parameter[geometry] = Open            

parameter[p0c]                    = 100
parameter[particle]               = Electron
parameter[absolute_time_tracking]    = T

beginning[beta_a]   = 1
beginning[beta_b]   = 1

!-------------------------------------------------------

IN.MAR.BEG: Marker
slave_drift_1: drift, l = 0.044
slave_drift_2: drift, l = 0.0571875
slave_drift_3: drift, l = 0.047625
slave_drift_4: drift, l = 1.1875E-3
IN.A1.MAR.BEG: Marker
slave_drift_5: drift, l = 0.1544625
slave_drift_6: drift, l = 0.117475
slave_drift_7: drift, l = 0.2220625
slave_drift_8: drift, l = 2.0000000000001E-3
IN.A1.BUN01: RFcavity, alias = "RA1CTB01", grid_field = call::in.a1.bun01_1.grid_field,
   L = 0.2, RF_FREQUENCY = 1.3E9, VOLTAGE = 50000, PHI0_AUTOSCALE = 0.05491984095791,
   FIELD_AUTOSCALE = 19.538316899305, DS_STEP = 0.02, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_calc = FieldMap
slave_drift_9: drift, l = 0.014
slave_drift_10: drift, l = 0.2902625
slave_drift_11: drift, l = 0.117475
slave_drift_12: drift, l = 0.0112625
IN.A1.MAR.END: Marker
IN.CRMOD.MAR.BEG: Marker
slave_drift_13: drift, l = 0.181
slave_drift_14: drift, l = 0.34
IN.CRMOD.RFC01: Lcavity, grid_field = call::in.crmod.rfc01_1.grid_field, L = 0.484,
   RF_FREQUENCY = 1.3E9, GRADIENT = 2.040909526405E6, N_CELL = 2, DS_STEP = 0.0484,
   mat6_calc_method = Tracking, field_calc = FieldMap
IN.CRMOD.P1_2: Pipe, L = 0.449
IN.CRMOD.RFC02: Lcavity, grid_field = call::in.crmod.rfc02_1.grid_field, L = 0.484,
   RF_FREQUENCY = 1.3E9, GRADIENT = 2.040909526405E6, N_CELL = 2, DS_STEP = 0.0484,
   mat6_calc_method = Tracking, field_calc = FieldMap
IN.CRMOD.P2_3: Pipe, L = 0.232
IN.CRMOD.RFC03: Lcavity, grid_field = call::in.crmod.rfc01_1.grid_field, L = 0.484,
   RF_FREQUENCY = 1.3E9, GRADIENT = 2.040909526405E6, N_CELL = 2, DS_STEP = 0.0484,
   mat6_calc_method = Tracking, field_calc = FieldMap
IN.CRMOD.P3_4: Pipe, L = 0.449
IN.CRMOD.RFC04: Lcavity, grid_field = call::in.crmod.rfc02_1.grid_field, L = 0.484,
   RF_FREQUENCY = 1.3E9, GRADIENT = 2.040909526405E6, N_CELL = 2, DS_STEP = 0.0484,
   mat6_calc_method = Tracking, field_calc = FieldMap
IN.CRMOD.P4_5: Pipe, L = 0.232
IN.CRMOD.RFC05: Lcavity, grid_field = call::in.crmod.rfc01_1.grid_field, L = 0.484,
   RF_FREQUENCY = 1.3E9, GRADIENT = 2.040909526405E6, N_CELL = 2, DS_STEP = 0.0484,
   mat6_calc_method = Tracking, field_calc = FieldMap
IN.CRMOD.P5_E: Pipe, L = 0.718
IN.CRMOD.MAR.END: Marker
IN.A3.MAR.BEG: Marker
slave_drift_15: drift, l = 0.1769
slave_drift_16: drift, l = 0.0251
IN.A3.BPM01: Marker, alias = "A3BPC01"
