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Nicolas ARNAUD ( [email protected] ) Laboratoire de l’Accélérateur Linéaire (IN2P3/CNRS). Status of the project. Laboratoire Leprince-Ringuet May 2 nd 2011. Outline.  Overview of the SuperB flavour factory  Detector status  Computing status  Accelerator status

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Status of the project

Nicolas ARNAUD ([email protected])

Laboratoire de l’Accélérateur Linéaire


Status of the project

Laboratoire Leprince-Ringuet

May 2nd 2011


 Overview of the SuperB flavour factory

 Detector status

 Computing status

 Accelerator status

 Physics potential

 Status of the project

For more information
For more information

 Detector Progress Report [arXiv:1007.4241]

 Physics Progress Report [arXiv:1008.1541]

 Accelerator Progress Report [arXiv:1009.6178]

 Public website:

 SuperB France contact persons

 Detector & Physics: Achille Stocchi ([email protected])

 Accelerator: Alessandro Variola ([email protected])

+ Guy Wormser ([email protected]) member of the management team

The flavour factory
The Flavour Factory

Superb in a nutshell
SuperB in a nutshell

 SuperB is a new and ambitious project of flavour factory

2nd generation B-factory – after BaBar and Belle

 Integrated luminosity in excess of 75 ab-1; peak @ 1036 cm-2 s-1

 Run above Y(4S) energy and at the charm threshold; polarized electron beam

 Detector based on BaBar

 Similar geometry; reuse of some components

 Optimization of the geometry; subdetectors improvement

 Need to cope with much higher luminosity and background

 Accelerator

 Reuse of several PEP-II components

 Innovative design of the interaction region: the crab waist scheme

 Successfully tested at the modified DAFNE interaction point (Frascati)

 IN2P3 involved in the TDR phase (so far)

 LAL, LAPP, LPNHE, LPSC, CC-IN2P3; interest from IPHC

 A lot of opportunities in various fields for groups willing to join the experiment


 2005-2011: 16 SuperB workshops

 2007: SuperB CDR

 2010: 3 SuperB progress reports – accelerator, detector, physics

 December 2010 & 1rst quarter 2011: project approbation by Italy

 May 28th June 2nd 2011: first SuperB collaboration meeting in Elba

 2nd half of 2011: choice of the site; start of the civil engineering

 Presentation to the IN2P3 Scientific Council next Fall

 Request to have the IN2P3 involvement into the SuperB experiment approved

 End 2011-beginning of 2012: detector and accelerator Technical Design Reports

 Computing TDR ~a year later

 First collisions expected for 2016 or 2017

The detector
The Detector

Detector layout
Detector layout





E(e-) = 4.2 GeV


E(e+) = 6.7 GeV




The superb detector systems
The SuperB detector systems

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH)

 Particle IDentification (PID)

 ElectroMagnetic Calorimeter (EMC)

 Instrumented Flux Return (IFR)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

Silicon vertex tracker svt
Silicon Vertex Tracker (SVT)

 Silicon Vertex Tracker (SVT) Contact: Giuliana Rizzo (Pisa)

 Drift CHamber (DCH)

 Particle IDentification (PID)

 ElectroMagnetic Calorimeter (EMC)

 Instrumented Flux Return (IFR)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

The superb silicon vertex tracker

Bp p, bg=0.28, hit resolution =10 mm

Dt resolution (ps)

20 cm

old beam pipe

new beam pipe

30 cm

40 cm


The SuperB Silicon Vertex Tracker

 Based on BaBar SVT: 5 layers silicon strip modules + Layer0 at small radius to improve vertex resolution and compensate the reduced SuperB boost w.r.t. PEPII

  •  Physics performance and background levels set

  • stringent requirements on Layer0:

    •  R~1.5 cm, material budget < 1% X0,, ,

    •  Hit resolution 10-15 μm in both coordinates

    •  Track rate > 5MHz/cm2 (with large cluster

    • too!), TID > 3MRad/yr

  •  Several options under study for Layer0


 SVT provides precise tracking and vertex reconstruction, crucial for time dependent measurements, and perform standalone tracking for low pt particles.

Superb svt layer 0 technology options
SuperB SVT Layer 0 technology options


in pixel sparsification

 Ordered by increasing complexity:

 Striplets

 Mature technology, not so robust

against bkg occupancy

 Hybrid pixels

 Viable, although marginal in

term of material budget


 New & challenging technology:

fast readout needed (high rate)

 Thin pixels with vertical integration

 Reduction of material and improved performance

 Several pixel R&D activities ongoing

 Performances: efficiency,

hit resolution

 Radiation hardness

 Readout architecture

 Power, cooling

Test of a hybrid

pixel matrix with

5050 mm2 pitch

Future activities
Future activities

 Present plan

 Start data taking with striplets in Layer0: baseline option for TDR

 Better perf. due to lower material w.r.t. pixel: thin options not yet mature!

