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  • Open Access

Control of Nonlinear Compton Scattering in a Squeezed Vacuum

Antonino Di Piazza*

Kenan Qu

  • Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA and Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA

  • *Contact author: a.dipiazza@rochester.edu

Phys. Rev. Lett. 136, 085001 – Published 24 February, 2026

DOI: https://doi.org/10.1103/gswv-7st8

Abstract

Electromagnetic radiation by accelerated charges is a fundamental process in physics. Here, we introduce a quantum-optical framework for controlling the emission of radiation of an electron in an intense laser field via squeezed vacuum states. By engineering the quantum fluctuations of the emission modes, we demonstrate that the probability of nonlinear Compton scattering can be significantly enhanced or suppressed through tunable squeezing amplitude and angle. We show numerically that our predictions are experimentally accessible with current squeezing technologies, establishing a new paradigm for quantum control in high-intensity light-matter interactions.

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References (59)

  1. V. B. Berestetskii, E. M. Lifshitz, and L. P. Pitaevskii, Quantum Electrodynamics (Elsevier Butterworth-Heinemann, Oxford, 1982).
  2. C. Itzykson and J.-B. Zuber, Quantum Field Theory (McGraw-Hill Inc., New York, 1980).
  3. J. D. Jackson, Classical Electrodynamics (John Wiley & Sons, New York, 1975).
  4. L. D. Landau and E. M. Lifshitz, The Classical Theory of Fields (Elsevier, Oxford, 1975).
  5. W. Dittrich and M. Reuter, Effective Lagrangians in Quantum Electrodynamics (Springer, Heidelberg, 1985).
  6. E. S. Fradkin, D. M. Gitman, and Sh. M. Shvartsman, Quantum Electrodynamics with Unstable Vacuum (Springer, Berlin, 1991).
  7. V. N. Baier, V. M. Katkov, and V. M. Strakhovenko, Electromagnetic Processes at High Energies in Oriented Single Crystals (World Scientific, Singapore, 1998).
  8. V. I. Ritus, J. Sov. Laser Res. 6, 497 (1985).
  9. A. Di Piazza, C. Müller, K. Z. Hatsagortsyan, and C. H. Keitel, Rev. Mod. Phys. 84, 1177 (2012).
  10. T. G. Blackburn, Rev. Mod. Plasma Phys. 4, 5 (2020).
  11. A. Gonoskov, T. G. Blackburn, M. Marklund, and S. S. Bulanov, Rev. Mod. Phys. 94, 045001 (2022).
  12. A. Fedotov, A. Ilderton, F. Karbstein, B. King, D. Seipt, H. Taya, and G. Torgrimsson, Phys. Rep. 1010, 1 (2023).
  13. Apollon Research Infrastructure, https://apollonlaserfacility.cnrs.fr/en/home/.
  14. Central Laser Facility (CLF), https://www.clf.stfc.ac.uk/Pages/home.aspx.
  15. Center for Relativistic Laser Science (CoReLS), https://www.ibs.re.kr/eng/sub02_03_05.do.
  16. Extreme Light Infrastructure (ELI), https://eli-laser.eu/.
  17. Zettawatt-Equivalent Ultrashort pulse laser System (ZEUS), https://zeus.engin.umich.edu/.
  18. National Science Foundation Optical Parametric Amplifier Lines (NSF OPAL), https://nsf-opal.rochester.edu/.
  19. Station of Extreme Light (SEL), https://en.wikipedia.org/wiki/Station_of_Extreme_Light.
  20. Vulcan 20-20 upgrade, https://www.clf.stfc.ac.uk/Pages/Vulcan-2020.aspx.
  21. V. M. Malkin, G. Shvets, and N. J. Fisch, Phys. Rev. Lett. 82, 4448 (1999).
  22. N. J. Fisch and V. M. Malkin, Phys. Plasmas 10, 2056 (2003).
  23. K. Qu, I. Barth, and N. J. Fisch, Phys. Rev. Lett. 118, 164801 (2017).
  24. N. Zaïm, A. Sainte-Marie, L. Fedeli, P. Bartoli, A. Huebl, A. Leblanc, J.-L. Vay, and H. Vincenti, Phys. Rev. Lett. 132, 175002 (2024).
  25. H. Vincenti, Phys. Rev. Lett. 123, 105001 (2019).
  26. V. M. Malkin and N. J. Fisch, Phys. Rev. E 101, 023211 (2020).
