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The LHCb VErtex LOcator

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preselect large impact parameter. tracks in Rz -match to m. Second step: 3D -preselected (5-10) 2D tracks -add information from F sensors for. 3D reconstruction ... – PowerPoint PPT presentation

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Title: The LHCb VErtex LOcator


1
The LHCb VErtex LOcator
Tracking, Vertexing and Triggering in a harsh
radiation environment
Doris Eckstein, CERN
2
The LHCb Experiment
  • Dedicated to the study of CP violation in the B
    system
  • LHC -pp collisions _at_ 14TeV
  • -full spectrum of B hadrons (
    )
  • -high intensity
  • LHCb -single arm spectrometer
  • -15-300mrad angular acceptance
  • -recently optimised to minimise
  • material

Vertex Locator
3
The requirements for the VELO
  • Reconstruction of pp interaction vertex
  • wide spread of interaction region in z
    (sz5.3cm)
  • many stations around z0
  • Reconstruction of b-hadron decay vertex
  • short track extrapolation distances
  • measure at smallest radii
  • minimal multiple scattering
  • minimise material between interaction and
  • first measured point
  • VELO is the tracker before the LHCb magnet
  • Angular coverage of full downstream detector
  • angular range
  • 21 Silicon stations allowing to measure at
    least 3 hits/track
  • 2 R- and 2 F-measuring sensors per station
  • overlap (acceptance, alignment)

4
The VELO Design
Mechanical design as consequence of these criteria
  • VELO sensors as close as possible to beam
  • no beam pipe, sensors 7mm away from beam
  • Injection larger aperture required retraction by
    30mm
  • Protect sensors against RF pickup from the LHC
    beam
  • Protect the LHC Vacuum from possible outgasing of
    detector modules
  • Place sensors in a secondary vacuum Roman pots

5
Secondary Vacuum RF Foil
  • Made from 250mm thick Al
  • Inner corrugations
  • Minimal material before the first
  • sensor is hit
  • Outer corrugations
  • allow for overlap of detector halves
  • for full azimuthal coverage and for
  • alignment
  • Prototyping at NIKHEF
  • method Hotgas Forming
  • full size foil
  • vacuum tight and stiff

6
More requirements for the VELO
  • Rejection of multiple interactions in L0 Trigger
  • additional VETO stations upstream of
  • interaction point
  • Fast stand-alone tracking and vertexing for L1
    Trigger
  • motivates R-and F-measuring sensors
  • Design allows to optimise resolution vs.
  • number of channels
  • Baseline design of sensors
  • Active area 8mm to 42 mm
  • R measuring sensors
  • division into 45o sectors
  • F measuring sensors
  • inner/outer region
  • increasing pitch from inner towards outer radii
  • 2nd metal layer to route signal to chips

7
Second Level Vertex Trigger
  • Forward flight direction of B Rz impact
    parameter
  • First step 2D
  • -build Triplets of clusters in R sensors
  • -form tracks in Rz
  • -fill z-vertex histogram
  • -preselect large impact parameter
  • tracks in Rz
  • -match to m

Second step 3D -preselected (5-10) 2D tracks
-add information from F sensors for 3D
reconstruction -match to L0 and TT
8
Optimisation of VELO sensor design
  • L1 Trigger speed, number of ghost tracks
  • sector division
  • Clustering/tracking efficiency Signal to Noise

  • strip length
  • Options of design studied (keeping constant
    number of strips)
  • Different strip pitches
  • Does impact parameter
  • resolution suffer?
  • max. 5
  • design chosen with gradual
  • increase of pitch (40mm
  • to 103mm)

9
Even more requirements for the VELO
This detector has to operate in an extreme
radiation environment
  • Maximum irradiation per station
  • 5x1012 to 1.3x1014 neq/cm2/year
  • Strongly non-uniform dependence on R and station
    (z)
  • Maintain a good S/N performance for at
    least 2 years (replacement)
  • Extensive RD program to select
  • Sensor and Front-End chip

10
Prototype testing in Lab and Test beam
Test beam CERN SPS (120 GeV p and m)
Irradiated Not irradiated
Irradiated Not irradiated
DELPHI-ds sensor Irradiated/Not irradiated
PR03 sensors
11
Tests of the p-on-n prototype
  • Efficiency of cluster reconstruction close to
    track
  • Box size efficiency
  • PR02 F-sensor routing lines in outer region
  • none in
    inner region
  • More efficient in inner region
  • Less efficient in irradiated region

12
P-on-n vs n-on-n
  • P-on-n
  • -Fraction of charge in routing line
  • reaches 20 in outer region
  • -5 in inner region
  • -Detector has undepleted and insulating
  • layer after irradiation
  • -Expected to be less for n-on-n
  • Compare efficiency for p-on-n and
  • n-on-n for different depletion depth
  • P-on-n efficiency degrades fast
  • N-on-n efficiency 100 for only 60 depletion
    depth

Chose n-on-n for VELO
13
Front-End chip decision
  • Two parallel developments SCTA_VELO (DMILL) and
    Beetle (0.25mm CMOS)
  • Features 128 input channels
  • 40MHz sampling (LHC clock)
  • Hybrids equipped with 16 chips tested in test
    beam
  • Decision taken at beginning of this year to use
    Beetle
  • Performance equally good
  • Availability, radiation hardness and usage in
    LHCb

SCTA_VELO
Beetle1.1
14
Beetle chip tests
  • Currently Beetle1.2 under study
  • Test set-up in Lab with one chip reading out a
    n-on-n 200mm thick
  • prototype sensor
  • Sensor close to final design
  • Measure S/N with Sr source
  • Prepare for test beam
  • Hybrid with 16 Beetle1.2
  • chips reading out a full
  • sensor
  • MPW submission of improved
  • Beetle1.3 soon

15
Summary Outlook
  • VELO design is close to completion
  • Important decisions finalised sensor design
  • choice of Front-End chip
  • Successfully tested module prototypes consisting
  • of Sensor, Hybrid and 16 chips
  • Plan to have first module end of 2003
  • Complete VELO in 2006
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