Diquark correlations in a hadron from lattice QCD

Using lattice QCD, a diquark can be studied in a gauge-invariant manner by binding it to a static quark in a heavylight-light hadron. We compute the simultaneous two-quark density of a diquark, including corrections for periodic boundary conditions. We define a correlation function to isolate the in...

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Bibliographic Details
Main Authors: Green, Jeremy Russell (Contributor), Engelhardt, M. (Author), Negele, John W. (Contributor), Varilly, Patrick (Author)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Institute of Physics, 2013-05-01T19:13:19Z.
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Online Access:Get fulltext
LEADER 01886 am a22002773u 4500
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042 |a dc 
100 1 0 |a Green, Jeremy Russell  |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 Negele, John W.  |e contributor 
100 1 0 |a Negele, John W.  |e contributor 
100 1 0 |a Green, Jeremy Russell  |e contributor 
700 1 0 |a Engelhardt, M.  |e author 
700 1 0 |a Negele, John W.  |e author 
700 1 0 |a Varilly, Patrick  |e author 
245 0 0 |a Diquark correlations in a hadron from lattice QCD 
260 |b American Institute of Physics,   |c 2013-05-01T19:13:19Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/78661 
520 |a Using lattice QCD, a diquark can be studied in a gauge-invariant manner by binding it to a static quark in a heavylight-light hadron. We compute the simultaneous two-quark density of a diquark, including corrections for periodic boundary conditions. We define a correlation function to isolate the intrinsic correlations of the diquark and reduce the effects caused by the presence of the static quark. Away from the immediate vicinity of the static quark, the diquark has a consistent shape, with much stronger correlations seen in the good (scalar) diquark than in the bad (axial-vector) diquark. We present results for mπ = 293 MeV as well as mπ = 940 MeV, and discuss the behavior as the pion mass changes. 
520 |a United States. Dept. of Energy (Grant DE-FG02-96ER40965) 
520 |a United States. Dept. of Energy (Grant No. DE-FG02- 94ER40818) 
520 |a Massachusetts Institute of Technology. Undergraduate Research Opportunities Program 
546 |a en_US 
655 7 |a Article 
773 |t Proceedings of the 19th International Conference on Particles and Nuclei (PANIC11)