Citation

BibTex format

@article{Chester:2023:10.1007/jhep01(2023)038,
author = {Chester, SM and Dempsey, R and Pufu, SS},
doi = {10.1007/jhep01(2023)038},
journal = {Journal of High Energy Physics},
title = {Bootstrapping $$ \mathcal(N) $$ = 4 super-Yang-Mills on the conformal manifold},
url = {http://dx.doi.org/10.1007/jhep01(2023)038},
volume = {2023},
year = {2023}
}
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RIS format (EndNote, RefMan)

TY  - JOUR
AB  - <jats:title>                    A                    <jats:sc>bstract</jats:sc>                  </jats:title>                  <jats:p>                    We combine supersymmetric localization results with numerical bootstrap techniques to compute upper bounds on the low-lying CFT data of                    <jats:inline-formula>                      <jats:alternatives>                        <jats:tex-math>$$ \mathcal{N} $$</jats:tex-math>                        <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">                          <mml:mi>N</mml:mi>                        </mml:math>                      </jats:alternatives>                    </jats:inline-formula>                    = 4 super-Yang-Mills theory as a function of the complexified gauge coupling                    <jats:italic>τ</jats:italic>                    . In particular, from the stress tensor multiplet four-point function, we extract the scaling dimension of the lowest-lying unprotected scalar operator and its OPE coefficient. While our method can be applied in principle to any gauge group                    <jats:italic>G</jats:italic>                    , we focus on                    <jats:italic>G</jats:italic>                    = SU(2) and SU(3) for simplicity. At weak coupling, the upper bounds we find are very close to the corresponding four-loop results. We also give preliminary evidence that these upper bounds become small islands under reasonable assumptions.                  </jats:p>
AU  - Chester,SM
AU  - Dempsey,R
AU  - Pufu,SS
DO  - 10.1007/jhep01(2023)038
PY  - 2023///
TI  - Bootstrapping $$ \mathcal{N} $$ = 4 super-Yang-Mills on the conformal manifold
T2  - Journal of High Energy Physics
UR  - http://dx.doi.org/10.1007/jhep01(2023)038
UR  - https://doi.org/10.1007/jhep01(2023)038
VL  - 2023
ER  -
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