Casimir operators of 4D , π©=2 supersymmetry in the harmonic approach
Abstract
We construct Casimir operators of 4D, π©=2 supersymmetry algebra in the harmonic superspace approach, and provide the explicit expressions for them in terms of covariant derivatives in the analytic basis. Specifically, the superisospin operator CI is expressed in terms of new 'long' harmonic derivatives βΒ±Β±, β0 as CI = 1/4(β0)2 + 1/2{β++,βββ}. These derivatives involve non-local terms with the inverse Box operator Boxβ1 and satisfy modified SU(2) algebra relations in which the eigenvalues of β0 on analytic superfields are shifted by -2 relative to the standard U(1) harmonic charges. We also construct π©=2 superhelicity and super-isohelicity operators relevant to the massless case (with vanishing Box) and find their eigenvalues for few instructive examples of 4D, π©=2 superfield theories.
Related
- Commuting Toeplitz operators with harmonic symbols on the Fock space
- Commuting analytic and co-analytic Toeplitz operators on the harmonic Bergman space
- The spectral structure of Toeplitz operators with polynomial symbols on the harmonic Bergman space
- Zero products of Toeplitz operators with harmonic symbols on the Bergman space of the unit ball
- Finite zero products of Toeplitz operators with harmonic symbols
BibTeX
@misc{eremeev2026casimir,
title = {{Casimir operators of $4D\,, \mathcalN=2$ supersymmetry in the harmonic approach}},
author = {Egor Eremeev and Evgeny Ivanov},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2608.27412},
eprint = {2608.27412},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2608.27412},
}
RIS
TY - UNPB
TI - Casimir operators of 4D , π©=2 supersymmetry in the harmonic approach
AU - Egor Eremeev
AU - Evgeny Ivanov
PY - 2026
DA - 2026/09/10
PB - arXiv
DO - 10.48550/arxiv.2608.27412
UR - https://arxiv.org/abs/2608.27412
AB - We construct Casimir operators of 4D, π©=2 supersymmetry algebra in the harmonic superspace approach, and provide the explicit expressions for them in terms of covariant derivatives in the analytic basis. Specifically, the superisospin operator C_I is expressed in terms of new 'long' harmonic derivatives β^Β±Β±, β^0 as C_I = 1/4(β^0)^2 + 1/2{β^++,β^ββ}. These derivatives involve non-local terms with the inverse Box operator Box^β1 and satisfy modified SU(2) algebra relations in which the eigenvalues of β^0 on analytic superfields are shifted by -2 relative to the standard U(1) harmonic charges. We also construct π©=2 superhelicity and super-isohelicity operators relevant to the massless case (with vanishing Box) and find their eigenvalues for few instructive examples of 4D, π©=2 superfield theories.
ER -