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Linear Collider TPC R

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9/4/09. Ron Settles MPI-Munich/DESY Vancouver WS July 2006 -- LCTPC ... AIDA tuples. American Large Detector Simulations. Detector: ldmar01. Hits: TPC (cyan) ... – PowerPoint PPT presentation

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Title: Linear Collider TPC R


1
Issues for the LC-TPC design and their feedback
to the RD program
  • OUTLINE of TALK
  • Overview
  • LCTPC Design Issues in the DODs
  • Next steps
  • More work with Small Prototypes (SP)
  • Build the Large Prototype (LP)
  • LCTPC ? RD plans

2
International Linear Collider (ILC)
3
(No Transcript)
4
Goal to build a high-performance TPC as
central tracker for an ILC detector
Expt (GeV) Decay Channel (GeV/c2) ln(1s/b) 115 GeV/c2
1 ALEPH 206.7 4-jet 114.3 1.73
2 ALEPH 206.7 4-jet 112.9 1.21
3 ALEPH 206.5 4-jet 110.0 0.64
4 L3 206.4 E-miss 115.0 0.53
5 OPAL 206.6 4-jet 110.7 0.53
6 Delphi 206.7 4-jet 114.3 0.49
7 ALEPH 205.0 Lept 118.1 0.47
8 ALEPH 208.1 Tau 115.4 0.41
9 ALEPH 206.5 4-jet 114.5 0.40
10 OPAL 205.4 4-jet 112.6 0.40
E.g.precision measurements of the Higgs
5
Large Detector Concept example
6x10-5
.30
Particle Flow
(N.B. below are TDR dimensions, which have
changed for latest LDC iteration)
-5
6
LDC
GLD
HCal
ECal
7
Physics determines detector design
  • momentum d(1/p) 10-4/GeV(TPC only)
  • 0.6x10-4/GeV(w/vertex)
  • (1/10xLEP)
  • ee-gZHgll X goal dMmm lt0.1x GZ
  • ? dMH dominated by beamstrahlung
  • tracking efficiency 98 (overall)
  • excellent and robust tracking efficiency by
    combining vertex detector and TPC, each with
    excellent tracking efficiency

8
American Large Detector Simulations
ee- -gt ZH -gt 4 jets
9
(No Transcript)
10
Excerpts from DODs for GLD and LDC used here as
examples
  • DESIGN ISSUES for the LCTPC
  • Performance
  • Endplate
  • Electronics
  • Chamber gas
  • Fieldcage
  • Effect of non-uniform field
  • Calibration and alignment
  • Backgrounds and robustness

11
Performance
  • Momentum precision needed for overall tracking?
  • Momentum precision needed for the TPC?
  • Good dE/dx resolution, Vº detection
  • Requirements for
  • 2-track resolution (in rf and z)?
  • track-gamma separation (in rf and z)?
  • Tolerance on the maximum endplate thickness?
  • Tracking configuration
  • Calorimeter diameter
  • TPC
  • Other tracking detectors
  • TPC OD/ID/length

12
LCTPC resolution in the DODs

13
LC TPC Endcaps

14
GLD
GLD
15
Arrangements of detectors on the active area of
the end cap (2/2) Trapezoidal shapes assembled in
iris shape
LDC
Annotations Px is the type number of PADS
boards or frames
12 sectors (30 each) as super modules are
defined On each, 7 modules are fixed The sizes
of detectors are varying from 180 to 420 mm
P2
P3
P4
P1
P2
P3
P4
By rotation of 15 around the axe, these frames
are the same
These arrangement seems to be the best as only 4
different PADS are necessary
Page 2
16
Principle for a Super Module equipped with
detector 1
Carbon wheel with frames 20x100 mm
Detector 1 made of 8 mm of epoxy or sandwich
Frame of the super module made of 10 mm epoxy
reinforced with 15x40 mm carbon bar
Deformation limit acceptability to define Here
is 20 µm / mbar of pressure
Complete wheel with 12 super modules
Page 3
17
Design
  • Gas-amplification technology ? input from RD
    projects
  • Chamber gas candidates crucial decision!
  • Electronics design LP WP
  • Zeroth-order conventional-RO design
  • Is there an optimum pad size for momentum, dE/dx
    resolution and electronics packaging?
  • Silicon RO proof-of-principle
  • Endplate design LP WP
  • Mechanics
  • Minimize thickness
  • Cooling
  • Field cage design LP WP

18
LC TPC Chamber gas(a) gas choice

19
LC TPC Chamber gas(b) Ion buildup

20
LC TPC Chamber gas(c) ion backdrift/gating

21
LC TPC Electronics

22
LC TPC Fieldcage

23
Backgrounds/alignment/distortion-correction
  • Revisit expected backgrounds
  • Maximum positive-ion buildup tolerable?
  • Maximum occupancy tolerable?
  • Effect of positive-ion backdrift gating plane
  • Tools for correcting inhomogeneous B-field or
    space charge effects in bad backgrounds?

