Compensated Phase Jump at Transition Crossing in the CERN PS
The transition energy must be crossed in the CERN PS to accelerate proton and ion beams to flat-top energy. A phase jump of the accelerating RF voltage with respect to the phase of the bunches by about 180 degrees minus twice the synchronous phase is required at the instant of transition. This phase...
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description | The transition energy must be crossed in the CERN PS to accelerate proton and ion beams to flat-top energy. A phase jump of the accelerating RF voltage with respect to the phase of the bunches by about 180 degrees minus twice the synchronous phase is required at the instant of transition. This phase offset is injected into the beam phase loop which locks the phase of the vector sum of the RF voltage in the cavities to the beam. The polarities of the cavity return signal and of the stable phase programme are usually flipped at transition. However, both actions are difficult to perfectly synchronize in time, causing the beam phase loop to partially lock out and relock at the new stable phase. The resulting glitch can be avoided by well-controlled phase jumps applied to both, cavity drive and return signals simultaneously. This improved implementation of transition crossing makes it virtually transparent to the beam phase loop. The new scheme has been successfully tested with proton and ion beams, and it will become fully operational in the CERN PS after the long shutdown. |
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A phase jump of the accelerating RF voltage with respect to the phase of the bunches by about 180 degrees minus twice the synchronous phase is required at the instant of transition. This phase offset is injected into the beam phase loop which locks the phase of the vector sum of the RF voltage in the cavities to the beam. The polarities of the cavity return signal and of the stable phase programme are usually flipped at transition. However, both actions are difficult to perfectly synchronize in time, causing the beam phase loop to partially lock out and relock at the new stable phase. The resulting glitch can be avoided by well-controlled phase jumps applied to both, cavity drive and return signals simultaneously. This improved implementation of transition crossing makes it virtually transparent to the beam phase loop. The new scheme has been successfully tested with proton and ion beams, and it will become fully operational in the CERN PS after the long shutdown.</description><identifier>EISSN: 2331-8422</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>CERN ; Electric potential ; Holes ; Ion beams ; Phase transitions ; Protons ; Shutdowns ; Synchrotrons ; Time synchronization ; Voltage</subject><ispartof>arXiv.org, 2019-10</ispartof><rights>2019. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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This phase offset is injected into the beam phase loop which locks the phase of the vector sum of the RF voltage in the cavities to the beam. The polarities of the cavity return signal and of the stable phase programme are usually flipped at transition. However, both actions are difficult to perfectly synchronize in time, causing the beam phase loop to partially lock out and relock at the new stable phase. The resulting glitch can be avoided by well-controlled phase jumps applied to both, cavity drive and return signals simultaneously. This improved implementation of transition crossing makes it virtually transparent to the beam phase loop. 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A phase jump of the accelerating RF voltage with respect to the phase of the bunches by about 180 degrees minus twice the synchronous phase is required at the instant of transition. This phase offset is injected into the beam phase loop which locks the phase of the vector sum of the RF voltage in the cavities to the beam. The polarities of the cavity return signal and of the stable phase programme are usually flipped at transition. However, both actions are difficult to perfectly synchronize in time, causing the beam phase loop to partially lock out and relock at the new stable phase. The resulting glitch can be avoided by well-controlled phase jumps applied to both, cavity drive and return signals simultaneously. This improved implementation of transition crossing makes it virtually transparent to the beam phase loop. The new scheme has been successfully tested with proton and ion beams, and it will become fully operational in the CERN PS after the long shutdown.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><oa>free_for_read</oa></addata></record> |
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subjects | CERN Electric potential Holes Ion beams Phase transitions Protons Shutdowns Synchrotrons Time synchronization Voltage |
title | Compensated Phase Jump at Transition Crossing in the CERN PS |
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