Double Stack Tracking Trigger Strawman
|
|
- Arabella Bennett
- 5 years ago
- Views:
Transcription
1 Double Stack Tracking Trigger Strawman
2 Scope of this Discussion: Outer Tracker The region of the inner-most Pixel Layers is fundamentally challenging g at the SLHC, especially for the Sensor Technology One may speculate as to the most promising way forward B-tagging, e/γ discrimination remain Very Important Assume 4 Layers of Fine-Pitch Pixels To be better defined Here focus on Outer Tracker Assume boundary between inner-most Pixel Layers and Outer Tracker is somewhere between 20 ~ 40cm In any future baseline layout, Outer Tracker and inner-most Pixel Layers will have to make a coherent Tracking System
3 CMS from LHC to SLHC cm -2 s At SLHC CMS faces new challenges, in particular for both Tracking and Triggering I. Osborne
4
5 An L1 Track Trigger for SLHC is not an Elective Project Joel
6 Required Functionality L1 Trigger Confirmation of Isolated High-pt μ Candidates Fast, Efficient & Clean Tracking Excellent Pt resolution Isolation Increased Rejection of fake e/γ Candidates Match with Track (nb conversions ) Isolation Tau Jet trigger Low Multiplicity, Isolation MET? Clean up High Pile-up environment Rejection of Uncorrelated Combinations, from different primary vertex? Match with Tracks at Vertex? Factor ~ 100 reduction For same Pt threshold
7 Required Functionality L1 Trigger Confirmation of High Pt Track Candidates Tracks with Pt above 15 ~ 20 GeV Excellent Efficiency Good Pt resolution Isolation Tracks with Pt above ~ 2 GeV Good Efficiency Longitudinal Vertex association Tracks with Pt above ~ 2 GeV Good Z Vertex resolution
8 Local Occupancy Reduction Cannot possibly transfer all Tracker data at 40MHz! Crossing Frequency / Event Read-Out ~ 40MHz / 100kHz ~ 1 / 400 L1 Data reduction by a factor of 100 ~ 200 is a reasonable target For L1 Trigger propose to transfer only hits from tracks with Pt > ~ 2 GeV The aim is to provide useful Isolation information Tracks with Pt > ~ 2 Gev are less than 1% of the Tracks inside acceptance This corresponds to the maximum plausibly manageable L1 data rate In addition, must provide means of rapidly & reliably identifying high Pt (isolated) tracks ( Pt > 15 ~ 25 GeV)
9 Local Occupancy Reduction Tracks with Pt > 1GeV < 10% of Tracks in acceptance Tracks with Pt > 2.5 GeV < 10% of the remaining Tracks
10 Local Occupancy Reduction with Local Track Vectors J. Jones (~2005) CMS Tracker SLHC Upgrade Workshops α
11 Local Occupancy Reduction with Local Track Vectors Pairs of Sensor Planes, for local Pt measurement High Pt tracks point towards the origin, low Pt tracks point away from the origin Use a Pair of Sensor Planes, at ~mmdistance Pairs of Hits provide Vector, that measure angle of track with respect to the origin Note: angle proportional to hit pair radius J. Jones (~2005) CMS Tracker SLHC Upgrade Workshops α Keep only Vectors corresponding to high Pt Tracks
12 Local Occupancy Reduction a Hierarchical scheme with Double Stacks Collect Pairs of Hits from each sensor doublet & match into Track Stub Pass onto L1 Trigger Local Information Gathering, and Processing Hierarchy ~2mm ~40mm Collect hits from each sensor & match Hit Pairs Collect hits from each sensor & match Hit Pairs Within a Stacked-Sensor Module Collect Hits from each Sensor Match into Hit Pairs & Reject Hit Pairs from Very low Pt Tracks: Pt < ~ 1GeV Nb one datum / Hit Pair Within a Double Stack Collect Hit Pairs from each Sensor Doublet Module Match into Track Vectors & Reject Track Vectors with Pt < ~ 2GeV Transmit to USC for High Pt & Isolation L1 Track Trigger Primitives
13 Recent results for a Stack of closely spaced sensors: pitch ~ 100um*2.4mm (M. Pesaresi) High rejection factors possible Mark Pesaresi Much Sharper Threshold For Low Threshold Value
14 Recent results for a Stack of closely spaced sensors: pitch ~ 100um*2.4mm (M. Pesaresi) Mark Pesaresi No useful discrimination at Pt ~ 20 GeV
15 Recent results for a pair of Double Stacks spaced ~ 10cm apart (M. Pesaresi) Excellent discrimination up to Pt ~ 20 GeV Mark Pesaresi
16 CMS SLHC Tracker Straw Man Layout Illustrations R-Phi Hermitic Double Stacks: get all 4 hits in one ROD or in the neighbor No communication across r-phi stacks ~ few cm ~mm
17 Full Double Stack Trigger Tracker Straw Man Layout Basic L1 Tracker Trigger concept: Local Data Reduction based on Track Vectors An r-phi hermetic Double Stack arrangement of BEAMs is proposed Rapid L1 High Pt Track identification (10~25 GeV), in hermetic r-phi sectors Isolation criteria with lowest possible Pt threshold (~ 2 GeV) The Double Stack layers will also provide Tracking Track Reconstruction for the HLT & Off-line should be very fast Track Parameters should be of high quality (to be verified in detail) The use of ~mm long Pixels provides opportunity for primary vertex association of Track Trigger Primitives The BEAMs provide opportunities for Material Budget Reduction
18 Stacked Tracking Trigger Straw Man This Simple Concept drives all aspects of the System, and Defines Requirements and Challenges throughout the System Module Sensors; Alignment; On Module Connectivity, Data Transmission & Reduction; Module I/O and Interface to ROD; Power & Cooling BEAM Module Alignment; On BEAM Data Transmission & Reduction; Power Distribution; Mechanics & Cooling Off-Detector BEAMt to USCD Data Transmission; i Tracking Ti Trigger Primitives; Pi iti Event tread- Out; CTRL System; Power System; Cooling System
19 Stacked Tracking Trigger Straw Man This Simple Concept drives all aspects of the System, and Defines Requirements and Challenges throughout the System Module Sensors; Alignment; On Module Connectivity, Data Transmission & Reduction; Module I/O and Interface to ROD; Power & Cooling BEAM Module Alignment; On BEAM Data Transmission & Reduction; Power Distribution; Mechanics & Cooling Off-Detector BEAM to USC Data Transmission; i Tracking Trigger Primitives; iti Event Read- Out; CTRL System; Power System; Cooling System
20 Some Numbers Basic Input: Occupancy at at tr ~ 35cm (TIBL2R Radius) Typical ~ 2 hits / cm 2 / 25ns Maximum < 10 * 2 = 20 hits / cm 2 / 25ns Strip Occupancy ~ 120MHz / cm 2 at R = 25cm Strip Occupancy ~ 80MHz / cm 2 at R = 34cm Strip Occupancy ~ 40MHz / cm 2 at R = 50cm 1/2 Strip Occupancy ~ 20MHz / cm 2 at R = 60cm 1/2 (Geoff Hall, compilation of full simulation results from Ian Tomalin) Nb these occupancy are for 320um~500um thick sensors: 2 ~ 4 hits/cluster Assume Reduction Factor ~ 2 from clustering To be verified Crossing Frequency / Event Read-Out ~ 40MHz / 100kHz ~ 1 / 400 L1 Data reduction by a factor of 100 ~ is a reasonable target
21 Some Numbers Material Budget ~ Material / cm 2 Consider rates and power / cm 2 Nb normalize to cm 2 of Silicon 1 module = 2 sensitive layers = 2 * x*y cm 2 (eg 2 * 100cm 2 ) Present CMS Tracker Event Read-Out ~ 4 channels / cm 100KHz Data Rate ~ 4MHz / cm 2 (analogue info ~ 10bits equivalent) Present CMS Tracker Power Inside Volume ~ 33kW over ~ 210m 2 Power Density ~ 16mW /cm 2 inside Tracking volume 6 Single-Sided + 4 Double-Sided = 14 Sensitive Layers
22 Data Transmission, Reduction, Power Density In the following Assume Zero Suppressed Read-Out Data rates ~ driven by Occupancy, NOT by Channel Count De-randomized Read-Out from Module to USC Available Bandwidth ~ Average Bandwidth, with * 2 safety margin Non De-randomized within Module: Available Bandwidth ~ 10 * Average Reduce Output Data Rates from Module by ~ 2 * 10 1 pair of accepted clusters = 1 datum per Hit Pair Output from Module Accept ~ 1 / 10 Hit Pairs: Pt Threshold 1 ~ 2 GeV Reduce Output Data Rates from ROD by ~ 5 2 accepted cluster pairs = 2 data per Track Vector Output from ROD Accept ~ 1 / 5 Track Vectors: Pt Threshold ~ 2GeV
