Skip to content
naulon

No retraction, correction or concern found when last checked on Oct 24, 2026.

Terahertz-driven linear electron acceleration

Emilio A. Nanni, Wenqian R. Huang, Kyung-Han Hong and 5 more

Nature Communications · 2015 · CC BY

doi:10.1038/ncomms9486

Abstract

The cost, size and availability of electron accelerators are dominated by the achievable accelerating gradient. Conventional high-brightness radio-frequency accelerating structures operate with 30–50 MeV m −1 gradients. Electron accelerators driven with optical or infrared sources have demonstrated accelerating gradients orders of magnitude above that achievable with conventional radio-frequency structures. However, laser-driven wakefield accelerators require intense femtosecond sources and direct laser-driven accelerators suffer from low bunch charge, sub-micron tolerances and sub-femtosecond timing requirements due to the short wavelength of operation. Here we demonstrate linear acceleration of electrons with keV energy gain using optically generated terahertz pulses. Terahertz-driven accelerating structures enable high-gradient electron/proton accelerators with simple accelerating structures, high repetition rates and significant charge per bunch. These ultra-compact terahertz accelerators with extremely short electron bunches hold great potential to have a transformative impact for free electron lasers, linear colliders, ultrafast electron diffraction, X-ray science and medical therapy with X-rays and electron beams.

Full text

Its licence does not allow us to show the full text. Read it at PubMed Central:

Read at PubMed Central

References 38

  1. 1.

    Emma P. et al. First lasing and operation of an ångstrom-wavelength free-electron laser. Nat. Photon. 4, 641–647 (2010 ).

    Not in our library

  2. 2.

    Ishikawa T. et al. A compact X-ray free-electron laser emitting in the sub-angstrom region. Nat. Photon. 6, 540–544 (2012 ).

    Not in our library

  3. 3.

    Kilpatrick W. Criterion for vacuum sparking designed to include both rf and dc. Rev. Sci. Instrum. 28, 824–826 (1957 ).

    Not in our library

  4. 4.

    Wang J. & Loew G. in Proceedings of the 1989 IEEE (Particle Accelerator Conference, 1989. Accelerator Science and Technology) 1137–1139Stanford, CA, USA (1989 ).

    Not in our library

  5. 5.

    Forbes R. G. & Deane J. H. Reformulation of the standard theory of fowler–nordheim tunnelling and cold field electron emission. Proc. R. Soc. Lond. A 463, 2907–2927 (2007 ).

    Not in our library

  6. 6.

    Thompson M. et al. Breakdown limits on gigavolt-per-meter electron-beam-driven wakefields in dielectric structures. Phys. Rev. Lett. 100, 214801 (2008 ).

    Not in our library10.1103/physrevlett.100.214801

  7. 7.

    Geddes C. et al. High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding. Nature 431, 538–541 (2004 ).

    Not in our library10.1038/nature02900

  8. 8.

    Plettner T. et al. Visible-laser acceleration of relativistic electrons in a semi-infinite vacuum. Phys. Rev. Lett. 95, 134801 (2005 ).

    Not in our library10.1103/physrevlett.95.134801

  9. 9.

    Hafz N. A. et al. Stable generation of GeV-class electron beams from self-guided laser-plasma channels. Nat. Photon. 2, 571–577 (2008 ).

    Not in our library

  10. 10.

    Plettner T. & Byer R. Proposed dielectric-based microstructure laser-driven undulator. Phys. Rev. Spec. Top. Accel. Beams 11, 030704 (2008 ).

    Not in our library

  11. 11.

    Kneip S. et al. Near-GeV acceleration of electrons by a nonlinear plasma wave driven by a self-guided laser pulse. Phys. Rev. Lett. 103, 035002 (2009 ).

    Not in our library10.1103/physrevlett.103.035002

  12. 12.

    Varin C. & Piché M. Acceleration of ultra-relativistic electrons using high-intensity tm01 laser beams. Appl. Phys. B 74, s83–s88 (2002 ).

    Not in our library

  13. 13.

    Payeur S. et al. Generation of a beam of fast electrons by tightly focusing a radially polarized ultrashort laser pulse. Appl. Phys. Lett. 101, 041105 (2012 ).

    Not in our library

  14. 14.

    Peralta E. et al. Demonstration of electron acceleration in a laser-driven dielectric microstructure. Nature 503, 91–94 (2013 ).

    Not in our library10.1038/nature12664

  15. 15.

    Breuer J. & Hommelhoff P. Laser-based acceleration of nonrelativistic electrons at a dielectric structure. Phys. Rev. Lett. 111, 134803 (2013 ).

    Not in our library10.1103/physrevlett.111.134803

  16. 16.

    Carbajo S., Wong L. J., Nanni E., Schimpf D. N. & Kärtner F. X. in High Intensity Lasers and High Field Phenomena, HTu2C-6 Optical Society of America (2014 ).

    Not in our library

  17. 17.

    Faure J. et al. A laser-plasma accelerator producing monoenergetic electron beams. Nature 431, 541–544 (2004 ).

