theodoros argyropoulos€¦ · followed by a squeeze to 40 cm (m. solfaroli, lhcc#130) crossing...
TRANSCRIPT
Theodoros ArgyropoulosBeams Department
Operation Group
On behalf of the LHC team
LHCC 13.09.2017
LHC machine status report
3LHCC#131 - 13th Sep 2017
Outline
LHC Run 2017 Timeline
Scrubbing run
Main achievements
Main operational limitations
Performance
Summary/Next steps
4LHCC#131 - 13th Sep 2017
The LHC schedule (Apr-Sep 2017)
5LHCC#131 - 13th Sep 2017
The LHC schedule (Apr-Sep 2017)Reported by M. Solfaroli at the previous LHCC
Powering Test
+
Machine Checkout
Recommissioning
with Beam
6LHCC#131 - 13th Sep 2017
The LHC schedule (Apr-Sep 2017)Reported by M. Solfaroli at the previous LHCC
Powering Test
+
Machine Checkout
Recommissioning
with Beam
Today
7LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline1st Stable
Beams
First Stable Beams on Tue 23rd of May Only 25 days after first injection!
• 3b + 3b with intensity ~3x1011 protons per beam
8LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline1st Stable
Beams
First Stable Beams on Tue 23rd of May Only 25 days after first injection!
• 3b + 3b with intensity ~3x1011 protons per beam
Intensity Ramp up + commissioningMPS validations, aperture measurements, orbit setup, RF full detuning, crossing angle
anti-levelling, optics measurement of the 30 cm beta*, VdM cycle, collimator alignment,
Transverse Damper set up, roman pots alignment, beam stability, …
Intensity
ramp up
+
Commissio
ning
9LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline1st Stable
Beams
First Stable Beams on Tue 23rd of May Only 25 days after first injection!
• 3b + 3b with intensity ~3x1011 protons per beam
Intensity Ramp up + commissioningMPS validations, aperture measurements, orbit setup, RF full detuning, crossing angle
anti-levelling, optics measurement of the 30 cm beta*, VdM cycle, collimator alignment,
Transverse Damper set up, roman pots alignment, beam stability, …
Stable beams with 600 bunches before the start of the scrubbing run
Sc
rub
bin
gIntensity
ramp up
+
Commissio
ning
10LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline1st Stable
Beams
Intensity ramp up continued 2556 bunches before the MD1 run.
But multiple beam dumps on fast losses in IR7 (typically 10 - 20 ms risetime)
correlated by losses in cell 16L2
Sc
rub
bin
gIntensity
ramp up
+
Commissio
ning
Physics
Run
11LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline
Machine Development MD1 for 3 days followed by the first Technical stop (TS1)
Slow recovery for physics 2556 bunches back on Wed 19/07 but dumps due
to losses at 16L2
Local bump of 0.5 mm at cell 18L2 to maintain high current in the 16L2
correctors reduced the steady state losses smoother fills afterwards
MD2 with good availability followed by 2 days of VdM run and 600 bunches low-
mu run for ATLAS/CMS
Tech
nic
al
Sto
p1 Physics
Run
12LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline
Smooth run in the first week of August with 2556b and bumps in
Beam screen at 16L2 flushed with temperature increase at 80 K (10/08) known
procedure used already in the past
Result was not as expected difficulties in increasing the number of bunches, steps
back and forth with only maximum of ~1500b into Stable Beams
Tech
nic
al
Sto
p1 Physics
RunPhysics
Run
13LHCC#131 - 13th Sep 2017
LHC 2017 Run Timeline
New beam scheme of 8b4e injected at 04/09 reduced e-cloud effect
Smooth and continuous intensity ramp up with this beam up to 1916 bunches
(limit for this beam scheme) operate just above design peak luminosity
Only few dumps due to 16L2 losses up to now when tried to increase the
beam intensity above 1.21011 p/bunch on average promising for the rest of
the run
Tech
nic
al
Sto
p1 Physics
RunPhysics
Run
14LHCC#131 - 13th Sep 2017
Scrubbing run (6-11 June)
Scrubbing is the technique used to mitigate the electron cloud effect: high
intensity beam with short bunch spacing is used to “clean” the beam pipe surface
and reduce the secondary electrons emission.