 Upgrade Layer0 to pixel (thin hybrid or CMOS MAPS), more robust against

background, for the full luminosity (1-2 years after start)

 Activities

 Development of readout chip(s) for strip(lets) modules

 Very different requirements among layers

 Engineering design of Layer0 striplets & Layer1-5 modules

 SVT mechanical support structure design

 Peripheral electronics & DAQ design

 Continue the R&D on thin pixel for Layer0

 Design to be finalized for the TDR; then move to construction phase

 A lot of activities: new groups are welcome!

 Potential contributions in several areas: development of readout chips,

detector design, fabrication and tests, simulation & reconstruction

 Now: Bologna, Milano, Pavia, Pisa, Roma3, Torino, Trento, Trieste, QM, RAL

 Expression of interest from Strasbourg (IPHC) & other UK groups

Drift chamber dch
Drift CHamber (DCH)

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH) Contacts: Giuseppe Finocchiaro (LNF)

 Particle IDentification (PID) Mike Roney (Victoria)

 ElectroMagnetic Calorimeter (EMC)

 Instrumented Flux Return (IFR)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

The superb drift chamber dch
The SuperB Drift CHamber (DCH)

 Large volume gas (BaBar: He 80% / Isobutane 20%) tracking system providing meas. of charged particle mom. and ionization energy loss for particle identification

 Primary device to measure speed of particles having momenta below ~700 MeV/c

 About 40 layers of centimetre-sized cells strung approximately parallel to the

beamline with subset of layers strung at a small stereo angle in order to provide

measurements along the beam axis

 Momentum resolution of ~0.4% for tracks with pt = 1 GeV/c

 Overall geometry

 Outer radius constrained to 809 mm by the DIRC quartz bars

 Nominal BaBar inner radius (236 mm) used until Final Focus cooling finalized

 Chamber length of 2764 mm (will depend on forward PID and backward EMC)

Recent activities
Recent activities

 2.5m long prototype with 28 sense wires arranged in 8 layers

 Cluster counting: detection of the single primary ionization acts

 Simulations to understand the impact of Bhabha and 2-photon pair backgrounds

 Lumi. bkg dominates occupancy – beam background similar than in BaBar

 Nature and spatial distributions dictate the overall geometry

 Dominant bkg: Bhabha scattering at low angle

 Gas aging studies

Future activities1
Future activities

 Current SuperB DCH groups

 LNF, Roma3/INFN group, McGill University, TRIUMF, University of British

Columbia, Université de Montréal, University of Victoria

 LAPP technical support for re-commissioning the BaBar gas system

 Open R&D and engineering issues

 Backgrounds: effects of iteration with IR shielding; Touschek, validation

 Cell/structure/gas/etc.

 Dimensions (inner radius, length, z-position) to be finalized

 Tests (cluster counting and aging) needed to converge on FEE, gas, wire, etc.

 Engineering of endplates, inner and outer cylinders

 Assembly and stringing (including stringing robots)

 DCH trigger

 Gas system recommissioning – Annecy

 Monitoring systems

Particle identification pid
Particle IDentification (PID)

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH)

 Particle IDentification (PID) Contacts: Nicolas Arnaud (LAL)

 ElectroMagnetic Calorimeter (EMC) Jerry Va’Vra (SLAC)

 Instrumented Flux Return (IFR)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

The focusing dirc fdirc
The Focusing DIRC (FDIRC)

 Based on the successful BaBar DIRC:

 Detector of Internally Reflected Cherenkov light


 Main PID detector for the SuperB barrel

 K/p separation up to 3-4 GeV/c

 Performance close to that of the BaBar DIRC

 To cope with high luminosity (1036 cm-2s-1) & high background

 Complete redesign of the photon camera [SLAC-PUB-14282]

 A true 3D imaging using:

 25 smaller volume of the photon camera

 10 better timing resolution to detect single photons

 Optical design is based entirely on Fused Silica glass

 Avoid water or oil as optical media

DIRC NIM paper

[A583 (2007) 281-357]

FDIRC concept

  • Re-useBaBar DIRC quartzbar radiators



  • Photoncameras at the end ofbar boxes





New photon camera

Fdirc photon camera 12 in total
FDIRC photon camera (12 in total)

 Photon camera design (FBLOCK)

 Initial design by ray-tracing


 Experience from the 1rst FDIRC prototype


 Geant4 model now


 Main optical components

 New wedge

 Old bar box wedge not long enough

 Cylindrical mirror to remove bar thickness

 Double-folded mirror optics to provide access to detectors

 Photon detectors: highly pixilated H-8500 MaPMTs

 Total number of detectors per FBLOCK: 48

 Total number of detectors: 576 (12 FBLOCKs)

 Total number of pixels: 576  32 = 18,432

Fdirc status
FDIRC Status

 FDIRC prototype to be tested this summer in the SLAC Cosmic Ray Telescope

 Ongoing activities

 Validation of the optics design

 Mechanical design & integration

 Front-end electronics

 Simulation: background, reconstruction...

