dc.creator |
Butler, Malcolm |
|
dc.creator |
Chen, Jiunn-Wei |
|
dc.date.accessioned |
2014-11-18T18:37:17Z |
|
dc.date.available |
2014-11-18T18:37:17Z |
|
dc.date.issued |
2001-11 |
|
dc.identifier.issn |
0370-2693 |
|
dc.identifier.uri |
http://library2.smu.ca/xmlui/handle/01/25913 |
|
dc.description |
Publisher's version/PDF |
en_CA |
dc.description.abstract |
The proton–proton fusion process pp [right arrow] de[superscript +] v[subscript e] is calculated at threshold to fifth order in pionless effective field theory. There are two unknown two-body currents contributing at the second and fourth orders. Combined with the previous results for ν[subscript e]d and ν[over bar][subscript e]d scattering, computed to third order in the same approach, we conclude that a ∼ 10% measurement of reactor ν[hyphen symbol above v][subscript e]d scattering measurement could constrain the pp [right arrow] de[superscript +]ν[subscript e] rate to ∼ 7% while a ∼ 3% measurement of ν[subscript e]d [right arrow] e[superscript −]pp could constrain the pp rate to ∼ 2%. |
en_CA |
dc.description.provenance |
Submitted by Janine Mills (janine.mills@smu.ca) on 2014-11-18T18:37:17Z
No. of bitstreams: 1
Butler_Malcolm_article_2001.pdf: 67440 bytes, checksum: 78a1d55e961a27eed5b6c3ff91a430f5 (MD5) |
en |
dc.description.provenance |
Made available in DSpace on 2014-11-18T18:37:17Z (GMT). No. of bitstreams: 1
Butler_Malcolm_article_2001.pdf: 67440 bytes, checksum: 78a1d55e961a27eed5b6c3ff91a430f5 (MD5)
Previous issue date: 2001-11 |
en |
dc.language.iso |
en |
en_CA |
dc.publisher |
Elsevier Science |
en_CA |
dc.subject.lcsh |
Nuclear fusion |
|
dc.subject.lcsh |
Field theory (Physics) |
|
dc.title |
Proton–proton fusion in effective field theory to fifth order |
en_CA |
dc.type |
Text |
en_CA |
dcterms.bibliographicCitation |
Physics Letters B 520(1-2), 87-91. (2001) |
en_CA |