Bounds on heavy axions with an X-Ray free electron laser

28 Jan 2025
Seminars and colloquia
Time
Venue
Dennis Sciama Lecture Theatre
Denys Wilkinson Building, Department of Physics, 91探花, Keble Road, 91探花 OX1 3RH
Speaker(s)

Professor Gianluca Gregori, 91探花

Dr Jack Halliday, 91探花

Seminar series
Experimental particle physics seminar

Abstract

The axion, a theoretical particle arising from the breaking of Peccei-Quinn (PQ) symmetry, was proposed to explain the absence of CP violation in quantum chromodynamics (QCD). Axion-like particles (ALPs) are similarly predicted in string theory and could account for cold dark matter if their mass falls within the range of 10-6 鈥 10-4 eV. While most experimental searches target this "light axion window," heavy axions with masses exceeding 10-2 eV have recently gained attention. These 鈥渉eavy鈥 

axions are associated with a low scale breaking of Peccei-Quinn so are less susceptible to the 鈥渁xion quality problem鈥, namely destabilizing effects from quantum gravity on global symmetries. The most sensitive experimental bounds on these heavy axions are from various searches which aim to detect axions from the sun. This entails a degree of model dependence due to the high temperatures and plasma frequencies associated with this generation mechanism. So-called 鈥渄irect detection鈥 experiments, which aim to generate and detect axions in the laboratory have been proposed as a search strategy which negates this model dependence.

In this seminar, we describe a novel direct-detection experiment, conducted at EuXFEL (European X-Ray Free Electron Laser). Our experiment exploits the Primakoff effect via which photons can decay into axions in the presence of a strong external electric field and then reconvert back into photons after passing through an opaque wall. This was previously employed in so-called 鈥渓ight shining through wall experiments鈥 with optical lasers and external magnetic fields. However, in our work we used a free electron laser combined with a pair of germanium crystals. Within these crystals, the electric fields can be as high as 10^11 V/m, corresponding to a magnetic field ~1 kT 鈥 much higher than the field strengths accessible using the best electromagnets. In our initial experiment we were able to probe down to coupling constants on the order of 10^-3/GeV, however we will describe modifications to this setup capable of bringing the estimated bounds down to ~10^6/GeV.  This is close to the expectation for QCD axions to be dark matter.