SuperB-DCH Servizio Elettronico Laboratori Frascati DCH FEE TDR contents discussion SuperB CERN EDT Meeting – November 11 1 G. Felici.

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SuperB-DCH Servizio Elettronico Laboratori Frascati DCH FEE TDR contents discussion SuperB CERN EDT Meeting – November 11 1 G. Felici

SuperB-DCH Servizio Elettronico Laboratori Frascati Outline  Design goals  Requirements Specification for charge measurement based DAQ dE/dx & time measurements : resolution, dynamic range and linearity Cluster Counting option dE/dx measurements : resolution, dynamic range and linearity  DCH front-end system: block diagram  ON DETECTOR electronics Preamplifiers dE/dX based on charge measurements dE/dX based on Cluster Counting  Cabling  HV Distribution dE/dX based on charge measurements dE/dX based on Cluster Counting  OFF DETECTOR electronics Triggered Data Path Digitizing Modules dE/dX based on charge measurements dE/dX based on Cluster Counting SuperB CERN EDT Meeting – November 11 2 G. Felici  OFF DETECTOR electronics Triggered Data Path Concentrators Modules UnTriggered Data Path Option #1 - Concentrators Modules Option #2 – See Trigger Section  Radiation Environment Policy  Grounding and shielding ….  Conclusion  Questionnaire

SuperB-DCH Servizio Elettronico Laboratori Frascati Design goals SuperB CERN EDT Meeting – November 11 3 G. Felici

SuperB-DCH Servizio Elettronico Laboratori Frascati Design goals SuperB CERN EDT Meeting – November 11 4 G. Felici SuperB Drift Chamber (DCH) front-end electronics is designed to extract and process the 8056 (to be finalized) sense wire signals to: measure the electron drift times to the sense wires for tracking purpose (momentum of charged particles) Measure the energy loss of particles per unit length, dE/dx (particle identification) provide hits information to the trigger system (trigger primitives) Measurement of the energy loss of particles per unit length, dE/dx (particle identification) can be implemented by Measuring the charge collected on the sense wire (discarding high values to remove Landau fluctuations) Counting the number of cluster generated by the particle crossing the cell Decision : within the first half of 2012

SuperB-DCH Servizio Elettronico Laboratori Frascati Requirements SuperB CERN EDT Meeting – November 11 5 G. Felici

SuperB-DCH Servizio Elettronico Laboratori Frascati Specifications for charge measurements SuperB CERN EDT Meeting – November 11 6 G. Felici Overall expected single cell σ E ≈ 30 % (dominated by chamber contribution)  Electronic contribution must be enough low to make it negligible. E.g.: σ EL = 15% of σ E (4.5%)  sqrt( σ E 2 + σ EL 2 ) ≈ σ E Assuming ≈ 50 fC the charge released from a mip (gas gain=10 5 ), σ EL = 5%  single channel ENC ≈ 50 fC * 0.05 ≈ 2.5 fC σ E dominated by gas amplification effects: Lower range: σ EL (2.5 fC ) (could be 3σ EL ) Higher range: ≈ 500 fC (BaBar experience) Dynamic range dE/dx Goal: measure particle energy loss with precision of the order of 7.5% (BABAR) despite large fluctuations involved in single measurement (“truncated mean” method) Resolution Linearity of the order of 2% matches system requirements Linearity

SuperB-DCH Servizio Elettronico Laboratori Frascati Specifications for time measurements SuperB CERN EDT Meeting – November 11 7 G. Felici Overall expected σ S ≈ 130μm  dominated by chamber contribution σ S limits: statistics of primary ionization, electrons diffusion, electronic  Chamber contribution (σ SC ) raw estimation ≈ 440/sqrt(N P ) ≈ 110 μm for a 90/10 He/Iso gas mixture σ EL ≈ sqrt( σ S 2 - σ SC 2 ) ≈ 70 μm  σ S ≤ 1.5 ns ( 3 * 16 μm/ns drift velocity) Main error sources are jitter (time walk + noise) and TDC (digitizing noise) Jitter Noise: Δt = σ N / (dV/dt) ≈ σ N * τ /V max ( τ = peaking time) Assuming σ N = 4 mV rms, V max = 30 mV, τ = 4 ns  σ EL ≈ 0.5 ns Time walk contribution: assuming τ = 4 ns a time walk of the order of 1.5 ns with 20 dB input signal dynamic is obtained  quite high  possible (partial) compensation using FADC sampled values Digitizing noise ≈ Δ/sqrt(12) with Δ ≈ 1 ns  ≈ 0.3 ns  Time resolution is dominated by signal time walk TDC range depends on gas mixture drift velocity and cell size  SuperB DCH max drift time ≈ 600 ns  TDC range ≈ 1us Dynamic range Particle tracks reconstruction based on (ionized) electrons drift time toward the sense wire Resolution A linearity of ≈ 1% fulfill measurement requirements Linearity

