Arai, Y

Emura, T

Ikeno, M

Shirasu, H

CERN Document Server

Lisbon, Porutogal, September 11 - 15, 1995. OCR Outputthe First Workshop on Electronics for LHC Experiments,Submitted to; gujé OYEEE ir:>AC5.Z2>·T=."Y. ARA1, M. 1KENO, H. SHIRASU and T. EMURATime Memory Cell VLSI and a High-Speed Serial InterfaceSeptember 1995KEK Preprint 95-111AE-mail: Library@kekvax.kek.jp (Internet Address) OCR OutputCable: KEK OHOFax: 0298-64-4604(0)3652-534 (Intemational)Telex: 3652-534 (Domestic)Phone: 0292%-64-5136JAPANIbaraki-ken, 3051-1 Oho, Tsukuba-shiNational Laboratory for High Energy PhysicsTechnical Information & LibraryKEK Reports are available from:National Laboratory for High Energy Physics, 1995parallel converter so that it is straitght forward to make it a comprising 8 stages and their timing diagram are shown in OCR OutputBasic structure of the TMC can be considered as a serial—to A simplified schematic of an asymmetric ring oscillatorATLAS muon high-precision tracker. signals.drift chamber readout and is proposed for the readout of which generates an equally spaced even number of timingThe TMC is adopted in DO and PHENIX experiments for those signals we developed an asymmetric ring oscillatorresolution of 250 ps RMS [7]. (especially in 2's power) is desirable for the TMC. To obtainimproved in a new chip (TMC—TEG3) and attained time can be obtained. However, an even number of timing signalsaround time, the time resolution and stability have also been number of inverter stages; an odd number of timing signalsoscillator. Besides the expected reduction of cost and the turn TMC—TEG3 chip. A ring oscillator normally comprises an oddspaced timing signals, we invented an asymmetric ring A new asymmetric ring oscillator was developed for theloop (PLL) circuit. To obtain an even number of equally CMOS gate-array technology.developed a new time digitizing circuit with a phase locked cost and high-density. The chip was fabricated in a 0.5 umnot tribual due to the difference in the technologies; we thus buffer of 3 ps, deadtime-less readout, dual—edge detection, lowThe direct conversion of the TMC circuit to a gate—a1·ray is muon detector; precise timing resolution of 250 ps, level—lstructure of transistors. This chip already fulfills most requirements for the ATLASradiation—hardened process due to the uniform physical The TMC-TEG3 chip (Fig. 1) was developed in 1994 [4].addition, the gate-array structure is more adequate for areduce development cost and turn—around time further. In A. TEG3 Chipbasic requirements, we proceeded to a gate array technology tokind [4,5,6]. Although the TMCIOO4 fulfills most of ourseveral groups are also developing TDC chips of the same II. TMC DEVELOPMENTSchannels of l usec buffer. After our success of the chip,(TMCIOO4) attained 520 ps RMS timing resolution and has 4[2,3] by using a Delay Locked Loop (DLL) circuit. The chip serial converter.At first, we developed a full—custom CMOS TDC chip development, and describe first test results of the parallel-toconventional CMOS LSI. In this paper, we present status of the TMC chipdelay element of around l ns is easily available in is greatly increased.variable delay element [1], it is realized that high precision trigger chip, number of trigger signals handled in a single chipsystem. Since our first idea to use an internal gate as a parallel/serial converter is implemented within a customelectronics for timing adjustment in trigger and readout signal is limited by pin counts of the package. If a simplesevere conditions require high precision delay elements in LSI, usable number of gates is huge, but the number of inputand many events will occur in each crossing. These very include such circuit in a custom LSI. Furthermore, in a recentIn LHC experiments, beam crossing interval will be 25 ns application is commercially available, it is not so easy toAlthough a high-speed serial interface chip for networkparallel-to-serial converter as well.I. INTRODUCTIONserial—to-parallel convener. Reversing the structure produces aresults of the parallel-to-serial converter are presented.converter to solve a pin-count problem in trigger chip. The present status of the TMC and the first testATLAS experiment. With this delay element, we also build a simple high-speedparallel-to-serialbeen adopted in several high-rate experiments and is proposed for the muon high-precision tracker of thepipeline TDC chips for high-rate tracking detectors. The chip, named Time Memory Cell (TMC), hasRealizing such delay with a PLL technique, we