E-cloud effects: beam degradation (blow-up, losses, instabilities), enhanced
heat-load on cryogenics, vacuum pressure rise, etc
Important for the LHC:
• Recovering from EYETS de-conditioning (as observed in 2016) (quick
process)
• Conditioning Sector 12 that has been exposed to air and the MKI2D
exchanged before the 2016 ion run
e-cloud
build-up for
LHC 25ns
beam
15LHCC#131 - 13th Sep 2017
Scrubbing run (6-11 June)
• 2820 bunches injected with total intensity 3.4 x1014 p/beam maximum at LHC
(setup needed both at injector and LHC, machine protection checks)
• Newly installed MKI2D conditioned quickly not limiting operation
• Heat-load at Sector 12 (vented during EYETS) reduced to 2016 levels
• No difficulty from the cryogenics side, instabilities well under control, improved
pumping in MKI areas (MKI8D limiting intensity at B2 in 2016)
The experience from 2015-16 and actions taken during EYETS clearly
beneficial
G. Iadarola et al. LMC 04/06/2017
16LHCC#131 - 13th Sep 2017
Main achievements
Enhanced Combined Ramp &
Squeeze (CRS) to reach 1 m β*
(IP1/IP5) at the end of the ramp,
followed by a squeeze to 40 cm (M.
Solfaroli, LHCC#130)
Crossing angle anti-levelling
operational
• Observed luminosity gain of 3-4 %
• Steps of -10 μrad at stable beams
after 2h, 4h, 8h
150 140 130 120 μrad
Energy vs β* in IP1/5/8
Fill 5872ATLAS Luminosity
M. Hostettler et al., LMC 28/06/2017
17LHCC#131 - 13th Sep 2017
Main achievements
LQQR
VP
8
2
0
Beam gone..
Minimal change in
power
RF full detuning fully operational since the 4th of June
• Power independent of the beam current
• Good agreement between measurements (RF, experiments) and
predictions (C. Schwick, J. Boyd, LMC 05/07/2017)
• Big step towards the HL-LHC era
P. Baudrenghien et al., LMC 05/07/2017
Main operation limitations: Losses@16L2Beam dumps due to losses at point 7 related to losses at 16L2
Possible reason: significant air inlet in 16L2 at the pumping port, used for the
first time during the EYETS. Same pump for both beam pipes (J. M. Jimenez,
LMC 23/08/2017)
Appeared already at injection during scrubbing run aperture
measurements showed no restrictions
MQ16L2
D. Mirarchi et al., LMC 14/06/2017
LHCC#131 - 13th Sep 2017 18
Main operation limitations: Losses@16L2
More frequent dumps while ramping up in intensity
Solutions in chronological order:
• Local bump of 0.5 mm at cell18L2 to keep current on the 16L2 ~3A
(dumps correlated to low orbit corrector current at 16L2)
smoother operation (fills with 2556 b)
• Warm up of beam screen at 16L2 (known procedure) difficult
to recover the performance (corrector current not helping)
• Reduced number of bunches and tried to ramp up slowly the
intensity Stability at ~1500bclear intensity dependence
• Change beam type to 8b4e (BCMS before) less e-cloud
activity
LHCC#131 - 13th Sep 2017 19
Main operation limitations: Losses@16L2 8b4e: reduced e-cloud (induced heat-load)
• Fast intensity ramp-up to 1916b without any dump with average
intensities 1.1x1011 p/b
• However could not increase intensity more than 1.2x1011 p/b
Study is ongoing with additional diagnostics in the cell
25ns 8b4eG. Iadarola Big
reduction in
the heat
load
LHCC#131 - 13th Sep 2017 20
Main operation limitations: Losses@16L2
25ns 8b4eG. Iadarola Big
reduction in
the heat
load
LHCC#131 - 13th Sep 2017 21
8b4e: reduced e-cloud (induced heat-load)
• Fast intensity ramp-up to 1916b without any dump with average
intensities 1.1x1011 p/b
• However could not increase intensity more than 1.2x1011 p/b
Study is ongoing with additional diagnostics in the cell
Main operation limitations:B2 dump During mid August, after a series of high intensity dumps following the
16L2 issue, the UD62 dump for B2 developed a nitrogen leak
Pack of 6 bottles installed and overpressure in the dump was reduced
to preserve the N2 flow as long as possible
Not critical for operation at the moment
The problem will be inspected and evaluated during TS2
S. Gilardoni et al., LMC 30/08/2017
LHCC#131 - 13th Sep 2017 22
Performance Machine Availability: 79.3 %
Stable beams: 34.6 %
Many faults due to beam loss (16L2)
Fault Duration [h]
Num
ber
of occurr
ences
60 faults due to
Beam Loss
34.6 %
Stable
Beams
1.7%
Precycle
21.7% in fault
(combining
overlapping )
42.0%
Operation
(other)
Data from: https://aft.cern.ch/dashboard
LHCC#131 - 13th Sep 2017 23
Performance
LuminosityRecord peak luminosity of
1.74x1034 cm-2s-1 (2556 b)
The slope seems to recover a bit after switching to 8b4e beam scheme.
