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Communications Physics

Acoustically controlled polarization states of resonant γ-photons

Vlastimil Vrba, Michal Koutný, Jan Kočiščák, Michal Hausner, Aleš Stejskal, Vítězslav Heger, Petr Novák, Petr Obšil, Tomáš Jüngling, Vít Procházka

Published Oct 30, 2026• 0 citations
Publisher

Abstract

Coherent control of light and its interactions with matter is a key aspect of quantum optics. Nuclear resonant interactions enable coherent manipulation of photons at X-ray and γ -ray energies. One promising approach to manipulating γ -photons emitted by radioactive sources exploits ultrasonically vibrating nuclear resonant absorbers. However, previous studies have focused on unpolarized γ -radiation interacting with isotropic resonant media without exploiting polarization effects. Here, we demonstrate simultaneous temporal control of the waveform and polarization state of γ -photons by combining ultrasonic vibrations of magnetically ordered resonant absorbers with anisotropy in nuclear resonant scattering. This method allows interlinking phase differences of individual resonant interaction paths with their polarization dependence. A particular consequence is the possibility to form double-pulse γ -radiation sequences with tunable time-dependent polarization states. Using the reported method, coherent control of γ -photons can be expanded to polarization-based experiments and related applications in quantum optics can be further explored using a tabletop γ -optical setup.

DOI
10.1038/s42005-026-02923-x

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Coherent control of light and its interactions with matter is a key aspect of quantum optics. Nuclear resonant interactions enable coherent manipulation of photons at X-ray and γ -ray energies. One promising approach to manipulating γ -photons emitted by radioactive sources exploits ultrasonically vibrating nuclear resonant absorbers. However, previous studies have focused on unpolarized γ -radiation interacting with isotropic resonant media without exploiting polarization effects. Here, we demonstrate simultaneous temporal control of the waveform and polarization state of γ -photons by combining ultrasonic vibrations of magnetically ordered resonant absorbers with anisotropy in nuclear resonant scattering. This method allows interlinking phase differences of individual resonant interaction paths with their polarization dependence. A particular consequence is the possibility to form double-pulse γ -radiation sequences with tunable time-dependent polarization states. Using the reported method, coherent control of γ -photons can be expanded to polarization-based experiments and related applications in quantum optics can be further explored using a tabletop γ -optical setup.
We report a method for coherent control of γ-photons, enabling the shaping of γ-ray intensity in nearly arbitrary waveforms. Different intensity waveforms are created by adjusting the motion profile of a resonant absorber (an ensemble of Mössbauer nuclei) and tuning the energy of the incident radiation. A crucial aspect of this method is the use of a low fundamental frequency of vibrations, which broadens the possibilities for γ-ray control. The results of numerical simulations are experimentally validated by generating single and double γ-pulses and inducing short-term absorption. For this, a resonant absorber containing 57Fe nuclei was vibrated with different motion profiles composed of 12 harmonics with a fundamental frequency of 1 MHz. The proposed technique represents an advancement in the manipulation of γ-rays, and potentially x rays, paving the way for the performance of unique types of γ-ray or x-ray quantum experiments and the development of tools such as adjustable table-top γ-pulse sources or γ-ray or x-ray delays and gates. Moreover, inverse application of the method enables investigation of motion at the picometer scale.
This study provides a detailed theoretical description of periodic γ -ray intensity signals. These signals are generated by the tabletop time coincidence experimental setups which utilize nuclear resonant interaction of γ -photons from a radioactive source with an absorber exhibiting ultrasonic vibrations. Transmission of the γ -radiation field through the absorber is described by semiclassical theory considering arbitrary periodic motion of the absorber. A key aspect of the presented work is the application of the Fourier analysis. A fundamental relation between the Fourier coefficients of the γ -ray intensity signal and the Fourier coefficients of a complex exponential of the absorber motion is derived. Application of this relation is shown on the example of the trapezoid motion, which demonstrates its usability for systematic inspection of the discussed signals. The results of the analysis expand the knowledge of the coherent manipulation of γ -photons and may find usage in a broad range of research fields utilizing γ -ray sources.
Abstract The induced transparency of opaque medium for resonant electromagnetic radiation is a powerful tool for manipulating the field-matter interaction. Various techniques to make different physical systems transparent for radiation from microwaves to x-rays were implemented. Most of them are based on the modification of the quantum-optical properties of the medium under the action of an external coherent electromagnetic field. Recently, an observation of acoustically induced transparency (AIT) of the 57Fe absorber for resonant 14.4-keV photons from the radioactive 57Co source was reported. About 150-fold suppression of the resonant absorption of photons due to collective acoustic oscillations of the nuclei was demonstrated. In this paper, we extend the AIT phenomenon to a novel phase-locked regime, when the transmitted photons are synchronized with the absorber vibration. We show that the advantages of synchrotron Mössbauer sources such as the deterministic periodic emission of radiation and controlled spectral-temporal characteristics of the emitted photons along with high-intensity photon flux in a tightly focused beam, make it possible to efficiently implement this regime, paving the way for the development of the acoustically controlled interface between hard x-ray photons and nuclear ensembles.
A method has been proposed to reconstruct at arbitrary time the spectral–temporal characteristics of a 14.4‑keV single-photon wave packet that is emitted by a 57Co source and is resonantly absorbed in the medium of 57Fe nuclei. The method is based on the frequency separation of the field emitted by the source and resonance nuclear polarization induced by this field by means of delayed acoustically induced transparency of the absorber, which appears after the activation of oscillations of the absorber at the corresponding frequency and amplitude. The proposed method has been compared to the known quantum-optical memory methods and methods of nuclear polarization control in the gamma-ray range. Experimental conditions have been proposed to implement the method. It has been shown that this method allows the implementation of the time-resolved Mössbauer spectroscopy of various media.
The possibility to control the coherent decay of resonant excitations in nuclear forward scattering is investigated. By changing abruptly the direction of the nuclear hyperfine magnetic field, the coherent scattering of photons can be manipulated and even completely suppressed via quantum interference effects between the nuclear transition currents. The efficiency of the coherent decay suppression and the dependence of the scattered light polarization on the specific switching parameters is analyzed in detail. Using a sophisticated magnetic switching sequence involving four rotations of the hyperfine magnetic field, two correlated coherent decay pulses with different polarizations can be generated out of one excitation, providing single-photon entanglement in the keV regime. The verification of the generated entanglement by testing a single-particle version of Bell's inequality in an X-ray optics experimental setup is put forward.
Means to coherently control single x-ray photons in resonant scattering of light off nuclei by electric or magnetic fields are investigated theoretically. In order to derive the time response in nuclear forward scattering, we adapt the Maxwell–Bloch equations known from quantum optics to describe the resonant light pulse propagation through a nuclear medium. Two types of time-dependent perturbations of nuclear forward scattering are considered for coherent control of the resonantly scattered x-ray quanta. Firstly, the simultaneous coherent propagation of two pulses through the nuclear sample is addressed. We find that the signal of a weak pulse can be enhanced or suppressed by a stronger pulse simultaneously propagating through the sample in counter-propagating geometry. Secondly, the effect of a time-dependent hyperfine splitting is investigated and we put forward a scheme that allows parts of the spectrum to be shifted forward in time. This is the inverse effect of coherent photon storage and may become a valuable technique if single x-ray photon wavepackets are to become the information carriers in future photonic circuits.