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Beam-loss detection for the high-rate superconducting upgrade to the SLAC Linac Coherent Light Source

Alan S. Fisher, Christine I. Clarke, Bryce T. Jacobson, Ruslan Kadyrov, Evan Rodriguez, Mario Santana Leitner, Leonid Sapozhnikov, and James J. Welch
Phys. Rev. Accel. Beams 23, 082802 – Published 14 August 2020
An article within the collection: IBIC 2019 Conference Edition

Abstract

The Linac Coherent Light Source (LCLS) x-ray free-electron laser is driven by the third kilometer of the 3-km SLAC linac, which accelerates electrons in normal-conducting copper cavities pulsed at 120 Hz. The first kilometer is being replaced by LCLS-II, a superconducting (SC) electron linac driven by continuous rf at 1.3 GHz and with a normal-conducting photocathode gun using continuous rf at a subharmonic, 186 MHz. Its 4-GeV, 120-kW beam has a 1-MHz maximum rate, with an upgrade to 8 GeV in planning. The beam from either linac can be switched pulse by pulse to either of two new undulators, to generate hard and soft x rays. Control of beam loss is critical for machine and personnel safety. Previous SLAC protection systems have depended on ionization chambers, including both local devices at expected loss sites and long gas-dielectric coaxial cables providing distributed coverage. These devices are unsuited to the SC-linac beam, because their ion collection time, over 1 ms, may allow the space charge of accumulated ions to null the electric field inside the detector, blinding it to an increase in loss. Instead, both the local and the distributed detectors have been replaced with faster devices. The full 4 km will be spanned by multiple radiation-hard optical fibers in lengths of up to 200 m, each coupled to a photomultiplier tube, to capture Cherenkov light from loss showers. These are supplemented by single-crystal diamond detectors at expected loss sites. Signals are integrated with a 500-ms time constant; the beam is stopped within 200μs if a threshold is exceeded. We report on our extensive tests of the detectors and the new signal processing.

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  • Received 18 March 2020
  • Accepted 16 July 2020

DOI:https://doi.org/10.1103/PhysRevAccelBeams.23.082802

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Accelerators & Beams

Collections

This article appears in the following collection:

IBIC 2019 Conference Edition

A collection of articles that expand upon original research presented at the IBIC 2019 International Beam Instrumentation Conference (IBIC 2019) (September 8-12, 2019, Malmö Sweden).

Authors & Affiliations

Alan S. Fisher*, Christine I. Clarke, Bryce T. Jacobson, Ruslan Kadyrov, Evan Rodriguez, Mario Santana Leitner, Leonid Sapozhnikov, and James J. Welch

  • SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA

  • *Corresponding author. afisher@slac.stanford.edu

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Issue

Vol. 23, Iss. 8 — August 2020

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