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 non-relativistic conformal group. We calculate the characters that can be used for generating the operators in a non-relativistic effective field theory, which accounts for redundancies from the equations of motion and integration by parts.
- Authors:
- 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 Name: Physics Letters B Journal Volume: 783 Journal Issue: C; Journal ID: ISSN 0370-2693
- Publisher:
- Elsevier
- Country of Publication:
- Netherlands
- 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. Netherlands: 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. Netherlands. 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". Netherlands. 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 non-relativistic conformal group. We calculate the characters that can be used for generating the operators in a non-relativistic 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 = C,
volume = 783,
place = {Netherlands},
year = {Wed Aug 01 00:00:00 EDT 2018},
month = {Wed Aug 01 00:00:00 EDT 2018}
}
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
Other availability
Cited by: 6 works
Citation information provided by
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Web of Science
Figures / Tables:
Table 1: Table for weights of generators P±, P3, H, J±, K±, K3, C under the Cartan generators E1 ≡ −iD , E2 ≡ J3, and E3 ≡ N . The i j-th entry is the weight of the i’th generator (i running over the possibilities P±, P3, H, J±,more »
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Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.