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Classical and quantum beam dynamics simulation of the RF photoinjector test bench

A. S. Dyatlov, A. V. Afanasyev, V. V. Kobets, A. E. Levichev, M. V. Maksimov, D. A. Nikiforov, M. A. Nozdrin, K. Popov, K. A. Sibiryakova, K. E. Yunenko, D. V. Karlovets

TL;DR

This work combines classical and quantum beam-dynamics simulations to assess a dedicated S-band RF photoinjector test bench at JINR for generating high-quality, low-emittance electron beams and preserving intrinsic orbital angular momentum. Using ASTRA with Dowell–Schmerge photoemission, the authors optimize injection phase and employ an emittance-compensation solenoid to achieve a final normalized emittance of $3.2\pi\ \mathrm{mm\,mrad}$ at $Q=0.63\ \mathrm{pC}$, while demonstrating robust operation despite RF-induced phase-space distortions. In parallel, they model single-electron Laguerre-Gaussian states with OAM up to $\ell=64\hbar$ and show that acceleration in both DC and RF fields substantially suppresses transverse quantum spreading, preserving the radial OAM structure up to multi-MeV energies. The results indicate the test bench can support forthcoming experimental studies of relativistic vortex electrons, with commissioning underway and plans to incorporate collective effects in future work. $\varphi_0 \approx 180^{\circ}$ and a gradient of $45\ \mathrm{MV/m}$ are key operational parameters, and the final emittance target is $3.2\pi\ \mathrm{mm\,mrad}$ for $Q=0.63\ \mathrm{pC}$.

Abstract

We present beam-dynamics simulations for an S-band RF photoinjector test bench under development at the Joint Institute for Nuclear Research. The facility is intended to produce high-quality electron beams and to enable future generation of relativistic vortex electrons carrying quantized orbital angular momentum (OAM). Simulations of a 1.5-cell RF photogun operating at the currently available accelerating gradient of 45 MV/m demonstrate stable bunch formation at low bunch charge (Q = 0.63 pC), where space-charge effects are weak and the transverse emittance is primarily determined by RF-induced correlations. Optimization of the injection phase and the cathode-region solenoid field results in a robust emittance-compensated regime, yielding a final normalized emittance of 3.2 pi mm mrad. To evaluate the prospects for accelerating vortex electron beams, we further model the quantum evolution of single-electron Laguerre-Gaussian wave packets. The simulations show that acceleration to the multi-MeV energy range significantly suppresses free-space wave-packet spreading and preserves the initial OAM structure, indicating that the proposed test bench provides suitable conditions for forthcoming experimental studies of relativistic vortex electrons.

Classical and quantum beam dynamics simulation of the RF photoinjector test bench

TL;DR

This work combines classical and quantum beam-dynamics simulations to assess a dedicated S-band RF photoinjector test bench at JINR for generating high-quality, low-emittance electron beams and preserving intrinsic orbital angular momentum. Using ASTRA with Dowell–Schmerge photoemission, the authors optimize injection phase and employ an emittance-compensation solenoid to achieve a final normalized emittance of at , while demonstrating robust operation despite RF-induced phase-space distortions. In parallel, they model single-electron Laguerre-Gaussian states with OAM up to and show that acceleration in both DC and RF fields substantially suppresses transverse quantum spreading, preserving the radial OAM structure up to multi-MeV energies. The results indicate the test bench can support forthcoming experimental studies of relativistic vortex electrons, with commissioning underway and plans to incorporate collective effects in future work. and a gradient of are key operational parameters, and the final emittance target is for .

Abstract

We present beam-dynamics simulations for an S-band RF photoinjector test bench under development at the Joint Institute for Nuclear Research. The facility is intended to produce high-quality electron beams and to enable future generation of relativistic vortex electrons carrying quantized orbital angular momentum (OAM). Simulations of a 1.5-cell RF photogun operating at the currently available accelerating gradient of 45 MV/m demonstrate stable bunch formation at low bunch charge (Q = 0.63 pC), where space-charge effects are weak and the transverse emittance is primarily determined by RF-induced correlations. Optimization of the injection phase and the cathode-region solenoid field results in a robust emittance-compensated regime, yielding a final normalized emittance of 3.2 pi mm mrad. To evaluate the prospects for accelerating vortex electron beams, we further model the quantum evolution of single-electron Laguerre-Gaussian wave packets. The simulations show that acceleration to the multi-MeV energy range significantly suppresses free-space wave-packet spreading and preserves the initial OAM structure, indicating that the proposed test bench provides suitable conditions for forthcoming experimental studies of relativistic vortex electrons.

Paper Structure

This paper contains 10 sections, 19 equations, 18 figures, 1 table.

Figures (18)

  • Figure 1: Assembled RF photoinjector test bench during commissioning. The main components are indicated: RF gun, emittance-compensation solenoid, focusing solenoid, steering magnet, RF waveguide, UV laser transport line, vacuum mirror, and beamline.
  • Figure 2: Internal geometry of the S-band RF photogun. The design consists of 1.5 accelerating cells operating in the $\pi$-mode at 2856 MHz. The central aperture serves both for laser injection and electron beam extraction.
  • Figure 3: Simulated axial distribution of the accelerating electric field along the beam propagation axis $z$, obtained using eigenmode analysis in CST Microwave Studio.
  • Figure 4: Mechanical layout and positioning of the emittance compensation solenoid along the beamline.
  • Figure 5: Measured axial magnetic field distribution of the emittance compensation solenoid. The measurement was carried out in 5 mm steps along the $z$-axis using a magnetic field meter with a coil current of 20 A.
  • ...and 13 more figures