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LCcal: a Calorimeter prototype for future Linear Colliders

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Contributors (Como, ITE-Warsaw, LNF, Padova, Trieste): M. ... Miscetti, B.Nadalut, M. Nicoletto, M. Prest, R. Peghin, L. Ramina, F. Simonetto, E. Vallazza ... – PowerPoint PPT presentation

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Title: LCcal: a Calorimeter prototype for future Linear Colliders


1
LCcal a Calorimeter prototype for future
Linear Colliders
TALK SUMMARY
  • Design principles
  • Prototype description
  • Construction details
  • Test Beam results
  • Conclusions and Future plans

Contributors (Como, ITE-Warsaw, LNF, Padova,
Trieste) M. Alemi, A.Anashkin, M. Anelli,
M.Bettini, S.Bertolucci, E. Borsato, M. Caccia,
P.C, C. Fanin, J.Marczewski, S. Miscetti,
B.Nadalut, M. Nicoletto, M. Prest, R. Peghin, L.
Ramina, F. Simonetto, E. Vallazza .
2
Design principles
From the LC Physics requirements
Tesla TDR solutions
  • Si W
  • Shashlik (thanks to CALEIDO)
  • Cristals
  • Fully compensating EcalHcal

Alternatives
Proposed solution
Keep SiW advantages (flat geometry, high
granularity) Erec. not from Si but from
Scintillator-WLS fibers Reduce (factor gt10) the
number of channels
3
Prototype description
Pb/Sc Si
  • 45 layers
  • 25 25 0.3 cm3 Pb
  • 25 25 0.3 cm3 Scint. 25 cells 5 5 cm2
  • 3 planes
  • 252 .9 .9 cm2 Si Pads
  • at 2, 6, 12 X0

Scintillation light transported with WLS s tail
fibers Cell separation with grooves in Sc.
plates with Tyvec strips inside
Coupled with clear fibers (to PM)
4
Prototype (cntd)
3 Si planes
  • Goal shower-shower separation, position
    measurement, e/h identification
  • Pad dimensionlt shower dimension .9x.9 cm2
  • Longitudinal sampling 3 planes
  • Analogic RO VA hdr9c from IDEas
  • See A. Bulgheronis talk for details

Pad diode ac(old)-dc(new) coupled
  • Actual design
  • - Detector 6x7 pads
  • - Plane 3x2 detectors

pcb contact with conductive glue
5
Construction detailsScintillator
  • 3 mm Kuraray SCSN-61 (25x25 cm2)
  • 3 mm Bicron BC-408 (25x25 cm2)

Machined with vacuum plate as holder
Whole Production (gt50 tiles) done in september
2002
6
Fibers Kuraray 1mm d. Y11 300 ppm multicladding
Face polished and aluminized by sputtering
To make the 2.4 cm radius curvature middle
temperature(500-700) oven
  • Splicing with optical glue
  • and a supporting tube
  • stable in gt30 day time

7
Detector Assembling
45 Layers calorimeter prototype completely built
in 2002
Fibres grouped
into 25x4 bundles making a 4-fold longitudinal
segmentation. Slots for the insertion of
the 3 Si pad planes (Motherboard).
Mechanical support for Photomultipliers
in the 3x3 central cells
8
Test beam activity
  • after a 2002 pre test with the 1st layer only
    (2.1 X0) at CERN
  • two runs at Frascati Beam Test Facility (n 50
    750 MeV)

it is possible to tune the multeplicity.....
  • run at CERN SPS H6 beam line (e/? 5 150 GeV)
    All tests two beam position
    monitors (telescope) put in front of the
    calorimeter.
  • - Each detector consisting of 400?400 xy Si
    strips with a pitch of 240 ?m
  • - They cover the central area of the prototype
    (9.5 ? 9.5 cm2)

