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AIP conference proceedings

Tunable sub-angstrom radiation generated by anti-stokes scattering from nuclear levels

C. B. Collins, Brett D DePaola

Published Jan 1, 1984• 1 citation
Publisher

Abstract

It was the intent of this work to use states of nuclear excitation in order to demonstrate coherent multiphoton processes that were the analogs of well‐known effects occurring at optical frequencies. Success in exciting radiofrequency sum and difference frequency sidebands on hyperfine components of the Mössbauer transition of 57Fe near 0.086 nm is described. The transition energy of those sidebands was shown to be tunable over five line‐widths by varying the radiofrequency component of the sum. A model is proposed that quantitatively explains these results in terms of coherently excited nuclear states and evidentally confirms the multiphoton nature of the process.

DOI
10.1063/1.34700

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We have used states of nuclear excitation to demonstrate coherent multiphoton processes that were the analogs of well-known effects occurring at optical frequencies. Success in exciting radio-frequency sidebands on hyperfine components of the 14.4-keV Mössbauer transition of (57)Fe is described. A distinctive feature of this experiment was that the absorbing foil was rigidly bound in a graphite sandwich intended to eliminate detrimental vibrations. A model is proposed that quantitatively explains these results in terms of coherently excited nuclear states and evidentially confirms the multiphoton nature of the sidebands observed in this experiment.

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This work concerns the demonstration of the feasibility of the tuning and perhaps even stimulation of nuclear radiation. Theory [1-3] has indicated that anti-Stokes Raman upconversion of intense but conventional long wavelength sources of radiation produced by scattering from isomeric states of nuclear excitation could lead to significant sources of tunable y-radiation characterized by the natural Mössbauer width of the lines. This would result in lines with sub-Angstrom wavelengths and widths of a few MHz. Further computations [4] have suggested that this type of coherent, as well as a new type of incoherent, optical pumping could even lead to appreciable levels of inversion of the population of nuclear levels that would be capable of supporting the growth of stimulated y-ray intensity. Whether or not these processes can reach threshold depends upon the resolution of basic issues lying in an interdisciplinary region between quantum electronics and nuclear physics that have not been previously addressed. It was the purpose of this work to study these issues experimentally.

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Resonance fluorescence of gamma radiation under conditions of coherent mixing of Mössbauer sublevels

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A method is proposed for calculating the resonance fluorescence spectrum of coherent gamma radiation with a finite linewidth under conditions when the sublevels of the ground nuclear state are coupled through a strong field. The spectrum line shape is substantially affected by both the coherent effects induced in the system by a strong field and the finite gamma-radiation width. The results obtained earlier and in this work give impetus to experimental investigations into the coherence of a quantum system and quantum interference of Mössbauer gamma transitions through the excitation of coherent magnetization dynamics or an optical subsystem in solids.

Physics of the Solid State•Apr 1, 2003•0 citations
It was the intent of this work to use states of nuclear excitation in order to demonstrate coherent multiphoton processes that were the analogs of well‐known effects occurring at optical frequencies. Success in exciting radiofrequency sum and difference frequency sidebands on hyperfine components of the Mössbauer transition of 57Fe near 0.086 nm is described. The transition energy of those sidebands was shown to be tunable over five line‐widths by varying the radiofrequency component of the sum. A model is proposed that quantitatively explains these results in terms of coherently excited nuclear states and evidentally confirms the multiphoton nature of the process.
We have used states of nuclear excitation to demonstrate coherent multiphoton processes that were the analogs of well-known effects occurring at optical frequencies. Success in exciting radio-frequency sidebands on hyperfine components of the 14.4-keV Mössbauer transition of (57)Fe is described. A distinctive feature of this experiment was that the absorbing foil was rigidly bound in a graphite sandwich intended to eliminate detrimental vibrations. A model is proposed that quantitatively explains these results in terms of coherently excited nuclear states and evidentially confirms the multiphoton nature of the sidebands observed in this experiment.
This work concerns the demonstration of the feasibility of the tuning and perhaps even stimulation of nuclear radiation. Theory [1-3] has indicated that anti-Stokes Raman upconversion of intense but conventional long wavelength sources of radiation produced by scattering from isomeric states of nuclear excitation could lead to significant sources of tunable y-radiation characterized by the natural Mössbauer width of the lines. This would result in lines with sub-Angstrom wavelengths and widths of a few MHz. Further computations [4] have suggested that this type of coherent, as well as a new type of incoherent, optical pumping could even lead to appreciable levels of inversion of the population of nuclear levels that would be capable of supporting the growth of stimulated y-ray intensity. Whether or not these processes can reach threshold depends upon the resolution of basic issues lying in an interdisciplinary region between quantum electronics and nuclear physics that have not been previously addressed. It was the purpose of this work to study these issues experimentally.
This work concerns the demonstration of the feasibility of the tuning and perhaps even stimulation of nuclear radiation. Theory1–3 has indicated that anti-Stokes Raman up- conversion of intense but conventional long-wavelength sources of radiation produced by scattering from isomeric states of nuclear excitation could lead to significant sources of tunable γ radiation characterized by the natural Mossbauer width of the lines. This would result in lines with sub-angstrom wavelengths and widths of a few megahertz. Further computations4 have suggested that this type of coherent, as well as a new type of incoherent, optical pumping could even lead to appreciable levels of inversion of the population of nuclear levels that would be capable of supporting the growth of stimulated γ-ray intensity. Whether these processes can reach threshold depends on the resolution of basic issues lying in an interdisciplinary region between quantum electronics and nuclear physics that have not been previously addressed.
The project is focused on theoretical and experimental studies of the quantum coherence effects at the atomic and nuclear transitions in solids. The main results are the following. 1. Electromagnetically Induced Transparency (EIT) and all-optical writing and probing of quantum coherence in room temperature solids are demonstrated experimentally in the first time. 2. The method for coherent suppression of excited state absorption in laser crystals is suggested. It opens the prospects for realization of the variety tunable solid state lasers including UV and VUV ranges. 3. High-efficient THz generation by means of resonant three-level mixing based on EIT in solids is predicted. 4. EIT in gamma-ray range of frequencies at the nuclear transitions via the nuclear level crossing is demonstrated experimentally in the first time. 5. Slowing of the gamma-ray photons due to the absorption line doublet is demonstrated in the first time. 6. Modifications of the Mossbauer absorption spectra under the action of laser radiation demonstrated experimentally in the first time. 7. The method for suppression of the inhomogeneous line broadening of the Mossbauer spectra is suggested.
A method is proposed for calculating the resonance fluorescence spectrum of coherent gamma radiation with a finite linewidth under conditions when the sublevels of the ground nuclear state are coupled through a strong field. The spectrum line shape is substantially affected by both the coherent effects induced in the system by a strong field and the finite gamma-radiation width. The results obtained earlier and in this work give impetus to experimental investigations into the coherence of a quantum system and quantum interference of Mössbauer gamma transitions through the excitation of coherent magnetization dynamics or an optical subsystem in solids.