2 nd International Conference on Technology and Instrumentation in Particle Physics Chicago June 8 th – 14 th 2011 Operational experience and aging studies.

Slides:

Advertisements

Similar presentations

Numbers Treasure Hunt Following each question, click on the answer. If correct, the next page will load with a graphic first – these can be used to check.

Advertisements

Warm Up Problem of the Day Lesson Presentation Lesson Quizzes.

F.Pastore II Workshop sulla fisica di ATLAS e CMS Oct Trigger di primo livello per gli esperimenti ATLAS & CMS ad LHC F.Pastore INFN Sezione.

Radiation damage in silicon sensors

LHCb Alignment 12 th April 2007 S. Viret Coseners Forum « LHC Startup » 1. Introduction 2. The alignment challenge 3. Conclusions.

Micron detector testing in Liverpool G. Casse – O. Lodge Laboratory, University of Liverpool.

TIME 2005: TPC for the ILC 6 th Oct 2005 Matthias Enno Janssen, DESY 1 A Time Projection Chamber for the International Linear Collider R&D Studies Matthias.

Break Time Remaining 10:00.

S. N. HOM Impedance in Vacuum … 1 of 40 Sasha Novokhatski SLAC, Stanford University Machine-Detector Interface Joint Session April 22, 2005 HOM Impedance.

1 ISMD 2005I. Ripp-Baudot Heavy flavour production results from DØ Run II Isabelle Ripp-Baudot IReS Strasbourg / IN2P3 for the DØ collaboration International.

PP Test Review Sections 6-1 to 6-6

10/24/2003Yu Chul Yang(CHEP,KNU) Layer0 Prototype Test Abstract,,,,,,,, Shabeer Ahmad Mian( ),,,, ( ),,, ( ). We have carried out prototype test for Silicon.

Bellwork Do the following problem on a ½ sheet of paper and turn in.

Clock will move after 1 minute

Select a time to count down from the clock above

B. List, ETH Zürich Page 1 Report from H1: PRC Open Session, H1: Status and Prospects Benno List Institute for Particle Physics, ETH Zürich.

H1 SILICON DETECTORS PRESENT STATUS By Wolfgang Lange, DESY Zeuthen.

Technical Board, 12 July 2005Børge Svane Nielsen, NBI1 Status of the FMD Børge Svane Nielsen Niels Bohr Institute.

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

New Operation Scenarios for Severely Irradiated Silicon Detectors G. Casse University of Liverpool 1 VERTEX 2009, Mooi Veluwe (NL) September 2009.

The Intermediate Silicon Layers detector OUTLINE ISL inside CDFII Why the ISL? Conceptual Design Ladders and Spaceframe Rasnik Online Alignment System.

CDF Run II Silicon John Zhou Rutgers University Z ee.

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.

November 3-8, 2002D. Bortoletto - Vertex Silicon Sensors for CMS Daniela Bortoletto Purdue University Grad students: Kim Giolo, Amit Roy, Seunghee.

SVX-II David Stuart, UC Santa Barbara May 11, 2006 David Stuart, UC Santa Barbara May 11, 2006.

ATLAS SCT module performance: beam test results José E. García.

Sensors for CDF RunIIb silicon upgrade LayerR min (cm)1 MeV eq-n cm * * * * * *10.

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.

February 19th 2009AlbaNova Instrumentation Seminar1 Christian Bohm Instrumentation Physics, SU Upgrading the ATLAS detector Overview Motivation The current.

Bond with current pulses Bond without current pulses A closer look with frames/second video equipment Single frames have been digitized and a quantitative.

SVX4 chip 4 SVX4 chips hybrid 4 chips hybridSilicon sensors Front side Back side Hybrid data with calibration charge injection for some channels IEEE Nuclear.

10 th INTERNATIONAL CONFERENCE ON INSTRUMENTATION FOR COLLIDING BEAM PHYSICS Budker Institute of Nuclear Physics, Siberian Branch of Russian Academy of.

Scientific Highlights : CDF Experiment 1.Introduction 2.CDF Run-II detector 3.Phyiscs highlights B Physics, Top, Higgs, … to be continued by Rob October.

Radiation Damage in the CMS Strips Tracker Christian Barth on behalf of the CMS Tracker Collaboration.

Semi-conductor Detectors HEP and Accelerators Geoffrey Taylor ARC Centre for Particle Physics at the Terascale (CoEPP) The University of Melbourne.