LCcal
trigger
beam
9
Test beam activity detector calibration
  • define cell as the calibrated sum of the 4
    longitudinal layers on the same lateral
    position Cibi?j1,4ajLij (4-19-116
    parameters)
  • process in two steps
  • equalise the layer response at the same
    incoming energy Lijbk/bi Lkj
  • minimise the Energy spread on the sum of 9
    cells (iterative process) aj min. width
    Ecal?n1,9Cn

L4
L3
L2
L1
Ci
Si L3
Si L2
Si L1
10
Test beam results Linearity and Energy Resolution
BTF test
?E?E
11.5??E
Ebeam (MeV)
  • Photoelectron statistics negligble
  • Stocastic Term 11.5 as in MC
  • Light disuniformity ltlt10 Effects on resolution
    to be measured at SPS (August 2003)?

Cern TB 2002
Nphegt5.1 /layer ?Cal(45 layers) 250 MeV/Mip
800Npe/GeV OK also _at_ BTF (E 500 MeV)
11
Test beam results Linearity and Energy Resolution
Cern TB 2003
?E?E
pm saturates
confirmed at high energy !!!
Ecal (GeV)
e-
11.1??E
Ebeam (GeV)
Ebeam (GeV)
75 GeV?
15 GeV e-
Ecal (GeV)
Ecal (GeV)
12
Test beam results Si pad detector (Position
Meas.)
Cern TB 2003
y pad Si L2 (cm)
30 GeV electrons
y telescope (cm)
Si L1L2
?3.27 mm
?1.76 mm
Si L3
Si L2
Si L1
y pad y telescope (cm)
13
Test beam results Si pad detector (Position
Meas.)
PRELIMINARY analysis pad noise subtraction not
optimised
Position resolution ? 2.5mm not
far from Monte
Carlo
10 GeV electrons
10 GeV simulated electrons
?2.5 mm
14
Test beam results uniformity in (light) Energy
response
Cern TB 2003
30 GeV e-
disuniformity lt 2 correction from pad
reconstruction can be applied!
Ecal (GeV)
x telescope
2
PRELIMINARY cell border effects dominated by
residual miscalibration
x pad
x (cm)
2
Cj
y(cm)
x telescope
Cj-1
x pad
x (cm)
Ecal (GeV)
15
Test beam results ( e/? rejection)
the redundancy of the information on the
linear/lateral shower development makes the
rejection very easy (difficult to quantify below
10-3 due to beam contamination)
Cern TB 2003
30 GeV e-
30 GeV e-
30 GeV?
30 GeV?
E Si pad Layer 1
E cal Layer 1
50 GeV e-
Si pad Layer 2
30 GeV e-
30 GeV?
75 GeV?
shower variance
16
Test beam results Si Pad two particle separation
exhaustive analysis not fully accomplished
Two electrons with energy 750 MeV
Y silicon chambers
X silicon chambers
First layer
BTF test
Second layer
NB not fully equipped problematic channels
Third layer
17
Conclusions and Future plans
  • A calorimeter prototype with the proposed
    technique has been built and fully tested. All
    the results are preliminary.
  • Energy and position resolution as expected
    ?E/E 11.-11.5 /?E, ?pos 2 mm (_at_ 30 GeV)
  • Light uniformity acceptable.
  • e/? rejection very good ( lt10-3).
  • Two particle separation results coming soon.
  • Next steps include a calorimeter made following
    this technique into the general LC simulation and
    Pattern recognition.
  • Combined test with Hcal (?)

18
backup
19
Detector Assembling
20
PMs
Fibres with PM support structure
Fibres faced to PMs
Scintill.
Piani Si
LCCAL in test _at_ BTF (Frascati)
21
Test beam results CALORIMETER (2.1 X0)
4 layers m.i.p.?check light output and uniformity
in Light collection Ratio signal/sigma ?lower
limit for photoelectrons
Nphegt5.1 /layer ? cal(45layers)gt220 phe/m.i.p.
good uniformity
Simulated Light collection disunifority(20)
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