    Not in our library10.1038/nature02963

  18. 18.

    Yoder R. & Rosenzweig J. Side-coupled slab-symmetric structure for high-gradient acceleration using terahertz power. Phys. Rev. Spec. Top. Accel. Beams 8, 111301 (2005 ).

    Not in our library

  19. 19.

    Hebling J. et al. Optical manipulation of relativistic electron beams using Thz pulses. Preprint at http://arxiv.org/abs/1109.6852 (2011 ).

    Not in our library

  20. 20.

    Pálfalvi L., Fülöp J., Tóth G. & Hebling J. Evanescent-wave proton postaccelerator driven by intense thz pulse. Phys. Rev. Spec. Top. Accel. Beams 17, 031301 (2014 ).

    Not in our library

  21. 21.

    Wimmer L. et al. Terahertz control of nanotip photoemission. Nat. Phys. 10, 432–436 (2014 ).

    Not in our library

  22. 22.

    Schibli T. et al. Attosecond active synchronization of passively mode-locked lasers by balanced cross correlation. Opt. Lett. 28, 947–949 (2003 ).

    Not in our library10.1364/ol.28.000947

  23. 23.

    Huang S.-W. et al. High conversion efficiency, high energy terahertz pulses by optical rectification in cryogenically cooled lithium niobate. Opt. Lett. 38, 796–798 (2013 ).

    Not in our library10.1364/ol.38.000796

  24. 24.

    Reagan B. A. et al. Demonstration of a 100 hz repetition rate gain-saturated diode-pumped table-top soft X-ray laser. Opt. Lett. 37, 3624–3626 (2012 ).

    Not in our library10.1364/ol.37.003624

  25. 25.

    Zapata L. E. et al. Cryogenic yb: Yag composite-thin-disk for high energy and average power amplifiers. Opt. Lett. 40, 2610–2613 (2015 ).

    Not in our library10.1364/ol.40.002610

  26. 26.

    Klingebiel S. et al. in CLEO: Science and Innovations, STu4O-2 Optical Society of America (2015 ).

    Not in our library

  27. 27.

    Mitrofanov O., James R., Fernández F. A., Mavrogordatos T. K. & Harrington J. A. Reducing transmission losses in hollow thz waveguides. IEEE Trans. THz Sci. Technol. 1, 124–132 (2011 ).

    Not in our library

  28. 28.

    ANSYS HFSS. Academic Research, Release v15.0 (Ansys Inc., 2013).

    Not in our library

  29. 29.

    Young L. & Billen J. in Proceedings of the 2003 IEEE Particle Accelerator Conference (PAC 03) (The particle tracking code parmela) (Portland, Oregon, 2003).

    Not in our library

  30. 30.

    Wong L. J., Fallahi A. & Kärtner F. X. Compact electron acceleration and bunch compression in THz waveguides. Opt. Express 21, 9792–9806 (2013 ).

    Not in our library10.1364/oe.21.009792

  31. 31.

    Chen Z., Zhou X., Werley C. A. & Nelson K. A. Generation of high power tunable multicycle teraherz pulses. Appl. Phys. Lett. 99, 071102 (2011 ).

    Not in our library

  32. 32.

    Vicario C. et al. Generation of 0.9-mj thz pulses in dstms pumped by a Cr:Mg2SiO4 laser. Opt. Lett. 39, 6632–6635 (2014 ).

    Not in our library10.1364/ol.39.006632

  33. 33.

    Fülöp J. A. et al. in CLEO: Science and Innovations, SW1F-5 Optical Society of America (2014 ).

    Not in our library

  34. 34.

    Hong K.-H. et al. Generation of 287W, 5.5ps pulses at 78 MHz repetition rate from a cryogenically cooled Yb:YAG amplifier seeded by a fiber chirped-pulse amplification system. Opt. Lett. 33, 2473–2475 (2008 ).

    Not in our library10.1364/ol.33.002473

  35. 35.

    Grosjean T. et al. Linear to radial polarization conversion in the thz domain using a passive system. Opt. Express 16, 18895–18909 (2008 ).

    Not in our library10.1364/oe.16.018895

  36. 36.

    Miyagi M. & Kawakami S. Design theory of dielectric-coated circular metallic waveguides for infrared transmission. J. Lightwave Technol. 2, 116–126 (1984 ).

    Not in our library

  37. 37.

    Zalkovskij M. et al. Terahertz-induced kerr effect in amorphous chalcogenide glasses. Appl. Phys. Lett. 103, 221102 (2013 ).

    Not in our library

  38. 38.

    Harbold J. et al. Highly nonlinear as-s-se glasses for all-optical switching. Opt. Lett. 27, 119–121 (2002 ).

    Not in our library10.1364/ol.27.000119

Reads

Read by people on this page

None yet.

Checked or read by AI through naulon

None yet.

A person counts once a day per paper. We keep no cookie and no address: a reader is a hash that changes every day. Any month under five reads shows no number.

Are you an author?

Is this your paper?

Claim it to add your note and be paid when agents cite it. Free.