24
LC TPC Non-uniform fields

25
LC TPC Backgrounds

26
LC TPC Calibration/alignment

27
RD Planning
  • 1) Demonstration phase
  • Continue work with small prototypes on mapping
    out parameter space, understanding resolution,
    etc, to prove feasibility of an MPGD TPC. For
    CMOS-based pisel TPC ideas this will include
    proof-of-principle tests.
  • 2) Consolidation phase
  • Build and operate the LP, large prototype, (Ø
    75cm, drift 100cm), with EUDET infrastructure
    as basis, to test manufacturing techniques for
    MPGD endplates, fieldcage and electronics. LP
    design is starting ? building and testing will
    take another 3-4 years.
  • 3) Design phase
  • After phase 2, the decision as to which endplate
    technology to use for the LC TPC would be taken
    and final design started.

28
LCTPC/LP Groups (18 July 06)
Americas Carleton Montreal Victoria Cornell Indi
ana LBNL MIT Purdue Yale
Europe LAL Orsay IPN Orsay Saclay Aachen Bonn DES
Y U Hamburg Freiburg Karlsruhe MPI-Munich Rostock
Siegen NIKHEF UMM Krakow Bucharest Novosibirsk PNP
I StPetersburg Lund CERN
Asia Tsinghua CDC Hiroshima KEK Kinki U Saga
Kogakuin Tokyo UAT U Tokyo U Tsukuba Minadano
SU-IIT
Other groups interested? More formal
collaboration now being organized
29


What have we been doing in Phase 1 ?
30
Gas-Amplification Systems Wires MPGDs?
GEM Two copper foils separated by kapton,
multiplication takes place in holes, uses 2 or 3
stages
Micromegas micromesh sustained by 50µm pillars,
multiplication between anode and mesh, one stage
P140 µm D60 µm
S1/S2 Eamplif / Edrift
S2
31
Pixel TPC Development

Freiburg
Nikhef
32
Examples of Prototype TPCs
Carleton, Aachen, Cornell/Purdue,Desy(n.s.) for
B0or1T studies Saclay, Victoria, Desy (fit in
2-5T magnets) Karlsruhe, MPI/Asia, Aachen built
test TPCs for magnets (not shown), other groups
built small special-study chambers
33
Facilities

Saclay 2T magnet, cosmics
Desy 5T magnet, cosmics, laser
Cern test-beam (not shown)
Kek 1.2T, 4GeV hadr.test-beam
Desy 1T, 6GeV e- test-beam
34
  • TPC RD summary to date
  • Now 4 years of MPGD experience gathered
  • Gas properties rather well understood
  • Limit of resolution being understood
  • Resistive foil charge-spreading demonstrated
  • CMOS RO demonstrated
  • Design work starting for the Large Prototype


35

  • Phase 2
  • Basic Idea LP should be a prototype for the LC
    TPC design and test as many of the issues as
    possible (like, e.g., TPC90 _at_ Aleph)
  • The Eudet infrastructure gives us a starting
    basis for the LP work
  • The general LC TPC RD issues in addition to the
    LP RD which will be planned in conjunction with
    it

36
This is for infrastructure for detector RD, but
not yet the RD itself, to which all of the TPC
RD groups will have to contribute if the LP is
going to be successful. The idea was that this
will provide a basis for the LC TPC groups to
help get funding for the LP and other LC TPC
work.
37
Work Packages for the LCTPC/LP 0) Workpackage
TPC RD program To be defined by the LCTPC
collaboration


38
e.g., Takeshi Matsuda et al discussing at
bi-weekly meetings
39
Work Packages for the LCTPC/LP 1) Workpackage
MECHANICS
Groups expressing interest to
date(others?)a) LP design (incl. endplate
structure) Cornell, Desy, IPNOrsay, MPI,

contribution from Eudet
b) Fieldcage, laser, gas
Aachen, Desy, St.Petersburg,

contribution from Eudet c) GEM
panels for endplate Aachen,
Carleton, Cornell, Desy/HH,

Karlsruhe, Kek/XCDC, Novosibirsk, Victoria
d) Micromegas panels for endplate
Carleton, Cornell, Kek/XCDC,

