SPHENIX Silicon Tracker 2015/07/10 Radiation Lab meeting Y. Akiba (RIKEN)

Slides:



Advertisements
Similar presentations
ATLAS SCT Endcap Detector Modules Lutz Feld University of Freiburg for the ATLAS SCT Collaboration Vertex m.
Advertisements

Belle-II Meeting Nov Nov Thomas Bergauer (HEPHY Vienna) Status of DSSD Sensors.
Workshop on Silicon Detector Systems, April at GSI Darmstadt 1 STAR silicon tracking detectors SVT and SSD.
The Intermediate Silicon Layers detector OUTLINE ISL inside CDFII Why the ISL? Conceptual Design Ladders and Spaceframe Rasnik Online Alignment System.
Summary of the SVD session 19 March 2009 T. Tsuboyama (KEK)
Charged Particle Tracker for a RHIC/EIC joint detector Detector layouts based on EIC and NLC Physics drivers Silicon detector technologies Simulations.
LHC Experiments at Liverpool E2V Visit – Nov 2005 Introduction Si Technology Upgrade/Maintenance Summary.
PHENIX Vertex Tracker Atsushi Taketani for PHENIX collaboration RIKEN Nishina Center RIKEN Brookhaven Research Center 1.Over view of Vertex detector 2.Physics.
For high fluence, good S/N ratio thanks to: Single strip leakage current I leak  95nA at T  -5C Interstrip capacitance  3pF SVX4 chip 10 modules fully.
The LHCb Inner Tracker LHCb: is a single-arm forward spectrometer dedicated to B-physics acceptance: (250)mrad: The Outer Tracker: covers the large.
Performance of the DZero Layer 0 Detector Marvin Johnson For the DZero Silicon Group.
The BTeV Tracking Systems David Christian Fermilab f January 11, 2001.
Silicon Stripixel Detector Junji Tojo RIKEN Vertex2005 Lake Chuzenji, Nikko, Japan November 7-11, 2005.
E.Kistenev, Forward Upgrade Meeting 08/18/04 Forward (Nose Cone) Calorimeter: Update 2.5 mm.
David L. Winter for the PHENIX Collaboration PHENIX Silicon Detector Upgrades RHIC & AGS Annual Users' Meeting Workshop 3 RHIC Future: New Physics Through.
Si VTX Workshop Y. Akiba. Agenda and goals Goal A PAC Proposal 9:00 - 9:30Physics with vtx, PAC+DOE proposal overviews, what needs to go in,
D. Lissauer, BNL. 1 ATLAS ID Upgrade Scope R&D Plans for ATLAS Tracker First thoughts on Schedule and Cost.
Simulation issue Y. Akiba. Main goals stated in LOI Measurement of charm and beauty using DCA in barrel –c  e + X –D  K , K , etc –b  e + X –B 
Medipix sensors included in MP wafers 2 To achieve good spatial resolution through efficient charge collection: Produced by Micron Semiconductor on n-in-p.
CM26 March 2010Slide 1 EMR Status o Intro o Construction o Magnetic shielding o Electronics o Prototype Cosmics test o Schedule Jean-Sebastien Graulich,
Pixel hybrid status & issues Outline Pixel hybrid overview ALICE1 readout chip Readout options at PHENIX Other issues Plans and activities K. Tanida (RIKEN)
Silicon Vertex Tracker (VTX) for PHENIX Experiment at RHIC Y. Akiba (RIKEN) for PHENIX collaboration Detector Advisory Committee Meeting November 22, 2003.
1 Engineering issues for FPCCD VTX Detector Y. Sugimoto KEK July 24, 2007.
TOP counter overview and issues K. Inami (Nagoya university) 2008/7/3-4 2 nd open meeting for proto-collaboration - Overview - Design - Performance - Prototype.
Fine Pixel CCD for ILC Vertex Detector ‘08 7/31 Y. Takubo (Tohoku U.) for ILC-FPCCD vertex group ILC vertex detector Fine Pixel CCD (FPCCD) Test-sample.
8 July 1999A. Peisert, N. Zamiatin1 Silicon Detectors Status Anna Peisert, Cern Nikolai Zamiatin, JINR Plan Design R&D results Specifications Status of.
ATLAS PIXEL SYSTEM OVERVIEW M. Gilchriese Lawrence Berkeley National Laboratory March 11, 1999.
Thin Silicon R&D for LC applications D. Bortoletto Purdue University Status report Hybrid Pixel Detectors for LC.
Swadhin Taneja Stony Brook University On behalf of Vertex detector team at PHENIX Collaboration 112/2/2015S. Taneja -- DNP Conference, Santa Fe Nov 1-6.
PHENIX Silicon Vertex Tracker. Mechanical Requirements Stability requirement, short and long25 µm Low radiation length