slave_drift_17: drift, l = 0.1749
slave_drift_18: drift, l = 0.4108
slave_drift_19: drift, l = 0.2
slave_drift_20: drift, l = 0.2423
IN.A3.SDR01: Marker, alias = "A3SDR01"
slave_drift_21: drift, l = 0.128
IN.A3.BPM02: Marker, alias = "A3BPC02"
slave_drift_22: drift, l = 0.015
slave_drift_23: drift, l = 0.2
slave_drift_24: drift, l = 0.357
IN.A3.BPM03: Marker, alias = "A3BPC03"
slave_drift_25: drift, l = 0.044
slave_drift_26: drift, l = 0.177
IN.A3.MAR.END: Marker
DIAG_FORK: Fork, to_line = IN.B1
IN.B2.MAR.BEG: Marker
slave_drift_27: drift, l = 0.023
slave_drift_28: drift, l = 0.06
IN.B2.BEN01: Sbend, L = 0.32724923474894, G = 0.8, FRINGE_TYPE = Full,
   E2 = 0.26179938779915, INTEGRATOR_ORDER = 6, DS_STEP = 7.6104473197427E-3
IN.B2.L1_1A: Pipe, L = 0.096
slave_drift_29: drift, l = 0.6195
slave_drift_30: drift, l = 0.010499999999999
IN.B2.BPM01: Marker
slave_drift_31: drift, l = 0.06
slave_drift_32: drift, l = 0.080500000000001
slave_drift_33: drift, l = 0.0245
IN.B2.BEN02: Sbend, L = 0.32724923474894, G = -0.8, FRINGE_TYPE = Full,
   E1 = -0.13089969389957, E2 = -0.13089969389957, INTEGRATOR_ORDER = 6,
   DS_STEP = 7.6104473197427E-3
slave_drift_34: drift, l = 0.0265
slave_drift_35: drift, l = 0.0785
slave_drift_36: drift, l = 0.060000000000001
IN.B2.BPM02: Marker
slave_drift_37: drift, l = 0.012499999999999
slave_drift_38: drift, l = 0.4727
slave_drift_39: drift, l = 0.1016
slave_drift_40: drift, l = 0.043199999999999
IN.B2.L1_2B: Pipe, L = 0.105
IN.B2.BEN03: Sbend, L = 0.32724923474894, G = 0.8, FRINGE_TYPE = Full,
   E1 = 0.26179938779915, INTEGRATOR_ORDER = 6, DS_STEP = 7.6104473197427E-3
IN.B2.L1_3A: Pipe, L = 0.105
slave_drift_41: drift, l = 0.0337
IN.B2.BPM03: Marker
slave_drift_42: drift, l = 0.072700000000001
slave_drift_43: drift, l = 0.1016
slave_drift_44: drift, l = 0.5801
slave_drift_45: drift, l = 0.1016
slave_drift_46: drift, l = 0.1016
IN.B2.SLT1A: Marker
slave_drift_47: drift, l = 0.076699999999999
IN.B2.SLT1B: Marker
slave_drift_48: drift, l = 0.0572
slave_drift_49: drift, l = 0.1016
slave_drift_50: drift, l = 0.40985
slave_drift_51: drift, l = 0.1967
slave_drift_52: drift, l = 0.033300000000001
slave_drift_53: drift, l = 0.1967
slave_drift_54: drift, l = 5.8500000000006E-3
slave_drift_55: drift, l = 0.1016
slave_drift_56: drift, l = 0.0892
IN.B2.SLT2A: Marker
slave_drift_57: drift, l = 0.076000000000001
IN.B2.SLT2B: Marker
slave_drift_58: drift, l = 1.204
IN.B2.BPM04: Marker
slave_drift_59: drift, l = 0.46
slave_drift_60: drift, l = 0.096
IN.B2.VSC01: Marker
slave_drift_61: drift, l = 0.404
IN.B2.MAR.END: Marker
IN.MAR.END: Marker