SuperB-DCH Servizio Elettronico Laboratori Frascati Cluster Counting option SuperB CERN EDT Meeting – November 11 8 G. Felici Pros Particle identification improvement Dedicated time measurement not required Possible improvement in spatial resolution Cons High sampling frequency digitizers Fast processing Wide bandwidth and high power requirement front-end (environment noise sensitivity increase) Good cables for on-detector  off-detector connection required (bigger size) Termination resistor required (system noise baseline) with dedicated PCB FADC resolution is a function of the lowest sampled signal and system noise  6 fC wire signal (gas gain 3x10 5 ), 10 mV/fC shaper-amplifier, safety factor = 2  30 mV signal  If we consider only the contribution of termination resistor (bottom limit – peaking time = 3 ns – gain = 10 mV/fC ) we get about 2 mV rms Resolution Pros & Cons Total ionization in 1.2 cm high cell (average) ≈ 30e (90/10 – He/Iso) Each electron correspond to a different level in output voltage  3 bits/electron  8 bits FADC Linearity ≈ 2% Dynamic range and linearity

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB CERN EDT Meeting – November 11 9 G. Felici DCH front-end system: block diagram

SuperB-DCH Servizio Elettronico Laboratori Frascati DCH Front-End system: Block diagram SuperB CERN EDT Meeting – November G. Felici < 5 m cables #173 (48 chs) #1152 (8 chs) 1 12  1 DAQ 173 OL 16 (12 cores) OL #16 DAQ 16 2Gbits/sec ECS 16 2Gbits/sec DIOM Pre-HV boards 12  1 TRIGGER TIOM Gbits/sec or Copper Links #16 ON-DETECTOR ELECTRONICS DCH BACKWARD END-PLATE 8056 chs 12  1 ECS 12 cores Fiber Optical Cable patch-panel 16 (12 cores) OL or Copper Links OFF-DETECTOR ELECTRONICS Data Conversion Trigger Primitive Generation Boards 173 OL 1 = Cluster Counting option Trigger option 1: Data Conversion generates trigger primitives Trigger option 2: Data Conversion board host a Trigger Mezzanine board for partial superlayer tracks reconstruction

SuperB-DCH Servizio Elettronico Laboratori Frascati DCH Front-End system: Block diagram SuperB CERN EDT Meeting – November G. Felici ON DETECTOR electronics

SuperB-DCH Servizio Elettronico Laboratori Frascati ON DETECTOR electronics - #1 SuperB CERN EDT Meeting – November G. Felici Front End Boards contain HV blocking capacitors, protection networks, preamplifiers and (eventually0 shapers. Boards are located on the backward end-plate to maximize S/N ratio and are connected to the Data Conversion boards (located on external crates) through coaxial or twisted pairs cables (Cluster Counting = coaxial) The end-plate will be divided in (sub)sectors  more cells will be grouped in a single multi-channel preamplifier-shaper board Preamplifier Wire signal is used both for charge and time measurement  preamplifier should not worsening too much signal time information (rise time). Because gas mixture slow drift velocity and moderate detector parasitic capacitance a 80/100 MHz bandwidth transimpedance preamplifier match system requirements Channel density is not so high and circuit design not so complex  approach based on SMT technology possible  profiting of high bandwidth, low noise SiGe devices developed for mobile-phone applications dE/dx based on charge measurement Preamplifier output must reflect as much as possible the wire current input signal, then current amplifier based on fast circuit topologies with low sensitivity to detector capacitance must be used (for example circuits based on current conveyor topology) dE/dx based on Cluster Counting

SuperB-DCH Servizio Elettronico Laboratori Frascati ON DETECTOR electronics - Preamplifier for charge measurements SuperB CERN EDT Meeting – November G. Felici C DET = 0 pF C DET = 24 pF 0 mV 100 mV 200 mV 300 mV 400 mV 0 mV 100 mV 200 mV 300 mV 400 mV 8 ns 10 ns 12 ns14 ns16 ns 18 ns20 ns 22 ns24 ns P D < 30 4V 10 fC 50 fC 10 fC 50 fC

