deuteron disintegration by charged-current neutrino (CCν) scattering offers the possibility to determine the energy of the incident neutrino by measuring in coincidence two of the three resulting particles: a charged lepton (usually a muon) and two protons, where we show that this channel can be isolated from all others-for instance, from those with a pion in the final state. We discuss the kinematics of the process for several detection scenarios, both in terms of kinematic variables that are natural from a theoretical point of view and others that are better matched to experimental situations. The deuteron structure is obtained from a relativistic model (involving an approximation to the Bethe-Salpeter equation) as an extension of a previous, well-tested model used in deuteron electrodisintegration. We provide inclusive and coincidence (semi-inclusive) cross sections for a variety of kinematic conditions, using the plane-wave impulse approximation, introducing final-state hadronic exchange terms (plane-wave Born approximation) and final-state hadronic interactions (distorted-wave Born approximation). 
520 |a Seventh Framework Programme (European Commission) (Marie Curie Outgoing Fellowship (ELECTROWEAK)) 
520 |a United States. Dept. of Energy. Office of Nuclear Physics (Grant Contract DE-FG02-94ER40818) 
546 |a en 
655 7 |a Article 
773 |t Physical Review D