!-------------------------------------------------------
! Overlays, groups, etc.

x__IN.GUN: null_ele
IN.GUN: E_Gun, superimpose, ele_origin = beginning, ref = x__IN.GUN,
   grid_field = call::in.gun_1.grid_field, L = 0.15, GRADIENT = 2E6, VOLTAGE = 300000,
   AUTOSCALE_PHASE = F, field_calc = FieldMap
x__IN.A1.PIP01: null_ele
IN.A1.PIP01: Pipe, superimpose, ele_origin = beginning, ref = x__IN.A1.PIP01, L = 0.496
x__IN.A1.SOL01: null_ele
IN.A1.SOL01: Solenoid, superimpose, ele_origin = beginning, ref = x__IN.A1.SOL01,
   grid_field = call::in.a1.sol01_1.grid_field, L = 0.6, BS_FIELD = 0.025331,
   mat6_calc_method = Tracking, tracking_method = Time_Runge_Kutta, field_calc = FieldMap,
   field_master = T
x__IN.A1.PIP02: null_ele
IN.A1.PIP02: Pipe, superimpose, ele_origin = beginning, ref = x__IN.A1.PIP02, L = 0.433
x__IN.CRMOD.PB_1: null_ele
IN.CRMOD.PB_1: Pipe, superimpose, ele_origin = beginning, ref = x__IN.CRMOD.PB_1,
   L = 0.521
x__IN.A1.SOL02: null_ele
IN.A1.SOL02: Solenoid, superimpose, ele_origin = beginning, ref = x__IN.A1.SOL02,
   grid_field = call::in.a1.sol01_1.grid_field, L = 0.6, BS_FIELD = -0.01661,
   mat6_calc_method = Tracking, tracking_method = Time_Runge_Kutta, field_calc = FieldMap,
   field_master = T
x__IN.A1.COR01: null_ele
IN.A1.COR01: Kicker, alias = "MA1CHA01_and_MA1CVA01", superimpose, ele_origin = beginning,
   ref = x__IN.A1.COR01, L = 0.047625, INTEGRATOR_ORDER = 2, DS_STEP = 0.047625,
   mat6_calc_method = Tracking, tracking_method = Time_Runge_Kutta, field_master = T
x__IN.A1.COR02: null_ele
IN.A1.COR02: Kicker, alias = "MA1CHB01_and_MA1CVB01", superimpose, ele_origin = beginning,
   ref = x__IN.A1.COR02, L = 0.117475, INTEGRATOR_ORDER = 2, DS_STEP = 0.117475,
   mat6_calc_method = Tracking, tracking_method = Time_Runge_Kutta, field_master = T
x__IN.A1.COR03: null_ele
IN.A1.COR03: Kicker, alias = "MA1CHB02_and_MA1CVB02", superimpose, ele_origin = beginning,
   ref = x__IN.A1.COR03, L = 0.117475, INTEGRATOR_ORDER = 2, DS_STEP = 0.117475,
   mat6_calc_method = Tracking, tracking_method = Time_Runge_Kutta, field_master = T
x__IN.A3.PIP01: null_ele
IN.A3.PIP01: Pipe, superimpose, ele_origin = beginning, ref = x__IN.A3.PIP01, L = 2.151
x__IN.A3.QUA01: null_ele
IN.A3.QUA01: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.A3.QUA01,
   L = 0.2, INTEGRATOR_ORDER = 2, field_master = T
x__IN.A3.QUA02: null_ele
IN.A3.QUA02: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.A3.QUA02,
   L = 0.2, INTEGRATOR_ORDER = 2, field_master = T
x__IN.A3.QUA03: null_ele
IN.A3.QUA03: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.A3.QUA03,
   L = 0.2, INTEGRATOR_ORDER = 2, field_master = T
x__IN.B2.ENDA3TOFIRSTBEND: null_ele
IN.B2.ENDA3TOFIRSTBEND: Pipe, superimpose, ele_origin = beginning,
   ref = x__IN.B2.ENDA3TOFIRSTBEND, L = 0.083000000000001
x__IN.A3.QUA04: null_ele
IN.A3.QUA04: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.A3.QUA04,
   L = 0.2, INTEGRATOR_ORDER = 2, field_master = T
x__IN.B2.PIP01: null_ele
IN.B2.PIP01: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B2.PIP01, L = 0.69
x__IN.B2.L1_1B: null_ele
IN.B2.L1_1B: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B2.L1_1B, L = 0.105
x__IN.B2.QUA01: null_ele
IN.B2.QUA01: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.B2.QUA01,
   L = 0.151, INTEGRATOR_ORDER = 2, DS_STEP = 0.151, field_master = T
x__IN.B2.L1_2A: null_ele
IN.B2.L1_2A: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B2.L1_2A, L = 0.105
x__IN.B2.PIP02: null_ele
IN.B2.PIP02: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B2.PIP02, L = 0.69
x__IN.B2.QUA02: null_ele
IN.B2.QUA02: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.B2.QUA02,
   L = 0.151, INTEGRATOR_ORDER = 2, DS_STEP = 0.151, field_master = T
x__IN.B2.COR01: null_ele
IN.B2.COR01: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR01,
   L = 0.1016, INTEGRATOR_ORDER = 2, DS_STEP = 0.1016, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.PIP03: null_ele
IN.B2.PIP03: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B2.PIP03, L = 4