SuperB-DCH Servizio Elettronico Laboratori Frascati ON DETECTOR electronics - #2 SuperB CERN EDT Meeting – November G. Felici

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB CERN EDT Meeting – November G. Felici Cabling

SuperB-DCH Servizio Elettronico Laboratori Frascati Cabling - Signal #1 SuperB CERN EDT Meeting – November G. Felici ON DETECTOR electronics will provide good amplification, but signal levels are still quite low. Micro-coaxial cables or shielded twisted cables must be used to minimize noise environmental pickup Problem can arise due to the cable jacket. Many halogen free cable are quite rigid (large bending radius) Braid shield twisted pairs offer a good compromise between cost, noise environmental shielding and bandwidth. Nevertheless shielded connectors could be a problem in the ON DETECTOR side Both micro-coaxial and braid shielded twisted pairs are available in round and flat assembling. Flat assembling is (generally) better for ON DETECTOR front end boards connection, while round cables are better for routing and Digitizing Boards connections. Decision will follow the technique adopted for dE/dx measurement dE/dx based on charge measurement Micro-coax: 50 Ω / 0.83 – 1.3 mm diameter

SuperB-DCH Servizio Elettronico Laboratori Frascati Cabling – Signal #2 SuperB CERN EDT Meeting – November G. Felici Besides considerations for dE/dx based on charge measurements cables for Cluster Counting must features high bandwidth, low losses and controlled impedance (Shielded Controlled Impedance) There are several assemblies available. Cost is a function of modularity, type of connector and type of cable, but is generally higher than solution for charge measurement because the BW requirement. Again, decision on type of cable will follow the technique adopted for dE/dx measurement dE/dx based on Cluster Counting Our Price:$1.83 Vol. Pricing:Quantity: Price:$1.67$1.52$1.38 Stock:65 Mated height:1.4 mm (55.12 mil) Cable diameter:0.7 mm (27.6 mil) Length:5.9" (150 mm) Connectors:Super micro plug Frequency:DC-7GHz VSWR:1.4:1 max Standard lead time:4 weeks ARO 1.88 mm diameter

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB CERN EDT Meeting – November G. Felici HV Distribution

SuperB-DCH Servizio Elettronico Laboratori Frascati HV distribution SuperB CERN EDT Meeting – November G. Felici Enough modularity to avoid too many dead channels in case of single chamber channel problem Modularity is function of the distance from inner layer (example: 2 boards in inner layer – 5 boards in outer layer) Good feedback of the current dragged by the inner layers (≈ 1 nA) and by the outer layers (≈ 10 nA) General considerations 1MΩ 2.2 nF 1MΩ 500 pF 10MΩ Ch 1 Ch 8 Filter Box [Outside Detector] Distribution Board [number of boards is a function of chamber layer] CH1 Main Power Supply BOARD #1 BOARD #N 1MΩ 500 pF 10MΩ Ch 1 Ch 8 HV Distribution – dE/dx by means of charge measurement

SuperB-DCH Servizio Elettronico Laboratori Frascati HV distribution SuperB CERN EDT Meeting – November G. Felici 1MΩ 2.2 nF Filter Box [Outside Detector] Distribution Board [number of boards is a function of chamber layer] CH1 Main Power Supply BOARD #1 BOARD #N HV Distribution – dE/dx by means of Cluster Counting 1MΩ 500 pF 10MΩ Ch 1 RTRT 10MΩ Ch 8 RTRT 1MΩ 500 pF 10MΩ Ch 1 RTRT 10MΩ Ch 8 RTRT 500 pF

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB CERN EDT Meeting – November G. Felici Triggered Data Path Digitizing Modules

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path : Digitizing Modules - Latency (pre-FEX) buffers SuperB CERN EDT Meeting – November G. Felici First electron(s) cluster arrival time dE/dx by means of wire signal charge measurement or Cluster Counting Feature Extraction ON BOARD Data continuously digitized and readout ONLY if L0 Trigger is delivered DISCR < 1 μs FADC LPF TDC < 1 μs FADC Buffer dE/dE by means of charge measurement – Latency buffers (pre-FEX) dE/dE by means of Cluster Counting – Latency buffers (pre-FEX) 32 samples (8 28 MHz ≈ 35.7 ns sampling period ≈ 1ns time resolution over-threshold TDC values Single event buffer size : 32 x 8 bits 32 x 8 x 6 ≈ 6.8 μs latency time Separated FADC and TDC buffers 1000 samples (8 1 GHz Single event buffer size = 1000 x 8 bits 1000 x 6 = 6 μs latency time 6 events buffer looks enough for trigger decision processing

