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Larmor Precession

拉莫尔进动

When a magnetic moment μ is placed in a magnetic field B, it experiences a torque which can be expressed in the form of a vector product

当磁矩μ置于磁场B中时,会受到一个可以表示为向量积的力矩。

For a static magnetic moment or a classical current loop, this torque tends to line up the magnetic moment with the magnetic field B, so this represents its lowest energy configuration. But if the magnetic moment arises from the motion of an electron in orbit around a nucleus, the magnetic moment is proportional to the angular momentum of the electron. The torque exerted then produces a change in angular momentum which is perpendicular to that angular momentum, causing the magnetic moment to precess around the direction of the magnetic field rather than settle down in the direction of the magnetic field. This is called Larmor precession.

对于静态的磁矩或经典电流环,这种力矩会使磁矩与磁场B对齐,因此这代表了其最低能量配置。但如果磁矩来源于电子绕核运动,那么磁矩与电子的角动量成正比。此时施加的力矩会使角动量发生变化,该变化量垂直于角动量,导致磁矩绕磁场方向进行进动,而不是最终稳定在磁场方向上。这种现象称为Larmor进动。

When a torque is exerted perpendicular to the angular momentum L, it produces a change in angular momentum ΔL which is perpendicular to L, causing it to precess about the z axis. Labeling the precession angle as φ, we can describe the effect of the torque as follows:

当作用力矩垂直于角动量 L 时,它会引起角动量 ΔL 的变化,该变化垂直于 L,导致其绕 z 轴进动。将进动角标记为 φ,我们可以描述力矩的作用如下:

The precession angular velocity (Larmor frequency) is

进动角速度(拉莫尔频率)是

These relationships for a finite current loop extend to the magnetic dipoles of electron orbits and to the intrinsic magnetic moment associated with electron spin. There is also a characteristic Larmor frequency for nuclear spins.

这些关系对于有限的电流回路也适用于电子轨道的磁偶极子,以及与电子自旋相关的内在磁矩。此外,还有与核自旋相关的特征拉莫尔频率。

In the case of the electron spin precession, the angular frequency associated with the spin transition is usually written in the general form

在电子自旋进动的情况下,与自旋跃迁相关的角频率通常以一般形式表示

where γ is called the gyromagetic ratio (sometimes the magnetogyric ratio) and g is the electron spin g-factor. This angular frequency is associated with the "spin flip" or spin transition, involving an energy change of 2μB. An example for magnetic field 1 Tesla follows.

其中γ称为旋磁比(有时也称为磁旋比),而g是电子自旋g因子。这个角频率与“自旋翻转”或自旋跃迁有关,涉及能量变化为2μB。例如,对于磁场为1特斯拉的情况。

The characteristic frequencies associated with electron spin are employed in electron spin resonance (ESR) experiments, and those associated with the nuclear spin in nuclear magnetic resonance (NMR) experiments.

与电子自旋相关的特征频率用于电子自旋共振(ESR)实验,而与核自旋相关的特征频率则用于核磁共振(NMR)实验。
Index

Magnetic force applications

Magnetic field concepts

Reference
Rohlf, Sec 8-4

Larmor precession wiki
索引 磁力应用 磁场概念 参考 Rohlf,第8-4节 Larmor 进动 wiki
 
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