 FDIRC goals

 Resolution per photon: ~200 ps

 Cherenkov resolution per photon: 9-10 mrad

 Cherenkov angle resolution per track: 2.5-3.0 mrad

 Design frozen for TDR; next: R&D  construction

 Groups: SLAC, Maryland, Cincinnati, LAL, LPNHE, Bari, Padova, Novosibirsk

 A wide range of potential contributions for new groups

 Detector design, fabrication and tests

 MaPMT characterization

 Simulation & reconstruction

 Impact of the design on the SuperB physics potential

R d on a forward pid detector
R&D on a forward PID detector

 Goal: to improve charged particle identification in forward region

 In BaBar: only dE/dx information from drift chamber

  •  Challenges

  •  Limited space available

  •  Small X0

  •  And cheap

  •  Gain limited by small solid angle

    [qpolar~1525 degrees]

     The new detector must be efficient

  •  Different technologies being studied

  •  Time-Of-Flight (TOF): ~100ps resolution needed

  •  RICH: great performances but thick and expensive

  •  Decision by the TDR time

  •  Task force set inside SuperB to review proposals

  •  Building an innovative forward PID detector

  • would require additional manpower & abilities




Forward PID location

Electromagnetic calorimeter emc
ElectroMagnetic Calorimeter (EMC)

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH)

 Particle IDentification (PID)

 ElectroMagnetic Calorimeter (EMC) Contacts: Claudia Cecchi (Perugia)

 Instrumented Flux Return (IFR) Frank Porter (Caltech)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

The superb electromagnetic calorimeter emc
The SuperB ElectroMagnetic Calorimeter (EMC)

 System to measure electrons and photons, assist in particle identification

 Three components

 Barrel EMC: CsI(Tl) crystals with PiN diode readout

 Forward EMC: LYSO(Ce) crystals with APD readout

 Backward EMC: Pb scintillator with WLS fiber to SiPM/MPPC readout [option]

 Groups: Bergen, Caltech, Perugia, Rome

 New groups welcome to join!

CsI(Tl) barrel


(5760 crystals)

Sketch of backward Pb-scintillator

calorimeter, showing both radial and

logarithmic spiral strips

(24 Pb-scint layers, 48 strips/layer,

total 1152 scintillator strips)

Design for forward

LYSO(Ce) calorimeter

(4500 crystals)\

Recent activities and open issues
Recent activities and open issues

 Beam test at CERN (next at LNF)

 Measurement of MIP width on LYSO

 Electron resolution: work in progress

 LYSO crystal uniformization

 Used ink band in beam test

 Studying roughening a surface

 Promising results from simulation

 Forward EMC mechanical design

 Prototype + CAD/finite elements analysis

 Backward EMC

 Prototype + MPPC irradiation by neutrons

 Open issues

 Forward mechanical structure; cooling; calibration

 Backward mechanical design

 Optimization of barrel and forward shaping times; TDC readout

 Use of SiPM/MPPCs for backward EMC; radiation hardness; use for TOF!?

 Cost of LYSO

Instrumented flux return ifr
Instrumented Flux Return (IFR)

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH)

 Particle IDentification (PID)

 ElectroMagnetic Calorimeter (EMC)

 Instrumented Flux Return (IFR) Contact: Roberto Calabrese (Ferrara)

 Electronics, Trigger and Data Acquisition (ETD)

 Computing

Instrumented flux return ifr the m and k l detector
Instrumented Flux Return (IFR): the m and KL detector

 Built in the magnet flux return

 One hexagonal barrel and two endcaps

 Scintillator as active material to cope with high flux

of particles: hottest region up to few 100 Hz/cm2

 82 cm or 92 cm of Iron interleaved by 8-9 active layers

 Under study with simulations/testbeam

 Fine longitudinal segmentation in front of

the stack for KL ID (together with the EMC)

 Plan to reuse BaBar flux return

 Add some mechanical constraints:

gap dimensions, amount of iron, accessibility

 4-meter long extruded scintillator bars readout

through 3 WLS fibers and SiPM

 Two readout options under study

 Time readout for the barrel (two coordinates read by the same bar)

 Binary readout for the endcaps (two layers of orthogonal bars)

Scintillator bar

+ WLS fibers

Detector simulation
Detector simulation

  •  Detailed description of hadronicinteraction needed

  • for detector optimization and background studies

  •  Full GEANT4 simulation developed for that purpose

  •  Complete event

  • reconstruction

  • implemented to evaluate

  • m detection performance

 A selector based on BDT algorithm is used to

discriminate muons and pions

 PID performance are evaluated for

different iron configurations

 Machine background rates on the detector

are evaluated to study

 the impact on detection efficiency and muon ID

 the damage on the Silicon Photo-Multipliers

Iron absorber thickness:

 920 mm

 820 mm

 620 mm

Pion rejection vsmuon efficiency

Neutron flux on the forward endcap

Beam test of a prototype
Beam test of a prototype

 Prototype built to test the technology on large scale and validate simulation results

