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Solvable model for a dynamical quantum phase transition from fast to slow scrambling

机译:从快速加扰到慢速加扰的动态量子相变的可解模型

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摘要

We propose an extension of the Sachdev-Ye-Kitaev (SYK) model that exhibits a quantum phase transition from the previously identified non-Fermi-liquid fixed point to a Fermi-liquid-like state, while still allowing an exact solution in a suitable large-N limit. The extended model involves coupling the interacting N-site SYK model to a new set of pN peripheral sites with only quadratic hopping terms between them. The conformal fixed point of the SYK model remains a stable low-energy phase below a critical ratio of peripheral sites p < p_c(n) that depends on the fermion filling n. The scrambling dynamics throughout the non-Fermi-liquid (NFL) phase is characterized by a universal Lyapunov exponent λ_L→ 2πT in the low-temperature limit; however, the temperature scale marking the crossover to the conformal regime vanishes continuously at the critical point p_c. The residual entropy at T → 0, nonzero in the NFL, also vanishes continuously at the critical point. For p > p_c the quadratic sites effectively screen the SYK dynamics, leading to a quadratic fixed point in the low-temperature and low-frequency limit. The interactions have a perturbative effect in this regime leading to scrambling with Lyapunov exponent λ_L ∝T~2.
机译:我们提出了Sachdev-Ye-Kitaev(SYK)模型的扩展,该模型展示了从先前确定的非费米液体固定点到费米液体状状态的量子相变,同时仍可以在合适的条件下进行精确求解大N限制。扩展模型涉及将相互作用的N站点SYK模型耦合到一组新的pN外围站点,它们之间只有二次跳跃项。 SYK模型的共形固定点保持稳定的低能量状态,低于外围位置的临界比率p _c(n),该临界比率取决于费米子填充n。整个非费米液体(NFL)阶段的加扰动力学特征是低温极限下的通用Lyapunov指数λ_L→2πT。然而,标志着与保形状态交叉的温度标度在临界点p_c处连续消失。 T→0处的残留熵在NFL中为非零,在临界点处也连续消失。对于p> p_c,二次位置有效地屏蔽了SYK动力学,从而导致了低温和低频极限中的二次固定点。相互作用在这种情况下具有微扰作用,导致以李雅普诺夫指数λ_L∝T〜2加扰。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第13期|134302.1-134302.16|共16页
  • 作者

    Sumilan Banerjee; Ehud Altaian;

  • 作者单位

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel,Department of Physics, Indian Institute of Science, Bangalore 560012, India;

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel,Department of Physics, University of California, Berkeley, California 94720, USA;

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