  27. V. M. Malkin and N. J. Fisch, Phys. Rev. E 108, 045208 (2023).
  28. A. J. Gonsalves et al., Phys. Rev. Lett. 122, 084801 (2019).
  29. J. M. Cole et al., Phys. Rev. X 8, 011020 (2018).
  30. K. Poder et al., Phys. Rev. X 8, 031004 (2018).
  31. M. Mirzaie, C. I. Hojbota, D. Y. Kim, V. B. Pathak, T. G. Pak, C. M. Kim, H. W. Lee, J. W. Yoon, S. K. Lee, Y. J. Rhee, M. Vranic, Ó. Amaro, K. Y. Kim, J. H. Sung, and C. H. Nam, Nat. Photonics 18, 1212 (2024).
  32. E. E. Los et al., arXiv:2407.12071.
  33. M. Khalaf and I. Kaminer, Sci. Adv. 9, eade0932 (2023).
  34. M. Even Tzur, M. Birk, A. Gorlach, M. Krüger, I. Kaminer, and O. Cohen, Nat. Photonics 17, 501 (2023).
  35. M. E. Tzur, M. Birk, A. Gorlach, I. Kaminer, M. Krüger, and O. Cohen, Phys. Rev. Res. 6, 033079 (2024).
  36. D. Theidel, V. Cotte, R. Sondenheimer, V. Shiriaeva, M. Froidevaux, V. Severin, A. Merdji-Larue, P. Mosel, S. Fröhlich, K.-A. Weber, U. Morgner, M. Kovacev, J. Biegert, and H. Merdji, PRX Quantum 5, 040319 (2024).
  37. T. Kashiwazaki, T. Yamashima, K. Enbutsu, T. Kazama, A. Inoue, K. Fukui, M. Endo, T. Umeki, and A. Furusawa, Appl. Phys. Lett. 122, 234003 (2023).
  38. H. Vahlbruch, M. Mehmet, K. Danzmann, and R. Schnabel, Phys. Rev. Lett. 117, 110801 (2016).
  39. T. Ikeda, S. Kanno, and J. Soda, arXiv:2506.14354.
  40. S. Zeytinoğlu, A. İmamoğlu, and S. Huber, Phys. Rev. X 7, 021041 (2017).
  41. K. Qu and N. J. Fisch, Phys. Rev. E 110, 065211 (2024).
  42. K. Qu and N. J. Fisch, arXiv:2507.12288.
  43. W. H. Furry, Phys. Rev. 81, 115 (1951).
  44. L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge University Press, Cambridge, England, 2013).
  45. G. S. Agarwal, Quantum Optics (Cambridge University Press, Cambridge, England, 2013).
  46. See Supplemental Material at http://link.aps.org/supplemental/10.1103/gswv-7st8 for details on the Furry picture and its relation with the conventional interaction picture in the presence of a coherent state of photons.
  47. D. M. Volkov, Z. Phys. 94, 250 (1935).
  48. A. Di Piazza, Phys. Rev. D 97, 056028 (2018).
  49. J. Ying, X. He, D. Su, L. Zheng, T. Kroh, T. Rohwer, M. Fakhari, G. H. Kassier, J. Ma, P. Yuan, N. H. Matlis, F. X. Kärtner, and D. Zhang, Nat. Photonics 18, 758 (2024).
  50. J. Ying, L. Liu, L. Zheng, D. Su, X. He, J. Ma, H. Xuan, and D. Zhang, Phys. Rev. X 15, 021095 (2025).
  51. Z.-M. Sheng, K. Mima, J. Zhang, and H. Sanuki, Phys. Rev. Lett. 94, 095003 (2005).
  52. Z.-Y. Chen and A. Pukhov, Phys. Plasmas 22, 103105 (2015).
  53. H. Lu, J. Liu, J. Cai, X. Wu, J. Zhang, Q. Ma, Z. Wang, Y. Xia, W. Ma, C. Lin, Z. Nie, J. Yu, X. Xu, and X. Yan, Phys. Plasmas 32, 023104 (2025).
  54. A qualitatively new feature arises in the case of large recoil: whereas without squeezed field the spectrum vanishes in the limit k−→p− due to light-cone energy conservation, this is not the case with the squeezed field precisely due to the new contribution to the transition amplitude proportional to Mj,−(k,p).

  55. V. S. Popov, Sov. Phys. Usp. 47, 855 (2004).
  56. A. Di Piazza, M. Tamburini, S. Meuren, and C. H. Keitel, Phys. Rev. A 98, 012134 (2018).
  57. The polarization state of the emitted photon has been chosen to depend on the emission angle. However, for the chosen aperture cone, the polarization is approximately constant and along the x direction.

  58. M. Sennary, J. Rivera-Dean, M. ElKabbash, V. Pervak, M. Lewenstein, and M. T. Hassan, Light Sci. Appl. 14, 350 (2025).
  59. P.-K. Chen, I. Briggs, S. Hou, and L. Fan, Opt. Lett. 47, 1506 (2022).

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