x__IN.B2.COR02: null_ele
IN.B2.COR02: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR02,
   L = 0.1016, INTEGRATOR_ORDER = 2, DS_STEP = 0.1016, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.COR03: null_ele
IN.B2.COR03: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR03,
   L = 0.1016, INTEGRATOR_ORDER = 2, DS_STEP = 0.1016, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.COR04: null_ele
IN.B2.COR04: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR04,
   L = 0.1016, INTEGRATOR_ORDER = 2, DS_STEP = 0.1016, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.COR05: null_ele
IN.B2.COR05: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR05,
   L = 0.1967, INTEGRATOR_ORDER = 2, DS_STEP = 0.1967, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.COR06: null_ele
IN.B2.COR06: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR06,
   L = 0.1967, INTEGRATOR_ORDER = 2, DS_STEP = 0.1967, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.COR07: null_ele
IN.B2.COR07: Kicker, superimpose, ele_origin = beginning, ref = x__IN.B2.COR07,
   L = 0.1016, INTEGRATOR_ORDER = 2, DS_STEP = 0.1016, mat6_calc_method = Tracking,
   tracking_method = Time_Runge_Kutta, field_master = T
x__IN.B2.DUM01: null_ele
IN.B2.DUM01: Instrument, type = "BEAMSTOP", superimpose, ele_origin = beginning,
   ref = x__IN.B2.DUM01, L = 0.5, aperture = 0.3
x__IN.B1.PIP01: null_ele
IN.B1.PIP01: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B1.PIP01, L = 0.69
x__IN.B1.L1_1B: null_ele
IN.B1.L1_1B: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B1.L1_1B, L = 0.105
x__IN.B1.QUA01: null_ele
IN.B1.QUA01: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.B1.QUA01,
   L = 0.151, INTEGRATOR_ORDER = 2, DS_STEP = 0.151, field_master = T
x__IN.B1.L1_2A: null_ele
IN.B1.L1_2A: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B1.L1_2A, L = 0.105
x__IN.B1.PIP02: null_ele
IN.B1.PIP02: Pipe, superimpose, ele_origin = beginning, ref = x__IN.B1.PIP02, L = 0.69
x__IN.B1.QUA02: null_ele
IN.B1.QUA02: Quadrupole, superimpose, ele_origin = beginning, ref = x__IN.B1.QUA02,
   L = 0.151, INTEGRATOR_ORDER = 2, DS_STEP = 0.151, field_master = T
x__IN.B1.EXTRA_TO_MLC: null_ele
IN.B1.EXTRA_TO_MLC: Pipe, superimpose, ele_origin = beginning,
   ref = x__IN.B1.EXTRA_TO_MLC, L = 0.219, N_REF_PASS = 1
IN.B1.BEN03: Sbend, L = 0.32724923474894, G = -0.8, FRINGE_TYPE = Full,
   E1 = -0.26179938779915, N_REF_PASS = 1, INTEGRATOR_ORDER = 6,
   DS_STEP = 7.6104473197427E-3
IN.B1.L1_3A: Pipe, L = 0.105, N_REF_PASS = 1
IN.B1.BPM03: Marker
IN.B1.MAR.END: Marker
MA3QUA01: overlay = {IN.A3.QUA01[B1_GRADIENT]:current*field_int}, var = {CURRENT,
   FIELD_INT}, FIELD_INT                                = -3.35E-3
MA3CHD01: overlay = {IN.A3.QUA01[BL_HKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.4E-4
MA3CVD01: overlay = {IN.A3.QUA01[BL_VKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.46E-4
MA3QUA02: overlay = {IN.A3.QUA02[B1_GRADIENT]:current*field_int/.2}, var = {CURRENT,
   FIELD_INT}, FIELD_INT                                = -3.1E-3
MA3CHD02: overlay = {IN.A3.QUA02[BL_HKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.4E-4
MA3CVD02: overlay = {IN.A3.QUA02[BL_VKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.46E-4
MA3QUA03: overlay = {IN.A3.QUA03[B1_GRADIENT]:current*field_int}, var = {CURRENT,
   FIELD_INT}, FIELD_INT                                = -3.35E-3
MA3CHD03: overlay = {IN.A3.QUA03[BL_HKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.36E-4
MA3CVD03: overlay = {IN.A3.QUA03[BL_VKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.46E-4
MA3QUA04: overlay = {IN.A3.QUA04[B1_GRADIENT]:current*field_int}, var = {CURRENT,
   FIELD_INT}, FIELD_INT                                = -3.35E-3
MA3CHD04: overlay = {IN.A3.QUA04[BL_HKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.4E-4
MA3CVD04: overlay = {IN.A3.QUA04[BL_VKICK]:current*field_int}, var = {CURRENT, FIELD_INT},
   FIELD_INT                                = -2.46E-4

