Classical Larmor formula through the Unruh effect for uniformly accelerated electrons

Physical Review D: Particles, Fields, Gravitation and Cosmology American Physical Society 109 (2024) 024044

Abstract:

We investigate the connection between the classical Larmor formula and the quantum Unruh effect by computing the emitted power by a uniformly accelerated charged particle and its angular distribution in the co-accelerated frame. We consider a classical particle accelerated with non-zero charge only for a finite period and then take the infinite-time limit after removing the effects due to the initial charging and final discharging processes. We show that the result found for the interaction rates agrees with previous studies in which the period of acceleration with non-zero charge was taken to be infinite from the beginning. We also show that the power and angular distribution of emission, which is attributed either to the emission or absorption of a Rindler photon in the co-accelerated frame, is given by the Larmor formula, confirming that, at tree level, it is necessary to take into account the Unruh effect in order to reproduce the classical Larmor radiation formula in the coaccelerated frame.

Quantum effects on dynamic structure factors in dense magnetized plasmas

Physical Review E: Statistical, Nonlinear, and Soft Matter Physics American Physical Society 6:1 (2024) 013089

Authors:

Tushar Mondal, Gianluca Gregori

Abstract:

We extend the classical magnetohydrodynamics formalism to include nonlocal quantum behavior via the phenomenological Bohm potential. We then solve the quantum magnetohydrodynamics equations to obtain a new analytical form of the dynamic structure factor (DSF), a fundamental quantity linking theory and experiments. Our results show that the three-peak structure—one central Rayleigh peak and two Brillouin peaks—of the DSF arising from quantum hydrodynamic fluctuations becomes (in general) a five-peak structure—one central Rayleigh peak and two pairs of peaks associated with fast and slow magnetosonic waves. The Bohm contribution influences the positions and characteristics (height, width, and intensity) of the peaks by introducing three significant modifications: (a) an increase in effective thermal pressure, (b) a reduction in the adiabatic index, and (c) an enhancement of effective thermal diffusivity. The multiple DSF peaks enable concurrent measurements of diverse plasma properties, transport coefficients, and thermodynamic parameters in magnetized dense plasmas. The potential for experimental validation of our theory looms large, particularly through future experiments conducted at state-of-the-art laser facilities.

Comment on “Matter-wave interferometry with helium atoms in low-l Rydberg states”

Physical Review A American Physical Society (APS) 109:1 (2024) 017301

Authors:

DZ Chan, JDD Martin

Phase transitions of Fe2O3 under laser shock compression

under review for Physical Review Letters

Authors:

A. Amouretti, C. Crépisson, S. Azadi, D. Cabaret, T. Campbell, D. A. Chin, B. Colin, G. R. Collins, L. Crandall, G. Fiquet, A. Forte, T. Gawne, F. Guyot, P. Heighway, H. Lee, D. McGonegle, B. Nagler, J. Pintor, D. Polsin, G. Rousse, Y. Shi, E. Smith, J. S. Wark, S. M. Vinko, M. Harmand

Abstract:

We present in-situ x-ray diffraction and velocity measurements of Fe2O3 under laser shock compression at pressures between 38-116 GPa. None of the phases reported by static compression studies were observed. Instead, we observed an isostructural phase transition from α-Fe2O3 to a new α′-Fe2O3 phase at a pressure of 50-62 GPa. The α′-Fe2O3 phase differs from α-Fe2O3 by an 11% volume drop and a different unit cell compressibility. We further observed a two-wave structure in the velocity profile, which can be related to an intermediate regime where both α and α′ phases coexist. Density functional theory calculations with a Hubbard parameter indicate that the observed unit cell volume drop can be associated with a spin transition following a magnetic collapse.

Proton imaging of high-energy-density laboratory plasmas

Reviews of Modern Physics American Physical Society 95:4 (2023) 045007

Authors:

Derek B Schaeffer, Archie FA Bott, Marco Borghesi, Kirk A Flippo, William Fox, Julian Fuchs, Chikang Li, Fredrick H Séguin, Hye-Sook Park, Petros Tzeferacos, Louise Willingale

Abstract:

Proton imaging has become a key diagnostic for measuring electromagnetic fields in high-energy-density (HED) laboratory plasmas. Compared to other techniques for diagnosing fields, proton imaging is a measurement that can simultaneously offer high spatial and temporal resolution and the ability to distinguish between electric and magnetic fields without the protons perturbing the plasma of interest. Consequently, proton imaging has been used in a wide range of HED experiments, from inertial-confinement fusion to laboratory astrophysics. An overview is provided on the state of the art of proton imaging, including a discussion of experimental considerations like proton sources and detectors, the theory of proton-imaging analysis, and a survey of experimental results demonstrating the breadth of applications. Topics at the frontiers of proton-imaging development are also described, along with an outlook on the future of the field.