23 Data Transmission, Reduction, Power Density In the following Assume Pixel Dimension ~ 100um * 1mm Pixels /cm 2 (more on this later) ~ 18 bits / L1 hit Address & Time Stamp info within Module Assume no analogue information for L1 ~ 24 bits / L1 hit Address & Time Stamp info from Module 32 bits / Read-Out hit info inside Tracker Assume ~ 8 bits analogue information for Read-Out Nb if Short Strips ~ 32bit address field is reduced by ~ 5bits ~ 20% reduction in Address Information for ~ 32 fewer channels / cm 2
24 Data Transmission, Reduction, Power Density Within a Doublet-Sensor Module: Un-terminated Lines Only transmit from one sensor plane to the other Transmission distance ~ few mm Input * Output Data reduction ~ 2 * 2 * 10 Power driven by by Actual Usage Available ~ 10 * Average Energy/bit of Link over ~ few mm < 2pJ/bit (1pJJ/bit possible?) Transmission rate ~ 320Mb/s (1Gb/s possible?) Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 400Mb/s < 4Gb/s Read-Out ~ 6Mb/s < 60Mb/s Power / cm 2 Average Bandwidth Available Bandwidth L1 ~ 1mW < 10mW Read-Out
25 Data Transmission, Reduction, Power Density Within a Doublet-Sensor Module: Un-terminated Lines Only transmit from one sensor plane to the other Transmission distance ~ few mm Input * Output Data reduction ~ 2 * 2 * 10 Power driven by by Actual Usage Available ~ 10 * Average Energy/bit of Link over ~ few mm < 2pJ/bit (1pJJ/bit possible?) Transmission rate ~ 320Mb/s (1Gb/s possible?) Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 400Mb/s < 4Gb/s Read-Out ~ 6Mb/s < 60Mb/s Links/Chip ~ 6cm 2 Average Bandwidth Available Bandwidth L1 ~ 6 ~ 60 Read-Out
26 Data Transmission, Reduction, Power Density To the End of a ROD ~ PP1: Transmission Line Transmission distance 3 ~ 10m Input * Output Data reduction ~ 200 Power driven by Available Bandwidth (~ 2 * Average) Energy/bit for Link over ~ 10m < 20pJ/bit (10pJ/bit over ~ 1m) Transmission Rate ~ 1Gb/s (is 1Gb/s possible?) Includes Clock & Error Recovery Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 50Mb/s ~ 100Mb/s Read-Out ~ 6Mb/s ~ 12Mb/s Power / cm 2 Average Bandwidth Available Bandwidth L1 ~ 1mW ~ 2mW Read-Out <0.1mW ~ 0.1mW
27 Data Transmission, Reduction, Power Density To the End of a ROD ~ PP1: Transmission Line Transmission distance 3 ~ 10m Input * Output Data reduction ~ 200 Power driven by Available Bandwidth (~ 2 * Average) Energy/bit for Link over ~ 10m < 20pJ/bit (10pJ/bit over ~ 1m) Transmission Rate ~ 1Gb/s (is 1Gb/s possible?) Includes Clock & Error Recovery Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 50Mb/s ~ 100Mb/s Read-Out ~ 6Mb/s ~ 12Mb/s Links/Module ~ 200cm 2 Average Bandwidth Available Bandwidth L1 ~ 10 ~ 20 Read-Out ~ 1 ~ 2
28 Data Transmission, Reduction, Power Density To USC: Optical Link Transmission distance ~ 100m Input Data Reduction ~ 200 Power driven by Available Bandwidth (~ 2 * Average) Energy/bit for Link over < 200pJ/bit (100pJ/bit possible?) Transmission Rate = 10Gb/s Includes Clock & Error Recovery Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 10Mb/s ~ 20Mb/s Read-Out ~ 6Mb/s ~ 12Mb/s Power / cm 2 Average Bandwidth Available Bandwidth L1 ~ 2mW ~ 4mW Read-Out ~ 15mW 1.5mW ~ 3mW
29 Data Transmission, Reduction, Power Density To USC: Optical Link Transmission distance ~ 100m Input Data Reduction ~ 200 Power driven by Available Bandwidth (~ 2 * Average) Energy/bit for Link over < 200pJ/bit (100pJ/bit possible?) Transmission Rate = 10Gb/s Includes Clock & Error Recovery Data Rates / cm 2 Average Bandwidth Available Bandwidth L1 ~ 10Mb/s ~ 20Mb/s Read-Out ~ 6Mb/s ~ 12Mb/s Links/Module ~ 200cm 2 Average Bandwidth Available Bandwidth L1 ~ 1/4 ~ 1/2 Read-Out ~ 1/8 ~ 1/4
30 Data Transmission, Reduction, Power Density At R ~ 35cm Based on 1/2*10 off Module * 1/10 off ROD data rate reduction Power for Data Transmission within Module L1@ 40MHz ~ 1mW/cm 2 100kHz < 0.1mW/cm 2 Power for Data Transmission i To the End of a ROD 40MHz ~ 2mW/cm 2 100kHz ~ 0.2mW/cm 2 Power for L1 Trigger Info Transmission To USC (at Bulk head) 40MHz ~ 4mW/cm 2 100kHz ~ 3mW/cm 2 Total Power Budget L1 & Read-Out Data R ~ 35cm Inside Tracking Volume: ~ 3mW/cm 2 At Bulkhead: ~ 7mW/cm 2
31 Data Transmission, Reduction, Power Density At R ~ 35cm Based on 1 / 2*10 off Module * 1 / 10 off BEAM data rate reduction Total Power Budget L1 & Read-Out Data R ~ 35cm Inside Tracking Volume: ~ 3 mw/cm 2 Compares with ~ 16mW /cm 2 inside present Strip Tracker volume At Bulkhead: ~ 7mW/cm 2 A L1 Track Trigger based on the scheme presented here is NOT ruled out by the Power requirements for the L1 Data Transfer Challenges for Data Transmission & Reduction include: Module interconnect technology High rate (1Gb/s) Low Mass Link over length of BEAM De-randomized L1 data transfer protocol Hit Doublet & Track Vector Logic
32 Granularity: Short Strips vs Long Pixels The CMS Silicon Strip Tracker is extremely effective because: Excellent Quality of Pixel Seeds Fine strip pitch, from 80um to 200um each hit has high resolution and track parameters are rapidly constrained Strip length, from 10cm to 20cm results in cell size ~ 0.5mm 2 occupancy ~ 2% or less at Pattern recognition converges ~ unambiguously with first few hits => fast At SLHC occupancy 10~20 times higher Short Strips Strip length in range 1 ~ 2cm to maintain low occupancy Long Pixels es Pixel length in range 1 ~ 2mm => reduce occupancy to ~ Inner Pixel like 3D info => 3D Tracking without Stereo Layers Sufficient Z resolution at L1 to sort Trigger Primitives by Interaction Vertex
33 Granularity: Short Strips vs Long Pixels Comparative Performance Studies are Important Guidance Rejection of tracks from different interaction vertices at L1? Cost and Manufacturability are a Key Input Implications on System, Read-Out Architecture etc. Reliable projections of Power Dissipation/cm 2 are a Fundamental Input Short Strips vs Long Pixels Extrapolate from Strip Tracker APV25 to reduced capacitance short strips Extrapolate from Pixel ROC to larger capacitance long pixel Compare: Power, Material, Cost, Feasibility, Performance Pursue both approaches until these points are sufficiently well understood to draw some conclusions
34 Front-End Power for Long Pixel Tracker Power of present CMS Pixel ROC ~ 30uW / channel 100um * 150um Pixel, Power Density ~ 200mW / cm 2 Pixel Front-End Read-Out chip Power Density ~ 16 * Strips Pixel Channel Density ~ * Strips! Assume 20 ~ 30uW / channel for 100um * 1 ~ 2mm Long Pixels Private communication from Roland Results in ~ 20mW / cm 2 Compares with ~ 16mW /cm 2 inside present Strip Tracker volume Compares with ~ 3mW/cm 2 for Data Transmission inside TK Volume Long Pixel Channel Density 100 ~ 200 * Strips Long Pixels not ruled out by Front-End Power requirements
35 Straw Man Layout The Function of the Straw Man is to Illustrate the Underlying Ideas, for a CMS SLHC Tracker with L1 Trigger capability It is intended to highlight the Pros and Cons of these Ideas, to allow informed decisions down the line And to Provide a Framework to help Direct and Focus different Lines of Activity Performance Studies Sensors / Front-End Read-Out / Interconnects Module Functionality & Design Mechanics / Cooling and Services Integration Data Reduction and Data Transmission Improved Power Distribution Scheme, Local Voltage Regulation etc Material Budget Reduction and Optimization Off-Detector Data Processing Etc. On the way to a Base-Line Layout