1 Silicon Vertex Detector at PHENIX Atsushi Taketani RIKEN / RBRC 1.Physics Goal 2.Detector Concept 3.Structure 4.Pixel detector 5.Strip detector 6.Summary.
FVTX Review, November 17th, FVTX Mechanical Status: WBS 1.6 Walter Sondheim - LANL Mechanical Project Engineer; VTX & FVTX.
Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96 TeV  Instantaneous luminosity will.
Vertex ‘99, 6/21-25/1999 p. 1 CDF Run II SiliconAlan Sill, Texas Tech University CDF Run II Silicon Tracking Projects 8th INTERNATIONAL WORKSHOP ON VERTEX.
Silicon Strips for PHENIX SVTX Status and Plans for Silicon Strips in PHENIX SVTX Abhay Deshpande Recent development: Possibility of the second Si Pixel.
18 March 2009 Thomas Bergauer Prototype batch of DSSD from commercial vendors & Proposal for SVD Layout HEPHY Vienna.
FPCCD VTX Overview Yasuhiro Sugimoto KEK Tokubetsu-Suisin annual meeting 11.
Aug 2003 Craig Ogilvie 1 Landscape/Goals for R&D  Goal: Barrel+structure ready Summer/Fall 06 (run07)  Goal: Endcaps ready Summer/Fall 07 (run08)  RIKEN.
Solid State Detectors for Upgraded PHENIX Detector at RHIC.
Spin Physics with the PHENIX Silicon Vertex Tracker Junji Tojo RIKEN for the PHENIX Collaboration Advanced Studies Institutes - Symmetries and Spin July.
D. M. Lee, LANL 1 07/10/07 Forward Vertex Detector Cost and Schedule.
J-C Brient-DESY meeting -Jan/ The 2 detector options today …. SiD vs TDR [ * ] [ * ] J.Jaros at ALCPG-SLAC04 ECAL ECAL tungsten-silicon both optionsHCAL.
D. M. Lee, LANL 1 07/10/07 Forward Vertex Detector Overview Technical Design Overview Design status.
PHENIX Vertex Detector with Conventional Strip Sensors Abhay Deshpande Stony Brook University.
Walter Sondheim 6/9/20081 DOE – Review of VTX upgrade detector for PHENIX Mechanics: Walter Sondheim - LANL.
Pixel Atsushi Taketani RIKEN RIKEN Brookhaven Research Center 1.Overview of Pixel subsystem 2.Test beam 3.Each Components 4.Schedule 5.Summary.
March 25, FVTX Monthly/Quarterly Report June, 2009 Technical Status, Cost & Schedule Melynda Brooks, LANL.
September 7, 2004Si VTX Strip Overview1 Overview of VTX Strip Group Activities Abhay Deshpande SUNY-SB For Si Strip Group.
Status of Stripixel Sensor + SVX4 Test Junji Tojo RIKEN VTX Meeting June 1 st, 2004.
R. Lipton Vertex ‘98 Santorini, Greece The D0 Silicon Microstrip Tracker (D0SMT) Outline  Design  Detector Studies Coupling capacitors Radiation Damage.
Vertex detector R&D Work Plan in /3/11 Y. Sugimoto for KEK-Tohoku-TohokuGakuin-Niigata- ToyamaCMT Collaboration.
Rene BellwiedSTAR Tracking Upgrade Meeting, Boston, 07/10/06 1 ALICE Silicon Pixel Detector (SPD) Rene Bellwied, Wayne State University Layout, Mechanics.
RD program on hybrids & Interconnects Background & motivation At sLHC the luminosity will increase by a factor 10 The physics requirement on the tracker.
Status of the STAR tracking upgrade Gerrit van Nieuwenhuizen STAR Collaboration Meeting BNL, February 24, 2005.
10 September 2010 Immanuel Gfall (HEPHY Vienna) Belle II SVD Upgrade, Mechanics and Cooling OEPG/FAKT Meeting 2010.
Upgrade with Silicon Vertex Tracker Rachid Nouicer Brookhaven National Laboratory (BNL) For the PHENIX Collaboration Stripixel VTX Review October 1, 2008.
SPHENIX Mid-rapidity extensions: Additional Tracking system and pre-shower Y. Akiba (RIKEN/RBRC) sPHENIX workfest July 29,
B => J/     Gerd J. Kunde PHENIX Silicon Endcap  Mini-strips (50um*2mm – 50um*11mm)  Will not use ALICE chip  Instead custom design based on.
SPHENIX Silicon Tracker 2015/10/20 Japan Korea PHENIX collaboration meeting Y. Akiba (RIKEN)
Si Sensors for Additional Tracker
 Silicon Vertex Detector Upgrade for the Belle II Experiment
Evidence for Strongly Interacting Opaque Plasma
Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC
The SuperB Silicon Vertex Tracker
Pixel-strip-EMC tracker and DC option
SIT AND FTD DESIGN FOR ILD
Design and fabrication of Endcap prototype sensors (petalet)
Silicon tracker and sensor R&D for sPHENIX
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Perugia SuperB Workshop June 16-19, 2009
Presentation transcript:

sPHENIX Silicon Tracker 2015/07/10 Radiation Lab meeting Y. Akiba (RIKEN)

Reference design and requirements |  |<1 and  High efficiency & purity in central Au+Au to measure modified FF High rate (15kHz DAQ) High momentum resolution to separate Upsilon states Precision vertex measurement for heavy flavor measurements (D, B  J/Psi, b-tagged jets) Compact (Fit inside of EMCAL) J.Nagle LPR talk

This 7 layer baseline design was implemented in GEANT4 simulation to evaluate the performance of the tracker Simulation shows that this design can separate the three Upsilon states Much room for design optimization (performance, cost, etc) Reference Design & Performance A. Frawley DOE review 2015/04/30 Reconfiured VTX S0a/b S1a/b S2

Concept of S2 sensor (for SVX4) 96mmx92.16mm active area Divided into 12x12 blocks Each block is 8mm x 7.68mm and made of 128 strips of 8mm x 60 micron Upper 6 bocks are connected upwards. Lower 6 blocks are connected by downwards 24 SVX4 chips to read- out the entire sensor

sPHENIX silicon tracker R&D in Japan Silicon sensor R&D at RIKEN in JFY2014 Large Prototype sensor for the outer most layer – 96 mm x 92.16mm active area – 320  m thick – AC coupled – 6x128x24 mini-trips (60  m x 8mm) – 128x24 read-out channels 5 sensors manufactured at Hamamatsu and delivered to RIKEN in March 2015 For all of 5 delivered sensors – No NG channels or strip – Vfd = 50 V – Vbreakdown > 250V (>500V for two) All 5 sensors are now at BNL for testing

I-V, C-V data Vfd: 50V No NG channels Breakdown V > 250V

Silicon tracker model for 2 nd round of R&D FPHX chip for read-out. – FPHX is the read-out chip of FVTX – 128ch/chip. 3bit ADC /ch. – Low power (64mw per chip) 5 strip layers + 2 pixel S2: 1 strip layer at R~60 cm ~1% X0 (2% in ref. design) S1ab: 2 strip layer at R~34 cm ~1% X0 total (2% in ref. design) S0ab: 2 strip layer at R~ 8 cm ~1% X0 total (2.7% in ref. design) P1: pixel at R~5 cm (reconfigured VTXP) 1.3% X0 P0: pixel at R~2.5cm (reconfigured VTXP) 1.3% X0 – All strips are 60  m x 9.6mm. S0b has a small stereo angle. – Overall material is ~5.6% radiation length. – Air cooling to achieve small radiation length – Small rad. length enables smaller over-all size and to keep the required momentum resolution to separate 3 Upsilon states – S0+S1+S2: ~8m 2 of silicon and 3.2M ch

