Title: ESPERIENZA%20di%20Commissioning%20a%20CDF
1ESPERIENZA di Commissioning a CDF
- Anna Maria Zanetti
- INFN Trieste
Bologna - 23 Novembre 2006
2CDF
Run I first data in 1985 (prehistoric
organization detector) ? not too
much to learn. (L 2 x 1031 cm-2 s-1 ) Run II
Official Start march 2001 almost New Detector!
(10-20xLrunI) From CDF I
solenoid, central calorimeter, part of muon system
- All the rest is NEW!
- Endplug Calorimeter
- Tracking
- -SiliconSVXII,ISL,Layer00
- -Central Outer Tracker
- Front End Electronics
- Trigger
- DAQ System
- Muon systems
- TOF
- Offline/Online Software
3La Sfida di LHC
La SFIDA di LHC
Energy 14 TeV 7 x Tevatron Length 27 km
4 x Tevatron Magnetic Field 8.3 T 2
x Tevatron Beam Energy 350 MJ 250 x
Tevatron Bunch Collisions 40 MHz 20 x
Tevatron Instantaneous Luminosity 60 x
Tevatron of Collisions in an event 10 x
Tevatron of Detector Channels 100 M 100 x
Tevatron of Scientists (2500/expt) 3 x
Tevatron
Tevatron proton-antiproton 7 accelerators
LHC proton-proton
LHC
4Commissioning CDFII
Tevatron LHC
Begin Cosmic Ray Run Commissioning Run with Partial Detectors Late 1999 2000 Oct. 2000 2006
Detector Completion Jan. 2001 Summer 2007
Commissioning Period Mar. 2001 - Feb. 2002 Nov 2007 (1 TeV) Start Spring 2008 (14TeV)
Beginning of Physics Run Feb. 2002 ?
but 2002 still struggling with fully
commissioning some detectors/electronics/software
and with problems in detectors and Beam.
5First Phase Late 1999-2000
- CDF non yet completed
- Integration of components into DAQ
- Daily running pedestals, calibration runs
- November 1999 Three system readout test (DAQ w/
multiple readout systems Calorimeter/TDC/Si DAQ - January 2000 L1 calorimeter trigger
established. Sum Et, Single tower, Missing Et
triggers - Cosmic Ray Running
- Once L1 trigger established, begin Timing-in of
Electronics - Across all detector subsystems, and across
trigger subsystems - Basic Level 3 filtering established
- Development of detector monitoring
- Calorimeter thresholds/noise rates
- A lot of work accomplished in debug and
commission all the trigger - systems and the Electronics
- Essential to be able to inject data/ read your
system, test it indipendently by the others and
in final environment
6Commission Trigger Electronics
- A lot accomplished with standalone test (no beam
or cosmics) - Take Silicon Vertex Tracker (SVT) as example
(100 custom VME boards - and a complex task) - but applies to all complex
trigger systems. - Note SVT was well thought on testing capability
and monitoring - the data flow on each board. Probably the best in
CDF - Independency from CDF DAQ (data driven device)
- Common data communication protocol
- Boards as building bricks that can be combined at
will (lego) - Can adapt SVT configuration to various test needs
- Ability to inject/read data from every board
- Can test most board functions with no additional
hardware - Software with board objects (ram, regs) in
common framework - Still it was not enough !!!
- System missing all these-gt struggle, building on
the fly - boards for testing purposes, suffered delays, etc
7..so what was missing?
- Plan for lack of input/output (done, but not
enough) - Must be able to test SVT in place, with proper
timing and data flow, even without
SVX/COT/L2/beam - Not only hw test, also operating/monitoring
software - More functions and flexibility for board/system
testing added on the road - Plan for long, demanding, integration/commissionin
g - Should have invested much more in software much
sooner - More features could be implemented
- More people easily trained (?less expert demand)
- When come to integrating electronics be
creative. - Any way to bypass/emulate other
system/boards must - be pursue and strongly looked for.
be creative
8First Phase Organization
- CDF has early established shifts/DAQ always
running ? once IN, a system must work and be
correctly monitored and checked - Sometimes testing activities not so easy.
- The payoff is a system kept working, running and
steady growing - Very important Fight hard the Entropy
- Train Shift Professionals ACEs. Stay in shift
for 3 monthes- overlap 1 monthes. CDF still works
this way.
9Begin Commissioning with Beam
- Oct 2000 Commissioning Run
- Si Barrel 4 only
- Many other systems partial
- COT recently on-line (seen 1st
- cosmics few days before roll-in)
- Nov. 2000-March 2001
- Complete the detector
- Continued integration work
- Daily cosmic running
- March 2001-February 2002
- Commission for physics data
Commiss.Run had some of everything enough to
shake down much of systems
10The Commissioning Run
Crucial event of CDF commissioning
Date 5/9 18/9
Ottobre 2000 Week -2
-1 0 1 2 3 4
5 6 Period Roll-in A
B C
Lum.
