Kodali Kameswara Rao TIFR, Mumbai

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Presentation transcript:

Kodali Kameswara Rao TIFR, Mumbai Belle II Silicon Vertex Detector Kodali Kameswara Rao TIFR, Mumbai 10th International "Hiroshima" Symposium on the Development and Application of Semiconductor Tracking Detectors 25-29 September 2015 Xi'an, China

Belle II @ SuperKEKB Search for physics beyond the standard model using high-statistics samples of B and D mesons and  leptons design luminosity 8×1035 cm2s1 CsI(Tl) EM calorimeter: waveform sampling electronics RPC μ & KL counter: scintillator + Si-PM for end-caps Particle identification: Time-of-Propagation (barrel), prox. focusing Aerogel RICH (forward) Vertex detector: 2 layer PXD + 4 layer SVD Central drift chamber: small cell size, long lever arm (50% He+50% C2H6) (positron, 4 GeV) e (electron, 7 GeV) e 2

Belle II Vertex Detector (VXD) Determine the vertex position of the weakly decaying particles Measure the two-dimensional track position and momentum for charged particles PiXel Detector (PXD) See the next talk Silicon Vertex Detector (SVD) Double-sided silicon strip detectors (DSSDs) SVD VXD requirements Fast – to operate in high rate environment Excellent spatial resolution Radiation hard (up to 100 kGray) Good tracking capability – to track particles down to 50 MeV in pT PXD

SVD Structure Overview SVD cut model Layer Institute 3 University of Melbourne 4 TIFR Mumbai 5 HEPHY Vienna 6 IPMU University of Tokyo FW & BW INFN Pisa Backward ~650mm Angular acceptance 17⁰<θ<150⁰ Forward 4 SVD layers (L3 to L6) composed of ladders arranged in a windmill structure Improved resolution at IP with respect to Belle I Very light weight – only 0.58% X0 per layer Track impact parameter resolution: σd₀ [mm] σd₀ ~ 40μm @ pT = 2GeV/c 4 pT [GeV/c]

SVD Ladder Layout L6 L5 L4 L3 Four layers Trapezoidal sensor Rectangular sensor RL3 = 38mm RL4 = 80mm RL5 = 115mm RL6 = 140mm Layer Ladders Sensors / Ladder APVs 6 16 5 800 12 4 480 10 3 300 7 2 168

SVD Sensors and Readout ASIC Double-sided Si strip detector Readout ASIC (APV25) As high hit rate is anticipated at Belle II, the readout chip should have a short signal shaping time for low noise and a good radiation hardness P⁺ strip Sensor thickness = 300-320μm Si We adopted the APV25 “DSSD” N⁺ strip The APV25 was originally developed for the CMS experiment Shaping time = 50 ns Radiation hardness > 1 MGray Other characteristics # of input channels = 128 / chip 192-deep analog pipeline for the dead-time reduction Thinned down to 100 μm for the material budget reduction Rectangular Trapezoidal # of p-strips 768 p-strip pitch 75 μm 50…75 μm # of n-strips 512 n-strip pitch 240 μm Active area 57.7x122.9mm² 5890mm²

Chip-on-Sensor “Origami” Concept APV25 on sensor APVs for the inner sensors are placed directly on DSSDs to reduce the analog path length (capacitive noise) P-side readout Signals on the sensor backside are brought to the upper side by other flex circuits and readout by APV25 chips mounted on the top … … DSSD n-side (512 strips) Signal readout by the APVs on the sensor Backside signal readout by the other APVs Fan-out flex circuit Wire-bonding between the sensor and flex The other flex Readout ASICs on the same side & line → easier chilling by a single cooling pipe

A Snapshot of the “Origami” Concept DSSD backside Flex APV25 DSSD The backside signals are transmitted to the APV25 via bent (and glued) flex circuits DSSD front side with APV25s

Sensors are aligned with a Precision DSSD alignment SVD Ladder Assembly Sensor fixed on a jig Sensor placement DSSDs are handled with precision assembly jigs [O(50μm)], on which the sensors are fixed by vacuum chucking Sensors are aligned with a precision of 10μm by a position tuning jig with monitoring through a CMM Precision DSSD alignment Flex circuit hybrid APV25 Thermal insulator Thermal insulator APV25 DSSD array Flex circuits APV25 Support ribs

