A pendular state is a field-dressed rotational quantum state in which a molecule's orientation is concentrated near a preferred direction, resembling small angular librations of a pendulum. It arises when the orienting or aligning field interaction competes strongly with rotational kinetic energy.
A permanent dipole in a static electric field has an interaction proportional to , which distinguishes opposite directions. An anisotropic induced-polarization interaction often depends on , aligning an axis without necessarily orienting its two ends. The field strength and rotational constant determine whether a weak-field perturbation treatment is adequate.

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