Requirement Details
Electron Ion Collider
P-HSR-ATR-MAG-SEPT2.11
Requirement details, history, relationships and interfaces associated with requirement P-HSR-ATR-MAG-SEPT2.11
- CURRENT RECORD
- ARCHIVE RECORDS
- RELATIONSHIPS
- INTERFACES
Record Date: 10/10/2024 14:48 | |||
Identifier: | P-HSR-ATR-MAG-SEPT2.11 | WBS: | 6.05.03.01 |
Date Modified: | TBD: | FALSE | |
Status Date: | Status: | Reviewed | |
Description: | The dipole field B shall be 1.82415625 T | ||
Comments: |
No archive versions
Parents | |
F-HSR-INJ.2 | Hadron ring injection system, consisting of the transport beamline, septum magnet and injection kickers, shall be capable of transporting the 23.8 GeV proton bunch coming from the ATR line to IR4 central area and injecting it into the HSR. |
F-HSR-INJ.3 | For transporting hadron beam from AGS for injection to the HSR the Y-line part of the present ATR beamline shall be modified and extended with several dipole and quad magnets (as described in the CDR Table 3.56 and Figure 3.142) in order to connect it with inner 6-4 (present Blue Ring) superconducting arc [3]. The connection shall be done at 5 o’clock Q10 (05BQ10) quadrupole. |
F-HSR-MAG.2 | The magnets shall have the required field quality to meet the operational needs. |
F-HSR-MAG.1 | The magnets shall meet the requirements defined by the physics lattice.   |
F-HSR-MAG.4 | The maximum acceptable magnetic stray field at the beam pipe shall be TBD gauss. |
F-HSR.1 | The HSR proton beam shall be ramped from injection energy to an operation energy of up to 275 GeV. |
F-HSR.2 | The HSR shall be designed for changing beam optics between the relaxed state for injection to collision beam optics with beam in the machine. |
F-HSR.11 | The operational availability design target for the IR shall be consistent with the operational availability target for the overall EIC as set forth in [Electron-Ion Collider Global Requirements, EIC-ORG-PLN-010]Â |
Children | |
No children. |
This function not yet implemented.