SVD Ladder Assembly Ladder fabrication: gluing Electrical connection: wire bonding Ladders are fabricated by gluing the components by Araldite®2011 The flex↔DSSD strips and flex↔APVs are electrically connected by the wire bonding Glue spread below bonding pads can affect the bonding yield and pull strength → glue amount and glue lining are controlled by a gluing robot with Aℓ(99%) wire (φ = 25μm) Number of total bonds = 450k Bonding machine parameters are fine tuned to realize yield > 99% and pull strength f:μf > 5g, σf/f < 20% Appropriate spread of glue to the flex edge Wire bonding pads μf = 10.7 g σf = 0.6 g (97 samples) t = 55+10 μm Entries / 0.5w Glue thickness [μm] Position on the gluing line [mm] Pull strength [g] 10

Assembled Ladders L3 L4 L5 L6

CO2 Cooling The total SVD(Origami) power dissipation 688(328) W Edge hybrids: APV25 chips cooled by end rings A pre-bent cooling pipe (OD=1.6mm) will be clipped onto the ladders on top of the Origami APVs

PXD region of interest gen FADC Readout System “COPPER” board RX x48 FADC Data stream CPU SVD FADC Zero supp. Formatter Repeater to HLT ~2m ~10m belle2link TX x1748 APV25s Aurora link TRG/CLK signals PXD region of interest gen VME to PXD x4 buffer Data size reduction FADC Ctrl APV trig gen Decoder Cu cable Trigger/ timing distributor Central TRG FADC-Ctrl SVD readout system Central DAQ Prototypes of all components have been developed

Electrical Performance Studies Study on the full functioning ladder Study on a single sensor Ladder cross-section Cluster charge The ladder is bombarded by β-rays from ⁹⁰Sr (12.3MBq) Shades by the support ribs are clearly observed in the hit maps Correlation between p- and n-side clusters Support ribs Cluster charge (p-side) [e] Hit maps FWD rectangular Cluster charge (n-side) [e] P-side cluster charge (#strip≥2) Central rectangular μ~23,000e Simultaneous operation of origami sensors worked as expected BWD rectangular The distribution (blue) well fits to a Landau (red) x10³ Cluster charge [e]

SVD+PXD DAQ Test @ DESY Beam Line Jan-Feb 2014 Event display w/ magnetic field Test SVD modules Reconstructed track 4-layers Test SVD modules APV25 chips in light-shielding box e⁻ beam (2-6 GeV)   DSSD sensor Test SVD modules Superconducting solenoid magnet (max. 1T) (max. 1T)

SVD+PXD DAQ Test @ DESY Beam Line Cluster charge distribution Cluster size distribution ( P side layer 3 DSSD ) The peak corresponds to ~22000 e⁻. Cluster hit efficiency for tracks extrapolated from other layers Efficiency efficiency: 99.4% Track position at layer 3 [cm]

SVD TEST @ CERN BEAM L5 module, with/without cooling Nov 2014 L5 module, with/without cooling FWD/BWD module, no cooling

VXD (PXD+SVD) Schedule Milestones First mass production ladder (L3-L6) Nov 2015 2nd beam test Jan-Feb 2016 Start of ladder mount to support structure July 2016 SVD readiness in KEK Feb 2017 PXD readiness in KEK Apr 2017 PXD+SVD integration Jun 2017 PXD+SVD combined cosmic ray test PXD+SVD installation Apr 2018 Start of physics run 4Q 2018

Summary SVD is a 4 layer silicon strip detector for the Belle II experiment Together with the PXD it will provide inner tracking Improved track resolution at the IP and better low momentum tracking w.r.t. to the Belle I SVD SVD ladders Assembly challenging because of the novel ‘origami chip-on-sensor’ concept The prototype phase is now coming to an end, mass production will start in autumn 2015 FADC readout Prototypes of the system exist and the full readout chain has been confirmed