Abstract

Novel laser-powered accelerating structures at the miniaturized scale of an optical wavelength [Formula: see text] open a pathway to high repetition rate, attosecond scale electron bunches that can be accelerated with gradients exceeding 1 GeV/m. Although the theoretical and computational study of dielectric laser accelerators dates back many decades, recently the first experimental realizations of this novel class of accelerators have been demonstrated. We review recent developments in fabrication, testing, and demonstration of these micron scale devices. In particular, prospects for applications of this accelerator technology are evaluated.

Highlights

  • Historical contextSince the first conceptualization of a laser-powered electron linear accelerator (linac) [1], various laser electron linac schemes have been proposed and demonstrated

  • We summarize the crucial technological developments and underlying physical principles of recently demonstrated microstructure dielectric laser accelerators (DLAs)

  • The motivation of the DLA is first outlined through the historical context of relevant scientific and technological developments

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Summary

Historical context

Since the first conceptualization of a laser-powered electron linear accelerator (linac) [1], various laser electron linac schemes have been proposed and demonstrated. Several experimental demonstrations have been made of electron acceleration by laser pulses at single-boundary structures, evading the Lawson-Woodward theorem [20,21,22,23,24] Such structures may prove useful as a diagnostic of femtosecond (and shorter) electron-photon interactions [25,26,27], they present practical difficulties in staging as a high-gradient laser-driven linear accelerator. The earliest proposal of a staged dielectric laser accelerator and focussing device was based on a periodic structure [31, 32] It employed absorptive thin metal gratings deposited onto flat dielectric surfaces. This structure functioned through the use of an amplitude mask with a period matching the wavelength of the incident electric field. DLAs have emerged at the interface of these blossoming technological developments

Microstructure geometries
Bragg mirrors
Slab geometry
Photonic band-gap structures
Grating structures
Plasmonic structures
Deflecting and focusing structures
Fundamentals of grating and pillar structures
Single grating
Dual grating
Dual pillars
Single grating demonstrations
Resonant structures
Dual pillar demonstrations
Two stage acceleration demonstrations
Potential applications
Medical therapy
Sub-optical cycle interaction
Attosecond photon generation
Beam position monitor
TeV-scale linear collider
Findings
Summary
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