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Current Background Situation in BaBar

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Title: Current Background Situation in BaBar


1
Current Background Situation in BaBar
  • Always a concern, often an issue but never a
    showstopper
  • The background sources
  • (Synchrotron Radiation), Beam-Gas, Radiative
    Bhabbas , Beam-Beam effects, Radiation bursts,
    Injection, (Touscheck)
  • The background effects
  • integrated dose, instantaneous damage,
    operational issues, data quality
  • The background remediation strategy
  • Babar protection system, budget policy, forward
    looking to bottlenecks
  • using projection and simulations
  • Todays questions
  • Trickle injection
  • Injection quality
  • Preparation for tomorrow
  • Conclusion

2
The background sources
  • Synchrotron radiation very well masked, has
    never been a problem for BABAR
  • Beam-Gas BABAR sees debris from electromagnetic
    showers of scattered electrons and photons.
  • Two subcomponents Brems and Compton scattering
  • Well described by simulation
  • Efficient collimator scheme

3
The background sources (2)
  • Radiative Bhabbas
  • Showers debris from off-energy electrons or
    positrons after Bhabbas scattering swept away by
    magnetic elements in interaction regions
  • Beam-beam effects
  •  Trapped/Dust events  (HER specific)
  • Touschek effects not observed yet

4
Predictability score
  • Predictables sources
  • Synchrotron
  • Beam gas
  • Bremstralhung
  • Compton
  • Touschek
  • In principle predictable source
  • Radiatvie Bhabbas
  • Unreliably predictable sources
  • Beam-beam
  • Electron cloud effects
  • Injection doses
  • Unpredictable sources
  • Radiation bursts, dust events

5
Agressive PEP-II plans
Can BABAR keep up? Present headroom
limited! Historically, the same challenge has
always been met!
6
Background parametrization based on February 2002
data
The observed background is roughly twice larger
than the sum of the single beam contributions
7
DCH background history
M. Kelsey
8
Serious problem in DCH readout if nothing is done
9
Remediation and Forward looking of bottlenecks
  • Example of DIRC TDC
  • In 1999, we predicted that the single rate PMT
    in the DIRC would in 2002-2003 exceed the 200 kHz
    limit
  • A lot of effort to improve the shiedling
  • Launch design of a new TDC, implemented in summer
    2002 with a 2 MHz capability.
  • The 200 kHz limit was indeed reached in fall 2002
  • Next on line DCH read out!

10
DIRC main source of background Radiative Bhabhas
striking Q4 magnet inboard flange
  • Source discovered empirically with a Geiger
    counter.
  • Shielding erected step-by-step slowly building
    empirically a proof that things are improving.
  • A final shield erected in 2001, and the whole job
    completed in 2002.
  • Carsten proved later, with a Turtle program, that
    a major source of DIRC background is the
    radiative Bhabhas striking Q4 inboard flange,
    which is too small.

11
IFR issues
  • IFR is the only BABAR subdetector where the
    existing hardware capabilities are presently
    significantly degraded because of background
  • Layers 13, 15,16 turned off in the forward endcap
    (loss of factor 2 in the mu/pi rejection in that
    region)
  • IFR background comes losses near collimator
    BSC3042 which is very sensitive to beam-beam
    effects and thus very useful to the rest of
    BABAR
  • Must provide a shielding wall (summer 2004)

12
IFR issues
13
IFR and beam loss monitor
14
SVT Background from HER
HER sensitive SVT module (Does not have threshold
shift problem)
(BWMID)
Background almost doubled after move to
half-integer Again it has come down a bit
during run-4 Note peak occupancy is 150 higher
than average occupancy!
Moves toward half-integer
For occupancies in all SVT modules, see
http//www.slac.stanford.edu/babarsvt/SectionOcc
upancies.ps
15
SVT rates in 2003 compared to 2002 extrapolation
16
Single beam and lumi sensitivity
HER HER2 LER LER2 Lumi
SVT(mid) X Y 0
DCH 110 30 25 7 52
DRC 13 0 18 0 10
EMC 2.2 0 2.2 0 1.4
17
MID Plane Doses
Stable beam contribution of FWMID and BWMID is
overestimated
Damage in SVT modules starts
Run 34 dose is 40-60 of Run12 Luminosity is
55 of Run12
18
TOP Doses
Dominated by injection dose (up to 90)
Getting HER to trickle quality would provide
large gains
19
Summary of Detector sensivities and main issues
  • SVT Integrated Dose, Occupancy, single beam and
    beam-beam, FE electronics strange effects
  • DCH Readout capabilities, radiative Bhabbas
  • DIRC No problem for now, radaitive Bhabbas
  • EMC Integrated dose in Endcap for the long term,
    leakage current in Diodes (neutrons?), occupancy,
  • IFR Single rate for external layers, beam-beam
    effects
  • SVTRAD integrated dose, will need to be
    replaced soon
  • Integrated dose SVT 2Mrad in the most exposed
    regions, EMC 1 krad in the most exposed regions
  • Rather similar to what BELLE received ?

20
MID Dose Rates until 2009
Use Seeman model for beam currents to predict
dose rates
Dose rates do not looking forbiddingly high Rates
peak at roughly the current soft abort limits -
DQ should still be reasonable
21
Midplane Doses until 2009
  • Module exchange in 2005 looks well timed with 4
    Mrad budget
  • One rotation in 2007 should be able to keep MID
    modules installed in 2005 below 5 Mrad

A rotation will move the high dose in FEMID to
other module
22
BABAR scorecard July 2004
23
BABAR scorecard July 2006
24
Dose in calorimeter
25
BABAR scorecard 2009
26
Data quality issues in SVT
27
Resolution degration with occupancy
28
Example in
29
HER Injection Problems
30
Characterization of injection aborts/inhibits
BP / LP ODF
31
A variety of fast radiation spikes (stored beams)
B. Petersen G. Wormser
32
A variety of fast radiation spikes (stored beams)
B. Petersen G. Wormser
33
Run 4 Trip Summary
Average of 4 trips/day Run 3 average was 3
trips/day
A couple of aborts are due to broken thermistor
Only one other abort looked suspicious
Last two weeks average is down to almost 1
trip/day
34
Some exemple of  Dust events 
35
Trickle solved top of fill beam_beam effects
36
Revided simulation efforts
  • Locations of the sources of Lumi terms and
    possible shielding
  • Improvment of collimators locations
  • Validation of new IR design

37
Evidence for neutron radiation?
  • Diode leakage current in EMC read-out
  • IFR background ?
  • J. Vavra developped a neutron detector very
    insensitive to photons that will be placed
    shortly along the beam pipe

38
Conclusions for short term issues
  • We have to look far ahead Minimum 3 years
  • Look for worst case scenarios!
  • Look for end-product effects!
  • BABAR issues
  • Immediate concerns SVT ATOM chip, IFRForward
    endcap
  • Next on-line DCH DAQ
  • Longer term issues SVT and EMC in 2008
  • Changes in background issues
  • Beam-beam tails
  • injections
  • trapped events

39
Background issues for a Super B factory
  • Detector has to stay always on!
  • Detector Protection system can we get rid of
    it? If not, it has to stand 100 MRad
  • Avoid all detector susceptible to instantaneous
    damage
  • Once proper rad hard technology has been chosen,
    occupancy will become the next major issue
    ultra fast and hyper-segmented

40
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41
BABAR scorecard today
x(trickle)
X visible effect with non-zero impact -
visible effect with no impact ? yet unknown
fixed det
upgrade to fix a significant issue
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