skip to main content

DOE PAGESDOE PAGES

Title: Duality invariance of s ≥ 3/2 fermions in AdS

The research show that in D = 4 AdS, s ≥ 3/2 partially massless (PM) fermions retain the duality invariances of their flat space massless counterparts. They have tuned ratios m 2/M 2 ≠ 0 that turn them into sums of effectively massless unconstrained helicity ±(s, ···, 3/2) excitations, shorn of the lowest (non-dual) helicity ±1/2-rung and — more generally — of succeeding higher rung as well. Each helicity mode is separately duality invariant, like its flat space counterpart.
Authors:
 [1] ;  [2]
  1. California Institute of Technology, Pasadena, CA (United States); Brandeis Univ., Waltham, MA (United States)
  2. Univ. di Firenze and INFN Sezione di Firenze, Sesto Fiorentino (Italy)
Publication Date:
Grant/Contract Number:
SC0011632
Type:
Published Article
Journal Name:
Physics Letters. Section B
Additional Journal Information:
Journal Volume: 738; Journal Issue: C; Journal ID: ISSN 0370-2693
Publisher:
Elsevier
Research Org:
California Institute of Technology, Pasadena, CA (United States)
Sponsoring Org:
USDOE Office of Science (SC)
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; electromagnetic duality; higher spins
OSTI Identifier:
1198369
Alternate Identifier(s):
OSTI ID: 1221788

Deser, S., and Seminara, D.. Duality invariance of s ≥ 3/2 fermions in AdS. United States: N. p., Web. doi:10.1016/j.physletb.2014.09.058.
Deser, S., & Seminara, D.. Duality invariance of s ≥ 3/2 fermions in AdS. United States. doi:10.1016/j.physletb.2014.09.058.
Deser, S., and Seminara, D.. 2014. "Duality invariance of s ≥ 3/2 fermions in AdS". United States. doi:10.1016/j.physletb.2014.09.058.
@article{osti_1198369,
title = {Duality invariance of s ≥ 3/2 fermions in AdS},
author = {Deser, S. and Seminara, D.},
abstractNote = {The research show that in D = 4 AdS, s ≥ 3/2 partially massless (PM) fermions retain the duality invariances of their flat space massless counterparts. They have tuned ratios m2/M2 ≠ 0 that turn them into sums of effectively massless unconstrained helicity ±(s, ···, 3/2) excitations, shorn of the lowest (non-dual) helicity ±1/2-rung and — more generally — of succeeding higher rung as well. Each helicity mode is separately duality invariant, like its flat space counterpart.},
doi = {10.1016/j.physletb.2014.09.058},
journal = {Physics Letters. Section B},
number = C,
volume = 738,
place = {United States},
year = {2014},
month = {9}
}