!-------------------------------------------------------
! Branch: IN.B1

IN.B1.MAR.BEG: Marker
IN.B1.ENDA3TOFIRSTBEND: Pipe, L = 0.083
IN.B1.BEN01: Sbend, L = 0.32724923474894, G = -0.8, FRINGE_TYPE = Full,
   E2 = -0.26179938779915, INTEGRATOR_ORDER = 6, DS_STEP = 7.6104473197427E-3
IN.B1.L1_1A: Pipe, L = 0.096
slave_drift_62: drift, l = 0.518
IN.B1.VSC01: Marker
slave_drift_63: drift, l = 0.112
IN.B1.BPM01: Marker
slave_drift_64: drift, l = 5.0000000000017E-4
slave_drift_65: drift, l = 0.0595
slave_drift_66: drift, l = 0.0915
slave_drift_67: drift, l = 0.0135
IN.B1.BEN02: Sbend, L = 0.32724923474894, G = 0.8, FRINGE_TYPE = Full,
   E1 = 0.13089969389957, E2 = 0.13089969389957, INTEGRATOR_ORDER = 6,
   DS_STEP = 7.6104473197427E-3
slave_drift_68: drift, l = 0.1017
slave_drift_69: drift, l = 3.3000000000001E-3
slave_drift_70: drift, l = 0.06
IN.B1.BPM02: Marker
slave_drift_71: drift, l = 0.0877
slave_drift_72: drift, l = 0.4463
IN.B1.COR01: Kicker
slave_drift_73: drift, l = 0.096
IN.B1.L1_2B: Pipe, L = 0.105
slave_drift_74: drift, l = 0.04
slave_drift_75: drift, l = 0.179

!-------------------------------------------------------

multi_line_01: line[multipass] = ( IN.B1.BEN03, IN.B1.L1_3A, x__IN.B1.EXTRA_TO_MLC,
   slave_drift_74, IN.B1.BPM03, slave_drift_75, IN.B1.MAR.END)