 Up to 9 active layers readout together

 ~230 independent electronic channels

 Active modules housed in light-tightened boxes

 4 Time Readout modules

 4 Binary Readout modules

 4 special modules

 Study different fibers or SiPM geometry

 Preliminary results confirm the R&D performances

 Low occupancy due to SiPM single counts even at low threshold

 Detection efficiency >95%

 Time resolution about 1 ns

 Data analysis still ongoing

 Refine reconstruction code

 Study hadronic showers

 Evaluate muon ID performance

 Tune the Monte Carlo simulation

 Study different detector configurations

Iron: 606092 cm3,

3cm gaps for the active layers

Tested in Dec. 2010 at the

Fermilab Test

Beam Facility with

muon/pion (4-8GeV)

Beam profile

Noise level:

15 counts / 1000 events


(# of photoelectrons)

Open issues and next activities
Open issues and next activities

  •  Define the Iron structure

  •  Various options currently under study to evaluate the most cost effective

    •  Use the existing Babar Structure, only adding Iron or brass

    •  BaBar structure + 10 cm  Modify the BaBar structure

    •  Build a brand new structure optimized for SuperB

  •  SiPM radiation damage

  •  Understand the effects of neutrons and how to shield the devices

    •  An irradiation test has just been performed at LNL

    •  More tests with absorbers are foreseen

  •  TDC Readout: meet the required specs

  •  Beam test at Fermilab in July to extend the studies al lower momentum (2-4 GeV/c)

  •  Start the construction-related activities

    • A lot of activities: new groups are welcome!

  •  Groups working at present on the IFR: Ferrara, Padova

Electronics trigger and data acquisition etd
Electronics, Trigger and Data Acquisition (ETD)

 Silicon Vertex Tracker (SVT)

 Drift CHamber (DCH)

 Particle IDentification (PID)

 ElectroMagnetic Calorimeter (EMC)

 Instrumented Flux Return (IFR)

 Electronics, Trigger and Data Acquisition (ETD) Contacts: Steffen Luitz (SLAC)

 Computing

Dominique Breton (LAL)

Umberto Marconi(Bologna)

Online system design principles
Online system design principles

  •  Apply lessons learned from BaBar and LHC experiments

  •  Keep it simple

    •  Synchronous design

    •  No “untriggered” readouts

    •  Except for trigger data streams from FEE to trigger processors

    •  Use off-the-shelf components where applicable

    •  Links, networks, computers, other components

    •  Software: what can we reuse from other experiments?

  •  Modularize the design across the system

  •  Common building blocks and modules for common functions

  •  Implement subdetector-specific functions on specific modules

  •  Carriers, daughter boards, mezzanines

  •  Design with radiation-hardness in mind where necessary

  •  Design for high-efficiency and high-reliability “factory mode”

  •  Where affordable – BaBar experience will help with the tradeoffs

  •  Minimal intrinsic dead time – current goal: 1% + trickle injection blanking

  •  Minimize manual intervention. Minimize physical hardware access requirements.

SuperB ETD system overview

Projected trigger rates and event sizes
Projected trigger rates and event sizes

  •  Estimates extrapolated assuming BaBar-like acceptance and BaBar-like open trigger

  •  Level-1 trigger rates (conservative scaling from BaBar)

  •  At 1036 cm-2 s-1: 50 kHz Bhabhas, 25 kHz beam backgrounds,

  • 25 kHz “irreducible” (physics + backgrounds)

  •  100 kHz Level-1-accept rate ( without Bhabha veto)

    •  75 kHz with a Bhabha veto at Level-1 rejecting 50%

    •  Safe Bhabha veto at Level-1 difficult due to temporal overlap in slow detectors.

    •  Baseline: better done in High-Level Trigger

    •  50% headroom desirable (from BaBar experience) for efficient operation

    •  Baseline: 150 kHz Level-1-accept rate capability

  •  Event size: 75-100 kByte (estimated from BaBar)

    •  Pre-ROM event size: 400-500 kByte

    •  Still some uncertainties for post-ROM event size

  •  High-Level Trigger (HLT) and Logging

    •  Expected logging cross-section: 25nb with a safe real-time high-level trigger

    •  Logging rate: 25kHz x 75kByte = 1.8 Gbyte/s

    •  Logging cross section could be improved by 5-10 nb by using a more aggressive

    • filter in the HLT (cost vs. risk tradeoff!)

