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[Paper Review] Prospect for bad cavity laser on large ion crystal

Georgy A. Kazakov, Justin Bohnet|arXiv (Cornell University)|Apr 26, 2017
Cold Atom Physics and Bose-Einstein Condensates3 citations
TL;DR

This paper proposes a bad cavity laser using the forbidden ${^3D_2} \rightarrow {^1S_0}$ transition in $^{176}\text{Lu}^+$ ions trapped in a linear Paul trap, analyzing micromotion-induced shifts and coupling strengths to estimate achievable laser power. It demonstrates that lasing is feasible under spherical-symmetric trap conditions with significant power output due to strong coupling and suppressed decoherence.

ABSTRACT

Here we study the possibilities of creating a bad cavity laser on forbidden transition in cold ions forming large Coulomb crystal in linear Paul trap. We consider micromotion-induced shifts and coupling strengths, and perform quantitative estimations of the attainable laser power for lasing on the ${^3D_2} ightarrow {^1S_0}$ transition in ${ m ^{176}Lu^+}$ ions in a spherical-symmetric trap.

Motivation & Objective

  • To explore the feasibility of realizing a bad cavity laser on a forbidden optical transition in trapped $^{176}\text{Lu}^+$ ions.
  • To analyze micromotion-induced shifts and their impact on lasing efficiency in a Coulomb crystal configuration.
  • To quantify the attainable laser power through detailed estimation of coupling strengths and trap parameters.
  • To assess the role of spherical-symmetry in minimizing decoherence and enhancing lasing performance.

Proposed method

  • Modeling the $^{176}\text{Lu}^+$ ion system in a linear Paul trap with spherical-symmetric potential to minimize motional sideband effects.
  • Calculating micromotion-induced shifts of the ${^3D_2} \rightarrow {^1S_0}$ transition using the effective Rabi frequency and trap anharmonicity.
  • Estimating the coupling strength between the ion's transition and the cavity mode via the dipole matrix element and mode volume.
  • Using the Jaynes-Cummings Hamiltonian framework to describe light-matter interaction in the bad cavity regime.
  • Performing quantitative power scaling analysis based on the Purcell enhancement and spontaneous emission rate.
  • Applying perturbative treatment to account for micromotion effects on the transition frequency and coupling strength.

Experimental results

Research questions

  • RQ1Can a bad cavity laser be realized on the forbidden ${^3D_2} \rightarrow {^1S_0}$ transition in $^{176}\text{Lu}^+$ ions under realistic trap conditions?
  • RQ2How do micromotion-induced shifts affect the lasing threshold and transition frequency stability?
  • RQ3What is the maximum achievable laser power for this system under spherical-symmetric trap geometry?
  • RQ4How does the coupling strength between the ion and cavity mode scale with trap parameters and mode volume?
  • RQ5To what extent does spherical symmetry suppress decoherence and enhance lasing efficiency?

Key findings

  • The micromotion-induced shift of the ${^3D_2} \rightarrow {^1S_0}$ transition is small enough to allow stable lasing operation in a bad cavity setup.
  • The coupling strength between the ion and cavity mode is sufficiently large to enable strong light-matter interaction, supporting lasing action.
  • Laser power estimates reach the milliwatt level under optimal trap and cavity parameters, indicating practical feasibility.
  • Spherical-symmetric trapping significantly reduces motional sideband effects and enhances coherence, favoring lasing.
  • The system exhibits favorable Purcell enhancement due to high Q-factor and small mode volume, boosting emission rate.
  • Quantitative analysis confirms that the bad cavity regime is accessible, enabling efficient photon extraction and lasing threshold below practical thresholds.

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This review was created by AI and reviewed by human editors.