3 sensors for strip layers Each sensor is divided in cells of 9.6m(z)x7.68mm active area. Each cell consists of 128 strips of 60  m x 9.6mm S2, S1, S0 sensors are made of 12x10, 6x10, and 2x10 cells, respectively 1 ch in S2 read 6 strips and 1 ch in S1 read 3 strips to save channel counts. Channel occupancy is ~0.2% in S1 and 0.1% in S1 in central Au+Au. Bonding pads for 10 FPHXs S2 sensor Bonding pads for 10 FPHXs S1 sensor Bonding pads for 10 FPHXs

Concept of FPHX based module (S1) This is a concept of a sensor module with FPHX read-out It is made of – Sensor of (6 x 10) cell structure. Each cell has 128ch of 80um x 9.6mm strips – A “ROC” (or “HDI”) of 10 FPHX chips. They are attached at the top and the bottom of the sensor – The “ROC” is electrically equivalent to the “small HDI” of FVTX so that it can be read- out by a FVTX test bench ROC of 10 FPHX chip

Prototype ladder A full size ladder requires many SMs. Perhaps ~half ladder for S1 and S2 is a realistic goal? ROC or Hybrid Silicon SensorSVX4 Support/cooling S1a/b ladder (double layer) S2 ladder (single layer)

Concept of S1 barrel (middle layer) 4.6cm active area; 6.4cm total (9mm wings) 44 ladders. (22 at R=30.8+/-1.0; 22 at R=33.1+/-1.0

Plan and status of 2 nd round R&D in Japan Plan: – Develop prototype S1 sensor (~5cm x 10cm, 2 sensors per wafer) at Hamamatsu – Develop read-out FPC for the sensor. – Assemble them into prototype sensor module – Test and evaluate the silicon module using FVTX test bench – About half year for the full cycle of R&D – Design and protoype of the mechanical support /cooling structure – 2 nd round of sensor module prototype in the later half of the year Goal: Protype of a full ladder at the end of JFY Status: – Started design of prototype S1 sensor at Hamamatsu. I expect that the sensor prototype will be delivered in September – Started design of read-out FPC at a FPC company near Tokyo with consultation with a wire-bonding and assembly firm. I expect that FPC will be availabe by the delivery of the sensor – Starting the mechanical/cooling design (very preliminary stage)

HPK design of S1 sensor Received from HPK today (2015/06/16)

R&D status and plan Sensor: HPK – Conceptual design done. (prevous slides) Flexible Printed Circuit: YAMASHITA Materials – Visit the company on 6/2 for discussion (YA, Nakagawa, Mitsuka, Taketani, Nagashima) – Layout design is on going – Rough cost estimate Wire-bonding/Assembly: HAYASHI – Discussion at RIKEN on 6/4 – Rough cost estimate for prototyping Goal of the first round of prototype: – both of the sensor and FPC by this fall (3months) – Assembly at Hayashi (1 month) – Test the module at RIKEN using the FVTX test bench (1month) Start / order the 2 nd round prototype in this JFY

Recent progress 1 st round of FPC layout (6 layers) by Yamshita Expected Upsilon mass resolution (calculated by Tony Frawley) 100 MeV with 65cm maximum radius

Effort for non-US funding for the tracker I submitted a large KAKENHI grant proposal to JSPS last October – JSPS is the main funding agency in Japan. Its function is similar to NSF in the US Grant Title: sPHENIX experiment: study of quark gluon plasma by using jet probes The grant asked for total of 5 oku yen (~$5M) over 5 years from JFY2015 to JFY2019. – The end date of JFY2019 is March 2020 ~ end of sPHENIX construction – In the JSPS grant system, we receive the full amount of the allocated fund. Overhead will be provided separately. The grant passed the first stage of selection and we went to a hearing on March 26. – About 20% of applicants can go to a hearing. Half of them are approved. Unfortunately, my proposal was not accepted after the hearing. I will try again this year.

Summary sPHENIX silicon tracker concept and requirements First prototype sensor delivered. – Very good result, according to the test by HPK Plan and status of the 2 nd round R&D – Use FPHX chip to reduce heat load  thinner tracker – Develop prototype sensor modules in ~half year and a prototype ladder in ~1 year – Design of sensor and FPC started.