have been developing low-power and high-densityA precision variable delay implemented in a LSI is one of the key elements in LHC experiments.T0ky0 University of Agriculture and TechnologyH. Shirasu and T. EmuraKEK, National Laboratory for High Energy PhysicsY. Arai and M. Ikeno,Time Memory Cell VLSI and a High—Speed Serial Interfacemm by 6_4 mm OCR Output implemented in two complex PLD's.Fig. 1 Photograph of the TMC-TEG3 chip, The dig size is 6_4 the DSP and from a VME bus. Most of the random logic isstored in a dual port memory which can be accessed both fromcommon start and common stop mode. The acquired data arei § tg@§¤vs¤¤»A.. 4 if module is shown in Fig. 5. The module works for bothchips (32 channels) and a DSP. A block diagram of thethe TMC—TEG3 chip. The module implements 8 TMC-TEG3A 6U VME module (Fig. 4) has been developed [8] withB. TMC-VME module6* ..,r -; =.-' M s$eA K,Clock frequency for the chip was 40 MHz.Fig. 3 Time—resolution measurement of the TMC—TEG3.@~~»1»» ~ .. ri ` xy Mt 'C V 2;.;; ,,_ . meal At[ns]-.·~ wv-1.0 -0.5 0.0 0.5 1.0 1.5»——~··~- .... ~=~ ~··» `Y XL-at ..»_ _ »..·-...- ..... we-;» .2..a..W·.- ~· = ~ ¤L ---»..·~ ·**‘**M ‘‘‘‘‘‘‘· 7 -*-·....... +>.·;¤W‘i**»¤=m¢= '50TZG>L;:--·.-. ) .,F, _ _, :_iw. .._.. »..;· __ e i ‘`*’‘ .. ~m~gm. ¤»» """"'··. ~·;,,.M...· M§'$»`*'““T"“."’”`“ki6·»·ié!» ,’ " “ ~tj;mm:..—n• s¤L»1 OO,., ._.Qiisg 150 1 Iz.I |--—- Ideal200 ; IT \_| I I-— Dara-_:. ..Package 0.5 mm lead pitch, 144-pin plastic QFP.250@40 MHz, l MHz input, 100 kHz readout.Power Consumption | < 200 mW (Vdd=3.3V)Double Pulse Reso. I S Clock PeriodEncoding Scheme | (hit tag + 5 bit) x 2 (rise and fall) schematic, (b) timing diagram.Phase Locked Loop | Response time : ~ 4 usec. VGN is a delay control signal from a PLL circuit. (a) A circuitMaster Gate Size | 66k Master where 32k gates were used. Fig. 2 An 8-bit example of the asymmetric ring oscillator.Input Channels | 4 ch (single ended or differential).Time Range | 2.56 ps ~ 12.8 us (clock period x 128).ted Non-linearity | < 0.1 LSBDifferentialllntegraTime Resolution | 250 ps rms @40 MHz.Digitization Step | 0.6 ~ 3.1 ns/bit (= clock period / 32).differential : AV > 50 mV (Vc = 2 i· 0.6 V).single ended : CMOS level, orSystem clock | 50 ~ 10 MHz (12.5 ~ 2.5 MHz z x4 mode).B ;]\ nTechnology | 0.5 pm CMOS Sea-of-Gates (TCl80G).Table l. Characteristics of the TMC-TEG3 chiwe we na we we wem_4 T r*——{"”—’ ly; llb)The characteristics of the TEG3 chip are summarized in Table.indicating that the inherent error of the chip is about 100 ps.ven781 ps, the quantization error is 226 ps ( = 781 ps / V12 ),The RMS value of the data is 249 i 6 ps. Since one LSB isFig, 3 shows a timing resolution of the TMC—TEG3 chip. IE AHC B HE CHE DME E r|EFlr|E GHEHlatchcd at thc timing cqually spaced by T/8 (T/32).all; dli dll di dll df} I :¤E dA through H. With thcsc timing signals, an input signal isimplcmcnts 32 stages. Timing signals arc cxtractcd from node(alFigs. 2-(a) and 2-(b), rcspcctivcly. Thc prcscnt TMC chipRG—l74/U cable. Clock frequency was 20 MHz. OCR Outputcorresponds to 220 Mbps. The rise and fall time of the signalFig. 8. Serial output wave form measured at I0 m point of themeasurement. Since ll bits were sent out in a cycle, thisI74/U cable. Clock frequency of 20 MHz was used in this 1.00VQ M§.00ns Chi f 1.66VFig. 8 shows a wave form measured after a IO m-long RGhigh-speed type) available.we were using, we used most powerful output driver (24 mA,Since there is no 500 driver in the gate-array library whichprovided a separate synchronizing signal in this test.cycle. For synchronization between P—to—S and S-to—P, we‘(parity) bits are included, thus in total ll bits are sent out in achange on one). Along with the data, a start bit and two stop.... E .... I .... .... .... .... .... i...,.., .... ,"l" and not change at the data of "0" (N RZI: non return to zeroexclusive OR's. The serial output will change at the data oftime interval, and outputs of the flip—flop are connected to ; w { _;7_‘, l3 .1- .2erig. .. E. ...,, ,,. .... ...,. .,. . ,,.. ,.A parallel data is latched in flip-fIop's sequentially at a fixedserial converter are shown in Fig. 7—(a) and 7—(b) respectively.The schematic and the output wave form of the parallel-toelements used in the TMC circuit.parallel-to-serial converter (P-to-S) by using the same delayto-parallel converter (S—to-P), we have built a test circuit of aTek Sto : 10.0GS/s ET _4497 AcqsSince the TMC circuit can be regarded as a kind of serialof the interconnection and boundary overlap are