Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper

A 56 MHz superconducting rf cavity was designed and installed in the Relativistic Heavy Ion Collider (RHIC). It is the first superconducting quarter wave resonator (QWR) operating in a high-energy storage ring. We discuss herein a design of the cavity and its key components and the cavity operation...

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Main Authors: Qiong Wu, Sergey Belomestnykh, Ilan Ben-Zvi, Michael M. Blaskiewicz, Thomas Hayes, Kevin Mernick, Freddy Severino, Kevin Smith, Alex Zaltsman
Format: Article
Language:English
Published: American Physical Society 2019-10-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.22.102001
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author Qiong Wu
Sergey Belomestnykh
Ilan Ben-Zvi
Michael M. Blaskiewicz
Thomas Hayes
Kevin Mernick
Freddy Severino
Kevin Smith
Alex Zaltsman
author_facet Qiong Wu
Sergey Belomestnykh
Ilan Ben-Zvi
Michael M. Blaskiewicz
Thomas Hayes
Kevin Mernick
Freddy Severino
Kevin Smith
Alex Zaltsman
author_sort Qiong Wu
collection DOAJ
description A 56 MHz superconducting rf cavity was designed and installed in the Relativistic Heavy Ion Collider (RHIC). It is the first superconducting quarter wave resonator (QWR) operating in a high-energy storage ring. We discuss herein a design of the cavity and its key components and the cavity operation with Au+Au collisions, and with asymmetrical Au+^{3}He collisions. The cavity is a storage cavity, meaning that it becomes active only at the energy of the experiment, after the acceleration cycle is completed. Without beam, the cavity reached 1.93 MV and a Q_{0} of 3.0×10^{8} after helium conditioning. The cavity voltage was limited at 300 kV with beam operation due to heating in the Higher Order Mode (HOM) coupler. With the cavity operating at 300 kV, an improvement in luminosity was detected from direct measurements, and the bunch length has been reduced. The uniqueness of the QWR necessitated development of an innovative design of the higher order mode dampers with high-pass filters, and a distinctive fundamental mode damper that enables the cavity to be transparent to the beam during acceleration.
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spelling doaj.art-b244939f26b640c88f660a54cc0e6e0a2022-12-21T19:25:57ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882019-10-01221010200110.1103/PhysRevAccelBeams.22.102001Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damperQiong WuSergey BelomestnykhIlan Ben-ZviMichael M. BlaskiewiczThomas HayesKevin MernickFreddy SeverinoKevin SmithAlex ZaltsmanA 56 MHz superconducting rf cavity was designed and installed in the Relativistic Heavy Ion Collider (RHIC). It is the first superconducting quarter wave resonator (QWR) operating in a high-energy storage ring. We discuss herein a design of the cavity and its key components and the cavity operation with Au+Au collisions, and with asymmetrical Au+^{3}He collisions. The cavity is a storage cavity, meaning that it becomes active only at the energy of the experiment, after the acceleration cycle is completed. Without beam, the cavity reached 1.93 MV and a Q_{0} of 3.0×10^{8} after helium conditioning. The cavity voltage was limited at 300 kV with beam operation due to heating in the Higher Order Mode (HOM) coupler. With the cavity operating at 300 kV, an improvement in luminosity was detected from direct measurements, and the bunch length has been reduced. The uniqueness of the QWR necessitated development of an innovative design of the higher order mode dampers with high-pass filters, and a distinctive fundamental mode damper that enables the cavity to be transparent to the beam during acceleration.http://doi.org/10.1103/PhysRevAccelBeams.22.102001
spellingShingle Qiong Wu
Sergey Belomestnykh
Ilan Ben-Zvi
Michael M. Blaskiewicz
Thomas Hayes
Kevin Mernick
Freddy Severino
Kevin Smith
Alex Zaltsman
Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
Physical Review Accelerators and Beams
title Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
title_full Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
title_fullStr Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
title_full_unstemmed Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
title_short Operation of the 56 MHz superconducting rf cavity in RHIC with higher order mode damper
title_sort operation of the 56 mhz superconducting rf cavity in rhic with higher order mode damper
url http://doi.org/10.1103/PhysRevAccelBeams.22.102001
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