June 28, 2002BEACH2002 B Physics at the Tevatron B Physics at the Tevatron Jack Cranshaw Texas Tech University For the CDF and D0 Collaborations.

P5 recommendation on Tevatron running Report of June 8 meeting FNAL.

1 Beam Induced Power Supply Failures at CDF and D0 R.J. Tesarek Fermilab 11/30/04.

LHCb VErtex LOcator & Displaced Vertex Trigger

Thin Silicon R&D for LC applications D. Bortoletto Purdue University Status report Hybrid Pixel Detectors for LC.

Brookhaven National Laboratory March 2 th 2012 The CDF Run II Silicon Vertex Detectors: operational experience, aging studies and trigger applications.

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.

Technology Overview or Challenges of Future High Energy Particle Detection Tomasz Hemperek

18 March 2009 Thomas Bergauer Prototype batch of DSSD from commercial vendors & Proposal for SVD Layout HEPHY Vienna.

All Experimenters MeetingDmitri Denisov Week of July 7 to July 15 Summary  Delivered luminosity and operating efficiency u Delivered: 1.4pb -1 u Recorded:

Run Iib Workshop Dec 12-13, 2002 Silicon sensors procurement and quality assurance WBS Regina Demina Kansas State University.

On a eRHIC silicon detector: studies/ideas BNL EIC Task Force Meeting May 16 th 2013 Benedetto Di Ruzza.

Production Readiness Review of L0/L1 sensors for DØ Run IIb R. Demina, August, 2003 Irradiation studies of L1 sensors for DØ 2b Regina Demina University.

Ideas for Super LHC tracking upgrades 3/11/04 Marc Weber We have been thinking and meeting to discuss SLHC tracking R&D for a while… Agenda  Introduction:

R. Lipton Vertex ‘98 Santorini, Greece The D0 Silicon Microstrip Tracker (D0SMT) Outline  Design  Detector Studies Coupling capacitors Radiation Damage.

Robert R. Wilson Prize Talk John Peoples April APS Meeting: February 14,

A New Inner-Layer Silicon Micro- Strip Detector for D0 Alice Bean for the D0 Collaboration University of Kansas CIPANP Puerto Rico.

F Monitor of Beam in the Abort Gap Randy Thurman-Keup DOE Review of Tevatron Operations at FNAL March 29-31, 2005 a.k.a. Abort Gap Integrator (AGI)

The Collider Detector at Fermilab (aka CDF) Jennifer Pursley Intermediate Seminar Oct. 28, 2003.

Performance of the LHCb Vertex Locator Thomas Latham (on behalf of the LHCb VELO group) 11/06/20111TIPP Chicago.

Atlas SemiConductor Tracker final integration and commissioning Andrée Robichaud-Véronneau Université de Genève on behalf of the Atlas SCT collaboration.

Making Tracks at DØ Satish Desai – Fermilab. Making Tracks at D-Zero 2 What Does a Tracker Do? ● It finds tracks (well, duh!) ● Particle ID (e/ separation,

Tracking detectors/2 F.Riggi.

Status of the CDF II silicon tracking system

Update on Annealing Studies for Severely Irradiated Silicon Detectors

Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC

14 paesi, 62 universita’ e laboratori

The Pixel Hybrid Photon Detectors of the LHCb RICH

Vertex Detector Overview Prototypes R&D Plans Summary.

Koji Ueno National Taiwan U.

Beam Test Results for the CMS Forward Pixel Detector

Presentation transcript:

2 nd International Conference on Technology and Instrumentation in Particle Physics Chicago June 8 th – 14 th 2011 Operational experience and aging studies on the CDF Run II Silicon Vertex Detectors Benedetto Di Ruzza on behalf of the CDF II Silicon Operation Group

06/11/2011 TIPP 2011 Benedetto Di Ruzza2 OUTLINE 1) The Tevatron 2) The CDF II detector 3)The CDF II silicon subdetectors 4)Silicon aging studies 5) Conclusions

06/11/2011 TIPP 2011 Benedetto Di Ruzza3 The Tevatron and the CDFII detector

Fermilab accelerators chain 406/11/2011 TIPP 2011 Benedetto Di Ruzza

5 The Tevatron BS=Beam sync ticks =132ns Bunches structure Available Pbars ( ) I nitial luminosity record: 4.05 x (cm -2 s -1 ) Mean Pbar production efficiency: ~ 22 x10 -6 Mean Pbar Accumulation rate: ~ 25x (hr -1 )