  • ReadOut



    Deadtime goal
    Deadtime goal

     Target: 1% event loss due to DAQ system dead time

     Not including trigger blanking for trickle injection

     Assume “continuous beams”

    2.1 ns between bunch crossings

     No point in hard synchronization of L1 with RF

     1% event loss at 150 kHz requires 70 ns maximum per-event dead time

     Exponential distribution of event inter-arrival time

     Challenging demands on

     Intrinsic detector dead time and time constants

     L1 trigger event separation

     Command distribution and command length (1 Gbit/s)

     Ambitious

     May need to relax goal somewhat

    Synchronous pipelined fixed latency design
    Synchronous, pipelined, fixed-latency design

     Global clock to synchronize FEE, Fast Control and Timing System (FCTS), Trigger

     Analog signals sampled with global clock (or multiples/integer fractions of clock)

     Samples shifted into latency buffer (fixed depth pipeline)

     Synchronous reduced-data streams derived from some sub-detectors

    (DCH, EMC, …) sent to the pipelined Level-1 trigger processors

     Trigger decision after a fixed latency referenced to global clock

     L1-accept  readout command sent to the FCTS and

    broadcast to FEE over synchronous, fixed-latency links

     FEE transfer data over optical links to the Readout Modules (ROMs)

     no fixed latency requirement here

     All ROMs apply zero suppression

    plus feature extraction and

    combine event fragments

     Resulting partially event-built

    fragments are then sent via the

    network event builder into

    the HLT farm

    Level-1 Trigger

     Baseline: “BaBar-like L1 Trigger”

     Calorimeter trigger:

    cluster counts and energy thresholds

     Drift chamber trigger:

    track counts, pT, z-origin of tracks

     Highly efficient, orthogonal

     To be validated for high-lumi

     Challenges: time resolution,

    trigger jitter and pile-up

     To be studied

     SVT used in trigger?

     Tight interaction with SVT and

    SVT FEE design

     Bhabha veto

     Baseline: Best done in HLT

     Fully pipelined

     Input running at 7(?) MHz

     Continuous reduced-data streams from

    sub-detectors over fixed latency links

    □ DCH hit patterns (1 bit/wire/sample)

    □ EMC crystal sums, properly encoded

     Total latency goal: 6 ms

     Includes detectors, trigger readout,

    FCTS, propagation

     Leaves 3-4ms for the trigger logic

     Trigger jitter goal  50 ns to accommodate short sub-detector readout windows

    Fast Control and Timing System (FCTS)

     Clock distribution

     System synchronization

     Command distribution

     L1-Accept

     Receive L1 trigger decisions

     Participate in pile-up and

    overlapping event handling

     Dead time management

     System partition

     1 partition / subdetector

     Event management

     Determine event destination

    in event builder / high level

    trigger farm

     Links carrying trigger data, clocks and commands

    need to be synchronous & fixed latency:

    ≈ 1GBit/s

     Readout data links can be asynchronous,

    variable latency and even packetized:

    ≈ 2 Gbit/s but may improve

    Common Front-End Electronics

     Digitize

     Maintain latency buffer

     Maintain derandomizer

    buffers, output mux and data

    link transmitter

     Generate reduced-data

    streams for L1 trigger

     Interface to FCTS

     Receive clock

     Receive commands

     Interface to ECS

     Configure

     Calibrate

     Spy


     etc.

     Provide standardized building blocks

    to all sub-detectors, such as:

     Schematics and FPGA “IP”

     Daughter boards

     Interface & protocol descriptions

     Recommendations

     Performance specifications

     Software

    We would like to use off-the shelf commodity hardware as much as possible

     R&D in progress to combine off-the shelf computers

    with PCI-Express cards for the optical link interfaces

    Readout MOdules (ROMs)

     Receive data from the sub-detectors

    over optical links

     8 links per ROM (?)

     Reconstitute linked/pointer events

     Process data

     feature extraction, data reduction

     Send event fragments into HLT farm

    via the network

    Event builder and network

    • Combines event fragments from ROMs into complete events in the HLT farm

       In principle a solved problem 

       Prefer the fragment routing to be determined by FCTS

       FCTS decides to which HLT node all fragments of a given events are sent

      (enforces global synchronization), distribute as node number via FCTS

       Event-to-event decisions taken by FCTS firmware (using table of node numbers)

       Node availability / capacity communicated to FCTS via a slow feedback protocol

      (over network in software)

       Choice of network technology

       Prime candidate: combination of 10 Gbit/s and 1 GBit/s Ethernet

       User Datagram Protocol vs. Transmission Control Protocol

       Pros and cons to both. What about Remote Direct Memory Access?

      •  Can we use DCB/Converged Ethernet for layer-2 end-to-end flow

      • control in the EB network?

    •  Can SuperB re-use some other experiment’s event builder?

      •  Interaction with protocol choices

    High level trigger farm and logging
    High-level trigger farm and logging

     Standard off-the shelf rack-mount servers

     Receivers in the network event builder

     Receive event fragments from ROMs, build complete events

     HLT trigger (aka Level-3 in BaBar)

     Fast tracking (using L1 info as seeds), fast clustering

     Baseline assumption: 10 ms/event

     5-10  what the BaBar L3 needed on 2005-vintage CPUs: plenty of headroom

     1500 cores needed on contemporary hardware:

    ~150 16-core servers;10 cores/server usable for HLT purposes

     Data logging & buffering

     Few TByte/node

     Local disk (e.g. BaBar RAID1) or storage servers accessed via back-end network?

