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This study identifies a previously unknown lattice quantum disordered phase that governs the onset of superconductivity, challenging conventional phonon theories by incorporating nuclear quantum many-body effects. By demonstrating that quantum fluctuations of atomic nuclei directly drive the superconducting transition, the research provides a more accurate framework for predicting new superconductors and refining condensed matter physics models.
Superconductivity’s left flank explained by nuclear quantum effects

Researchers linked a lattice quantum disordered phase to superconductivity’s “left flank”, revealing how lattice vibrations—and the quantum behavior of nuclei within them—drive the transition.
Yu-Cheng Zhu, Jia-Xi Zeng and Xin-Zheng Li of Peking University report the discovery of a previously unknown lattice quantum disordered phase within superconductors. Their work reveals this phase occupies a triangular region in the P-T phase diagram, with its left boundary aligning precisely with the critical temperature where superconductivity begins on a material’s “left flank.” Identifying this alignment, the researchers establish lattice quantum disorder as a key component of the superconducting pairing mechanism and a unifying framework for both predicting new superconductors and understanding condensed matter physics more broadly. Prevailing models of superconductivity have long centered on electron behavior. But new calculations reveal a previously unrecognized lattice quantum disordered (LQD) phase that precisely defines the onset of superconductivity on one side of the material’s performance range. This phase, discovered through first-principles calculations incorporating nuclear quantum…
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