page 1 Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99 Upgrade of the SPS injection kicker system MKP l Present system l Why do we need a new system? l Presentation of the new system l Status of the PFN l Status of the magnets l Magnetic field measurements l Changes to the layout of BA1 l Work in the coming shutdowns
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Upgrade of the SPS injection kicker system MKP · Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99 page 1 Upgrade of the SPS injection kicker system MKP l Present system l Why do we
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page 1Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Upgrade of the SPS injectionkicker system MKP
l Present systeml Why do we need a new system?l Presentation of the new systeml Status of the PFNl Status of the magnetsl Magnetic field measurementsl Changes to the layout of BA1l Work in the coming shutdowns
page 2Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Model of the present system
0 10 20 30 40 50longitudinal position@mD
-0.1
0
0.1
0.2
latnozirohnoitisop
@m D
Kicker layout: oldsetup Optics: standard Calculated 12-1 -1999 at 11:19Particle = fixedtpEmittance = 0.75 mm mraddpêp =0.0005Size of injected beam is 5 sigma.
page 3Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Present MKP system lay-out
page 4Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
MKP system requirementsBeam Injection
EnergyRise time Flat top Fall Time Ripple
LHCprotons
26 GeV/c < 220 ns 2.1 [µµs] machine3/11 full
< ±± 0.5 %
FixedtargetProtons
14 GeV/c <1000 ns 10.5 [µµs] 1.0 [µµs] < ±± 1.0 %
LHC ions 12.9GeV/c
< 115 ns 0.5 [µµs] machine3/11 full
< ±± 0.5 %
Fixedtargetions
12.9GeV/c
< 1000 ns 2.0 [µµs] 3.8 [µµs < ±± 1.0 %
Short rise time to keepPS bunch structure
Present kicker rise timeis more than 220 ns
Shorter rise time will beobtained by:- larger magnet impedance- shorter magnets
But:- extra magnets to have sufficient strength
Tighter !!
page 5Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Model of the new system for theLHC type proton beam
0 10 20 30 40 50longitudinal position@mD
-0.1
0
0.1
0.2
latnozirohnoitisop
@mD
Kicker layout: tank3two17 Optics: standard Calculated 12-1 -1999 at 14:3Particle = LHCpEmittance = 0.11 mm mraddpêp =0.0011Size of injected beam is 5 sigma.
page 6Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
New system for the fixed target protonbeam: don’t use fourth tank!
0 10 20 30 40 50longitudinal position@mD
-0.1
0
0.1
0.2
latnozirohnoitisop
@m D
Kicker layout: tank3two17 Optics: standard Calculated 12-1 -1999 at 12:13Particle = fixedtpEmittance = 0.75 mm mraddpêp =0.0005Size of injected beam is 5 sigma.
In this case MKP4has to produce amaximum pulselength of 2.1 µs instead of 10.5 µs
page 7Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
New system: dumped ion beamTightest on clearance
0 10 20 30 40 50longitudinal position@mD
-0.1
0
0.1
0.2
latnozirohnoitisop
@m D
Kicker layout: tank3two17 Optics: standard Calculated 12-1 -1999 at 14:20Particle = ionsEmittance = 0.8 mm mraddpêp =0.00015Size of injected beam is 5 sigma.
page 10Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Status of the MKP PFNsl 1.5 m long test coil made. Impedance checked: within 1 %.
l One PFN assembled with this test coil. Low voltagemeasurements with low power switch.
l Comparison of measurements and calculations» HV measurement of MKA switch characteristics ->
adaptation of the low power switch
» Adaptation of front cells
l Coming soon:» High voltage tests with this PFN» Adaptation of the front cells» Long coils, three different diameters to compensate
for resistive losses
l Still a lot of work to do!
page 11Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Status of the MKP magnets I
page 12Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Status of the MKP magnets II
l One prototype S-type magnet finished» High voltage measurement with PFL in air» Fast inductive and capacitive probes developed» Will have to be disassembled and modified for final version
l First ‘LS magnet’ should be under vacuum in 4 weeks time» Damping resistors
» Incorporated magnetic field probes →» Outgassing tests of ferrites
l New baseplates, frames etc.
l Production of second LS module started
l Series started, another 18 magnets to go!
page 13Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Magnetic field probes
l Fast risetime and small ripple of magnetic fieldrequired
l New probes developed to measure this accurately» Inductive probe (two shielded coax cables) in the aperture:
most accurate, but can’t install this in the machine
» Capacitive pick-ups incorporated in the earth connectionplates
– Stays in the machine to check magnet and PFNs– Calibrated with inductive pick-ups
page 14Jan Uythoven SL/BT. Group meeting 9 Nov. ‘99
Results from the two different types ofmagnetic field probes
Capacitive pick −up incorporated , temporary shielding . Input filter on switch . Scaling factor 1.003Tek00006 .csv measured 4−11−1999 at 17:16Tek00009 .csv measured 4−11−1999 at 17:22Calculated 5−11−1999 at 14:36
-1. ×10 - 7 0 2.5 ×10 - 7 5.×10 - 7
0.92
0.94
0.96
0.98
1
1.02
1.04
Tek00006 .csv − Tek00007 .csv Hred L andTek00008 .csv − Tek00009 .csv Hblue L