In quantum mechanics, Lx, Ly, and Lz are the components of angular momentum operators addressing the amount of "rotation" or "orbital" movement of a particle.
Angular momentum operators:
Lx, Ly, and Lz are the x, y, and z components of the orbital angular momentum vector (L). They are characterized as,
Lx = yPz - zPy
Ly = zPx - xPz
Lz = xPy - yPx
where
x, y, z are position vectors
Px, Py, Pz are momentum operators (partial derivative with respect to x, y, z)
Physical Interpretation:
Lx, Ly, and Lz address the projection of the orbital angular momentum vector onto the x, y, and z axes respectively.
Lx: measures rotation around the x-axis
Ly: measures rotation around the y-axis
Lz: measures rotation around the z-axis
Mathematical Representation:
In Cartesian coordinate, the angular momentum operators can be represented as:
Lx = - iℏ(y∂/∂z - z∂/∂y)
Ly = - iℏ(z∂/∂x - x∂/∂z)
Lz = - iℏ(x∂/∂y - y∂/∂x)
where I is the imaginary unit and ℏ is the reduced Planck constant.
Importance:
Understanding Lx, Ly, and Lz is crucial in quantum mechanics, as they:
1. Decide the rotational energy levels of atoms and molecules.
2. Influence the behavior of particles in magnetic fields.
3. Play a key role in the Zeeman effect and spin-orbit coupling.
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