reduced.processed in a chip can be greatly increased. Thus the problemcoincidence logic in the same chip, number of channels converter. (b) Serial output wave form.problem. If we can implement a serial interface and the Fig. 7. (a) Simplified schematic of the parallel-to—serialserial interface chips, but this does not solve the pin countsicyeeNumber of cables can be reduced by using commercialinterconnections between trigger chips are necessary.the detector part covered by a trigger chip is limited and many gsi? il é Ia chip is limited by available pin counts of the package. Thus(bl Sian oo oi o2 oa D4 os be D1 S‘°¤ $*°¤logic is relatively simple but the number of signals handled in20-40MHz crock.: PL'logic is required to generate a trigger signal. Each coincidenceIn an ATLAS muon trigger, a large number of coincidenceHI. SERIAL INTERFACE§.|rL"1.|¤-Ll" rUJrL.-|*‘ rL11i-U.|r&|S¤<>•> rl>.£¤°l'“|6¤F'·I¤°}·'“I°°I"1°¤I*“I¤d*‘1¤d'“I*$<$* '·{¤°sundata are read out and transferred to the readout FIFO. 04 | |os ID0 los |¤1 ID7 |o2 | oaFIFO stores the corresponding event position from where thethe requirement of the PHENIX experiment, and the triggerchip can accept up to 5 consecutive trigger signals which isSerial •Outthe double pulse resolution is reduced to less than 14 ns. The(alThere are two encoders and each encoder covers 16 bit. Thusdual port memory is increased from 128 of the TEG3 to 256.related sequencers besides the TMC circuit. The depth of theThis chip includes a trigger FIFO, readout FIFO's andchannels).collection and so on.and contains 2 channels of circuit (production chip will have 4differential signal, clock synchronization method, errorTEG5 chip is a prototype chip for the PHENIX experimentThere are still many items to be optimized; use of aadded. The block diagram of the chip is shown in Fig. 6. Thevariation of delay time between bits was observed.functions which are rcquircd in high—ratc cxpcrimcnts werecircuit layout was done automatically and not optimized, someOCR OutputIn thc latest version of thc TMC chip (TMC—TEG5), more2.7V while the power supply voltage was 3.3 V. Since thesee eye patterns clearly. High level output voltage reachedwas still less than 2 ns after the I0 m long cable, and we can5 _ OCR Outputin IEEE Trans. on Nucl. Sci.32 ch pipeline TDC module with TMC LSI", to be published[8] Y. Arai, M. Ikeno, T. Murata, H. Shirasu and T. Emura, "A VMESolid—State Circuits, Jan. 1, 1996.with a 250 ps Time Resolution", to be published in IEEE J. of[7] Y. Arai and M. Ikeno, "A Time Digitizer CMOS Gate-Arraypp.1104—1108, 1994.Digital Converter", IEEE Trans. on Nucl. Sci. vol. 41,[6] C. Ljuslin et al., "An Integrated 16-channel CMOS Time toConference, May 1993, pp. 28.6.1 - 28.6.4.Proceedings of the IEEE 1993 Custom Integrated CircuitsDigitizer for High-Energy Physics Instrumentation",[5] M. I. Loinaz and B. A. Wooley, "A BiCMOS Time IntervalLeCroy Co., May, 1993, pp. 91- 98.International Conference on Electronics for Future CollidersMultihit TDC ASIC with Buffers", Proceedings of the[4] M. Campbell, I. Chapman and J. Mann, "A Deadtime—LessState Circuits, vol. 27, pp. 359-364, March 1992.Time Memory LSI with l ns Resolution", IEEE J. of Solid[3] Y. Arai and T. Matsumura and K. Endo, "A CMOS 4 ch x l kCircuits Digest of Technical Papers, pp. 121-122, June 1988.VLSI for I-Iigh—Energy Physics", in Symposium on VLSI[2] Y. Arai and T. Baba, "A CMOS Time to Digital ConverterSupercollider, Snowmass, (l986)455.Summer Study on the Physics of the SuperconductingSystem by Using Time Memory Cell", Proceedings of the[1] Y. Arai and T. Ohsugi, "An Idea of Deadtimeless ReadoutREFERENCESfor their technical support.We also thank O. Umeda and T. Takada of the Toshiba Corp.their continuous support and encouragement for this project.The author wish to thank T. Kondo and T. K. Ohska forACKNOWLEDGEMENTrun at LHC clock frequency of 40 MHz.for developing a serial interface for a trigger chip which willthe signal after 10 m—long cable. This result is very promisingsucceeded to measure up to 220 Mbps serial transmission ofWe also tested a new parallel-to-serial converter, andlevel bufferring.recent chip includes data handling functions for the secondhigh—precision tracker. In addition to the TDC functions, thehigh—rate experiments and proposed for the ATLAS muonconverter chip (TMC) and its module. The TMC is used inWc have bccn developing a high-precision Time-t0-Digital

Time memory cell VLSI and a high-speed serial interface

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