36 Straw Man Layout The Function of the Straw Man is to Illustrate the Underlying Ideas, for a CMS SLHC Tracker with L1 Trigger capability It is intended to highlight the Pros and Cons of these Ideas, to allow informed decisions down the line And to Provide a Framework to help Direct and Focus different Lines of Activity An Effective L1 Track Trigger is a Major Challenge: A Straw-Man is Required in order to make Effective Progress On the way to a Base-Line Layout
37 Straw Man Layout: Double Stack Layers η 1040 Each Double Stack Layer requires 4/4 hits Minimal potentially viable configuration is 2 Double Stack Layers Require 1 OR the Other Double Stack L1 & Tracking Layers, with full acceptance up to η ~ 2.5: Each Layer provides 2 * 2 = 4 hits 2 Layers = 8 hits 2700
38 Straw Man Layout: 2 Double Stack Layers + Outer Tracker η Double Stack L1 & Tracking Layers, with full acceptance up to η ~ 2.5: Each Layer provides 2 * 2 = 4 hits 2 Layers = 8 hits 2700 Outer Tracker: Optimized for Tracking No L1 functionality Introduces 3 rd System, in two flavors
39 Straw Man Layout: 3 Double Stack Layers η 1040 Build on Minimal, Potentially Viable Parts Kit Focus the Effort Add complexity only if / when Needed Double Stack L1 & Tracking Layers, Each Layer provides 2 * 2 = 4 hits 3 Layers = 12 hits Single System provides Full L1 & Tracking functionality 2700
40 Build on Minimal, Potentially Viable Parts Kit Focus the Effort Add complexity only if / when Needed Hole above η ~ 1.7 Straw Man Layout: 3 Double Stack Layers η Double Stack L1 & Tracking Layers, with full acceptance up to η ~ 1.7: Each Layer provides 2 * 2 = 4 hits 3 Layers = 12 hits Single System provides Full L1 & Tracking functionality 2700
41 Build on Minimal, Potentially Viable Parts Kit Focus the Effort Add complexity only if / when Needed Use Short Forward Cylinders to Avoid Hole above η ~ 1.7 Straw Man Layout: 3 Double Stack Layers η Double Stack L1 & Tracking Layers, with full acceptance up to η ~ 2.1: Each Layer provides 2 * 2 = 4 hits 3 Layers = 12 hits 2700 Single System provides Full L1 & Tracking functionality Short FWD Cylinders close acceptance Total Silicon Surface ~ 375m 2 Present Tracker ~ 210m 2
42 Full Stacked Trigger Tracker Straw Man Layout Propose that a Full Stacked Trigger Tracker Straw Man be studied A a Potentially Viable Single Concept providing Both Tracking and Triggering Functions, and to establish its performance potential and possible shortcomings As a means of providing a focus for the System Design & defining sets of work-packages for each subsystem in the Upgraded Tracker As a Benchmark for alternative Stacked Trigger + Outer Tracker Layouts There are Many Challenges BUT CMS needs a viable Trigger for SLHC Robust L1 Track Trigger primitives are a Must An all Pixel Stacked Trigger Tracker will be Game Changing detector Just as the present CMS Tracker is a Game Changing g detector
43 Scope of the Tracking Trigger Project On Module Processing Off Detector Data Transmission On Rod Data Transmission To Trigger Power, Cooling, Mechanical Structures Sensors On Rod Processing Front End Electronics Interconnection Technology Off Detector Processing
44 Basic Units for Tracking Trigger Project Module Unit 100 * 100 * 2mm Sensors, FE Electronics, Interconnections, On module Processing Mechanical Structure 100 mm 40 mm 2mm 2700 mm On BEAM Data Transmission 100 mm 100 mm Power Unit ~12V in ~1.8V out C0 2 Cooling System
45 Basic Units for Tracking Trigger Project On Rod Processing Off Detector Processing Trigger Off Detector Data Transmission FED DAQ Cooling System Power System
46 Module Design Basic Units for Tracking Trigger Project Sensor, FEE, Interconnection, On Module Processing Construction On BEAM Data Transmission i On BEAM Processing Simulation Off Detector Data Transmission and Off Detector Processing System FEDs and DAQ system Engineering Powering and DCS System (Grounding and Shielding) and Cooling System Optimization Mechanical Layout and Structures
47 FNAL Tracking Trigger Summary The FNAL Workshop was an Opportunity to sign up additional US groups to the CMS SLHC Tracker Upgrade, and strengthen the present Tracker Collaboration This was very successful About 40 ~ 50 people attended the Tracking Trigger Sessions Many new groups signed on to work on various aspects of the proposed system There is a substantial re-focusing of people and developments, originally projected towards the ILC, on the CMS SLHC Tracker Upgrade Strong FNAL groups working on Vertical Integration (maps onto doublet module) and Very Low Mass Mechanics Next steps: consolidate newcomers into existing working groups Define goals, plan of work, milestones, etc.
48 Proposed Project Time Scales 2009 Define and prove the Viability of All Systems within the New Straw Man and Review Progress 2010 Optimize the Layout and System Developments in the light of the work in Prepare Demonstrators of all the Systems 2012 Prepare the TDR for an Upgraded Tracker Double January Stack 2009 Tracking Trigger Strawman
49 Straw Man Design Study: V0 Starting Point Strawman Design Study V0 Starting Point
50 Straw Man Design Study: V0 Starting Point Agree on basic inputs to layout Module size, Tiling strategy & Overlaps, Stacked Barrel layer radii & length, Agree on parameters to vary Pixel dimensions, Module Separation within Doublet, Doublet Separation within ROC, Cluster Finding Efficiency Agree on basic inputs to Structures & Materials in Tracking volume Module: Sensors, ROC, PCB, Connector, Mechanics, Power Dissipation ROD: Mechanics, Cooling, Data Transmission, Power Distribution, Controls & monitoring Mechanical Supports & End-Flanges, Manifolds & Connections Propose to start with day 0 set of educated guesses Then input more realistic estimates/targets Use Layout Task-Force Tools for consistent comparative studies etc
51 Straw Man Design Study: V0 Starting Point Progress since FNAL Workshop Working towards detailed V0 Starting Point Design Study Progressing on First pass through the system, from Front-End to Back-End See presentation by Bill Cooper on Layout and Mechanics
52 Straw Man Design Study: V0 Starting Point Sensor Characteristics Agree on basic inputs to layout Sensor Active Area Dimensions 9.4cm * 9.4cm * 160um Sensor Physical Dimensions 9.6cm * 9.6cm * 320um Tiling strategy in phi Propose High-Low as in TOB with no Lorentz Angle Tilt (Presently with Lorentz AngleTilt) Tiling strategy in Z Modules are butted end-to-end Overlaps in Phi Stacked doublets are hermetic in phi for tracks from IP Min. projective overlap between Stacked Doublets (4/4 hits) 2 ~ 4mm Provide overlap with up to 5mm radial displacement of IP Overlaps in Z No overlaps in Z: modules are butted end-to-end Clearances All sensor clearances > 1mm
53 Straw Man Design Study: V0 Starting Point Agree on basic inputs to layout Stacked-Doublet Barrel Super-Layer radii & length Layer 1 Radius ~ 30cm Length to η ~ 2.5 Layer 2 Radius ~ 50cm Length ~ 270cm to η ~ 2.5 Layer 3 Radius ~ 100cm Length ~ 270cm Forward Layers 1 & 2 Radius & Length to optimize η coverage
54 Straw Man Design Study: V0 Starting Point Agree on basic inputs to layout Stacked-Doublet Barrel Super-Layer Z overlap at η = 0 The 3 main stations are each ½ the length of the Tracker Ensure all hits over full length of IP contained in one or other ½ Barrel Guesstimate is Z Interlocking overlap 1 ~ 2cm; ΔR ~ 4mm Set Z overlap to to minimum required to ensure coverage η = 0 ~ 4mm 1 ~ 2cm