Saclay/Orsay e) Pixel panels for endplate
Cern,Freiburg,Nikhef,Saclay,Kek/XCDC,

contribution from Eudet f) Resistive
foil for endplate Carleton,
Kek/XCDC, Saclay/Orsay

convener in white color
Ron Settles
Dan Peterson
Ties Behnke
Akira Sugiyama
Paul Colas
Jan Timmermans
Madhu Dixit
40
Work Packages for the LCTPC/LP 2) Workpackage
ELECTRONICS
Groups expressing
interest to date(others?) a)"Standard"
RO/DAQ for LP Aachen, Desy/HH,
Cern, Lund,
Rostock,
Montreal, Tsinghua,

contribution from Eudet b) CMOS RO
electronics Freiburg,
Cern, Nikhef, Saclay,

contribution from Eudet c) Electr.,powerswitchi
ng,cooling Aachen, Desy/HH,
Cern, Lund, for LC TPC
Rostock, Montreal, St.Petersburg,
Tsinghua,
contribution from
Eudet

Leif Joennson
Leif Joennson ?
Harry van der Graaf
Luciano Musa
41
Work Packages for the LCTPC/LP 3) Workpackage
SOFTWARE
Groups expressing interest
to date(others?) a) LP SWsimul./reconstr.
framework Desy/HH,Cern,Freiburg, Carleton,

Victoria, contribution from
Eudet b) TPC simulation, backgrounds
Aachen, Carleton, Cornell, Desy/HH,

Kek/XCDC, St.Petersburg,Victoria
c) Full detector simulation
Desy/HH, Kek/XCDC, LBNL



Peter Wienemann
Peter Wienemann
Stefan Roth
Keisuke Fujii
42
Work Packages for the LCTPC/LP 4) Workpackage
CALIBRATION
Groups expressing interest to
date(others?) a) Fieldmap
Cern,

contribution from Eudet b)
Alignment
Kek/XCDCc) Distortion correction
Victoria d) Rad.hardness of
material St.Petersburg
e) Gas/HV/Infrastructure
Desy, Victoria,

contribution from Eudet

Dean Karlen
Lucie Linssen
Takeshi Matsuda
Dean Karlen
Anatoliy Krivchitch
Desy Postdoc
43
  • Here are some ideas for the evolution up to the
    Design Phase 3
  • (under discussion with the collab.)
  • 2007-08 SP (small prototype) tests,
  • LP1 gt two endplates
    Gempixel,

  • Microm.pixel
  • 2009-10 LP2 -gt real LCTPC prototype endplate
  • Gem or Mm carbon-fibre
    sandwich,
  • gating grid,
  • sector/panel shape,
  • LCTPC electronics,
  • gas,
  • etc


44
  • TPC RD breakdown (prel.)
  • Gem, Micromegas, Pixel
    LP1_at_Desy
  • Large, small, odd-shaped panels
    LP1_at_Desy
  • Fieldcage
    LP1_at_Desy
  • Sandwich structure
    SP/LP2
  • Gating/max. space charge
    SP/LP2
  • Point/2-track resolution
    LP1_at_Desy
  • Momentum meas. in inhomog. B-field LP1_at_Desy
  • dE/dx measurement
    LP1_at_Desy
  • Gas studies
    SP
  • Pad shapes
    Simulation?LP1,LP2
  • Jet environment
    SP_at_Cern/FermiLab
  • Beams
  • 1-6 GeV/c electrons
    LP1_at_Desy
  • 1-20 GeV/c hadrons (dE/dx) LP2_at_Cern/FermiL
  • 100 GeV hadrons (jets) LP2_at_Cern/FermiL


45
TPC milestones
2006-2010 Continue LCTPC RD via
small-prototypes
and LP tests 2010
Decide on all parameters 2011
Final design of the LCTPC 2015
Four years construction
2016 Commission/Install TPC in the
LC Detector

46
No conclusionsBackup slides

47
  • LC-TPC Motivation/Goals
  • to be tested_at_the LP where possible
  • continuous 3-D tracking, easy pattern
    recognition throughout large volume, well suited
    for large magnetic field
  • 98-99 tracking efficiency in presence of
    backgrounds
  • time stamping to 2 ns together with inner
    silicon layer
  • minimum of X_0 inside Ecal (lt3 barrel, lt30
    endcaps)
  • s_pt 100µm (rf) and 500µm (rz) _at_ 3or4T for
    right gas if diffusion limited
  • 2-track resolution lt2mm (rf) and lt5-10mm (rz)
  • dE/dx resolution lt5 -gt e/pi separation, for
    example
  • easily maintainable if designed properly, in
    case of beam accidents, for example
  • design for full precision/efficiency at 30 x
    estimated backgrounds

48
  • Two other LC-TPC features
  • ?will be compensated by good design
  • 50 µs drift time integrates over 150 BX
  • ? design for very large granularity 2 20
    x 109 voxels
  • (two orders of magnitude more if CMOS
    pixel version)
  • end caps with large density of electronics
    (several million
  • pads) are a fair amount of material
  • ? design for smallest amount 30X0 or less
    is feasible
  • design for full precision/efficiency at 30 x
    estimated backgrounds
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