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@inproceedings{sun:ipac2021-thpab082,
author = {Y. Sun and M. Borland and G.I. Fystro and X. Huang and H. Shang},
title = {{Recent Operational Experience with Thermionic RF Guns at the APS}},
booktitle = {Proc. IPAC'21},
pages = {3959--3962},
eid = {THPAB082},
language = {english},
keywords = {gun, linac, operation, cathode, injection},
venue = {Campinas, SP, Brazil},
series = {International Particle Accelerator Conference},
number = {12},
publisher = {JACoW Publishing, Geneva, Switzerland},
month = {08},
year = {2021},
issn = {2673-5490},
isbn = {978-3-95450-214-1},
doi = {10.18429/JACoW-IPAC2021-THPAB082},
url = {https://jacow.org/ipac2021/papers/thpab082.pdf},
note = {https://doi.org/10.18429/JACoW-IPAC2021-THPAB082},
abstract = {{The electron beam at the Argonne Advanced Photon Source (APS) is generated from an S-band thermionic RF gun. There are two locations at the frontend of the linac where thermionic RF guns are installed – RG1 and RG2. Three so-called generation-III guns are available, two are installed at RG1 and RG2, one is a spare. In recent years, these guns are showing signs of aging after over a couple of decades of operations. RF trips started to occur, and we had to reduce the nominal operating rf power to alleviate the problem. In addition, beam generated by RG1 suffers from low transportation efficiency from the gun to the linac, and beam trajectory is unstable which results in charge instabilities. Recently, APS obtained a new type of prototype gun and it was beam commissioned in the linac. In this paper, we report our operational experience with these thermionic rf guns including thermionic-cathode beam extraction, gun front-end optimization for maximum charge transmission through the linac, linac lattice setup to match beam for injection into the Particle Accumulator Ring (PAR) and optimization for maximum PAR injection efficiency.}},
}