论文标题
部分可观测时空混沌系统的无模型预测
Quantum phase diagram of high-pressure hydrogen
论文作者
论文摘要
电子相关和核量子效应之间的相互作用使我们对元素氢的理解成为巨大的挑战。 Here, we present the phase diagram of hydrogen and deuterium at low temperatures and high-pressure ($P > 300$ GPa by accounting for highly accurate electronic and nuclear enthalpies. We evaluated internal electronic energies by diffusion quantum Monte Carlo, while nuclear quantum motion and anharmonicity have been included by the stochastic self-consistent harmonic approximation. Our results show that the long-sought atomic metallic预计将以$ 577 \ pm 10 $ GPA形成氢气($ 640 \ pm 14 $ gpa)的氢气确实会使这种阶段的稳定性推向稳定的稳定性。 (第六阶段)$ 422 \ pm 40 $ gpa($ 442 \ pm30 $ gpa在氘中,我们都可以在光谱和直流电导率上进行清晰的签名,这些签名可在我们的发现下,可以通过实验来区分两个结构性过渡。
The interplay between electron correlation and nuclear quantum effects makes our understanding of elemental hydrogen a formidable challenge. Here, we present the phase diagram of hydrogen and deuterium at low temperatures and high-pressure ($P > 300$ GPa by accounting for highly accurate electronic and nuclear enthalpies. We evaluated internal electronic energies by diffusion quantum Monte Carlo, while nuclear quantum motion and anharmonicity have been included by the stochastic self-consistent harmonic approximation. Our results show that the long-sought atomic metallic hydrogen, predicted to host room-temperature superconductivity, forms at $577\pm 10$ GPa ($640\pm 14$ GPa in deuterium). Indeed, anharmonicity pushes the stability of this phase towards pressures much larger than previous theoretical estimates or attained experimental values. Before atomization, molecular hydrogen transforms from a conductive phase III to another metallic structure that is still molecular (phase VI) at $422\pm 40$ GPa ($442\pm30$ GPa in deuterium). We predict clear-cut signatures in optical spectroscopy and DC conductivity that can be used experimentally to distinguish between the two structural transitions. According to our findings, the experimental evidence of metallic hydrogen has so far been limited to molecular phases.