55 Straw Man Design Study: V0 Starting Point Agree on basic inputs to Structures & Materials in Tracking volume Module Sensors: Silicon Physical Dimensions: 9.6cm * 9.6cm * 320um ROC: Silicon 9.4cm * 9.4cm total coverage; 25um thickness Interposer/Interconnect: Silicon 11cm * 9.4cm * module separation within Doublet Remove ~ 50% of the material Cable & Connector 1 * 60 pin Flex Kapton Cables with low mass connectors Mechanics Protective Kapton envelope covering sensors: 50um thick High TC Carbon Composite heat spreader plates: 2 * 11cm * 10cm * 300~500um Remove ~ 50% of the material Power Dissipation: < 4W / Module + 0.8W / DC-DC ~ 5W Module + DC-DC <15mW/cm 2 ROC; < 3mW/cm 2 Data Transmission; i < 7mW/cm 2 Digitalit
56 Straw Man Design Study: V0 Starting Point Sensor to Read-Out Chip (ROC) Connections pitch ~ 100um * 1mm ROC to Interposer Connections density 40 ~ 100 / cm 2 Use ROC through -vias ROC 1 to ROC 2 Connections density ~ 20 ~ 80 / cm 2 Use Interposer through-vias Carbon Fiber heat spreader ~ 320um thick ~ 12um thick ROC 1 Sensor 1 0,5mm ~ 2.mm thick Interposer ROC 2 Kapton Sensor protection Sensor 2
57 Straw Man Design Study: V0 Starting Point Agree on basic inputs to Structures & Materials in Tracking volume ROD Mechanics Box-like structure supporting doublet modules on inner and outer faces 1000um thick high modulus CFC, with 50% coverage (50% material removed) Cooling Assume a cooling circuit above & one below doublet => 2 circuits for a ROD Not required for power rating May be needed for temperature homogeneity Assume CO 2 cooling, with 1.5/1.3mm outer/inner diameter pipes p Assume Copper-Nickel (TOB) or Titanium (TEC) Assume pipe embedded in Al heat spreader ~ 1.25mm * 4mm * 90mm
58 Straw Man Design Study: V0 Starting Point Agree on basic inputs to Structures & Materials in Tracking volume Cables Twisted pair with each strand = 150um Al with 20um Cu cladding (Roland) Used for Data Transmission, Power Distribution, Controls & Monitoring Data Transmission Assumes 1Gbps data electrical data transmission 24 * twisted pair cables / doublet module (1/ chip) Power Distribution Assume 10% worst case power loss on 6m long cable, from PP1 to module Assumes doublet module power dissipation ~ 4W Assumes DC-DC with 6 / 1 Voltage step-down close to module, 80% Efficiency 4 * twisted pair cables / doublet module Controls 4 * twisted pair cables / doublet module
59 Straw Man Design Study: V0 Starting Point Agree on basic inputs to Structures & Materials in Tracking volume DC-DC converters: One pair of converters / Doublet Module One for Analogue and one for Digital power Each converter consists of An IC with a high voltage power transistor Silicon, 500um thick * 1cm * 1cm A Toroid FR4 PCB, 3mm thick, 1cm * 1cm, 50% of material removed Two Copper layers, each 20um thick, 1cm * 1 cm The pair of converters is housed on a PCB & shielded FR4 PCB, 500um thick, 3cm * 3cm Cu circuit, 4 layers, 10um thick, 3cm * 3cm, 50% coverage Cu shield, 1 layer, 20um thick, 2* (2cm * 2cm)
60 Straw Man Design Study: V0 Starting Point Agree on basic inputs to Structures & Materials in Tracking volume Mechanical Supports & End-Flanges For V0 assume ~ TOB 2 CF skins + spacers: 2mm thick CF, ~ 20% of material removed Manifolds & Connections Outside of Tracking volume
61 Straw Man Design Study: V0 Starting Point In the present Tracker, pipes & cable are light within Barrels They blow up when exit barrels: connectors, manifolds, routing There is a lot of Electronics : Inter-Connect Boards, Opto-hybrids, CCU etc
62 Straw Man Design Study: V0 Starting Point Preliminary Straw Man Material Budget indications based on initial set of assumptions Supports the potential advantage of long barrels: look forward to improved estimates Nb Red points are edges of short fwd barrels ~ 110% ~ 40% ~ 20%
63 Backup Slides
64 Straw Man Design Study: V0 Starting Point Agree on parameters to vary Pixel dimensions: phi pitch 80 ~ 100um ~ 120 Pixel dimensions: Z Length 1.0 ~ 1.5mm ~ 2.0 Module Separation within Doublet: 0.5 ~ 0.75mm ~ 1.0 Doublet Separation within ROD: 4.0 ~ 6.0cm ~ 8.0 Cluster Finding Efficiency: 90 ~ 98% ~ 99
65 Straw Man Design Study: Performance Potential Strawman Design Study Performance Potential
66 Straw Man Design Study: Performance Potential Tracking Trigger with Stacked-Doublet Tracker Single mu, pion, e, tau Inclusive Tracks in Min Bias SLHC Luminosity Environment L1 Trigger performance for Benchmark Channels
67 Straw Man Design Study: Performance Potential Hit Pairs within Stacks: Target data Reduction: 2 * 6 ~ 10 ~ 16 Get factor of 2 by transmitting single combined info for the cluster pair Range of Nominal Thresholds: ~ 1GeV ~ 1.5 Efficiency vs Pt over range of Nominal Thresholds Rate & reduction versus Nominal Threshold Purity versus Nominal Threshold Compare performance with/without cluster centroid interpolation
68 Straw Man Design Study: Performance Potential Track Vectors within Double Stacks Target data Reduction: 6 ~ 10 ~ 16 Range of Nominal Thresholds: 1.5 ~ 2GeV ~ 2.5 Efficiency vs Pt over range of Nominal Thresholds Rate & reduction versus Nominal Threshold Purity versus Nominal Threshold Pt Resolution Longitudinal Vertex Resolution vs Pt Compare performance with/without cluster centroid interpolation
69 Straw Man Design Study: Performance Potential Trigger Primitives from combined Double Stack Layers For 2 Inner Stacked Doublet Stations: require 1/2 Stations For all 3 Stacked Doublet Stations: compare 1/3 and 2/3 Stations Range of Nominal Low Pt Thresholds: 1.5 ~ 2GeV ~ 2.5 Range of Nominal High Pt Thresholds: 15 ~ 20GeV ~ 25 Efficiency vs Pt over range of Nominal Low & High Thresholds Rate versus Nominal Low & High Thresholds Purity versus Nominal Low & High Thresholds Pt Resolution Longitudinal Vertex Resolution vs Pt
70 Straw Man Design Study: Performance Potential Tracking with the Double Stack Straw Man Assume 4 Inner Pixel Layers, with 50um * 150um Pixels Single mu, pion, e, tau Inclusive Tracks in Min Bias SLHC Luminosity Environment Tracking Performance for Benchmark Channels Timing Performance Efficiency vs Pt & η Fake Rate vs Pt & η Pt Resolution vs Pt & η Impact Parameter & Longitudinal Vertex Resolution vs Pt & η
71 Straw Man Design Study: Performance Potential Using Kalman Filter CTF: Tracking with the Double Stack Straw Man Standard Tracking, with Pt > 1 GeV Iterative Tracking: 1 st iteration: Use only hits passing Low Pt Stack & Double Stack L1 cuts & reconstruct tracks with Pt > 1 GeV 2 nd iteration: add singlet hits to tracks already identified, refit etc. 3 rd iteration: Use remaining singlet hits, reconstruct tracks with Pt > 1GeV 4 th iteration: Use remaining singlet hits, reconstruct tracks with Pt > 0.5GeV
72 Straw Man Design Study: Performance Potential Tracking with the Stacked-Doublet Straw Man Develop algorithms adapted to Stacked-Doublet Layout Kalman Filter CTF starts from a seed, and combines seed/track hypothesis with compatible hit Could think of Kalman Filter Combinatorial Vector Track Finder (CTFV)? Treat Inner Pixels as Seed Generator Treat Double Stack Layers as Vector Generators Combine seed/track hypothesis with compatible Vector Iterative implementation, so finally use also singlet hits & extend to lowest Pt
73 Strawman Proposal Common usage Strawman Proposal Common usage
74 Straw Man Proposal from Wikipedia A "straw-man proposal", also known as an Aunt Sally, is a brainstormed simple business proposal intended to generate discussion of its disadvantages and to provoke the generation of new and better proposals. p Often, a straw man document will be prepared by one or two people prior to kicking off a larger project. In this way, the team can jump start their discussions with a document that is likely to contain many, but not all the key aspects to be discussed. As the document is revised, it may be given other edition names such as the more solid-sounding "stone-man", "iron-man", and so on, etc.
