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1. The role of Co valence in charge transport in the entropy‐stabilized oxide (Mg _0.2 Co _0.2 Ni _0.2 Cu _0.2 Zn _0.2 )O

   https://doi.org/10.1111/jace.18820  

   Jacobson, V.; Huang, J.; Titus, C.J.; Smaha, R.W.; Papac, M.; Lee, S.J.; Zakutayev, A.; Brennecka, G.L. (February 2023, Journal of the American Ceramic Society)
2. Emergent properties in the natural composite Ni ₂ MnSb _0.5 Al _0.5

   https://doi.org/10.1088/1361-6463/ab7c9f  

   Samanta, Tamalika; Salas, D; Srihari, V; Karaman, I; Bhobe, P A (May 2020, Journal of Physics D: Applied Physics)
3. A quantum dynamical study of the rotation of the dihydrogen ligand in the Fe(H) ₂ (H ₂ )(PEtPh ₂ ) ₃ coordination complex

   https://doi.org/10.1063/1.5026637  

   Gonzalez, Megan E.; Eckert, Juergen; Aquino, Adelia J.; Poirier, Bill (April 2018, The Journal of Chemical Physics)
4. Nonadiabatic coupling of the dynamical structure to the superconductivity in YSr ₂ Cu _2.75 Mo _0.25 O _7.54 and Sr ₂ CuO _3.3

   https://doi.org/10.1073/pnas.2018336117  

   Conradson, Steven D.; Geballe, Theodore H.; Jin, Chang-Qing; Cao, Li-Peng; Gauzzi, Andrea; Karppinen, Maarit; Baldinozzi, Gianguido; Li, Wen-Min; Gilioli, Edmondo; Jiang, Jack M.; et al (December 2020, Proceedings of the National Academy of Sciences)

   null (Ed.)

   A crucial issue in cuprates is the extent and mechanism of the coupling of the lattice to the electrons and the superconductivity. Here we report Cu K edge extended X-ray absorption fine structure measurements elucidating the internal quantum tunneling polaron (iqtp) component of the dynamical structure in two heavily overdoped superconducting cuprate compounds, tetragonal YSr 2 Cu 2.75 Mo 0.25 O 7.54 with superconducting critical temperature, T c = 84 K and hole density p = 0.3 to 0.5 per planar Cu, and the tetragonal phase of Sr 2 CuO 3.3 with T c = 95 K and p = 0.6. In YSr 2 Cu 2.75 Mo 0.25 O 7.54 changes in the Cu-apical O two-site distribution reflect a sequential renormalization of the double-well potential of this site beginning at T c , with the energy difference between the two minima increasing by ∼6 meV between T c and 52 K. Sr 2 CuO 3.3 undergoes a radically larger transformation at T c , >1-Å displacements of the apical O atoms. The principal feature of the dynamical structure underlying these transformations is the strongly anharmonic oscillation of the apical O atoms in a double-well potential that results in the observation of two distinct O sites whose Cu–O distances indicate different bonding modes and valence-charge distributions. The coupling of the superconductivity to the iqtp that originates in this nonadiabatic coupling between the electrons and lattice demonstrates an important role for the dynamical structure whereby pairing occurs even in a system where displacements of the atoms that are part of the transition are sufficiently large to alter the Fermi surface. The synchronization and dynamic coherence of the iqtps resulting from the strong interactions within a crystal would be expected to influence this process. 

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5. The spontaneous symmetry breaking in Ta ₂ NiSe ₅ is structural in nature

   https://doi.org/10.1073/pnas.2221688120  

   Baldini, Edoardo; Zong, Alfred; Choi, Dongsung; Lee, Changmin; Michael, Marios H.; Windgaetter, Lukas; Mazin, Igor I.; Latini, Simone; Azoury, Doron; Lv, Baiqing; et al (April 2023, Proceedings of the National Academy of Sciences)

   The excitonic insulator is an electronically driven phase of matter that emerges upon the spontaneous formation and Bose condensation of excitons. Detecting this exotic order in candidate materials is a subject of paramount importance, as the size of the excitonic gap in the band structure establishes the potential of this collective state for superfluid energy transport. However, the identification of this phase in real solids is hindered by the coexistence of a structural order parameter with the same symmetry as the excitonic order. Only a few materials are currently believed to host a dominant excitonic phase, Ta 2 NiSe 5 being the most promising. Here, we test this scenario by using an ultrashort laser pulse to quench the broken-symmetry phase of this transition metal chalcogenide. Tracking the dynamics of the material’s electronic and crystal structure after light excitation reveals spectroscopic fingerprints that are compatible only with a primary order parameter of phononic nature. We rationalize our findings through state-of-the-art calculations, confirming that the structural order accounts for most of the gap opening. Our results suggest that the spontaneous symmetry breaking in Ta 2 NiSe 5 is mostly of structural character, hampering the possibility to realize quasi-dissipationless energy transport. 

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