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自旋弛豫的几何框架

A geometric framework for spin relaxation

Sophia N. Fricke, Kieren A. Harkins, Ashok Ajoy, Jeffrey A. Reimer

arXiv 2607.21569首次发表:更新:

AI 中文总结

研究自旋弛豫问题,开发几何框架,用单个协变弛豫张量表示耗散,$R_1$和$R_2$为互补投影。通过超极化$^{13}C$自旋实验证明弛豫是定向过程,此框架统一多种描述,为相关自旋系统弛豫提供语言。

AI 中文摘要

自旋弛豫传统上由纵向($R_1$)和横向($R_2$)两个独立的唯象速率描述,其分离掩盖了更深层次的结构统一性。本文开发了一个几何框架,其中耗散由作用于刘维尔空间的单个协变弛豫张量表示,$R_1$和$R_2$作为互补投影出现。该张量结构不仅形式上存在,还可通过探测自旋空间中非对易方向的脉冲序列进行实验获取。利用金刚石中含氮空位中心的超极化$^{13}C$自旋,发现对易脉冲序列产生近似对角的有效弛豫矩阵,非对易序列产生随发射机频率偏移和脉冲排序变化的非对角分量,证明弛豫是由张量而非一对标量速率控制的定向过程。几何相位的互补测量表明非对易动力学引入了与排序相关的效应,可与耗散分离,这与将弛豫解释为状态流形上的几何传输一致。该框架在与坐标无关的表述中统一了布洛赫、雷德菲尔德和林德布拉德描述,为驱动、各向异性和非平衡自旋系统中的弛豫提供了自然语言。

英文摘要

Spin relaxation is conventionally described by two independent phenomenological rates - longitudinal ($R_1$) and transverse ($R_2$) - whose separation obscures a deeper structural unity. Here we develop a geometric framework in which dissipation is represented by a single covariant relaxation tensor acting in Liouville space, from which $R_1$ and $R_2$ emerge as complementary projections. This tensor structure is not merely formal but is experimentally accessible through pulse sequences that probe noncommuting directions in spin space. Using hyperpolarized $^{13}C$ spins in diamond with nitrogen-vacancy centers, we show that commuting pulse trains yield effective relaxation matrices that are approximately diagonal, while noncommuting sequences produce off-diagonal components that vary with transmitter frequency offset and pulse ordering, providing evidence that relaxation is a directional process governed by a tensor rather than a pair of scalar rates. Complementary measurements of geometric phase demonstrate that noncommuting dynamics introduce ordering-dependent effects that are separable from dissipation, consistent with the interpretation of relaxation as geometric transport on the state manifold. This framework unifies Bloch, Redfield, and Lindblad descriptions within a coordinate-independent formulation and provides a natural language for relaxation in driven, anisotropic, and non-equilibrium spin systems.

论文原文

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