Band Y B, Japha Y
Department of Chemistry, Department of Physics, and the Ilse Katz Center for Nano-Science, Ben-Gurion University, Beer-Sheva 84105, Israel.
Department of Physics, and the Ilse Katz Center for Nano-Science, Ben-Gurion University, Beer-Sheva 84105, Israel.
J Phys Condens Matter. 2022 Apr 20;34(25). doi: 10.1088/1361-648X/ac60d1.
We study the spin dynamics of diamond nitrogen vacancy (NV) centers in an oscillating magnetic field along the symmetry axis of the NV in the presence of transverse magnetic fields. It is well-known that the coupling between the otherwise degenerate Zeeman levels |= ±1⟩ due to strain and electric fields is responsible for a Landau-Zener process near the pseudo-crossing of the adiabatic energy levels when the axial component of the oscillating magnetic field changes sign. We derive an effective two-level Hamiltonian for the NV system that includes coupling between the two levels via virtual transitions into the third far-detuned level |= 0⟩ induced by transverse magnetic fields. This coupling adds to the coupling due to strain and electric fields, with a phase that depends on the direction of the transverse field in the plane perpendicular to the NV axis. Hence, theof the Zeeman levels can be tuned to control the adiabaticity of spin dynamics by fully or partially compensating the effect of the strain and electric fields, or by enhancing it. Moreover, by varying the strength and direction of the transverse magnetic fields, one can determine the strength and direction of the local strain and electric fields at the position of the NV center, and even thestress and electric field. The nuclear spin hyperfine interaction is shown to introduce a nuclear spin dependent offset of the axial magnetic field for which the pseudo-crossing occurs, while the adiabaticity remains unaffected by the nuclear spin. If the NV center is coupled to the environment, modeled by a bath with a Gaussian white noise spectrum, as appropriate for NVs near the diamond surface, then the spin dynamics is accompanied by relaxation of the Zeeman level populations and decoherence with a non-monotonic decrease of the purity of the system. The results presented here have important impact for metrology with NV centers, quantum control of spin systems in solids and coupled dynamics of spin and rotations in levitated nano-objects in the presence of magnetic fields.
我们研究了在存在横向磁场的情况下,沿金刚石氮空位(NV)对称轴方向的振荡磁场中NV中心的自旋动力学。众所周知,由于应变和电场,原本简并的塞曼能级| = ±1⟩之间的耦合,在振荡磁场的轴向分量改变符号时,会在绝热能级的伪交叉附近引发一个朗道 - 齐纳过程。我们推导了NV系统的有效二能级哈密顿量,其中包括通过横向磁场诱导的进入第三远失谐能级| = 0⟩的虚拟跃迁在两个能级之间的耦合。这种耦合叠加在由应变和电场引起的耦合之上,其相位取决于垂直于NV轴平面内横向场的方向。因此,可以通过完全或部分补偿应变和电场的影响,或者增强这种影响,来调节塞曼能级的,以控制自旋动力学的绝热性。此外,通过改变横向磁场的强度和方向,可以确定NV中心位置处局部应变和电场的强度和方向,甚至应力和电场。核自旋超精细相互作用表明会引入一个与核自旋相关的轴向磁场偏移,伪交叉发生在该偏移处,而绝热性不受核自旋的影响。如果将NV中心与环境耦合,用具有高斯白噪声谱的浴来建模,这适用于金刚石表面附近的NV,那么自旋动力学伴随着塞曼能级布居的弛豫以及系统纯度非单调下降的退相干。这里给出的结果对于使用NV中心的计量学、固体中自旋系统的量子控制以及在磁场存在下悬浮纳米物体中自旋与旋转的耦合动力学具有重要影响。