A quantum interference effect that makes an opaque medium transparent to a probe beam when a second beam is applied.Electromagnetically induced transparency (EIT) is a quantum optical effect in which a medium that would normally absorb a light beam becomes transparent when a second, stronger 'control' beam is applied. The effect arises from quantum interference between two excitation pathways in the atoms of the medium, which cancels the absorption for a narrow frequency range of the probe beam. This makes EIT a powerful tool for slowing light dramatically, even to a standstill, and for storing light pulses as atomic excitations.
The effect was first predicted theoretically by Olga Kocharovskaya and Ya. I. Khanin in 1988, and independently by Stephen Harris and collaborators in 1990. The first experimental demonstration was by Harris and colleagues at Stanford University in 1991.
In a typical EIT setup, a medium of atoms has three energy levels arranged in a lambda configuration: two lower states and one excited state. The probe beam couples one lower state to the excited state, while the control beam couples the other lower state to the same excited state. When both beams are on, the atoms can be in a coherent superposition of the two lower states, a 'dark state' that does not interact with the light. Because the atoms are trapped in this dark state, they cannot absorb the probe beam, so the medium becomes transparent. The transparency is accompanied by a steep dispersion, which slows the group velocity of the probe pulse.
EIT is used in quantum memory devices for storing and retrieving light pulses, in slow-light experiments for optical delay lines, and in precision magnetometry and atomic clocks.
In EIT experiments, light has been slowed to speeds as low as a few meters per second, and even brought to a complete halt and then released intact.












