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Joshua T. Y. Chu

Publications and source records attributed to Joshua T. Y. Chu.

2 recordsLinked to original sources

Measuring electron density and electromagnetic fields in low-density laser-driven plasmas using proton radiography

In this paper, we describe a novel technique for inferring electron density in laser plasmas from proton-radiography data. Proton radiography is primarily a diagnostic for imaging electromagnetic field structures in such plasmas. In the presence of strong field gradients, `caustic' features arise and are broadened by the process of collisional scattering between the imaging protons and the plasma. This effect has a well defined density dependence, allowing for a robust measurement of electron number density. We validate the method on data from the turbulent-dynamo experiments performed at the Omega laser facility (with electron densities in the range of ${\sim}10^{20}\,\mathrm{cm^{-3}}$), achieving good agreement with values obtained from Thomson scattering, x-ray imaging and simulations. This research enables one of the most robust techniques for measuring electromagnetic fields on laser-plasma experiments to simultaneously provide density measurements along the same line of sight, improving our ability to diagnose such plasmas.

physics.plasm-ph↗

Probing keV mass QCD axions with the SACLA X-ray free electron laser

Axions are hypothetical particles, proposed to account for the invariance of CP symmetry in quantum chromodynamics. While axions and axion-like-particles are well-motivated by string theory and beyond-Standard-Model extensions, they have remained elusive to experimental searches even after significant effort over many decades. Building on a recent development using an X-ray free electron laser to search for cosmologically favoured axions of mass $m_{a} \lesssim 0.01$ eV, we extend previous bounds on the ALP-photon coupling, $g_{aγγ}$, by over an order of magnitude. We exploit the Bormann effect of Laue crystals in a light-shining-through-wall experiment, with broad sensitivity to $m_a \lesssim$ 22 eV. Moreover for $m_{a} \in$ (3460, 3480) eV our sensitivity reaches down to the QCD axion coupling prediction, providing the most stringent laboratory constraints in this mass range.

hep-ph↗