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AIP Advances

Stimulated dipole–dipole interaction: A highly efficient mechanism for amplifying light-generated effects

Guan‐Zhang Lu, Che-Sheng Chou, H Y Lin, Yu‐Ching Kuo, Ya‐Ping Hsieh, Yang‐Fang Chen

Published Apr 1, 2026• 0 citations
Publisher

Abstract

A concept termed “stimulated dipole–dipole interaction” as a framework is proposed to describe coherence-enhanced light–matter interactions. Unlike conventional dipole–dipole interactions, excitation-induced dipoles, generated through external perturbations, coherently stimulate and couple with each other, leading to reinforced transition pathways and modified physical characteristics. Theoretically, the phenomenon of stimulated dipole–dipole interaction can be well understood and calculated based on the additional interference terms between transition dipole matrix elements of perturbed Hamiltonians in Fermi’s golden rule, where coherent coupling between excitation-induced and intrinsic dipoles alters the overall transition probability. This framework can be applied to many platforms, including wrinkled graphene, quantum dots, plasmonic dipoles, exciton–polaritons in stacked two-dimensional materials, and electric and magnetic dipoles in spin resonance, offering a versatile approach for engineering light–matter interactions. It is pointed out that the underlying mechanism of the originally proposed stimulated emission can also be understood well based on stimulated dipole–dipole interaction. Therefore, the proposed stimulated dipole–dipole interaction paves a milestone to advance the further exploration of not-yet realized quantum optics phenomena.

DOI
10.1063/5.0313706

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A concept termed “stimulated dipole–dipole interaction” as a framework is proposed to describe coherence-enhanced light–matter interactions. Unlike conventional dipole–dipole interactions, excitation-induced dipoles, generated through external perturbations, coherently stimulate and couple with each other, leading to reinforced transition pathways and modified physical characteristics. Theoretically, the phenomenon of stimulated dipole–dipole interaction can be well understood and calculated based on the additional interference terms between transition dipole matrix elements of perturbed Hamiltonians in Fermi’s golden rule, where coherent coupling between excitation-induced and intrinsic dipoles alters the overall transition probability. This framework can be applied to many platforms, including wrinkled graphene, quantum dots, plasmonic dipoles, exciton–polaritons in stacked two-dimensional materials, and electric and magnetic dipoles in spin resonance, offering a versatile approach for engineering light–matter interactions. It is pointed out that the underlying mechanism of the originally proposed stimulated emission can also be understood well based on stimulated dipole–dipole interaction. Therefore, the proposed stimulated dipole–dipole interaction paves a milestone to advance the further exploration of not-yet realized quantum optics phenomena.
Abstract The quantum mechanical description of the interaction of light with atoms treats absorption, gain, and recombination as upward and downward induced transitions of electrons between two states by perturbation due to the optical electric field. This provides the basis for a quantitative theory of diode lasers. The chapter begins with Einstein’s description of absorption, stimulated emission, and spontaneous emission, setting the scene for calculation of the transition probability by solving the time-dependent Schrödinger equation for a coherent superposition of the wavefunctions of two states. The resulting absorption spectrum has a Lorentzian lineshape due to dephasing of these wavefunctions. Expressions for the optical absorption cross section and Einstein coefficients are derived in terms of the dipole matrix element, and the dipole is illustrated using a hypothetical one-dimensional atom. Fermi’s Golden Rule for transitions to a continuum of states (as in quantum wells) is introduced in terms of the momentum matrix element.
The two-photon absorption by a pair of two-level atoms interacting with an incident field is examined. If the laser field is weak, then the existence of the dipole-dipole interaction-induced two-photon resonance follows from the higher-order Fermi golden rule. The effects of spontaneous emission and intense fields on the dipole-dipole interaction-induced two-photon resonance is studied using density-matrix methods. The presence of an intense field is shown to result in a significant enhancement of the two-photon resonance. Numerical results for the probability of simultaneous excitation of two atoms, for the atomic correlations, and for the radiated field intensity are presented.
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