     Probably 2 days’ worth of local storage (2TByte/node?)

     Depends on SLD/SLA for data archive facility

     No file aggregation into “runs”

     bookkeeping

     Back-end network to archive facility

    Data quality monitoring control systems
    Data quality monitoring, control systems

     Data Quality Monitoring based on the same concepts as in BaBar

     Collect histograms from HLT and data from ETD monitoring

     Run fast and/or full reconstruction on sub-sample of events and collect histograms

     May include specialized reconstruction for e.g. beam spot position monitoring

     Could run on same machines as HLT processes (in virtual machines?)

    or on a separate small farm (“event server clients”)

     Present to operators via GUI

     Automated histogram comparison with reference histograms and alerting

     Control Systems

     Run Control provides a coherent management of the ETD and Online systems

     User interface, managing system-wide configuration, reporting,

    error handling, start and stop data taking

     Detector/Slow Control: monitor and steer the detector and its environment

     Maximize automation across these systems

     Goal: 2-person shifts like in BaBar

     “Auto-pilot” mode in which detector operations is controlled by the machine

     Automatic error detection and recovery when possible

     Assume we can benefit from systems developed for the LHC,

    the SuperB accelerator control system and commercial systems

    Opens questions and areas for r d
    Opens questions and areas for R&D

     Upgrade paths to 41036 cm-2 s-1

     What to design upfront, what to upgrade later, what is the cost?

     Data link details: jitter, clock recovery, coding patterns, radiation qualification,

    performance of embedded SERDES

     ROM: 10 GBit/s networking technology, I/O sub-system, using a COTS

    motherboard as carrier with links on PCIe cards, FEX & processing in software

     Trigger: latency, time resolution and jitter, physics performance, details of event

    handling, time resolution and intrinsic dead time, L1 Bhabha veto, use of SVT in

    trigger, HLT trigger, safety vs. logging rate

     ETD performance and dead time: trigger distribution through FCTS, intrinsic dead

    time, pile-up handling/overlapping events, depth of de-randomizer buffers

     Event builder: anything re-usable out there? Network and network protocols, UDP

    vs. TCP, applicability of emerging standards and protocols (e.g. DCB, Cisco DCE),

    HLT framework vs. Offline framework (any common grounds?)

     Software Infrastructure: sharing with Offline, reliability engineering and tradeoffs,

    configuration management (“provenance light”), efficient use of multi-core CPUs


     Silicon Vertex Tracker (SVT)

     Drift CHamber (DCH)

     Particle IDentification (PID)

     ElectroMagnetic Calorimeter (EMC)

     Instrumented Flux Return (IFR)

     Electronics, Trigger and Data Acquisition (ETD)

     Computing Contact: Fabrizio Bianchi (Torino)

    Superb computing activities
    SuperB computing activities

     Development and support of

     Software simulation tools: Bruno & FastSim

     Computing production infrastructure

     Goals: help detector design and

    allow performance evaluation studies

     Computing model

     Very similar to BaBar’s computing model

     Raw & reconstructed data permanently stored

     2-step reconstruction process

    □ prompt calibration (subset of events)

    □ Full event reconstruction

     Data quality checks during the whole processing

     Monte-Carlo simulation produced in parallel

     Mini (tracks, clusters, detector info.) &

    Micro (info. essential for physics) formats

     Skimming: production of selected subsets of data

     Reprocessing following each major code improvement


     Full Geant4-based C++ simulation

     Detector + beamline (currently up to  16 m)

     Rewritten from scratch

     Benefit from BaBar legacy

    and LHC experience

     Code development ongoing

     Main features

     Use of the Geometry Description Markup Langage

     Event generators run either inside the executable

    or as separate process

     Outputs in ROOT format

     Particle snapshots can be reused as

    Bruno inputs in staged simulations

     Interplay with the fast simulation (FastSim)

     Production of background frames @ CNAF

     Luminosity-scaling (Bhabha) and

    intensity-scaling (Touschek) backgrounds

     Tracking of neutrons

    Fast sim
    Fast Sim

     Goals

     Optimize detector design in terms of physics performances

     Realistic comparison of detector configurations

     Compute physics sensitivity for rare processes

     Requirements

     Easy configuration

     Fast (> 1 Hz including analysis)

     Compatible with BaBar software

     Features

     Overall cylindrical symmetry; detector elements modelized as surfaces

     Parameterized material cross-sections and detector responses

     Reconstruction of tracks, clusters and particle ID

    Fast sim1
    Fast Sim

     C++ Software

     XML-based configuration langage (EDML)

     SL and MacOS platforms

     Various dependencies: ROOT, BaBar, etc.