06/11/2011 TIPP 2011 Benedetto Di Ruzza 6

06/11/2011 TIP 2011 Benedetto Di Ruzza7 Dose rate during beam dump Clean abort Quench

06/11/2011 TIPP 2011 Benedetto Di Ruzza8 Dose rate during data taking Dose rate

06/11/2011 TIPP 2011 Benedetto Di Ruzza9 Beam doses during data taking

06/11/2011 TIPP 2011 Benedetto Di Ruzza10 Beam condition during data taking

06/11/2011 TIPP 2011 Benedetto Di Ruzza11 The CDFII Detector

06/11/2011 TIPP 2011 Benedetto Di Ruzza12 L00 1 Layer ( ISL) The Silicon Detectors

06/11/2011 TIPP 2011 Benedetto Di Ruzza13 The CDFII Silicon detectors L00: Single-sided strips: “Narrows” (SGS Thomson and 2 Microns) “Wides” (Hamamatsu). SVX: Double-sided strips: Layers 0,1,3 (Hamamatsu) perpendicular strips, Layers 2,4 (Micron) small angled strips. ISL: Double-sided strips: (Hamamatsu+Micron) small angled strips OVERVIEW

06/11/2011 TIPP 2011 Benedetto Di Ruzza14 <== X-Y (r-phi) and Y-Z (r-z) views The Silicon Detectors L00 detail ==> Beam pipe Cooling lines narrow sensors wide sensors carbon support

06/11/2011 TIPP 2011 Benedetto Di Ruzza15 The Silicon Detectors SVXII detail: 3 barrels 5 layers 12 wedges SVXII: the readout is used in the trigger too

06/11/2011 TIPP 2011 Benedetto Di Ruzza16 The Silicon Detectors: ISL ISL central ISLforward: (inner and external barrels) ISL detail

06/11/2011 TIPP 2011 Benedetto Di Ruzza17 Radiation Field inside the detector

06/11/2011 TIPP 2011 Benedetto Di Ruzza18 Radiation damage

06/11/2011 TIPP 2011 Benedetto Di Ruzza19 Aging studies: variables of interest

06/11/2011 TIPP 2011 Benedetto Di Ruzza20 Depletion Voltage M.Moll, PhD Thesis, (1992) UniHamburg ;

06/11/2011 TIPP 2011 Benedetto Di Ruzza21 Depletion voltage Measurement

06/11/2011 TIPP 2011 Benedetto Di Ruzza22 Depletion Voltage study – Signal Vs. Bias

06/11/2011 TIP 2011 Benedetto Di Ruzza23 Depletion Voltage study – Signal Vs. Bias

Depletion Voltage Projections L00-L0 24 Prediction for L00 Prediction for SVX-L0 06/11/2011 TIPP 2011 Benedetto Di Ruzza

Very preliminary result on L /11/2011 TIPP 2011 Benedetto Di Ruzza Studies still ongoing

06/11/2011 TIPP 2011 Benedetto Di Ruzza26 Depletion Voltage study Noise Vs. Bias GOOD: does not require beam time BAD: not possible for single side strip or after inversion type

06/11/2011 TIPP 2011 Benedetto Di Ruzza27 Signal / Noise projection

06/11/2011 TIPP 2011 Benedetto Di Ruzza28 Not only the sensors are in a radiation environment VME crates SY527

Wirebond Resonances: Problems induced by trigger rates: 06/11/2011 TIPP 2011 Benedetto Di Ruzza29

06/11/2011 TIPP 2011 Benedetto Di Ruzza30 Other Operational Challenges

06/11/2011 TIPP 2011 Benedetto Di Ruzza31 Conclusions 10

Benedetto Di Ruzza32 Back-up slides

Measured Radiation Field 33 Radiation field measured with TLDs outside the silicon volume in NIM A (2003) Bias current evolution consistent with this radiation dose

Benedetto Di Ruzza34 Inversion point (SGS Thomson)

Benedetto Di Ruzza35 Silicon D.A.Q. for SVX II

Benedetto Di Ruzza36 Evolution of Bias currents (R. J. Tesarek et al. NSS 2003)

Benedetto Di Ruzza37 Depletion Voltage

Benedetto Di Ruzza38 Depletion Voltage Projection L1

Benedetto Di Ruzza39 ISL cooling lines

40

Benedetto Di Ruzza41 SVXII.

Benedetto Di Ruzza42

43 Laser diode/photo diode

44

45 ISL

46 ISL

Benedetto Di Ruzza47 Readout Chip Accounting

48 END