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1. Supersymmetry and T T ¯ $$ T\overline{T} $$ deformations

   https://doi.org/10.1007/JHEP04(2019)131  

   Chang, Chih-Kai; Ferko, Christian; Sethi, Savdeep (April 2019, Journal of High Energy Physics)
2. dS/dS and T T ¯ $$ T\overline{T} $$

   https://doi.org/10.1007/JHEP03(2019)085  

   Gorbenko, Victor; Silverstein, Eva; Torroba, Gonzalo (March 2019, Journal of High Energy Physics)
3. Structure and Bonding in [Sb@In ₈ Sb ₁₂ ] ³⁻ and [Sb@In ₈ Sb ₁₂ ] ⁵⁻

   https://doi.org/10.1002/anie.201904109  

   Liu, Chao; Tkachenko, Nikolay V.; Popov, Ivan A.; Fedik, Nikita; Min, Xue; Xu, Cong-Qiao; Li, Jun; McGrady, John E.; Boldyrev, Alexander I.; Sun, Zhong-Ming (June 2019, Angewandte Chemie International Edition)
4. Search for $${\text {Z}{}{}} {\text {Z}{}{}} $$ and $${\text {Z}{}{}} {\text {H}{}{}} $$ production in the $${\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} {\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} $$ final state using proton-proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$

   https://doi.org/10.1140/epjc/s10052-024-13021-z  

   Hayrapetyan, A; Tumasyan, A; Adam, W; Andrejkovic, J W; Bergauer, T; Chatterjee, S; Damanakis, K; Dragicevic, M; Hussain, P S; Jeitler, M; et al (July 2024, The European Physical Journal C)

   Abstract A search for$${\text {Z}{}{}} {\text {Z}{}{}} $$ $\text{Z}\text{Z}$and$${\text {Z}{}{}} {\text {H}{}{}} $$ $\text{Z}\text{H}$production in the$${\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} {\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} $$ $\text{b}\overline{\text{b}}\text{b}\overline{\text{b}}$final state is presented, where H is the standard model (SM) Higgs boson. The search uses an event sample of proton-proton collisions corresponding to an integrated luminosity of 133$$\,\text {fb}^{-1}$$ ${\text{fb}}^{-1}$collected at a center-of-mass energy of 13$$\,\text {Te}\hspace{-.08em}\text {V}$$ $\text{Te}\text{V}$with the CMS detector at the CERN LHC. The analysis introduces several novel techniques for deriving and validating a multi-dimensional background model based on control samples in data. A multiclass multivariate classifier customized for the$${\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} {\text {b}{}{}} {\bar{{\text {b}{}{}}}{}{}} $$ $\text{b}\overline{\text{b}}\text{b}\overline{\text{b}}$final state is developed to derive the background model and extract the signal. The data are found to be consistent, within uncertainties, with the SM predictions. The observed (expected) upper limits at 95% confidence level are found to be 3.8 (3.8) and 5.0 (2.9) times the SM prediction for the$${\text {Z}{}{}} {\text {Z}{}{}} $$ $\text{Z}\text{Z}$and$${\text {Z}{}{}} {\text {H}{}{}} $$ $\text{Z}\text{H}$production cross sections, respectively. 

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5. Geometrizing $$ T\overline{T} $$

   https://doi.org/10.1007/JHEP03(2021)140  

   Caputa, Pawel; Datta, Shouvik; Jiang, Yunfeng; Kraus, Per (March 2021, Journal of High Energy Physics)

   null (Ed.)

   A bstract The $$ T\overline{T} $$ T T ¯ deformation can be formulated as a dynamical change of coordinates. We establish and generalize this relation to curved spaces by coupling the undeformed theory to 2d gravity. For curved space the dynamical change of coordinates is supplemented by a dynamical Weyl transformation. We also sharpen the holographic correspondence to cutoff AdS 3 in multiple ways. First, we show that the action of the annular region between the cutoff surface and the boundary of AdS 3 is given precisely by the $$ T\overline{T} $$ T T ¯ operator integrated over either the cutoff surface or the asymptotic boundary. Then we derive dynamical coordinate and Weyl transformations directly from the bulk. Finally, we reproduce the flow equation for the deformed stress tensor from the cutoff geometry. 

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