75 Straw Man Proposal from Mind Tools In a culture that values being right, the notion of constructing a straw man is difficult to embrace. Why spend time drafting something that, ultimately, isn't going to be used? If you can get past this perception you will be surprised at how useful the technique can be. One of its main advantages is that it forces you to do something. Taking too long to deliberate the merits of an idea or hypothesis can be costly, as you risk never making a decision at all. With a straw man, you force an early, if incomplete, decision. This ensures that a final decision will be reached because doing nothing means accepting a poor plan by default. Tip: Be very careful when you're using a Straw Man approach that people p understand what you're doing: The last thing you want is to develop a reputation for "coming up with half-baked ideas." Make sure that your document is clearly labeled as such, and that the people receive it understand what it is.
76 Straw Man Proposal from Mind Tools A straw man is also useful in ensuring that everyone involved has a tangible concept to work from. Otherwise, there is a risk that people are working with different pieces of the whole, different perceptions, and different, unstated assumptions, as they continue to research and discuss aspects of the idea or solution. The risk of using a straw man proposal is that, by definition, you are jumping to conclusions. Providing you are aware of this risk, you'll challenge, test, and retest the real solution and so use "jumping to a conclusion" as a vehicle to find a better conclusion.
77
78 Straw Man Layout: 3 Stacked Doublet Layers + Outer Tracker η Stacked Doublet L1 & Tracking Layers, with full acceptance up to η ~ 2.5: Each Layer provides 2 * 2 = 4 hits 3 Layers = 12 hits Minimize Stacked Doublet Layer Surface 2700 Outer Tracker: Optimized for Tracking No L1 functionality Introduces 3 rd System, in two flavors More Material in the Tracker Volume
79 Straw Man Layout: 2 Stacked Doublet + 3 Stacked Single Layers η Stacked Doublet L1 & Tracking Layers, 3St Stacked dsingle L1&T Tracking Layers: with full acceptance up to η ~ 2.5: Use Cluster Width Each Layer provides 2 * 2 = 4 hits Each Layer provides 2 * 1 = 2 hits 2 Layers = 8 hits 3 Layers = 6 hits Minimize Stacked Doublet Layer Surface Introduces 2 nd System flavor More Material in the Tracker Volume 2700
80 Full Stacked Trigger Tracker Straw Man Layout 12 Measurement Layers Organized in 3 Super-Layers Each Super-Layer consists of a Stack of Doublet Sensor Modules (4 measurement layers / Super-Layer) Inner Super-Layer ~ 30cm (Geometry of Inner Vtx layers?) Middle Super-Layer ~ 50cm Outer Super-Layer ~ 100cm
81 Full Stacked Trigger Tracker Straw Man Layout 12 Measurement Layers Organized in 3 Super-Layers Each Super-Layer consists of a Stack of Doublet Sensor Modules (4 measurement layers / Super-Layer) Can search for high Pt Track Stubs Independently in each Super-Layer Can Combine Super-Layers to ensure High Efficiency & Low Fake rate Can use for L1 Trigger And for Prompt Tracking at HLT
82 Full Stacked Trigger Tracker Straw Man Layout Material Budget Reduction Stack of Sensor Pairs provide opportunity for shared mechanics and services A Double-Sided ROD = 2 hits For 1.5 * X0 of Single-Sided ROD 6L Layers of fdouble Modules = 12hit hits For 9 * X0 of Single Module layer Current Tracker = 14 hits For 12 * X0 of Single Module layer (If all TOB - Like ) Stacking Doublets onto Beams could allow to further reduce X0 with respect to RODs?
83 Simulation and Performance Issues Basic Things to Check Hit Pair Pt Resolution & Discrimination Rate vs threshold Track Stub Pt Resolution & Discrimination Rate vs threshold Track Quality Combinatorial Complexity & Calculational Efficiency: L1 & HLT Fake Rate & Efficiency if require Single Hit Efficiency: 95%~99.5% 4/4 hits in sensor pair 1/2 vs 2/3 Track Stubs All the above varying the design parameters over the Plausible Range
84 Straw Man Design Study: V0 Starting Point In the present Tracker, pipes & cable are light within Barrels They blow up when exit barrels: connectors, manifolds, routing There is a lot of Electronics : Inter-Connect Boards, Opto-hybrids, CCU etc
85 Straw Man Design Study: V0 Starting Point Straw Man Material Budget estimate based on above assumptions: Supports the potential advantage of long barrels Straw Man design also does without Interconnects etc inside Tracker volume Nb Red points are edges of short fwd barrels ~ 160% No Pixels ~ 105% With present Pixels ~ 75% ~ 40% ~ 20% ~ 25%
CMS SLHC Tracker Upgrade: Selected Thoughts, Challenges and Strategies
: Selected Thoughts, Challenges and Strategies CERN Geneva, Switzerland E-mail: marcello.mannelli@cern.ch Upgrading the CMS Tracker for the SLHC presents many challenges, of which the much harsher radiation
More informationTrack Triggers for ATLAS
Track Triggers for ATLAS André Schöning University Heidelberg 10. Terascale Detector Workshop DESY 10.-13. April 2017 from https://www.enterprisedb.com/blog/3-ways-reduce-it-complexitydigital-transformation
More informationA common vision of a new Tracker is now essential It may not be final but a focus for shared efforts is now vital
CMS Tracker Phase II Upgrade planning A common vision of a new Tracker is now essential It may not be final but a focus for shared efforts is now vital G Hall New injectors + IR upgrade phase 2 Linac4
More informationTest Beam Measurements for the Upgrade of the CMS Phase I Pixel Detector
Test Beam Measurements for the Upgrade of the CMS Phase I Pixel Detector Simon Spannagel on behalf of the CMS Collaboration 4th Beam Telescopes and Test Beams Workshop February 4, 2016, Paris/Orsay, France
More informationPhase 1 upgrade of the CMS pixel detector
Phase 1 upgrade of the CMS pixel detector, INFN & University of Perugia, On behalf of the CMS Collaboration. IPRD conference, Siena, Italy. Oct 05, 2016 1 Outline The performance of the present CMS pixel
More informationExpected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC
Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC Noemi Calace noemi.calace@cern.ch On behalf of the ATLAS Collaboration 25th International Workshop on Deep Inelastic Scattering
More informationStatus of ATLAS & CMS Experiments
Status of ATLAS & CMS Experiments Atlas S.C. Magnet system Large Air-Core Toroids for µ Tracking 2Tesla Solenoid for inner Tracking (7*2.5m) ECAL & HCAL outside Solenoid Solenoid integrated in ECAL Barrel
More informationUpgrade of the CMS Tracker for the High Luminosity LHC
Upgrade of the CMS Tracker for the High Luminosity LHC * CERN E-mail: georg.auzinger@cern.ch The LHC machine is planning an upgrade program which will smoothly bring the luminosity to about 5 10 34 cm
More informationStatus of SVT front-end electronics M. Citterio on behalf of INFN and University of Milan
XVII SuperB Workshop and Kick Off Meeting: ETD3 Parallel Session Status of SVT front-end electronics M. Citterio on behalf of INFN and University of Milan Index SVT: system status Parameter space Latest
More informationWhat do the experiments want?