1029 1030
Bunches proton 1 x 8
1 x 8 36 x 8 36 x 36
- Period A Proton only beam (1.5 wks)
- Period B Observe first collision (1 wk)
- Period C Subsystem commissioning (3.5 wks)
Y.K. Kim/Sep.2000
11Commissioning Run Plan
- Period C (1x8, 36x8, 36x36 bunches)
- Understand operation of COT with colliding beam
- Stability of the chamber with a large amount of
ionization - Determine hit occupancies / efficiencies per
superlayer - Begin to understand tracking issues / t0, drift
velocity - Synchronous noise from Silicon readout ?
- Understand operation of Si Barrel-4, new
endplugs. - Commission calorimetry and muon systems.
- Commission DAQ system (Hardware Event Builder,
L3, Data Logger ) - Establish operation of L1 Trigger system
functionality - Calorimeter muon stubs triggers
- Tracking slice COT XFT XTRP to Muon /
Calorimeter - Capture data in L2 processors, simple
tagging/prescaling - Read-in L1 and XFT info, Cluster and ISO cluster
operation - SVT for instrumented region
- Take a few hundred k good events for the COT for
the post-run
Y.K. Kim/Sep.2000
12The First Collisions!!
L1
Beam profile Good Tracks
L2
Non dimentichiamo!! A volte pochi giorni di
collisioni producono risultati straordinari
Impulso alla collaborazione
13From the Commissioning Run
K short peak
SET500 GeV di-jets
Cambiare plots
- a lot of work accomplished
- and a better understood list of the work to be
done
Still 4 monthes to go Begin Run II March 01
14Downtime logger
- Detailed accounting of the reason CDF is not
taking data (loosing luminosity) - Very powerful tool to immediately identify what
systems are causing inefficiency (not always so
obvious) - Used by operation/commissioning manager to
prioritize and decide work schedules - Identify weakness/limitations of systems
15Silicon Commissioning
- Only prototype Si installed for commissioning run
- Allowed Si DAQ commissioning.
- Si readout did not cause noise problems
elsewhere. - BUT most of Silicon commissioning still to be
done! - Si was installed in Jan 2001 with just 2 months
to start of Run II (722K channels) - - shifts 24 hours a day, 7 days a week
- But Installation completed
- in May 2001 (beam in Mar 01)
- Access to collision hall restricted before
- connection completeschedule complicated
16E iniziato il run II..Commissioning with Data
- Early J/y data (few pb-1)
- basic momentum scale for tracking
- measure muon chamber efficiencies
- SVX vertex resolution
- Photon conversions used to
- understand the radial material
- distribution
August 2001 1pb-1
17Tracking Chamber Alignment
- Cosmic ray based alignment Cell tilts/shifts
- Includes corrections for electrostatics and
gravity
Impact parameter vs. phi
18First unexpected problems
- Early TeV beam had high losses
- Silicon frequently off for protection
- Muon chamber currents very high (installed
shielding) - Power supply failures with beam
- Transistor deaths due to single event burnout
- Reduced bias/more resistant transistors/shielding
- ISL cooling lines blocked
- Initially could not operate detector
- Blockage due to epoxy in 90o bends
- Cleared using Yag LASER prism
?Recovered June 02
19Beginning of Physics Run
- February 2002 is the START OF PHYSICS date
- Still 2002 was a painful year still a lot to
learn and improve - Unexpected problem in detectors
- Beam incidents
- Still in 2003
- The first run II paper published
D?,Ds???
?M 99.41?0.38?0.21 MeV PDG 99.2?0.5 MeV
20Silicon Jumper failure
Aging COT
A small but steadily growing number of CDF
silicon detector modules were dying. Breakage of
a wirebond
CDF central tracking chamber Aging ? resolved
- Some broke during a trigger test at 20 kHz
- Oriented orthogonal to 1.4 T B field
- Fundamental frequency for 2 mm
- Al bond 20 kHz
- Resonant oscillation from Lorentz forces during
special trigger conditions! - Reduced current through jumper
- Eliminated guilty trigger test mode
- Lost some sensors (z-side mainly)
Resolved!
21Beam Incidents CDF Safety
- Based on Run I experience
- Procedures for store fill and scrape, and store
end - hardware and procedures for minimizing radiation
dose to silicon detector intended to lengthen
life of detector - Measure losses from p and pbar bunches
- NOT ENOUGH !!
- Not well protected
against - beam incidents. A run II
news - LHC beam power 250 x Tevatron!
