ATLAS small wheels and muon trigger upgrade Osamu Sasaki High Energy Accelerator Research Organization (KEK) INPUTS from RPC : S.Veneziano sTGC : N.Lupu.

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ATLAS small wheels and muon trigger upgrade Osamu Sasaki High Energy Accelerator Research Organization (KEK) INPUTS from RPC : S.Veneziano sTGC : N.Lupu and G.Mikenberg mMegas : V.Polychronakos MDT : R.Richter and O.Sasaki CERN, 9 March, 20111ACES 2011

Present system and improvement scenario CERN, 9 March, 2011ACES 20112

RPC Barrel Upgrade in the Feet Region LVL1 muon trigger efficiency in the feet sectors is about 50% lower than the one for standard sectors. In order to recover the efficiency loss, a fourth layer of the RPC (RPC4) has been installed, wherever possible. Improved to be 80% (pT = 20GeV). CERN, 9 March, 2011ACES RPC4

Upgraded RPC system CERN, 9 March, 2011ACES Low pT & 1/2 coin.  coin.  : 3/4 coin.  : 3/4 coin. pT calculation   : 3/4 coin.  : 3/4 coin.  coin. RPC1 RPC2 RPC3 RPC4 Low-pT Pad High-pT Pad New Low-pT Pad Sector Logic MUCTPI 40 new Low-pT Pad boards with optical link and 56 splitter boards are needed. It is under study how to handle the new trigger outputs in terms of sector logic and MUCTPI.

Present detectors of SW + TGC of BW’s CERN, 9 March, 2011ACES /3 coin. hit position 3/4 coin. track position and deviation H-pT Board R-  coin. track fitting pT calculation Doublets TGCTriplet TGC Small Wheel MDT + CSC Doublet TGC  1/2 coin. hit position (VERY COARSE) RoI, dR, d 

New detectors of SW + TGC of BW’s CERN, 9 March, 2011ACES track fitting track position (R,  ) d  : deviation of incidence angle from infinite pT muons 2/3 coin. hit position 3/4 coin. track position and deviation H-pT Board R-  coin. track fitting crossing angle :  pT calculation Doublets TGCTriplet TGC Small Wheel  hit information (R,  ), d   Precision Detector  < 100  m Level-1 Trigger angular resolution of incidence angle < 1 mrad Level-1 latency RoI, dR, d 

Detector Candidates for the Small Wheel aa CERN, 9 March, 2011ACES 20117

TGC for LVL-1 and precision measurement Each of the so-called TGC packages consists of 4 TGC gaps. – Each gap contains 3 mm pitch strips (R), pad-wires (f) and pads for local trigger. – ~400k independent electronics channels. Time-over-Threshold signals from strips are used for precision measurement. – The position resolution with better than 100  m has been demonstrated in test beam. Hardware centroid circuits of the ToT signals are used for LVL-1 trigger. CERN, 9 March, 2011ACES Layer σ corr (σ nocorr )+/- ∆σ [μm] 1 new66.2 (120.9) +/ new66.7 (79.8) +/ new63.55 (75.95) +/ new63.8 (116.4) +/ old144.6 (264.1) +/ old152.3 (182.1) +/ old163.6 (195.6) +/ old146.4 (267.2) +/-2.2

CERN, 9 March, 2011ACES 20119

CERN, 9 March, 2011ACES TDC BLOCK DIAGRAM ( CONCEPT WHICH WORKS) 4 PH. CLK. GEN. 200 MHz DIFF. CLK 400 MHz 4 PHASES CLK COUNTER SUMMING 12 BITS CLK 0 CLK 90 CLK 180 CLK 270 ToTh PULSE 12 BITS RESULT of CONVERSION THE ToTh INPUT PULSE WIDTH IS FROM 0 TO 255 ns

CERN, 9 March, 2011ACES COMPARATOR & SELECTOR to find the MAXIMUM CHARGE and its INDEX Q0Q0 Q1Q1 Q2Q2 Q 14 Q2Q2 Q 15 / 8 Q max ADD max Q max-1 Q max+1 ADD max -1 ADD max +1 / 8 / 4 Compares the 16 Inputs Finds the Maximum and its Address. Outputs the 3 groups of numbers MAX and the 2 Adjacent groups.

CERN, 9 March, 2011ACES X SIGMA X PROG. DELAY X X ADDm-1 ADDm ADDm+1 Qmax-1 Qmax Qmax+1 / CoM STRIP PITCH 3500 um BLOCK DIAGRAM of CENTER of MASS CALCULATION DIVIDEND DIVISOR ADDi Relative address in the 16 strips slice Qi Charge in units of TDC / 4 / 12 / 16 / / 12 / 28 / 12/ / 28

CERN, 9 March, 2011ACES Additional latency calculation The table shows the latency added by the insertion of the sTGC precision strip trigger logic into the existing path from the Inner Layer coincidence logic to the Sector Logic. We take as a model the Xilinx Virtex6. All numbers are estimates except that for the centroid finder for which a realistic design has been simulated. Clock speed = ~400MHz Yields 2.74/2.80  sec latency (Existing = 2.55  sec) Min (ns)Max (ns) deskew25 ROI selector/ mpx1015 serializer510 deserializer816 RLE1624 latency for the last sample of the pulse 64 find largest signal1013 centroid of a layer2535 centroid chooser1012 centroid average58 tracklet calc (LUT)1013 output serializer