What do the experiments want? prepared by N. Hessey, J. Nash, M.Nessi, W.Rieger, W. Witzeling LHC Performance Workshop, Session 9 -Chamonix 2010 slhcas a luminosity upgrade The physics potential will be
More informationCMS Tracker Upgrade for HL-LHC Sensors R&D. Hadi Behnamian, IPM On behalf of CMS Tracker Collaboration
CMS Tracker Upgrade for HL-LHC Sensors R&D Hadi Behnamian, IPM On behalf of CMS Tracker Collaboration Outline HL-LHC Tracker Upgrade: Motivations and requirements Silicon strip R&D: * Materials with Multi-Geometric
More informationLayout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC
Layout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC Ankush Mitra, University of Warwick, UK on behalf of the ATLAS ITk Collaboration PSD11 : The 11th International Conference
More information2 nd ACES workshop, CERN. Hans-Christian Kästli, PSI
CMS Pixel Upgrade 2 nd ACES workshop, CERN Hans-Christian Kästli, PSI 3.3.2009 Scope Phase I (~2013): CMS pixel detector designed for fast insertion/removal Can replace system during normal shutdown Planned
More informationPrototyping stacked modules for the L1 track trigger
Prototyping stacked modules for the L1 track trigger tbc Aachen (tbc) D. Newbold, C. Hill Bristol University D. Abbaneo, K. Gill, A. Marchioro CERN P. Hobson Brunel University A. Ryd Cornell University
More informationSilicon Sensor and Detector Developments for the CMS Tracker Upgrade
Silicon Sensor and Detector Developments for the CMS Tracker Upgrade Università degli Studi di Firenze and INFN Sezione di Firenze E-mail: candi@fi.infn.it CMS has started a campaign to identify the future
More informationCMS Tracker Upgrades. R&D Plans, Present Status and Perspectives. Benedikt Vormwald Hamburg University on behalf of the CMS collaboration
R&D Plans, Present Status and Perspectives Benedikt Vormwald Hamburg University on behalf of the CMS collaboration EPS-HEP 2015 Vienna, 22.-29.07.2015 CMS Tracker Upgrade Program LHC HL-LHC ECM[TeV] 7-8
More informationThe LHCb Vertex Locator : Marina Artuso, Syracuse University for the VELO Group
The LHCb Vertex Locator : status and future perspectives Marina Artuso, Syracuse University for the VELO Group The LHCb Detector Mission: Expore interference of virtual new physics particle in the decays
More informationCMS Silicon Strip Tracker: Operation and Performance
CMS Silicon Strip Tracker: Operation and Performance Laura Borrello Purdue University, Indiana, USA on behalf of the CMS Collaboration Outline The CMS Silicon Strip Tracker (SST) SST performance during
More informationPoS(EPS-HEP2017)476. The CMS Tracker upgrade for HL-LHC. Sudha Ahuja on behalf of the CMS Collaboration
UNESP - Universidade Estadual Paulista (BR) E-mail: sudha.ahuja@cern.ch he LHC machine is planning an upgrade program which will smoothly bring the luminosity to about 5 34 cm s in 228, to possibly reach
More information`First ep events in the Zeus micro vertex detector in 2002`
Amsterdam 18 dec 2002 `First ep events in the Zeus micro vertex detector in 2002` Erik Maddox, Zeus group 1 History (1): HERA I (1992-2000) Lumi: 117 pb -1 e +, 17 pb -1 e - Upgrade (2001) HERA II (2001-2006)
More informationA Large Low-mass GEM Detector with Zigzag Readout for Forward Tracking at EIC
MPGD 2017 Applications at future nuclear and particle physics facilities Session IV Temple University May 24, 2017 A Large Low-mass GEM Detector with Zigzag Readout for Forward Tracking at EIC Marcus Hohlmann
More informationTowards a 10 μs, thin high resolution pixelated CMOS sensor system for future vertex detectors
Towards a 10 μs, thin high resolution pixelated CMOS sensor system for future vertex detectors Rita De Masi IPHC-Strasbourg On behalf of the IPHC-IRFU collaboration Physics motivations. Principle of operation
More informationA new strips tracker for the upgraded ATLAS ITk detector
A new strips tracker for the upgraded ATLAS ITk detector, on behalf of the ATLAS Collaboration : 11th International Conference on Position Sensitive Detectors 3-7 The Open University, Milton Keynes, UK.
More informationLarge Silicon Tracking Systems for ILC
Large Silicon Tracking Systems for ILC Aurore Savoy Navarro LPNHE, Universite Pierre & Marie Curie/CNRS-IN2P3 Roles Designs Main Issues Current status R&D work within SiLC R&D Collaboration Tracking Session
More informationThe LHCb Upgrade BEACH Simon Akar on behalf of the LHCb collaboration
The LHCb Upgrade BEACH 2014 XI International Conference on Hyperons, Charm and Beauty Hadrons! University of Birmingham, UK 21-26 July 2014 Simon Akar on behalf of the LHCb collaboration Outline The LHCb
More informationTracking Detectors for Belle II. Tomoko Iwashita(Kavli IPMU (WPI)) Beauty 2014
Tracking Detectors for Belle II Tomoko Iwashita(Kavli IPMU (WPI)) Beauty 2014 1 Introduction Belle II experiment is upgrade from Belle Target luminosity : 8 10 35 cm -2 s -1 Target physics : New physics
More informationThe Run-2 ATLAS. ATLAS Trigger System: Design, Performance and Plans
The Run-2 ATLAS Trigger System: Design, Performance and Plans 14th Topical Seminar on Innovative Particle and Radiation Detectors October 3rd October 6st 2016, Siena Martin zur Nedden Humboldt-Universität
More informationTracking and Alignment in the CMS detector
Tracking and Alignment in the CMS detector Frédéric Ronga (CERN PH-CMG) for the CMS collaboration 10th Topical Seminar on Innovative Particle and Radiation Detectors Siena, October 1 5 2006 Contents 1
More informationStatus of the LHCb Experiment
Status of the LHCb Experiment Werner Witzeling CERN, Geneva, Switzerland On behalf of the LHCb Collaboration Introduction The LHCb experiment aims to investigate CP violation in the B meson decays at LHC
More informationResolution studies on silicon strip sensors with fine pitch
Resolution studies on silicon strip sensors with fine pitch Stephan Hänsel This work is performed within the SiLC R&D collaboration. LCWS 2008 Purpose of the Study Evaluate the best strip geometry of silicon
More informationL1 Track Finding For a TiME Multiplexed Trigger
V INFIERI WORKSHOP AT CERN 27/29 APRIL 215 L1 Track Finding For a TiME Multiplexed Trigger DAVIDE CIERI, K. HARDER, C. SHEPHERD, I. TOMALIN (RAL) M. GRIMES, D. NEWBOLD (UNIVERSITY OF BRISTOL) I. REID (BRUNEL
More informationThe CMS Pixel Detector Upgrade and R&D Developments for the High Luminosity LHC
The CMS Pixel Detector Upgrade and R&D Developments for the High Luminosity LHC On behalf of the CMS Collaboration INFN Florence (Italy) 11th 15th September 2017 Las Caldas, Asturias (Spain) High Luminosity
More informationVertex Detector Mechanics
Vertex Detector Mechanics Bill Cooper Fermilab (Layer 5) (Layer 1) VXD Introduction The overall approach to mechanical support and cooling has been developed in conjunction with SiD. The support structures
More informationData acquisition and Trigger (with emphasis on LHC)
Lecture 2 Data acquisition and Trigger (with emphasis on LHC) Introduction Data handling requirements for LHC Design issues: Architectures Front-end, event selection levels Trigger Future evolutions Conclusion
More informationReadout architecture for the Pixel-Strip (PS) module of the CMS Outer Tracker Phase-2 upgrade
Readout architecture for the Pixel-Strip (PS) module of the CMS Outer Tracker Phase-2 upgrade Alessandro Caratelli Microelectronic System Laboratory, École polytechnique fédérale de Lausanne (EPFL), Lausanne,
More informationModule Integration Sensor Requirements
Module Integration Sensor Requirements Phil Allport Module Integration Working Group Sensor Geometry and Bond Pads Module Programme Issues Numbers of Sensors Required Nobu s Sensor Size Summary n.b. 98.99
More informationThe ATLAS tracker Pixel detector for HL-LHC
on behalf of the ATLAS Collaboration INFN Genova E-mail: Claudia.Gemme@ge.infn.it The high luminosity upgrade of the LHC (HL-LHC) in 2026 will provide new challenges to the ATLAS tracker. The current Inner
More informationCMS Compact Muon Solenoid Super LHC: Detector and Electronics Upgrade
CMS Compact Muon Solenoid Super LHC: Detector and Electronics Upgrade HCAL Muon chambers Tracker ECAL 4T solenoid 1 Total weight: 12,500 t Overall diameter: 15 m Overall length 21.6 m Magnetic field 4
More informationQ1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4 Q1-2 Q3-4. Final design and pre-production.
