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This theoretical study explores how molecular orientation in H$_2^+$ can precisely tune optical Schrödinger cat states through high-harmonic generation, offering unique control mechanisms distinct from atomic systems. By leveraging dipole selection rules and two-center interference, the research establishes a tunable parameter for engineering non-classical light without relying on external laser intensity or focal geometry adjustments. Such advancements in controlling quantum superpositions via molecular alignment represent significant progress toward scalable photonic quantum information processing architectures.
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Tailoring optical Schr\"odinger cat states via orientation-dependent high-harmonic generation in $\rm{H}_2^+$

arXiv2 min read

arXiv:2607.21248v1 Announce Type: new Abstract: We theoretically demonstrate that the molecular orientation angle $\theta$ provides a structurally intrinsic, continuously tunable control parameter for engineering optical Schr\"{o}dinger cat states via high-harmonic generation (HHG) in H$_2^+$. Coupling time-dependent Schr\"{o}dinger equation simulations to the fully quantized HHG framework, we evaluate the Wigner functions of the post-selected harmonic-mode states under two complementary conditioning strategies. Conditioning on resonance-enhanced low-order harmonics exploits the complementary dipole selection rules of the $1\sigma_g\to1\sigma_u$ and $1\sigma_g\to1\pi_u$ transitions, driving a kitten-cat crossover whose direction is opposite in the two channels as $\theta$ is varied. Conditioning on plateau harmonics instead exploits two-center destructive interference, producing a reentrant cat$\to$kitten$\to$cat transition controlled by the order-dependent interference angle $\theta^*(q)$. In both cases the crossover is decoupled from the laser intensity, focal geometry, and molecular density, offering a degree of control with no counterpart in atomic targets.

Abstract:We theoretically demonstrate that the molecular orientation angle $\theta$ provides a structurally intrinsic, continuously tunable control parameter for engineering optical Schrödinger cat states via high-harmonic generation (HHG) in H$_2^+$. Coupling time-dependent Schrödinger equation simulations to the fully quantized HHG framework, we evaluate the Wigner functions of the post-selected harmonic-mode states under two complementary conditioning strategies. Conditioning on resonance-enhanced low-order harmonics exploits the complementary dipole selection rules of the $1\sigma_g\to1\sigma_u$ and $1\sigma_g\to1\pi_u$ transitions, driving a kitten-cat crossover whose direction is opposite in the two channels as $\theta$ is varied. Conditioning on plateau harmonics instead exploits two-center destructive interference, producing a reentrant cat$\to$kitten$\to$cat transition controlled by the order-dependent interference angle $\theta^*(q)$. In both cases the crossover is decoupled from the laser intensity, focal geometry, and molecular density, offering a degree of control with no counterpart in atomic targets.

Quantum Physics (quant-ph); Atomic Physics (physics.atom-ph); Computational Physics (physics.comp-ph); Optics (physics.optics)

arXiv:2607.21248 [quant-ph]

(or arXiv:2607.21248v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.21248 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 238 words

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