LHCC#131 - 13th Sep 2017 24
Performance
LuminosityRecord peak luminosity of
1.74x1034 cm-2s-1 (2556 b)
Peak luminosities around 1.1 x1034 cm-2s-1 per fill with 1916 b of ~1.05x1011 p/bunch
Peak Luminosity zoom
LHCC#131 - 13th Sep 2017 25
8b4e
Performance Integrated Luminosity per fill for the last 1916b 8b4e beam show that we
can produce ~0.3 fb-1 in 10-11 hours.
With ~56 to 68% in stable beams we can reach the target of 45 fb-1 with
present beam conditions (12 days of 2.5 TeV run excluded)
J. Wenninger
Tight but
still on
track!
LHCC#131 - 13th Sep 2017 26
SummaryExcellent beginning of the Run
• 1st Stable Beams only 25 days after first injection
• Record peak Luminosity at 1.7x1034 cm-2s-1
Losses at 16L2 currently limiting operation
• Studies ongoing
• Solution during YETS
Alternative beam scheme of 8b4e less critical
• 1916 bunches with 1.05x1011 p/b
• Operation above design peak luminosity at
1.1 x1034 cm-2s-1
• The target integrated luminosity of 45 fb-1 is still
achievable.
• Possible intensity increase in the future (conditioning),
although difficult at the moment
LHCC#131 - 13th Sep 2017 27
28LHCC#131 - 13th Sep 2017
LHC Schedule
Around 11 weeks remaining
Next in schedule Continue with 8b4e at the current bunch intensities
• Possible attempts to gently increase intensity in the coming weeks
(after some conditioning?).
beta* reduction to 30 cm in preparation
• Run for the rest of 2017 and 2018 10% gain in integrated
Luminosity
• Decision to restart with 30 cm after TS2 will be taken at LMC
Preparation of special physics runs are ongoing
• High b* at 450 GeV and 2.51 TeV runs
Try to advance special runs currently planned for 2018 toward the
end of 2017 (?)
• No special runs in 2018 significant luminosity production to
satisfy the Run-2 targets (90 fb-1)
LHCC#131 - 13th Sep 2017 29
Thank you for your attention
LHCC#131 - 13th Sep 2017 30
BUCK UP SLIDES
31
32LHCC#131 - 13th Sep 2017
Spikes at 16L2
• Low number of spikes with 8b4e no spikes at all for the last few fills
• Increased number of spike in the fills with higher intensity (also on the
one after with reduced intensity)
• All dumps in the last period from Beam 1
8b4e
B. M. Salvachua Ferrando
33LHCC#131 - 13th Sep 2017
E-cloud with 8b4e Sector12
G. Iadarola
34LHCC#131 - 13th Sep 2017
Arc UFO rate in SB until 31/08/2017
M. AlbertTS #1 MD #2 BS heating
16L2Transf
P8
Performance
Comparing with 2016 run show a similar slope on the
integrated luminosity curve
LHCC#131 - 13th Sep 2017 35
36LHCC#131 - 13th Sep 2017
Machine Developments (MD1, MD2)The availability for both blocks reached resp. 85% and 90%. A wide variety of
exciting new results “at the forefront of accelerator R&D” was obtained, including:
• Successful ATS optics measurements and correction at low beta*
• Validation of the lower impedance of low impedance collimators for HL- LHC
• Diamond BLM calibration in IR6
• The effect of a direct compensation of the beam-beam compensation wire was
observed for the first time
• ADT gain impact on beam quality for high brightness bunches
• Channeling with crystal goniometers in beam 2
• Identification of UFO plane with diamond BLMs
• Scraping studies in view of addressing the case of a non-working dump
• Faster ramp by 110 s
• Instability thresholds with trains revealed unexpected instability in beam 1
horizontal
• Emittance exchange
• IR non-linearities studies
• Aperture measurements at 30 cm
• Landau damping measurement with BTF
Important tests for improving LHC performance
BCMS vs 8b4e
LHCC#131 - 13th Sep 2017 37
8b4e: 8 bunches & 4 empty buckets
(repeatedly)
• As mitigation scheme for electron cloud
in LHC
• 7 PSB injections double splitting at
2.5 GeV twice double splitting at 26
GeV/c
7x2x2x2 = 56 bunches
BCMS: Batch Compression, Merging &
Splitting
• 8 PSB injections Merging to 4
bunches triple splitting at 2.5 GeV
twice double splitting at 26 GeV/c
8/2x3x2x2 = 48 bunches
• For same LHC bunch intensity PSB
bunch intensity and transverse
emittance is ~50% of standard scheme