22Beam related Problems
- Very Serious
- Fast beam loss (risk was known, but..) Damage
Silicon - Damage to silicon from low doses (100s of rads)
at high rate (100 nsec) particular failure mode
not reproduced in tests - Serious
- Damage to various electronics in collision hall
due to SEB (single event burnout) or similar
single events ? abnormally high losses - One bad example beampipe misaligned during
access ? proton - halo scraped ? Lost 12 crate power supplies
over about an hour - Actions
- Added shielding around low-b quads
- Reduced bias voltage in VME power supplies /
modify power supplies - Annoying
- Example Beam induced background in missing ET
trigger ? halo scraping upstream of CDF
23Abort Kickers
- Kickers are very fast ? Danger of fast beam loss
- Kicker prefire
- Actions
- Reduce prefire rate (kicker conditioning)
- Add collimator for almost perfect shadowing ?
needed full latticeMARS simulation
A11 collimator Already in place
a task force in AD end 2004
A0 proton abort kickers
Add .5 m Collimator at A48 to shield against
prefires
24The Abort Gap
- Kickers fire correctly, but beam in the abort gap
- Discovered beam in the abort gap when quenched
and suffered silicon damage on abort! - Monitor the gap
- CDF added monitoring of local losses in abort gap
? useful diagnostic for accelerator adopted
jointly, in TevMon - Accelerator added better instrumentation adopted
jointly - Failure of specific Accelerator systems can spill
beam into the abort gap - Early incident RF problem drove significant beam
into abort gap ?1 of silicon detector lost
(unable to talk to chips) - Added beam abort interlock, monitored in TevMon
- Tevatron Electron Lens used to clean the abort
gap, monitored in TevMon
25(No Transcript)
26Important Lesson
- monitor state of potentially dangerous systems in
the accelerator - RF system, electron lens etc - Learned by analyzing each serious machine
accident - monitor the accelerator as if it were a detector
system
27Important Lesson
- Experiment must worry about its own safety and
work closely with Accelerator Division to ensure
it - CDF enjoyed good communications with AD
Operations Manager and Tevatron experts this is
important - Joint CDFAD instrumentation for monitoring
- Determine the cause of every serious beam
incident and take corrective action (bullet may
not miss you next time) - Corrective actions may require significant work
from the Accelerator Division
(quoting J. Spalding) - LHC
- LHC, ATLAS, CMS failure modes will not be the
same. - But potentially all loss issues will be more
severe - Importance monitoring, diagnostic tools,
collimater, - shielding, communication between machine and
exp. teams
28A Physics Heaven?a Very Complex Trigger!
29Trigger L
- Principle physics process trigger cross section,
s B (const) - Reality a trigger cross section, s A/L B
CL DL2 - CDF has worked a lot on trigger
- rates -gt still failed to correctly
- predict how they grow with L.
- It is a difficult task!
- A good trigger system allows one to easily
adopt - (CDF trigger has lot of features L enable,
Dyn.Presc. etc) - ?Still hard choices could be needed
(drop some physics) - ?Still one of the top CDF headaches today
-
MET252JET
30Trigger Summary
- A flexible trigger table handling is essential
to cope with the continuous changes and
increasing performance demand - Work to insert relevant physics channels in the
trigger table since the beginning. Late insertion
can turned to be painful - A very good trigger simulation is an essential
tool be sure all you need is in since early days
31and now Where can I run my jobs?
- While in the commiss. period (2001) it became
clear the Computing model for data analysis was
not good anymore. Needed CPU x10 painful tape
access -gt Old system trashed - 2002? a new model (CAF). In 6 monthes a small
CAF was working -gt In 1 year users enjoyed our
beloved CAF - ?First impact with data (and users) could destroy
all your planning -gt Dont panic there is some
time -gt A complete - revolution is possible and sometimes desirable
- Are CPU and human energy waisted? Yes - CDF did
not provide - simple tools to manage the analysis of large
datasets - strong set of easily available debugging and code
analysis tools - Motivation/organizations to more centralized
processing - When conference pressure-gt too late. Users find
their way
32Non manca molto al passaggio del testimone
- ? It is time to begin running together!
- Still CDF has his best years of physics
- production ahead. Should get 4 X Lint.
- CDF work for LHC in many areas (backgrounds, MC
tuning, QCD, Wtop mass etc) dont overlook the
possibility to learn something today of your
favorite physics channel. - Put your request on the table now but this does
not mean you will get it (manpower) The best
attitude do it yourself!
Why not begin to commission LHC using CDF ??
Join CDF as a Visitor you could play with
your favorite CDF data with no duties
33..ce il rischio (o la speranza!) che qualcuno
esageri un po
TEVATRON
LHC
Dont tell me you discovered Higgs!!
Cartoon courtesy of Young Kee Kim
Many thanks to Y.K.Kim, T. Liss, T.Liu, J.
Spalding and many others
34BACKUP
35Beam Loss Monitor snapshot for a messy abort
D0
low b quads
CDF
note CDF shields D0
abort dump
36Run II
37 Tevatron Run-II
- Data set has doubled every year
38Triggering in Run 2
45 kHz
300Hz
60 Hz 20MB/s
39Commissioning with Data
- Additional J/y data used to understand material
- And alignment
M(J/y) vs. Pt
Additional 0.455 g/cm2
Corrected for nominal material in simulation
No corrections
Residuals in 5 SVXII layers
40Abort Gap
- Tevatron has 3x12 bunch trains and 3 abort gaps
(2 ms long)
41Average Luminosity
0.9 fb-1
1E32cm-2s-1
By fiscal year