3–7 Sept 2007
Prague
Europe/Zurich timezone

The ALICE Silicon Pixel Detector system

5 Sept 2007, 11:45
25m
Prague

Prague

Czech Republic

Speaker

Dr Alex Kluge (CERN)

Description

The ALICE silicon pixel detector (SPD) comprises the two innermost layers of the ALICE inner tracker system. The SPD includes 120 half staves each consisting of 10 ALICE pixel chips bump bonded to two silicon sensors and one multi-chip read-out module. Each pixel chip contains 8,192 active cells, so that the total number of pixel cells in the SPD is ≈ 10^7. The on-detector read-out is based on a multi-chip-module containing 4 ASICs and an optical transceiver module. The constraints on material budget detector module dimensions are very demanding. An overview of the electronics integration, test results and test procedures are presented.

Summary

  1. SPD layout
    The ALICE silicon pixel detector (SPD) consists of two barrel layers at radii of 3.9cm and 7.6cm, respectively. The
    basic detector module is the half-stave, in which the active elements are two ladders glued to a multi-layer Al
    flexible flat cable carrying power and signal lines. Each half-stave consists of 10 pixel chips bump bonded to two
    silicon pixel sensors (70.7 x 16.8 mm2) and is read out by a multi-chip module. Each pixel chip contains a matrix
    of 8192 cells. The SPD contains 9.83 x 10^6 pixel cells in total.
    The half-staves are mounted on 10 light-weight carbon fiber sectors, each sector supporting 4 half-staves on the
    inner layer and 8 half-staves on the outer layer. The pseudorapidity coverage of the inner layer is |η| < 1.95.
  2. SPD electronics
    2.1. Electronics system architecture
    The pixel chips provide binary hit information, which is stored in a delay line during the L1 trigger latency. In case
    of a positive L1 decision the hit is stored in one out of four multi event buffers where the data wait for the L2
    trigger decision to be read out or discarded.
    In each half-stave, a multi-chip module (MCM) initiates the read-out and performs the configuration process of
    the pixel chips. The connection to the control room is established via three optical fibers. The MCM contains three
    ASICs and a custom developed 800 Mbit/s optical link for the data transfer between the detector and the control
    room. All on-detector ASICs have been implemented using a commercial 0.25µm CMOS process; radiation
    hardness is obtained by appropriate gate design rules and by redundancy in the critical nodes.
    In the control room FPGA-based electronics performs zero suppression, data formatting and sends the data to the
    ALICE data acquisition system.

2.2. Electronics integration
The compactness of the design sets severe constraints on the material budget and dimensions of the detector
elements and the interconnects.
The very small clearance between the SPD inner layer and the wall of the beam pipe requires that the overall
radial thickness of the half staves is less than 3 mm. The width of the half-staves is determined by the pixel chip
dimensions; the clearance between the edges of adjacent half-staves is down to ≈ 0.2mm and the width of the
MCM substrate is limited to 11mm in order to avoid interference with the other structural elements. In order to
keep the material budget within 1% X0 (each layer), the read-out chip and the sensors are 200 µm thick and the
pixel chips are thinned down to 150 µm. The interconnection between the pixel chips and the read-out MCM is
established via an multi-layer flexible bus in which aluminium layers are used as conductor to even further reduce
the material budget.

2.3. Full system and production tests
Full system tests in beam setups and in the laboratory of the entire detector system including the sensors, pixel
read-out chips, the multi-chip module, the optical links, the off-detector electronics, the ALICE trigger system and
the ALICE data acquisition system have been performed.
2.4. Summary
The tight material budget and the limitation in physical dimensions required by the detector design introduce new
challenges for the integration of the on-detector electronics. The full system as well as an overview of the
integration of the on-detector electronics are presented.

Primary author

Dr Alex Kluge (CERN)

Presentation materials