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Asynchronous Beam Dump Studies C.Bracco, B.Goddard. Worst-case for 1 bunch with TCDQ position OK. Initial distribution: one bunch of 32’000 particles centered at 7.5 mm on TCDQ. - PowerPoint PPT Presentation
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Asynchronous Beam Dump Studies
C.Bracco, B.Goddard
Worst-case for 1 bunch with TCDQ position OK
Initial distribution: one bunch of 32’000 particles centered at 7.5 mm on TCDQ
Beam 2 tracked from TCDQ to TCTs in IP5, that is the most critical region for losses in case of asynchronous beam dump.
p+ Absorbed at: * TCTH* TCSG
* TCDQ
Worst-case: particles absorbed at collimators
626 seeds for scattering routine ~ 11E6 p+
Collimators set at the physical aperture (in mm) defined during beam based alignment
p+ Absorbed at: * TCTV
All the particles reaching the TCTH and TCTV have been scattered by the TCSG or grazed by the TCDQ (< 1%) no primary protons
TCTHTCTH TCSG TCSGTCDQ
TCTV
TCTV
Density of Particles at the TCTH Density [p/sigma]
x [sigma]
y [sigma]
Den
sity
[p/s
igm
a]
y [sig
ma]
x [sigma]
Den
sity
[p/s
igm
a]
• All losses come from p+ scattered through TCSG which fill acceptance with scattered primaries
• Total p+ on TCTH is 0.3% of single bunch (8% impacting TCSG in this simulation) or 3.3108 p+
• Peak p+ density is about 0.016% of single bunch (equivalent to 2.5106 p+ with nominal ex,y)
• Consistent with expectations - full bunch on TCSG would be attenuated by 10, and have 180 emittance increase
CollimatorsCold Magnets
Warm Magnets
TCDQ +TCSG
TCTH+TCTV
Loss Map for Beam 2, 3.5 TeV, 2m b* in IP5 From SixTrack simulations:
120
Local cleaning inefficiency: = h
# particles lost in Ds
Ds × Totabs
Ds = 10 cm @ magnetsDs = 1 m @ collimators (jaw length)Totabs = 8’463’489
Collimator N [p+] % Totabs
TCDQ 7’639’643 90
TCSG 697’298 8
TCTH 22’186 0.3
TCTV 875 0.01
Statistical error = 1/√N max = 0.03
Beam2
Only primary protons losses.
1 bunch case
Nominal bunch (1.1E11 p+):3.3E8 p+ on TCT(3e-3 ratio)
3.5 TeV, 2m b*, 2mm (=1σ) offset
IR6 saturatedIR7 15Gy/sTCTH.4R5.B2 0.6 Gy/s 2E7 p+
Leakage from TCDQ ~2E-2 from BLMs (but saturated).
Measured ~4e9 p+ with abort gap monitor (AGM) at moment of dump
Using abort gap population and, according to our assumptions, the leakage from TCDQ is ~2E-3
BSRA
Possible worst-case scenarios...
• During setup with beam at 3.5 TeV:o Single bunch hitting metal collimator
o Requires asynchronous dump/kicker pretrigger, PLUS ‘unlucky’ timing, PLUS collimator at correct phase to be exposed
o Any way for single bunch to hit triplet aperture??o Seems unlikely (TCDQ/TCSG should protect TCT, and this is inside triplet)o Should check carefully through details of setup procedure and see what asynch dump would give at each
stage
• During normal operation:o Multiple bunches hitting metal collimatoro Requires another ‘non standard’ error somewhere (orbit at TCDQ, or TCDQ/TCT position, ...)o Studied by T.Kramer in PhD thesis o Detailed results obtained for different TCDQ retractions (same as orbit error)
Impacts on metal collimators from asynch dump
'TCSG.6R7.B1'
'TCSG.D4L7.B1'
0,0E+00
2,0E+11
4,0E+11
6,0E+11
8,0E+11
1,0E+12
1,2E+12
1,4E+12
1,6E+12
8 8,5 9 9,5 10 10,5 11 11,5 12 12,5 13 13,5 14 14,5 15
# o
f lo
sses
TCDQ setting in sigma
'TCTH.4L2.B1'
'TCTH.4L1.B1'
'TCSG.D4L7.B1'
'TCSG.B5R7.B1'
'TCSG.A6L7.B1'
'TCSG.A4L7.B1'
'TCSG.6R7.B1'
'TCP.C6L7.B1'
'TCLA.C6R7.B1'
'TCLA.A7R7.B1'
7 TeV prefire dump case with0.5 m * and all LHC errors.
Work needed to give FLUKA input...
• Define machine parameters for study (b*, optical errors, orbit, setup errors, ...)o Already some issues here – make many runs with many different machines, to find average and worst case, or take
a typical case (but what is ‘typical’?)
• Choose failure case to give more ‘realistic’ input for FLUKA
o For setup, need to choose “worst” time in procedure to have asynch dumpo Check with tracking the impact parameters and distribution
o For operational scenarios, more difficult o Need some assumption on the “concurrent” failure at time of asynch dump – orbit, setup errors, ...o Not to forget the “multiple pre-trigger” cases which are still possible until 2013
o Also need not to forget the basic case with the transmission of particles through 1 stage cleaningo Should not have damage during “normal” asynch dump at 0.55 m b*
Conclusions
Asynchronous beam dump simulations for a single bunch at 3.5 TeV (2m b* in point 5) have been performed with SixTrack for beam 2 – all movable elements at nominal positions
Simulations show that losses at the TCT come from particles scattered at the TCSG (less than 1% from particles grazing the TCDQ), no losses of primary protons are observed
Simulations allow to visualize the distribution of particles absorbed at the TCT: peak density is equivalent of 0.016% of full bunch with nominal emittance
An asynchronous beam dump, performed for the same case (3.5 TeV, 2m b* in point 5), and losses (from PM) have been analyzed.
Measurements agreed well with simulations
For worst-case situations, need to carefully choose conditions AND methodology easier for setup scenarios beam experience for the operational scenarios? detailed input from both LBDS and COLL teams needed – then simple 1 turn tracking