Dipole dataset v3

Version 3

There is a need to establish an exhaustive dataset covering all Common SPS supercycle configurations. We can find interesting events using the Injectors schedule 2024.

The following supercycle transitions have been identified in v3 datasets retrieval.

SFT to LHC

• SFTdy_x2 → SFTx2
• SFTx3 → SFT_LHC1
• SFTx3 → SFT_LHC1_SPARE_INDIVdy → SFT_LHC1_SPARE_INDIV
• SFTx2 → SFT_LHC4
• SFTx3 → SFT_LHC25NS
• SFTx3 → SFT_LHC3
• SFT_LHC3 → SFTdy_LHCINDIVdy
• SFT_LHC1 → SFTx3
• SFT_LHCINDIV → SFTx3
• SFT_LHC3 → SFTx3
• SFT_LHC25NS → SFTx3
• SFTdy_LHC25NS_SFT → SFTx2_LHC25NS
• SFT_LHC1_SPARE_INDIVdy → SFTx3

AWAKE

• SFTx3 → SFT_AWAKE

• SFTx3 → SFT_AWAKE1fu → SFT_AWAKE1

• SFT_AWAKE1___SFTx3

• SFT_LHC1 → SFT_AWAKE1

• SFT_LHCINDIV → SFT_AWAKE1

• SFT_AWAKE1 → SFT_LHCMD4

• SFT_AWAKE1___SFT_LHCINDIV

HiRadMat

• SFTx2_HIRADMT1 → SFTx2

• SFTx2 → SFTx2_HIRADMT1

• SFT_HIRADMT1 → SFTx2

• SFTx2_HIRADMT1 → SFT_LHC1

• SFTx2 → SFT_HIRADMT1

• SFTx3 → SFTx2_HIRADMT2

• SFT_HIRADMT2 → SFTx3

• SFT_HIRADMT2_MD1x2 → SFTx3

• SFTdy_HIRADMT2 → SFTdy_HIRADMT1

• SFT_HIRADMT2_MD1x2 → SFTx2_HIRADMT1

• SFT_HIRADMT1 → SFT_HIRADMT1_HIRADMT2

• SFT_HIRADMT2 → SFTdy_HIRADMT2 → SFT_LHCINDIV

• SFT_HIRADMT2 → SFTdy_LHCINDIV

• SFT_HIRADMT1 → SFT_HIRADMT2

• SFT_HIRADMT1 → SFT_HIRADMT2_MD1x2

• SFTx2_HIRADMT1 → SFT_LHC4

• SFT_LHC1 → SFTx2_HIRADMT1

• SFT_LHC3 → SFT_HIRADMT2_MD1x2_SFT

• SFT_LHCINDIV → SFT_HIRADMT1

• SFT_LHCINDIV → SFT_HIRADMT2

LHC supercycles

• LHCPILOTx3 → SFT_LHC25NS
• SFT_LHC3 → SFT_LHC1
• SFT_LHC1_SPARE_INDIVdy → SFT_LHC1
• SFT_LHC1dy → SFT_LHC1_SPARE_INDIVdy
• SFT_LHC1 → SFT_LHC1_SPARE
• SFT_LHC3 → SFT_LHC1_SPARE

Ion run

• SFTdy_x3 → SFTION1_LHCION2

• SFTION1dy_x2 → SFTION1x2

• SFTIONx2 → SFTION1_LHCION2

• SFTION1_SFT → SFTION1_ZERO_LHC2

• SFTION_LHC2_MD4 → SFTION_LHCION4_MD4

• SFTION2_ZERO_MD1 → SFTION2_MD1_ZEROx2

• SFTION_SFT → SFTION_LHC2

• SFTION1dy_SFT_MD2 → SFTION1_LHC2_MD2

MD supercycles

• SFT_MD → SFTx3 → SFTdy_x3

• SFTdy_MD1_MD3 → SFT_MD1_MD3

• SFT_AWAKE1 → SFT_AWAKE1_MD

• SFTdy_AWAKE1_MD3 → SFT_AWAKE1_MD3

• SFTdy_AWAKE1dy_MD3 → SFT_AWAKE1dy_MD3

• SFTdy_AWAKE1_MD → SFT_AWAKE1_MD

• SFT_LHC1_DYNECO_SPARE_INDIV → SFTPRO1_MD3_SFTPRO1_MD3

• SFT_LHC3 → LHCMD2_MD1

• SFT_LHCINDIV → SFT_AWAKE_LHCMD_SFT_AWAKE_MD

• SFT_AWAKE_LHCMD → SFT_LHCINDIVdy → SFT_LHCINDIV

• SFT_LHCMD1_MD1x2 → SFT_LHC3

• SFTdy_x3 → LHCMD1_LHC25NS_MD1

• SFT_LHCMD → SFT_AWAKE_LHCMD

• SFTSHIP_LHC3 → SFTSHIP_LHC1_MD1x2

• MD4_MD1_LHCPILOT_MD1 → SFT_LHCPILOT_MD1

• LHCMD2_MD1 → SFT_LHCINDIV

• LHCPILOT_MD3 → LHCPILOT_MD3_ZERO

• SFT_LHCPILOT_MD → SFT_LHC25NS_AWAKE1_SFTSHIP

• LHCPILOT_MDx2_ZERO → SFT_LHC3

Additional supercycles

We additionally use the

• SPS-BTRAIN-20231102-091712---20231102-092616_phys+lhcfill_zero_precycle_preprocessed.parquet
• SPS-BTRAIN-20231102-093421---20231102-094342_phys+lhcfill_md1_precycle_preprocessed.parquet
• SPS-BTRAIN-20231102-095113---20231102-104543_funky_preprocessed.parquet

for training

Validation

We validate on Dataset MD 2024-09-04, which is representative of a typical operation of the SPS.

Testing

We test on Dataset MD 2024-11-29, which has an unusual low energy SFTION cycle.

We also test on data from Dedicated MD 2024-10-09 with 3x SFTPRO and 1x LHC cycle.