• DocumentCode
    897271
  • Title

    Use of CCDs in the Time Projection Chamber

  • Author

    Jared, Richard C. ; Fujita, Ted Y. ; Jackson, Horace G. ; Sidman, Steven B. ; Goulding, Frederick S.

  • Author_Institution
    Lawrence Berkeley Laboratory University of California Berkeley, California 94720 U.S.A.
  • Volume
    29
  • Issue
    1
  • fYear
    1982
  • Firstpage
    282
  • Lastpage
    285
  • Abstract
    The Time Projection Chamber produces 3-dimensional information about the multiple tracks of reaction products produced by e+ e-collisions at the center of the chamber. Two dimensions (r,ÿ) result from processing signals from proportional wires and induction pads (a total of 17,000 signals) mounted at the end planes. The third (axial) dimension is obtained by measuring the drift time of ionization from the particle tracks to the end planes. To achieve this, all wire and pad signals (suitably shaped to about 500 ns width) are stored in Charge Coupled Devices (CCDs) which, at any moment, hold 45.5 ¿s of signal history clocked in at a sampling rate of 10 MHz. About 40 ¿s after a master trigger, the history is frozen by stopping the clocking action, and a slow clock mode (20 kHz) is initiated to read out the stored samples which are then digitized (9 bits) and processed by an on-line computer. A total of 17,000 channels × 455 samples (each digitized to 9 bit accuracy) is stored in the CCDs (i.e., about 70M bits) for each event. This paper describes the pulse shaping philosophy, the design of the CCD units, the drivers and the testing procedures.
  • Keywords
    Charge-coupled image sensors; Clocks; History; Ionization; Particle measurements; Particle tracking; Signal processing; Signal sampling; Time measurement; Wires;
  • fLanguage
    English
  • Journal_Title
    Nuclear Science, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-9499
  • Type

    jour

  • DOI
    10.1109/TNS.1982.4335846
  • Filename
    4335846