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path : Digitizing Modules - Event Buffers SuperB CERN EDT Meeting – November G. Felici COUNTER (0 – n) L1 FIFO Sampled data DATA RO SM (FEX) Pushing mode ADDR Ev7Ev7 Ev6Ev6 Ev5Ev5 Event RO buffer (Derandomizer) Concentrator board Trigger Latency Time + n samples (Dual-port memory) 210n Sampling clock ADDR L1 (synchronized by sampling clock) Read ADDR FiFO Empty FiFO Read Data (counter L1) (counter L1) - Latency 32 word (16 bits) block data readout Over-Threshold data (from comparator) 210n Ev4Ev4 Ev3Ev3 Ev2Ev2 Ev1Ev1 Ev0Ev0 ≈ 72 ns (Dead Time) 56 MHz x 4 clk 16 bits bus ≈ 50 ns (Dead Time) 56 MHz x 6 clk 16 bits bus NB: Higher transfer rates are possible but as Digitizer Modules SHOULD use Rad Tol components. Then we can not use high performances SRAM based FPGAs. Es : ACTEL ProAsic max internal frequency ≈ 350 MHz 16/32 data path Digitizer Module Address (2 Bytes) Flag (1 Byte) Trigger Tag (1 Byte) – 5 bits in BaBar Counter (1 Byte) Charge (2 Bytes) Time (2 Bytes) ADC Time Data Stream Example (10 bytes) BW requirements = 8056 (N. channels) x 10% (occupancy) x 20 (bytes) x 8 (bits) x 150 kHz ≈ 19 Gbits/sec (foreseen: 16 2 Gbits/sec = 32 Gbits/sec) NB: we have used 20 bytes in calculation instead of 10 (safety factor) Ev3Ev3 Ev2Ev2 Ev1Ev1 Ev0Ev0 Data RO Buffer

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path : Digitizing Modules – Event Readout SuperB CERN EDT Meeting – November G. Felici SAMPLING CLK L1 SAMPLED DATA READOUT CLK READOUT ADC DATA

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path: TDC Implementation SuperB CERN EDT Meeting – November G. Felici  Simulations show it is possible to implement a 4xOversampling – 1ns time resolution TDC in a ACTEL ProAsic3 device  Caveat No radiation mitigation technique can be applied to PLLs and (probably) to the high frequency section of 4xOversampling TDC FPGA internal resources could be not enough to manage data conversion & feature extraction for an acceptable number of channels. At the moment no Ser-Des are available

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path : Digitizer Modules – CC SuperB CERN EDT Meeting – November G. Felici After FEature Extraction (primary cluster detection): 30 words (16 bits) containing time arrival information (worst case) Assuming FEX implemented on Digitizing Board BW requirements = 8056 (N. channels) x 10% (occupancy) x 32 (words) x 16 (bits) x 150 kHz ≈ 62 Gbits/sec (foreseen: 16 2 Gbits/sec = 32 Gbits/sec)

SuperB-DCH Servizio Elettronico Laboratori Frascati Triggered Data Path : Concentrators SuperB CERN EDT Meeting – November G. Felici Data 12 chs connector DAQ section Data Conversion 48 CHS 2Gbits/sec DAQ ECS DAQ section ECS section DATA CONVERSION CONCENTRATORS/OL Data Conversion OL (576 channels): 48 (chs) x 12 (Data Conversion) x 0.10 (occupancy) x 20 (bytes) x 8 (bits) x 150 kHz ≈ 1.4Gbits/sec Total amount of DATA CONCENTRATORS OL : 14 (foreseen 16) Total amount of ECS CONCENTRATORS OL : 14 (foreseen 16) 12 cores Fiber Optical Cable Splitter ECS 12 chs connector ECS section CONCENTRATORS DATA CONVERSION BOARD 12