DIAG_LINE: line = ( IN.MAR.BEG, x__IN.GUN, slave_drift_1, x__IN.A1.SOL01, slave_drift_2,
   x__IN.A1.COR01, slave_drift_3, slave_drift_4, IN.A1.MAR.BEG, x__IN.A1.PIP01,
   slave_drift_5, x__IN.A1.COR02, slave_drift_6, slave_drift_7, slave_drift_8, IN.A1.BUN01,
   x__IN.A1.PIP02, slave_drift_9, x__IN.A1.SOL02, slave_drift_10, x__IN.A1.COR03,
   slave_drift_11, slave_drift_12, IN.A1.MAR.END, IN.CRMOD.MAR.BEG, x__IN.CRMOD.PB_1,
   slave_drift_13, slave_drift_14, IN.CRMOD.RFC01, IN.CRMOD.P1_2, IN.CRMOD.RFC02,
   IN.CRMOD.P2_3, IN.CRMOD.RFC03, IN.CRMOD.P3_4, IN.CRMOD.RFC04, IN.CRMOD.P4_5,
   IN.CRMOD.RFC05, IN.CRMOD.P5_E, IN.CRMOD.MAR.END, IN.A3.MAR.BEG, x__IN.A3.PIP01,
   slave_drift_15, x__IN.A3.QUA01, slave_drift_16, IN.A3.BPM01, slave_drift_17,
   slave_drift_18, x__IN.A3.QUA02, slave_drift_19, slave_drift_20, IN.A3.SDR01,
   slave_drift_21, IN.A3.BPM02, slave_drift_22, x__IN.A3.QUA03, slave_drift_23,
   slave_drift_24, IN.A3.BPM03, slave_drift_25, x__IN.A3.QUA04, slave_drift_26,
   IN.A3.MAR.END, DIAG_FORK, IN.B2.MAR.BEG, x__IN.B2.ENDA3TOFIRSTBEND, slave_drift_27,
   slave_drift_28, IN.B2.BEN01, IN.B2.L1_1A, x__IN.B2.PIP01, slave_drift_29, x__IN.B2.QUA01,
   slave_drift_30, IN.B2.BPM01, slave_drift_31, x__IN.B2.L1_1B, slave_drift_32,
   slave_drift_33, IN.B2.BEN02, x__IN.B2.L1_2A, slave_drift_34, x__IN.B2.QUA02,
   slave_drift_35, x__IN.B2.PIP02, slave_drift_36, IN.B2.BPM02, slave_drift_37,
   slave_drift_38, x__IN.B2.COR01, slave_drift_39, slave_drift_40, IN.B2.L1_2B, IN.B2.BEN03,
   IN.B2.L1_3A, x__IN.B2.PIP03, slave_drift_41, IN.B2.BPM03, slave_drift_42, x__IN.B2.COR02,
   slave_drift_43, slave_drift_44, x__IN.B2.COR03, slave_drift_45, slave_drift_46,
   IN.B2.SLT1A, slave_drift_47, IN.B2.SLT1B, slave_drift_48, x__IN.B2.COR04, slave_drift_49,
   slave_drift_50, x__IN.B2.COR05, slave_drift_51, slave_drift_52, x__IN.B2.COR06,
   slave_drift_53, slave_drift_54, x__IN.B2.COR07, slave_drift_55, slave_drift_56,
   IN.B2.SLT2A, slave_drift_57, IN.B2.SLT2B, slave_drift_58, IN.B2.BPM04, slave_drift_59,
   x__IN.B2.DUM01, slave_drift_60, IN.B2.VSC01, slave_drift_61, IN.B2.MAR.END, IN.MAR.END)

IN.B1: line = ( IN.B1.MAR.BEG, IN.B1.ENDA3TOFIRSTBEND, IN.B1.BEN01, IN.B1.L1_1A,
   x__IN.B1.PIP01, slave_drift_62, IN.B1.VSC01, slave_drift_63, IN.B1.BPM01, slave_drift_64,
   x__IN.B1.QUA01, slave_drift_65, x__IN.B1.L1_1B, slave_drift_66, slave_drift_67,
   IN.B1.BEN02, x__IN.B1.L1_2A, slave_drift_68, x__IN.B1.QUA02, slave_drift_69,
   x__IN.B1.PIP02, slave_drift_70, IN.B1.BPM02, slave_drift_71, slave_drift_72, IN.B1.COR01,
   slave_drift_73, IN.B1.L1_2B, multi_line_01)

IN.B1[geometry] = Open

use, DIAG_LINE