high-granularity sfcal Performance simulation, option selection and R&D Figure 41. Overview of the time-line and milestones for the implementation of the high-granularity sfcal. tooling and cryostat modification,
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2010/043 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 23 March 2010 (v4, 26 March 2010) DC-DC
More informationarxiv: v2 [physics.ins-det] 13 Oct 2015
Preprint typeset in JINST style - HYPER VERSION Level-1 pixel based tracking trigger algorithm for LHC upgrade arxiv:1506.08877v2 [physics.ins-det] 13 Oct 2015 Chang-Seong Moon and Aurore Savoy-Navarro
More informationATLAS Phase-II Upgrade Pixel Data Transmission Development
ATLAS Phase-II Upgrade Pixel Data Transmission Development, on behalf of the ATLAS ITk project Physics Department and Santa Cruz Institute for Particle Physics, University of California, Santa Cruz 95064
More informationThin Silicon R&D for LC applications
Thin Silicon R&D for LC applications D. Bortoletto Purdue University Status report Hybrid Pixel Detectors for LC Next Linear Collider:Physic requirements Vertexing 10 µ mgev σ r φ,z(ip ) 5µ m 3 / 2 p sin
More informationReal-time flavour tagging selection in ATLAS. Lidija Živković, Insttut of Physics, Belgrade
Real-time flavour tagging selection in ATLAS Lidija Živković, Insttut of Physics, Belgrade On behalf of the collaboration Outline Motivation Overview of the trigger b-jet trigger in Run 2 Future Fast TracKer
More informationUpgrade tracking with the UT Hits
LHCb-PUB-2014-004 (v4) May 20, 2014 Upgrade tracking with the UT Hits P. Gandini 1, C. Hadjivasiliou 1, J. Wang 1 1 Syracuse University, USA LHCb-PUB-2014-004 20/05/2014 Abstract The performance of the
More informationCMOS pixel sensors developments in Strasbourg
SuperB XVII Workshop + Kick Off Meeting La Biodola, May 2011 CMOS pixel sensors developments in Strasbourg Outline sensor performances assessment state of the art: MIMOSA-26 and its applications Strasbourg
More informationData acquisition and Trigger (with emphasis on LHC)
Lecture 2! Introduction! Data handling requirements for LHC! Design issues: Architectures! Front-end, event selection levels! Trigger! Upgrades! Conclusion Data acquisition and Trigger (with emphasis on
More informationAttilio Andreazza INFN and Università di Milano for the ATLAS Collaboration The ATLAS Pixel Detector Efficiency Resolution Detector properties
10 th International Conference on Large Scale Applications and Radiation Hardness of Semiconductor Detectors Offline calibration and performance of the ATLAS Pixel Detector Attilio Andreazza INFN and Università
More informationPerformance of the ATLAS Muon Trigger in Run I and Upgrades for Run II
Journal of Physics: Conference Series PAPER OPEN ACCESS Performance of the ALAS Muon rigger in Run I and Upgrades for Run II o cite this article: Dai Kobayashi and 25 J. Phys.: Conf. Ser. 664 926 Related
More informationThe Vertex Tracker. Marco Battaglia UC Berkeley and LBNL. Sensor R&D Detector Design PhysicsBenchmarking
The Vertex Tracker Marco Battaglia UC Berkeley and LBNL Sensor R&D Detector Design PhysicsBenchmarking Sensor R&D CCD Sensors N. de Groot Reports from LCFI progress with successful tests of CPCCD clocked
More informationCMS Tracker studies. Daniel Pitzl, DESY
CMS Tracker studies Daniel Pitzl, DESY Present CMS silicon tracker Design Material budget Upgrade phase I: 4 layer pixel 5 layer pixel? Resolution studies with broken line fits CMS Si Tracker 2 Phase I
More informationOperation and Performance of the ATLAS Level-1 Calorimeter and Level-1 Topological Triggers in Run 2 at the LHC
Operation and Performance of the ATLAS Level-1 Calorimeter and Level-1 Topological Triggers in Run 2 at the LHC Kirchhoff-Institute for Physics (DE) E-mail: sebastian.mario.weber@cern.ch ATL-DAQ-PROC-2017-026
More informationOperational Experience with the ATLAS Pixel Detector
The 4 International Conferenceon Technologyand Instrumentation in Particle Physics May, 22 26 2017, Beijing, China Operational Experience with the ATLAS Pixel Detector F. Djama(CPPM Marseille) On behalf
More informationMicromegas calorimetry R&D
Micromegas calorimetry R&D June 1, 214 The Micromegas R&D pursued at LAPP is primarily intended for Particle Flow calorimetry at future linear colliders. It focuses on hadron calorimetry with large-area
More informationTotem Experiment Status Report
Totem Experiment Status Report Edoardo Bossini (on behalf of the TOTEM collaboration) 131 st LHCC meeting 1 Outline CT-PPS layout and acceptance Running operation Detector commissioning CT-PPS analysis
More informationLevel-1 Track Trigger R&D. Zijun Xu Peking University
Level-1 Trigger R&D Zijun Xu Peking University 2016-12 1 Level-1 Trigger for CMS Phase2 Upgrade HL-LHC, ~2025 Pileup 140-250 Silicon based Level 1 Trigger Be crucial for trigger objects reconstruction
More informationA High Granularity Timing Detector for the Phase II Upgrade of the ATLAS experiment
3 rd Workshop on LHCbUpgrade II LAPP, 22 23 March 2017 A High Granularity Timing Detector for the Phase II Upgrade of the ATLAS experiment Evangelos Leonidas Gkougkousis On behalf of the ATLAS HGTD community
More informationNikhef jamboree - Groningen 12 December Atlas upgrade. Hella Snoek for the Atlas group
Nikhef jamboree - Groningen 12 December 2016 Atlas upgrade Hella Snoek for the Atlas group 1 2 LHC timeline 2016 2012 Luminosity increases till 2026 to 5-7 times with respect to current lumi Detectors
More informationWhere do we use Machine learning and where do want to improve?
Tracking@LHCb Where do we use Machine learning and where do want to improve? Sascha Stahl, CERN Paul Seyfert, INFN On behalf of LHCb DS@HEP 07.07.2016 The LHCb detector Vertex and track finding Particle
More informationATLAS strip detector upgrade for the HL-LHC
ATL-INDET-PROC-2015-010 26 August 2015, On behalf of the ATLAS collaboration Santa Cruz Institute for Particle Physics, University of California, Santa Cruz E-mail: zhijun.liang@cern.ch Beginning in 2024,
More informationITk silicon strips detector test beam at DESY
ITk silicon strips detector test beam at DESY Lucrezia Stella Bruni Nikhef Nikhef ATLAS outing 29/05/2015 L. S. Bruni - Nikhef 1 / 11 Qualification task I Participation at the ITk silicon strip test beams
More informationTests of the CMS Level-1 Regional Calorimeter Trigger Prototypes
Tests of the CMS Level-1 Regional Calorimeter Trigger Prototypes W.H.Smith, P. Chumney, S. Dasu, M. Jaworski, J. Lackey, P. Robl, Physics Department, University of Wisconsin, Madison, WI, USA 8th Workshop
More informationThe upgrade of the ATLAS silicon strip tracker
On behalf of the ATLAS Collaboration IFIC - Instituto de Fisica Corpuscular (University of Valencia and CSIC), Edificio Institutos de Investigacion, Apartado de Correos 22085, E-46071 Valencia, Spain E-mail:
More informationThe LHCb trigger system
IL NUOVO CIMENTO Vol. 123 B, N. 3-4 Marzo-Aprile 2008 DOI 10.1393/ncb/i2008-10523-9 The LHCb trigger system D. Pinci( ) INFN, Sezione di Roma - Rome, Italy (ricevuto il 3 Giugno 2008; pubblicato online
More informationThe BaBar Silicon Vertex Tracker (SVT) Claudio Campagnari University of California Santa Barbara
The BaBar Silicon Vertex Tracker (SVT) Claudio Campagnari University of California Santa Barbara Outline Requirements Detector Description Performance Radiation SVT Design Requirements and Constraints
More informationATLAS Muon Trigger and Readout Considerations. Yasuyuki Horii Nagoya University on Behalf of the ATLAS Muon Collaboration
ATLAS Muon Trigger and Readout Considerations Yasuyuki Horii Nagoya University on Behalf of the ATLAS Muon Collaboration ECFA High Luminosity LHC Experiments Workshop - 2016 ATLAS Muon System Overview
More informationCMS Conference Report
Available on CMS information server CMS CR 23/2 CMS Conference Report arxiv:physics/312132v1 [physics.ins-det] 22 Dec 23 The CMS Silicon Strip Tracker: System Tests and Test Beam Results K. KLEIN I. Physikalisches
More informationA High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Calorimeter system Detector concept description and first beam test results
A High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Calorimeter system Detector concept description and first beam test results 03/10/2017 ATL-LARG-SLIDE-2017-858 Didier Lacour On
More informationStatus of UVa
Status of GEM-US @ UVa Kondo Gnanvo University of Virginia, Charlottesville, SoLID Collaboration Meeting @ JLab 05/15/2015 Outline GEM trackers for SoLID GEM R&D program @ UVa Plans on SoLID-GEM specific
More informationPoS(LHCP2018)031. ATLAS Forward Proton Detector
