Conformal structure of the heavy particle EFT operator basis
Abstract
An operator basis of an effective theory with a heavy particle, subject to external gauge fields, is spanned by a particular kind of neutral scalar primary of the nonrelativistic conformal group. We calculate the characters that can be used for generating the operators in a nonrelativistic effective field theory, which accounts for redundancies from the equations of motion and integration by parts.
 Authors:

 Univ. of California, San Diego, CA (United States). Physics Dept.
 Publication Date:
 Research Org.:
 Univ. of California, San Diego, CA (United States)
 Sponsoring Org.:
 USDOE Office of Science (SC), High Energy Physics (HEP)
 OSTI Identifier:
 1459733
 Alternate Identifier(s):
 OSTI ID: 1499176
 Grant/Contract Number:
 SC0009919
 Resource Type:
 Published Article
 Journal Name:
 Physics Letters. B
 Additional Journal Information:
 Journal Volume: 783; Journal ID: ISSN 03702693
 Publisher:
 Elsevier
 Country of Publication:
 United States
 Language:
 English
 Subject:
 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
Citation Formats
Kobach, Andrew, and Pal, Sridip. Conformal structure of the heavy particle EFT operator basis. United States: N. p., 2018.
Web. doi:10.1016/j.physletb.2018.06.060.
Kobach, Andrew, & Pal, Sridip. Conformal structure of the heavy particle EFT operator basis. United States. https://doi.org/10.1016/j.physletb.2018.06.060
Kobach, Andrew, and Pal, Sridip. Wed .
"Conformal structure of the heavy particle EFT operator basis". United States. https://doi.org/10.1016/j.physletb.2018.06.060.
@article{osti_1459733,
title = {Conformal structure of the heavy particle EFT operator basis},
author = {Kobach, Andrew and Pal, Sridip},
abstractNote = {An operator basis of an effective theory with a heavy particle, subject to external gauge fields, is spanned by a particular kind of neutral scalar primary of the nonrelativistic conformal group. We calculate the characters that can be used for generating the operators in a nonrelativistic effective field theory, which accounts for redundancies from the equations of motion and integration by parts.},
doi = {10.1016/j.physletb.2018.06.060},
journal = {Physics Letters. B},
number = ,
volume = 783,
place = {United States},
year = {2018},
month = {7}
}
Free Publicly Available Full Text
Publisher's Version of Record
https://doi.org/10.1016/j.physletb.2018.06.060
https://doi.org/10.1016/j.physletb.2018.06.060
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Cited by: 7 works
Citation information provided by
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Web of Science
Figures / Tables:
Table 1: Table for weights of generators P_{±}, P_{3}, H, J_{±}, K_{±}, K_{3}, C under the Cartan generators E_{1} ≡ −iD , E_{2} ≡ J_{3}, and E_{3} ≡ N . The i jth entry is the weight of the i’th generator (i running over the possibilities P_{±}, P_{3}, H, J_{±},more »
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Reparameterization Invariant Operator Basis for NRQED and HQET
text, January 2018
 Kobach, Andrew; Pal, Sridip
 arXiv
Figures/Tables have been extracted from DOEfunded journal article accepted manuscripts.