MicroMegas 2-layer + 2-layer (4 gaps in total) mMegas is foreseen. – Charge information for precision measurement. Two-dimensional readout per gap (2D MM) – 2 M channels in total. Strips with 0.5mm pitch. – The pitch is fine enough for LVL-1 trigger to reconstruct and find a track with the required resolution using simple discriminator outputs of hit signals. (Information of charge is not necessary.) CERN, 9 March, 2011ACES PCB Mesh Resistive strips x strips y strips

Some desirable features for mMegas frontend CERN, 9 March, 2011ACES Real Time Peak Amplitude, Time Detection and on-chip ADC (10-12 bits?) – Appropriate for a variety of detectors (mMegas, TGC, TPC, GEM, etc) requiring amplitude and time measurement – on-detector zero suppression, dramatic reduction of data bandwidth Neighbor channel enabling circuitry (allows relatively high thresholds without losing small amplitudes). 64/128 Channels/chip, simultaneous read/write with Derandomizing Buffers Able to provide Trigger Primitives for possible on-detector track segment finding logic – The address of the earliest cluster arrival associated with a given bunch crossing. – Powerful zero-suppression scheme has to be designed to transmit Trigger Primitives to USA15. – Address of the strips can be directly used in a Look-up-Table, similar to FTK, in USA15. Detailed Specifications of back-end to be finalized.

VMM1 IC Block Diagram (not yet finalized) CERN, 9 March, 2011ACES channels/chip, CMOS 130nm, 1.2V, MPW adj. polarity, adj. gain (0.11 to 2 pC), adj. peaking time ( ns) derandomizing peak detection (10-bit) and time detection (1.5 ns) real-time event peak trigger and address integrated threshold with trimming, sub-threshold neighbor acquisition integrated pulse generator, calibration circuits, analog monitor, channel mask and temperature sensor continuous measurement and readout, derandomizing FIFO few mW per channel, chip-to-chip (neighbor) communication, LVDS interface

CERN, 9 March, 2011ACES Small Tube MDT & TGC of SW + TGC of BW’s hit signal alignment 2 x 3/4 coin. 2/3 coin. hit position (R,  ) 3/4 coin. Mx track position (R,  ) deviation (dR,d  ) coin. Mx track position (R,  ) deviation (dR,d  ) R-  coin. Mx track fitting crossing angle :  pT calculation Doublets TGCTriplet TGC Thin Tube MDT & Doublet TGC  BCID signal 3/4 coin. Mx track position (R,  ) deviation (dR,d  )  ASD + BCID (40MHz) track position (R) angle deviation (d  )

BCID and Decoding circuits CERN, 9 March, 2011ACES

CERN, 9 March, 2011ACES

Station (4 x 2 layers) coincidence logic CERN, 9 March, 2011ACES / nn+1n+2n+3…………. Aligned hit signals from each layer (1,2,3,4,5,6,7,8 layers) : 0.5mm step Inner layers The expected track deviations from infinite pT muons is less than ± 1 o (pT > 20 GeV), so that one can restrict the track finding window within very narrow area. 3-out-of-4 and 3-out-of-4 coincidences are made for both super-layers individually. Information of position and deviation from both super-layers are combined. The Level-0 trigger signal from TGC assists the track finding and the BCID. The tracking efficiency, efficiency holes and the probability of the wrong tacking are to be estimated by the simulation works using real data. Level-0 3/4 Super-layer 1 Super-layer 2 track position/deviation

Latency Estimation (<3.2  sec) CERN, 9 March, 2011ACES Present TGC Level-1 TriggerThin Tube MDT (SW) + TGC nsecCLKTotal CLK nsecCLKTotal CLK TOF from interaction point to TGC652.5 TOF from interaction point to SW (10 m)341.5 Propagation delay on wire/strip Propagation delay along wire TGC response MDT drift time ( ns) ASD ASD Cable to PS-Board (12.5m max.) Bunch ID 213 Variable Delay, Bunch ID, OR and signal routing 29.5 Serializer 80MHz) + Optical Tx 215 Variable Delay Optical Fibre Cable (90m) /4 Coincidence Matrix or 2/3 Coincidence Logic Optical Rx + De-serializer 80MHz) 336 LVDS Tx (SN65LV1023) Shift Register (28-steps, ns) 036 Cable to H-pT Board (15m max.) coincidence 238 LVDS Rx (SN65LV1224A) track find 240 Variable Delay encoding 141 H-pT Matrix MDT (SW) – TGC(BW) combined HERE 44 G-Link Tx (HDMP-1032A) + Optical Transmitter TGC R-  coin. (LUT) MDT-TGC coin. 347 Optical Cable to USA15 (90m max.) 1841 crossing angle calculation 350 Optical Receiver + G-Link Rx (HDMP-1034A) pT calculation (LUT) 3 53 Sector Logic pT encoding 1 54 Cable to MUCTPI (10m) Cable to MUCTPI (10m) 256 MUCTPI (4 + variable) MUCTPI 1167 Cable to CTP (2.4m) Cable to CTP (2.4m) CTP (5 + varable[0-11]) 670 CTP Cable to LTPi (10m) 272 Cable to LTPi (10m) LTPi + LTP + TTCvi + TTCex 274 LTPi + LTP + TTCvi + TTCex Variable Delay 276 Variable Delay Optical Cable to TGC frontend (110m) 2298 Optical Cable TTCrq + fanout 3101 TTCrq + fanout Cable to PS-Board (5m max.) 1102 Cable to Frontend Electronics  sec2.625  sec

Summary CERN, 9 March, 2011ACES