Title: Development of An Abort Gap Monitor for High-Energy Proton Rings
1Development of An Abort Gap Monitor for
High-Energy Proton Rings
- J.-F. Beche, J. Byrd, S. De Santis, P. Denes, M.
Placidi,W. Turner, M. Zolotorev
Lawrence Berkeley National Laboratory
2LHC Accelerator Research Program
Instrument under development at LBNL as part of
the US contribution to LHC. Historically, a
Longitudinal Density Monitor project spin-off
aimed to provide a reliable and simple device
suitable for being included in the LHC interlock
chain.
work in progress
3What is the Abort Gap and Reasons for Monitoring
It
- 3.3 ms gap in the machine fill, corresponding to
the raise time of the abort kicker. - Gap can populate by
- Injection errors (450 GeV, fast mechanism)
- Diffusion (mainly 7 TeV, slow mechanism)
- Debunching (mainly 7 TeV, slow mechanism)
- SC magnets quenching
4LHC Specifications(C. Fischer, LHC-B-ES-0005)
- Maximum allowable charge density 60 p/ps (4 104
p/ps) average over 100 ns _at_ 7 Tev (450 GeV). - Accuracy 50 (5) _at_ 7 TeV (450 GeV).
- Integration time 100 ms (1000 turns)
5Hamamatsu R5916U-50 Gated Photomultiplier Tube
Gate min. raise time 1 ns lt2.5 ns RF bucket
spacing Gate voltage 10 V Low voltage switching
required Gain at 3.4 kV 106 High gain lt 10
dark counts/sec Low noise Max duty cycle
1 100 ns -gt 100 kHz max sampling rate -gt 3 ms
to measure entire abort gap (w/o integration)
6Light Source in the LHC
Superconducting undulator (5T) _at_ IR4 Used for
both longitudinal and transverse
diagnostics. Possible permanent magnets undulator
dedicated to longitudinal diagnostics only. (R.
Jung M. Facchini)
7Tests at the ALS
(LHC parameters)
328 RF buckets 2761 filled
(280-620 ps)
Bunch width 50 ps
(2808/35640)
(2.5 ns)
Bunch spacing 2 ns
Camshaft pulse
120 ns gap
(no camshaft)
(3.3 µs)
8MCP-PMT experimental setup (old)
SROC
Hamamatsu Streak Trigger Unit
Stanford DG535 Delay
1.5 MHz
100 kHz
HP8114A Pulser
10 V Gate
MCP PMT
Visible Light
Tektronix TDS3052
Bending dipole
Hamamatsu C3360 HV
-3 kV
(neutral density filter)
9Gate signal on
10(No Transcript)
11Gate signal on
12MCP-PMT experimental setup (present)
SROC
Hamamatsu Streak Trigger Unit
Stanford DG535 Delay
1.5 MHz
100 kHz
HP8114A Pulser
10 V Gate
MCP PMT
Visible Light
Tektronix TDS754D
Hamamatsu C3360 HV
-3 kV
13Empty buckets (gap)
Regular bunches
Parasitic bunch
Camshaft
14Parasitic bunch
Gate signal on
Gate signal delayed 28 ns
Gate signal on
Parasitic bunches
15Gate signal on
Parasitic bunch
Last bunch in train
16MCP-PMT looks promising
- Can be easily switched at the required speed
- S/N ratio seems adequate
- Fast photocatode recovery (100s ps, Pockels
cell not required) - Can we simulate the expected LHC photon flux at
the ALS (10-5 ph/p) ? - MCP-PMT available in different bands. Which is
the most suitable for LHC ? - 100 ns integrating circuit ?
- Future test on the Tevatron (particularly for
unbunched beam)