SuperB-DCH Servizio Elettronico Laboratori Frascati UnTriggered Data Path – Option #1 SuperB CERN EDT Meeting – November G. Felici 1.2Gbits/sec TRIGGER 12 cores Fiber Optical Cable Splitter Data Conversion 48 CHS 12 (number of boards) x 48 (number of chs per board) x 7 MHz (Channel sampling frequency) ≈ 4 Gbits/sec Trigger Concentrators : 14 – Trigger OL : 56 (foreseen 64) TRIGGER CONCENTRATOR Trigger Concentrators Data Conversion Board #3 ≈ 1 Gbits/sec Data Conversion Board #3 Data Conversion Board #3 Data Conversion Board #3 ≈ 1 Gbits/sec Data Conversion Board #3 Data Conversion Board #3 Data Conversion Board #3 ≈ 1 Gbits/sec Data Conversion Board #3 Data Conversion Board #3 Data Conversion Board #3 ≈ 1 Gbits/sec Data Conversion Board #3 Data Conversion Board #3 TRIGGER

SuperB-DCH Servizio Elettronico Laboratori Frascati Radiation Environment Policy SuperB CERN EDT Meeting – November G. Felici Only qualified components will be used. Anyway SiGe HBT transistors technology is inherently radiation hard ON DETECTOR electronics OFF DETECTOR electronics - NO CC Only Rad Tol components will be used in Data Conversion and Concentrators Boards We have already shown it is possible to implement a ≈ 1 ns resolution TDC and FADC readout by means of (lash-ROM based) Rad Tol FPGA (Actel ProAsic) OFF DETECTOR electronics - CC Cluster Counting requires lots high performances FPGA  NO Rad Tol People think to to use neutron shielding (pure polyethylene..)

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #1 SuperB CERN EDT Meeting – November G. Felici Author: G.Felici, G. Finocchiaro, M. Roney v1.0 Number of channels 8056 (to be finalized according to minimum allowed inner DCH radius) ON DETECTOR - Power dissipation per channel - Preamplifier Boards Standard dE/dx by means of charge measurement: 30 mW/ch - BW ≈ 80/100 MHz Cluster Counting: 100 mW/ch - BW ≈ 250MHz OFF DETECTOR - Power dissipation per channel - Data Conversion Boards (contribution to Feature Extraction to be checked) Standard dE/dx: 0.9 W/ch (48 chs/board – 43W/board) ≈ 7.3kW total could be 0.7 W/ch (64 chs/board - 45 W/board) due to improvement in component power requirements ≈ 5.7 kW total Cluster Counting: 5 W/ch (8 chs boards – 40W/board) ≈ 41kW could be 2.5W/ch (16 chs/board – 40W/board) due to improvement in component power requirements ≈ 20kW total OFF DETECTOR - Power dissipation per channel - Concentrators Assuming the same number of concentrators for both options (Feature Extraction on Data Conversion boards): 70 mW/ch (Concentrators boards must be located in non hostile environment): 650W

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #2 SuperB CERN EDT Meeting – November G. Felici OFF DETECTOR - Trigger - Primitives Generation Option1: Off-Detector electronics generates only primitives  power requirement already considered in Data Conversion board Option2: Off-Detector electronics includes electronics for partial super-layer track reconstruction  Off- Detector power and housing requirement would (slightly) change. The option is under study. ON DETECTOR - Volume occupied by the electronics (drawings of electronic modules – non available yet) HV distribution boards on forward endplate - Preamplifier boards on backward endplate. Position (both boards): 2-3 cm from endplate. Height (board + support) 8-10 cm  Nitrogen gas enclosure volumes are being determined ???? OFF DETECTOR - Volume occupied by the electronics (drawings of electronic modules – non available yet) HV: 2 Crates 19"- wide, 8U-high Euro-mechanics rack (Ref: CAEN SY1527LC) Standard dE/dx - 48 chs/board - 16 boards/crate: 173 boards (according to superlayer geometry)  11 VME crates 19" x 8U (6+2) enclosure (Ref : CAEN VME8100 ) 64 chs/board - 16/boards/crate boards  could be 9 VME crates 19" x 8U (6+2) enclosure (Ref : CAEN VME8100) Cluster Counting - 8 chs/board - 16 board/crate: 63 VME crates 19" x 8U (6+2) enclosure (Ref : CAEN VME8100 ) 16 chs/board - 16 bards/crate  could be 32 crates VME crates 19" x 8U (6+2) enclosure (Ref : CAEN VME8100)

