Presentation is loading. Please wait.

Presentation is loading. Please wait.

The Silicon Vertex Detector of the Belle-II Experiment

Similar presentations


Presentation on theme: "The Silicon Vertex Detector of the Belle-II Experiment"— Presentation transcript:

1 The Silicon Vertex Detector of the Belle-II Experiment
Tomoko Iwashita-Morii University of Tokyo, KAVLI IPMU On behalf of the Belle-II SVD Group Delivered by Francesco Forti University and INFN, Pisa May 28th, 2015 The 13th Pisa Meeting

2 The Belle II Experiment
Belle II is an e⁺-e⁻ collider experiment with √s̄ ≈ mΥ(4S). Target luminosity is L = 8.0 x 10³⁵/cm²s. New physics search beyond the SM in Belle II CP-violating parameters in various B-decay modes will isolate a NP model out of the several hypotheses. b → sqq̄, b → cc̄s, B⁰ → KS⁰π⁰γ, B⁰ → KS⁰KS⁰KS⁰, … The B-decay vertex is essential information to access to the parameters. Belle II detector KEK, Japan e⁻ e⁺

3 Belle II Vertex Detectors
See Poster by L.Vitale:Belle-II VXD radiation monitoring and beam abort with scCVD diamond sensors. Belle II Vertex Detectors PiXel Detector (PXD) The inner most detector comprised of DEPFET pixels. Silicon Vertex Detector (SVD) Next inner detector to the PXD comprised of double-sided strip detectors of silicon. SVD Track impact parameter resolution: σd₀ [mm] σd₀ ~ 40μm @ pT = 2GeV/c PXD Two vertex detectors are installed at the Belle II center. pT [GeV/c]

4 The PiXel Detector (PXD)
Depleted p-channel FET Fully depleted → large signal, fast signal collection. Low capacitance, internal amplification → low noise. Collected q in the internal gate is digitized only when the FET is on → low power consumption. Readout ASIC functions FET array switcher Drain current digitizer Data handler (zero suppression) Monolithic silicon sensor Two-layer structure Thickness = 75μm # of pixel = 768 x 256 Pixel size ~50 x 55µm² 100ns / 250 pixels S/N > 17 30 wafers has been produced so far. Layer Radius L1 14mm L2 22mm

5 SVD Structure L6 L5 L4 L3 SVD cut model Layer structure Four layers
# of ladders L6 16 L5 12 L4 10 L3 7 SVD cut model Four layers Layer structure RL3 = 38mm RL4 = 80mm RL5 = 115mm RL6 = 140mm ~650mm L6 L5 L4 L3 Sensor Trapezoidal sensor Sensor Rectangular sensor Angular acceptance 17⁰<θ<150⁰ Forward In order to have a better vertex resolution and KS⁰ reconstruction efficiency, the outer SVD radius is doubled w.r.t. the Belle SVD. The traditional cylindrical shape detector demands many sensors. The Belle II SVD is designed with a lantern shape. Sensors have an alignment mark “F” at its four corners.

6 SVD Sensors and Readout ASIC
Double-sided Si strip detector Readout ASIC (APV25) Since a high hit rate is anticipated in Belle II, a readout chip should have a short signal shaping time for low noise and a good radiation hardness. P⁺ strip Sensor thickness = μm Si We adopted the APV25 “DSSD” N⁺ strip The APV25 was originally developed for the CMS. Shaping time = 50ns. Radiation hardness > 1MGy. Other characteristics # of input channels = 128 / chip. 192-deep analog pipeline for the dead-time reduction. Thinned to 100μm for the material budget reduction. Rectangular Trapezoidal # of p-strips 768 p-strip pitch 75μm 50…75μm # of n-strips 512 n-strip pitch 240μm Active area 57.72x122.9mm² 5890 mm²

7 Chip-on-Sensor and “Origami” Concepts
APV25 on the sensor An APV25, reading out a sensor, is placed on the sensor to minimize the analog path length for the capacitive noise reduction. Sensor backside readout Signals on the sensor backside are transferred to the sensor front side by other flex circuits and readout by APV25 chips mounted on the front side. … … DSSD n-side (512 strips) Signal readout by the APV25s on the sensor Backside signal readout by the other APV25s Fan-out flex circuit Wire bonding between the sensor and flex The other flex Readout ASICs on the same side & same line → easier chilling by a single cooling pipe.

8 Snapshot – 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

9 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 in O(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

10 See Poster by V.Babu: Belle-II SVD ladder assembly procedures
Ladder fabrication: gluing Electrical connection: wire bonding Ladders are fabricated by gluing the components by Araldite®2011. The flex↔DSSD strips and flex↔APV25s are electrically connected by the wire bonding Glue spread below bonding pads affects to 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 so tuned to realize yield>99% and pull strength f: μf>5gw, σf/f<20%. Appropriate spread of glue to the flex edge Wire bonding pads μf = 10.7gw σf = 0.6gw (97 samples) t = 55+10μm Entries / 0.5gw Glue thickness [μm] Position on the gluing line [mm] Pull strength [gw]

11 Electrically Full Functioning Ladder
L5 ladders Mechanical mockup ladder The first electrically full functioning ladder completed in Apr. 2015 Sensor displacement is measured by the CMM. All sensor displacement are found <160μm from the design. The ladder assembly procedure has been consistently established with achieving a good sensor placement precision.

12 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-charge is obvious. 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 All studies so far indicate good performance. BWD rectangular The distribution(blue) well fits to the Landau(red). x10³ Cluster charge [e]

13 PXD region of interest gen
SVD Readout Backend “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 other remaining components have been developed as well.

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

15 SVD+PXD DAQ Test @ DESY Beam Line
Cluster charge distribution Cluster size distribution The peak corresponds to ~22000 e⁻. Cluster hit efficiency for tracks From the resulting high efficiency, we confirm our common mode correction and zero-suppression keep SVD hits with high efficiency. Efficiency efficiency: 99.4% Position of track projection [cm]

16 SVD TEST @ CERN BEAM FWD/BWD module, no cooling
L5 module, with cooling

17 Global Schedule High level milestones
First mass production ladder (L4-L6) Oct. 2015 2nd beam test Jan.-Feb. 2016 Start of ladder mount to support structure Apr. 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

18 Summary Precision B-decay vertex detection is a crucial issue to access to physics beyond the SM. Highly hermetic vertex detectors had been designed. DAQ system design is confirmed working in the beam test. The first electrically full functioning ladder completed in the April demonstrates well established ladder assembly procedure. Ladder mass production is forthcoming. Belle II physics run will start in 4Q 2018.


Download ppt "The Silicon Vertex Detector of the Belle-II Experiment"

Similar presentations


Ads by Google