Abstract

We study the weak mixing of photons and relativistic axionlike particles (axions) in plasmas with background magnetic fields, $\mathbf{B}$. We show that, to leading order in the axion-photon coupling, the conversion probability, ${P}_{\ensuremath{\gamma}\ensuremath{\rightarrow}a}$, is given by the one-dimensional power spectrum of the magnetic field components perpendicular to the particle trajectory. Equivalently, we express ${P}_{\ensuremath{\gamma}\ensuremath{\rightarrow}a}$ as the Fourier transform of the magnetic field autocorrelation function, and establish a dictionary between properties of the real-space magnetic field and the energy-dependent conversion probability. For axions more massive than the plasma frequency, (${m}_{a}>{\ensuremath{\omega}}_{\mathrm{pl}}$), we use this formalism to analytically solve the problem of perturbative axion-photon mixing in a general magnetic field. In the general case where ${\ensuremath{\omega}}_{\mathrm{pl}}/{m}_{a}$ varies arbitrarily along the trajectory, we show that a naive application of the standard formalism for ``resonant'' conversion can give highly inaccurate results, and that a careful calculation generically gives nonresonant contributions at least as large as the resonant contribution. Furthermore, we demonstrate how techniques based on the Fast Fourier Transform provide a new, highly efficient numerical method for calculating axion-photon mixing. We briefly discuss magnetic field modeling in galaxy clusters in the light of our results and argue, in particular, that a recently proposed ``regular'' model used for studying axion-photon mixing (specifically applied to the Perseus cluster) is inconsistent with observations. Our formalism suggests new methods to search for imprints of axions, and will be important for spectrographs with percent level sensitivity, which includes existing X-ray observations by Chandra as well as the upcoming Athena mission.

Highlights

  • Determining the elementary particle content beyond the established Standard Model is a central goal of contemporary high-energy physics

  • We review the arguments for turbulence in the intracluster medium (ICM), and the classes of models used in astrophysical axion searches

  • We suggest that future studies of the magnetic field autocorrelation function in state-of-the-art magnetohydrodynamic simulations of the ICM will be very useful in improving the sensitivity of axion searches

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Summary

INTRODUCTION

Determining the elementary particle content beyond the established Standard Model is a central goal of contemporary high-energy physics. To leading order (LO) in gaγ, the axion-photon transition amplitude involving such massive axions is given by a sum of Fourier cosine and sine transforms of the (relevant component of the) magnetic field, B. Our formalism could lead to new methodologies for axion searches, e.g. by generating the relevant mixing probabilities directly from an observationally inferred class of autocorrelation functions, without ever explicitly solving the Schrödinger equation. (30), (79), and (115); (ii) accounting carefully for both resonant and nonresonant contributions when ωpl 1⁄4 ma at one or more points along the trajectory, cf Sec. V B; (iii) the demonstration that one can use highly efficient FFT methods to calculate the conversion probabilities, cf Sec. VI B; (iv) the identification of new, promising methods that are made possible by the new formalism, and which can open up new directions for axion searches, cf Sec. VII C

CLASSICAL AXION-PHOTON CONVERSION USING “QUANTUM” PERTURBATION THEORY
FOURIER TRANSFORM FORMALISM
Examples
Example 1: A single cell of constant B
Example 2
B2i i cosðηdi η2
Example 3
Example 4
Example 6: “Regular” magnetic fields
THE FOURIER TRANSFORM FORMALISM
The transition amplitude and the conversion probability
Example 7
Resonant contributions
Nonresonant contribution
Example 8
NUMERICAL TESTS OF THE FORMALISM
The discrete cosine and sine transforms
Numerical implementations applied to the Perseus cluster
Performance improvement
Perturbativity
Magnetic fields in clusters
Galaxy cluster magnetic field models in axion searches
Outlook
Findings
VIII. CONCLUSIONS

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