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Title: 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:
ORCiD logo [1];  [1]
  1. 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) (SC-25)
OSTI Identifier:
1459733
Alternate Identifier(s):
OSTI ID: 1499176
Grant/Contract Number:  
SC0009919
Resource Type:
Published Article
Journal Name:
Physics Letters. Section B
Additional Journal Information:
Journal Volume: 783; Journal ID: ISSN 0370-2693
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. doi:10.1016/j.physletb.2018.06.060.
Kobach, Andrew, and Pal, Sridip. Wed . "Conformal structure of the heavy particle EFT operator basis". United States. doi: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. Section B},
number = ,
volume = 783,
place = {United States},
year = {2018},
month = {7}
}

Journal Article:
Free Publicly Available Full Text
Publisher's Version of Record
DOI: 10.1016/j.physletb.2018.06.060

Citation Metrics:
Cited by: 2 works
Citation information provided by
Web of Science

Figures / Tables:

Table 1 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 » K±, K3, C under the Cartan generator E j .« less

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    Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.