. Institut de Física d Altes Energies (IFAE) Barcelona Edifici CN UAB Campus, 08193 Bellaterra (Barcelona), Spain E-mail: cgrieco@ifae.es The purpose of the ATLAS Forward Proton (AFP) detector is to measure
More informationPoS(Vertex 2007)034. Tracking in the trigger: from the CDF experience to CMS upgrade. Fabrizio Palla 1. Giuliano Parrini
Tracking in the trigger: from the CDF experience to CMS upgrade 1 INFN Pisa Largo B. Pontecorvo 3, 56127 Pisa, Italy E-mail:Fabrizio.Palla@cern.ch Giuliano Parrini University and INFN Florence Via G. Sansone
More informationarxiv: v1 [physics.ins-det] 25 Oct 2012
The RPC-based proposal for the ATLAS forward muon trigger upgrade in view of super-lhc arxiv:1210.6728v1 [physics.ins-det] 25 Oct 2012 University of Michigan, Ann Arbor, MI, 48109 On behalf of the ATLAS
More informationCMS electron and _ photon performance at s = 13 TeV. Francesco Micheli on behalf of CMS Collaboration
CMS electron and _ photon performance at s = 13 TeV on behalf of CMS Collaboration 2 Electrons and Photons @ CMS Electrons and photons are crucial for CMS physics program: SM precision physics, Higgs coupling
More informationATLAS ITk and new pixel sensors technologies
IL NUOVO CIMENTO 39 C (2016) 258 DOI 10.1393/ncc/i2016-16258-1 Colloquia: IFAE 2015 ATLAS ITk and new pixel sensors technologies A. Gaudiello INFN, Sezione di Genova and Dipartimento di Fisica, Università
More informationReminder on the TOB electronics architecture Test of the first SS rod prototype
Reminder on the TOB electronics architecture Test of the first SS rod prototype Results Further steps Duccio Abbaneo CMS Electronics Week November 2002 1 The rod CCU Module SC out LV out SC in LV in LV
More informationATLAS Phase-II trigger upgrade
Particle Physics ATLAS Phase-II trigger upgrade David Sankey on behalf of the ATLAS Collaboration Thursday, 10 March 16 Overview Setting the scene Goals for Phase-II upgrades installed in LS3 HL-LHC Run
More informationarxiv: v1 [physics.ins-det] 26 Nov 2015
arxiv:1511.08368v1 [physics.ins-det] 26 Nov 2015 European Organization for Nuclear Research (CERN), Switzerland and Utrecht University, Netherlands E-mail: monika.kofarago@cern.ch The upgrade of the Inner
More informationThe CMS Pixel Detector Phase-1 Upgrade
Paul Scherrer Institut, Switzerland E-mail: wolfram.erdmann@psi.ch The CMS experiment is going to upgrade its pixel detector during Run 2 of the Large Hadron Collider. The new detector will provide an
More informationTrigger Overview. Wesley Smith, U. Wisconsin CMS Trigger Project Manager. DOE/NSF Review April 12, 2000
Overview Wesley Smith, U. Wisconsin CMS Project Manager DOE/NSF Review April 12, 2000 1 TriDAS Main Parameters Level 1 Detector Frontend Readout Systems Event Manager Builder Networks Run Control System
More informationDAQ & Electronics for the CW Beam at Jefferson Lab
DAQ & Electronics for the CW Beam at Jefferson Lab Benjamin Raydo EIC Detector Workshop @ Jefferson Lab June 4-5, 2010 High Event and Data Rates Goals for EIC Trigger Trigger must be able to handle high
More informationSerial Powering vs. DC-DC Conversion - A First Comparison
Serial Powering vs. DC-DC Conversion - A First Comparison Tracker Upgrade Power WG Meeting October 7 th, 2008 Katja Klein 1. Physikalisches Institut B RWTH Aachen University Outline Compare Serial Powering
More informationConstruction and Performance of the stgc and MicroMegas chambers for ATLAS NSW Upgrade
Construction and Performance of the stgc and MicroMegas chambers for ATLAS NSW Upgrade Givi Sekhniaidze INFN sezione di Napoli On behalf of ATLAS NSW community 14th Topical Seminar on Innovative Particle
More informationarxiv: v2 [physics.ins-det] 20 Oct 2008
Commissioning of the ATLAS Inner Tracking Detectors F. Martin University of Pennsylvania, Philadelphia, PA 19104, USA On behalf of the ATLAS Inner Detector Collaboration arxiv:0809.2476v2 [physics.ins-det]
More informationData acquisi*on and Trigger - Trigger -
Experimental Methods in Par3cle Physics (HS 2014) Data acquisi*on and Trigger - Trigger - Lea Caminada lea.caminada@physik.uzh.ch 1 Interlude: LHC opera3on Data rates at LHC Trigger overview Coincidence
More informationPixel sensors with different pitch layouts for ATLAS Phase-II upgrade
Pixel sensors with different pitch layouts for ATLAS Phase-II upgrade Different pitch layouts are considered for the pixel detector being designed for the ATLAS upgraded tracking system which will be operating
More informationCMS Phase II Tracker Upgrade GRK-Workshop in Bad Liebenzell
CMS Phase II Tracker Upgrade GRK-Workshop in Bad Liebenzell Institut für Experimentelle Kernphysik KIT University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association
More informationEfficiency and readout architectures for a large matrix of pixels
Efficiency and readout architectures for a large matrix of pixels A. Gabrielli INFN and University of Bologna INFN and University of Bologna E-mail: giorgi@bo.infn.it M. Villa INFN and University of Bologna
More informationA 130nm CMOS Evaluation Digitizer Chip for Silicon Strips readout at the ILC
A 130nm CMOS Evaluation Digitizer Chip for Silicon Strips readout at the ILC Jean-Francois Genat Thanh Hung Pham on behalf of W. Da Silva 1, J. David 1, M. Dhellot 1, D. Fougeron 2, R. Hermel 2, J-F. Huppert
More informationTowards a 10μs, thin high resolution pixelated CMOS sensor for future vertex detectors
Towards a 10μs, thin high resolution pixelated CMOS sensor for future vertex detectors Yorgos Voutsinas IPHC Strasbourg on behalf of IPHC IRFU collaboration CMOS sensors principles Physics motivations
More informationSLHC Trigger & DAQ. Wesley H. Smith. U. Wisconsin - Madison FNAL Forward Pixel SLHC Workshop October 9, 2006
SLHC Trigger & DAQ Wesley H. Smith U. Wisconsin - Madison FNAL Forward Pixel SLHC Workshop October 9, 2006 Outline: SLHC Machine, Physics, Trigger & DAQ Impact of Luminosity up to 10 35 Calorimeter, Muon
More informationIntegrated CMOS sensor technologies for the CLIC tracker
CLICdp-Conf-2017-011 27 June 2017 Integrated CMOS sensor technologies for the CLIC tracker M. Munker 1) On behalf of the CLICdp collaboration CERN, Switzerland, University of Bonn, Germany Abstract Integrated
More informationThe CMS Silicon Strip Tracker Overview and Status
Overview and Status 1.Physikalisches Institut B, RWTH Aachen DCMS Meeting Hamburg, January 20th, 2006 Overview Requirements for tracking at the LHC Expected performance of the CMS tracker The design of
More informationA High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Detector system
A High-Granularity Timing Detector for the Phase-II upgrade of the ATLAS Detector system C.Agapopoulou on behalf of the ATLAS Lar -HGTD group 2017 IEEE Nuclear Science Symposium and Medical Imaging Conference
More informationRP220 Trigger update & issues after the new baseline
RP220 Trigger update & issues after the new baseline By P. Le Dû pledu@cea.fr Cracow - P. Le Dû 1 New layout features Consequence of the meeting with RP420 in Paris last September Add 2 vertical detection
More informationD. Ferrère, Université de Genève on behalf of the ATLAS collaboration
D. Ferrère, Université de Genève on behalf of the ATLAS collaboration Overview Introduction Pixel improvements during LS1 Performance at run2 in 2015 Few challenges met lessons Summary Overview VCI 2016,
More informationLHCb Preshower(PS) and Scintillating Pad Detector (SPD): commissioning, calibration, and monitoring
LHCb Preshower(PS) and Scintillating Pad Detector (SPD): commissioning, calibration, and monitoring Eduardo Picatoste Olloqui on behalf of the LHCb Collaboration Universitat de Barcelona, Facultat de Física,
More informationSemiconductor Detector Systems
Semiconductor Detector Systems Helmuth Spieler Physics Division, Lawrence Berkeley National Laboratory OXFORD UNIVERSITY PRESS ix CONTENTS 1 Detector systems overview 1 1.1 Sensor 2 1.2 Preamplifier 3
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2015/213 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 05 October 2015 (v2, 12 October 2015)
More informationLHC Experiments - Trigger, Data-taking and Computing
Physik an höchstenergetischen Beschleunigern WS17/18 TUM S.Bethke, F. Simon V6: Trigger, data taking, computing 1 LHC Experiments - Trigger, Data-taking and Computing data rates physics signals ATLAS trigger
More informationSTUDY OF THE RADIATION HARDNESS OF VCSEL AND PIN ARRAYS
STUDY OF THE RADIATION HARDNESS OF VCSEL AND PIN ARRAYS K.K. GAN, W. FERNANDO, H.P. KAGAN, R.D. KASS, A. LAW, A. RAU, D.S. SMITH Department of Physics, The Ohio State University, Columbus, OH 43210, USA
More information