Continuously live image processor for drift chamber track segment triggering

A. Berenyi, H. K. Chen, K. Dao, S. F. Dow, S. K. Gehrig, M. S. Gill, C. Grace, R. C. Jared, J. K. Johnson, A. Karcher, D. Kasen, F. A. Kirsten, J. F. Kral, C. M. LeClerc, M. E. Levi, H. Von Der Lippe, T. H. Liu, K. M. Marks, A. B. Meyer, R. MinorA. H. Montgomery, A. Romosan

Research output: Contribution to journalArticlepeer-review

7 Scopus citations

Abstract

The first portion of the BABAR experiment Level 1 Drift Chamber Trigger pipeline is the Track Segment Finder (TSF). Using a novel method incorporating both occupancy and drift-time information, the TSF system continually searches for segments in the supercells of the full 7104-wire Drift Chamber hit image at 3.7 MHz. The TSF was constructed to operate in a potentially high beam-background environment while achieving high segment-finding efficiency, deadtime-free operation, a spatial resolution of < 0.7mm and a per-segment event time resolution of < 70 ns. The TSF system consists of 24 hardware-identical TSF modules. These are the most complex modules in the BABAR trigger. On each module, fully parallel segment finding proceeds in 20 pipeline steps. Each module consists of a 9U algorithm board and a 6U interface board. The 9U printed circuit board has 10 layers and contains 0.9 million gates implemented in 25 FPGAs, which were synthesized from a total of 50,000 lines of VHDL. The boards were designed from the top-down with state-of-the-art CAD tools, which included gate-level board simulation. This methodology enabled production of a flawless board with no intermediate prototypes. It was fully tested with basic test patterns and 105 simulated physics events.

Original languageEnglish (US)
Pages (from-to)348-353
Number of pages6
JournalIEEE Transactions on Nuclear Science
Volume46
Issue number3 PART 1
DOIs
StatePublished - 1999
Externally publishedYes

Bibliographical note

Funding Information:
The first recipient of B4B4R Drift Chamber data is the Track Segment Finder (TSF), described in this paper. The Drift Chamber consists of 7104 small hexagonal drift cells, 'This work was supported by the Division of High Energy Physics of the US. Department of Energy under Contract No. DE-AC03-76SF00098. In addition, A.B.M. was supported by the Alexander von Humboldt Foundation, Bonn, Germany.

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