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A new scheme for isomer pumping and depletion with high-power lasers

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abstract

We propose a novel scheme for the population and depletion of nuclear isomers. The scheme combines the $\gamma$-photons with energies $\gtrsim 10$ keV emitted during the interaction of a contemporary high-intensity laser pulse with a plasma and one or multiple photon beams supplied by intense lasers. Due to nonlinear effects, two- or multi-photon absorption dominates over the conventional multi-step one-photon process for an optimized gamma flash. Moreover, this nonlinear effect can be greatly enhanced with the help of externally supplied low-energy photons coming from another laser. These low-energy photons act such that the effective cross-section experienced by the $\gamma$-photons becomes tunable, growing with the intensity $I_0$ of the beam. Assuming $I_{0}\sim 10^{18}$ Wcm$^{-2}$ for the photon beam, an effective cross-section as large as $10^{-21}$ cm$^2$ to $10^{-28}$ cm$^2$ for the $\gamma-$photon can be achieved. Thus, within state-of-the-art 10 PW laser facilities, the yields from two-photon absorption can reach $10^6$ to $10^9$ isomers per shot for selected states that are separated from their ground state by E2 transitions. Similar yields for transitions with higher multipolarities can be accommodated by multi-photon absorption with additional photons provided.

fields

nucl-th 1

years

2025 1

verdicts

CONDITIONAL 1

representative citing papers

Isomer production by multi-photon excitation

nucl-th · 2025-04-26 · conditional · novelty 5.0

A numerical time-dependent Schrödinger study predicts that the n-photon excitation probability of the 8 eV 229mTh isomer scales as intensity^n times pulse width squared in the perturbative regime, with saturation at higher intensities.

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  • Isomer production by multi-photon excitation nucl-th · 2025-04-26 · conditional · none · ref 33 · internal anchor

    A numerical time-dependent Schrödinger study predicts that the n-photon excitation probability of the 8 eV 229mTh isomer scales as intensity^n times pulse width squared in the perturbative regime, with saturation at higher intensities.