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #4 SuperB CERN EDT Meeting – November G. Felici OFF DETECTOR - Number and size of Read-out cables or fibers Data Conversion  Trigger (option 1): 64 fibers (150 kHz trigger rate - 10% occupancy - 20% safety Gbits/s link) Data Conversion  Trigger (option 2): partial super-layer track reconstruction in Data Conversion Board : 48 chs/board  173 links - 64 chs/board  132 links Number and size of slow control cables 16 fibers Minimum bending radius Fibers: depends on assembly. Single fiber: 2 in; bundle: 15 times external bundle diameter. Waiting for ETD decision ON-DETECTOR LVPS cables: depends on the assembling. Assuming a round shielded (aluminum foil) bundle of 12 cables  12 x cable diameter (12 conductors – 1.5 mm^2 size  outer diameter ≈.520 in ≈ 13.2 mm ON-DETECTOR HV cables: depends on the assembling. Assuming a shielded (aluminum foil) bundle of 12 cables  12 x cable diameter (12 conductors overall cable diameter ≈ 9 mm) ON-DETECTOR Signal cables [Very Preliminary] Standard dE/dx: assuming a flat assembly of 12 cables  24 x cable diameter (micro-coax cable diameter ≈ 0.5 mm - aluminum foil shielding) ON-DETECTOR Signal cables [Very Preliminary] Cluster counting: assuming a flat assembly of 12 cables  12 x cable diameter (RG178 cable diameter ≈ 1.8 mm)

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #3 SuperB CERN EDT Meeting – November G. Felici Max tolerable distances between the detectors to the electronic modules: ON-DETECTOR – OFF-DETECTOR ≈ 5 m Access frequency on the external electronic per year 12 access/year (after debug) Frequency access on the detector per year 1-2 access/year (after debug) (including HV) Modularity of the electronic unit (housing racks) 200 cm (45 rack units) ON DETECTOR - Number and size of power cable Preamp LV power cables: 12 chs/board modularity  768 cables – 1.5 mm^2 size HV cables: less than 100 OFF DETECTOR - Number and size of Read-out cables or fibers Data Conversion  Concentrators: 168 fibers Concentrators  DAQ: 16 fibers

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #5 SuperB CERN EDT Meeting – November G. Felici Shielding requirements (thermal and electrical) Thermal: NO Electromagnetic: if cluster counting will be implemented some shielding could be useful. For standard approach (dE/dx by means of charge measurement) the magnetic field return iron should be enough May be SVT shielding required ?? Information drawings on the cable distribution on the detector geometry: non available yet Only preamplifiers should be installed on backward-end plate. Connection to off-detector electronics will be implemented by coax cables (Cluster Counting) or coax/twisted cables (standard dE/dx). Cables should leave the detector along the outer diameter Requirement of cooling system - Backward Endplate - flow, temperature and type of fluid Standard dE/dx: 300W  air flow cooling should be enough to provide good air exchange ≈ 1000 m^3/h - coarse calculation: (3.16 x Watt) /(Dt*0.589) à Dt = 4 (!), degrees, PD = 300W  500 m^3/h) Cluster counting: 1 kW  liquid cooling required Requirement of cooling system - Allowed detector temperature variations: backward end-plate 4 degrees (????) Size of the chiller ON DETECTOR + OFF DETECTOR electronics ??

SuperB-DCH Servizio Elettronico Laboratori Frascati SuperB Integration Questionnaire - #6 SuperB CERN EDT Meeting – November G. Felici Cooling pipes distribution at sub detector ends (drawings) Not available yet Describe other requirements that have an impact of the space available like auxiliary equipment, minimum space for accessibility, etc 1.5 mt in front of racks 0.5/1 mt behind racks Full access to end-plates (backward and forward) during detector access OPTIONAL : electronics for local debug (table, PC etc.) Describe other requirements that have an impact of the space available like space for the commissioning operations and assembly Full access to end-plates (backward and forward) during detector access

SuperB-DCH Servizio Elettronico Laboratori Frascati Conclusions SuperB CERN EDT Meeting – November G. Felici Design goals have been defined Two different implementation of dE/dx measurements have been evaluated and will be reported in TDR. Measurements on Cluster Counting are going on and final decision about the technique that will be used to measure dE/dx will be taken within the first half of 2012 The technique used for dE/dx measurement has a NOT minor impact on number of boards, power requirement, interconnections cables, HV distribution boards and grounding (shielding). HV distribution modularity will follow the chamber layer (less cells for the internal layers, more cells for the external ones) Only Rad Tol components will be used in front-end boards (NO CC). If selected components has no qualification they will be qualified. Grounding/shielding policy has not been defined yet Probable (!!!) number of (optical) links : 16 for DATA, 16 for ECS and 64 (173) for TRIGGER Board design will start after the decision on dE/dx technique to be used