     Not used only by SuperB

     Plan to separate generic FastSim code

    from BaBar/SuperB specific code

     Project lead by Dave Brown (LBL)

     ~20 contributors

    mu2e FNAL


    Distributed computing
    Distributed computing

     Based on the HEP grid worldwide computing infrastructure

     Central site: CNAF (Bologna)

     Job submission management, bookeeping DB, data repository

     Several (currently 18) other sites in Europe (CC-IN2P3, GRIF, etc.) and USA

     Several productions already completed

     Example: FastSim Summer 2010

     15 sites, 160 kJobs (10% failures), 8.6 BEvents, 25 TB

    Collaborative tools
    Collaborative tools

     Directory service based on LDAP application protocol

     Unique authentification

     Website based on Joomla

     Wiki for easy documentation

     Alfresco for internal content management

     SVN used as source code management

     Primary platform: SL5 64-bits

     Use of CMake as alternative building system

     Works in parallel with the SRT system used in BaBar

    Computing r d
    Computing R&D

     New CPU architecture, new software architecture and new framework

     Code development: languages, tools, standards and QA

     Persistence, data handling models and DBs

     User tools and interfaces

     Distributed computing, GRID

     Performance and efficiency of large storage systems

     Yearly SuperB computing workshops

     Ferrara in 2010

     R&D program

    The accelerator
    The Accelerator

    The luminosity goals of superb
    The luminosity goals of SuperB

     SuperB is a new generation flavor factory aiming for a luminosity of

    1036 cm-2 s-1 1 kHz/nb

     The two orders of magnitudes luminosity gain with respect to the first generation

    B-factories is obtained by increasing the density of the bunches at the interaction

    point (IP) by demagnifying their vertical size to ~30 nm

     To reach this goal, the amplitude of the betatron oscillations must be kept at minimum

     Optimal ring lattice design to minimize the radial emittance

     Precise magnets alignment and machine tuning to minimize the emittance coupling

     Large Piwinsky angle and crab waist collision scheme to overcome the beam-beam

    luminosity limit

     Paths to high luminosity

     Increase the numerator – currents: 1÷2 Amp  10÷20 Amp

     Wall plug power ~ proportional to current

    Longitudinal fast instability limits the luminosity ~ 5  1035 cm-2 s-1

     Decrease the denominator

    Bunch size: PEP-II 100  3 μm2  SuperB 100 μm  30 nm

     How to squeeze the vertical bunch size to 30 nm?

    Hourglass shaped bunch @ sy = 30 nm

    Cross Section  Angular Divergence @ IP


    Emittance (Characteristics of the Ring)

     Hence, the more the bunch is squeezed, the higher

    the angular divergence: a squeezed bunch remains

    small for a very limited length

     Loss of luminosity: the Hourglass effect

     Examples

     PEP-II emittance = 1.5 nm  rad and

    angular divergence ~ 50 mrad = 50 micron / mm

     Bunch collision length should be ~ μm!

     ATF state of the art emittance = 2 pm  rad

    Angular divergence ~ 67 mrad =67 nm / mm

     SuperB emittance ~ 5 pm  rad

    + angular divergence ~ 166 mrad =166 nm / mm

     bunch collision length can be ~ mm

    Bunch shape at the IP

    Large crossing angle collision

     With large crossing angle q, reduced overlap region

     Can have by @ IP ~ sx/q << sz: significant luminosity gain!

     No need to have short bunches anymore

    β is the amplitude of

    the betatron oscillation

    Collision length ~ 0.3 mm

    2 σx/ϑ

    Crab waist transform

     y waist moved along z with a sextupole on both sides of the IP at proper phase

     Both beams collide in the minimum by region

     Net luminosity gain

     Suppress beam-beam effects: help tuning the beams

     Successfully tested at DAFNE:

    Luminosity  ~3, consistent with expectations

    Low energy beam

    High energy beam

    Machine layout

    Length ~ 1258 m

    60 mrad IR





    Lattice systems

     Two arcs

     Provide the necessary bending to close the ring

     Optimized to generate the design horizontal emittance

     Correct arc chromaticity and sextupole aberrations

     Interaction region

     Provides the necessary focusing for required small beam size at IP

     Corrects FF chromaticity and sextupole aberrations

     Provides the necessary optics conditions for Crab cavities

     Dogleg

     Provides crossing on the opposite to IR side of the ring

     LER spin rotator

     Includes solenoids in matched sections adjacent to the IR

     RF system

     Up to 24 HER and 12 LER cavities in the long adjacent

    straight section opposite to IP













    Dogleg 140 mRad

    SuperB accelerator crew

     Accelerator organisation chart still very preliminary

     Many opportunities for individuals/groups interested in joining the machine crew

     Innovative machine; importance of the Machine-Detector Interface

     D. Alesini, M. E. Biagini, R. Boni, M. Boscolo, T. Demma, A. Drago, M. Esposito, S. Guiducci,

    G. Mazzitelli, L. Pellegrino, M. Preger, P. Raimondi, R. Ricci, C. Sanelli, G. Sensolini, M. Serio,

    F. Sgamma, A. Stecchi, A. Stella, S. Tomassini, M. Zobov (INFN/LNF, Italy)

    K. Bertsche, A. Brachmann, Y. Cai, A. Chao, A. DeLira, M. Donald, A. Fisher, D. Kharakh, A. Krasnykh,

    N. Li, Y. Nosochkov, A. Novokhatski, M. Pivi, J. Seeman, M. Sullivan, U. Wienands, J. Weisend,

    W. Wittmer, G. Yocky (SLAC, USA)

     A. Bogomiagkov, S.Karnaev, I. Koop, E. Levichev, S. Nikitin, I. Nikolaev, I. Okunev, P. Piminov,

    S. Siniatkin, D. Shatilov, V. Smaluk, P. Vobly (BINP, Russia)

     G. Bassi, A. Wolski (Cockroft Institute, UK)

     S. Bettoni (CERN, Switzerland, )

     M. Baylac, J. Bonis, R. Chehab, J. DeConto, Gomez, A. Jeremie, G. Lemeur, B. Mercier, F. Poirier,

    C. Prevost, C. Rimbault, Tourres, F. Touze, A. Variola (IN2P3/CNRS, France)

     A. Chance, O. Napoly (CEA Saclay, France)

     F. Meot, N. Monseu (Grenoble, France)

     F. Bosi, E. Paoloni (INFN & Università di Pisa)

    The physics potential
    The Physics potential

    Data sample

     Y(4S) region:

     75ab−1 at the 4S

     Also run above and

    below the 4S

     ~75 109 B, D and τ pairs

     ψ(3770) region:

     500fb−1 at threshold

     Also run at nearby


     ~2 x 109 D pairs

    τ Lepton Flavor Violation (LFV)

     ν mixing leads to a low level of charged LFV (B~10−54)

     Enhancements to observable levels are possible with new physics

     e− beam polarisation helps suppress background

     Two orders of



    at SuperB over

    current limits

     Hadron machines

    are not competitive

    with e+e− machines

    for these measurements

    Only a few modes extrapolated so far for SuperB

    Bu,d physics: rare decays

    •  Example:

      •  Rate modified by presence of H+

    2 Higgs Doublet Model

    Bu,d physics: rare decays

     Example:

     Need 75 ab−1 to observe this mode

     With more than 75 ab−1 we could measure polarisation

    Sensitive to models with Z penguins and RH currents.

    e.g. see Altmannshofer, Buras, & Straub

    Constraint on (ε, η) with 75ab−1

    fL not included

    Who - title

    Bs physics

     Can cleanly measure using 5S data

     SuperB can also study rare decays with many neutral particles,

    such as which can be enhanced by SUSY

    Little Higgs (LTH) scenario


     Collect data at threshold and at the 4S

     Benefit charm mixing and CPV measurements

     Also useful for measuring the Unitarity triangle angle γ

     Strong phase in D  Kππ Dalitz plot


    Precision Electroweak

     sin2θW can be measured with polarised e− beam

     √s=ϒ(4S) is theoretically clean, c.f. b-fragmentation at Z pole

     Measure LR asymmetry in at the ϒ(4S) to same precision as

    LEP/SLC at the Z-pole

     Can also perform crosscheck at ψ(3770)



     More information on the golden matrix can be found in

    arXiv:1008.1541, arXiv:0909.1333, and arXiv:0810.1312.

     Combine measurements to elucidate

    structure of new physics



    NP enhancement:

     Observable effect

      Moderately large effect

       Very large effect

    Precision CKM constraints

     Unitarity Triangle Angles

     σ(α) = 1−2°

     σ(β) = 0.1°

     σ(γ) = 1−2°

     CKM Matrix Elements

     |Vub|

    □ Inclusive σ = 2%

    □ Exclusive σ = 3%

     |Vcb|

    □ Inclusive σ = 1%

    □ Exclusive σ = 1%

     |Vus|

     Can be measured precisely

    using τ decays

     |Vcd| and |Vcs|

     Can be measured at/near charm threshold.

     SuperB measures the sides and angles of the Unitarity Triangle

    The "dream" scenario with 75ab-1

    Golden measurements: CKM

     Comparison of relative benefits of SuperB (75ab-1)

    existing measurements

    vs. LHCb (5fb-1)

    LHCb upgrade (50fb-1)

    LHCb can only use ρπ

    β theory error Bd

    β theory error Bs

    Need an e+e− environment to do a precision measurement using semi-leptonic B decays.

    Experiment: No Result Moderate Precision Precise Very Precise

    Theory: Moderately clean Clean Need lattice Clean

    Golden measurements: General

    Experiment: No Result Moderate Precision Precise Very Precise

    Theory: Moderately clean Clean Need lattice Clean

    Benefit from polarised e− beam

    very precise with improved detector

    Statistically limited: Angular analysis with >75ab-1

    Right handed currents

    SuperB measures many more modes

    systematic error is main challenge

    control systematic error with data

    SuperB measures e mode well, LHCb does μ

    Clean NP search

    Theoretically clean

    b fragmentation limits interpretation

    Who - title

    Physics program in a nutshell

    SuperB is a versatile flavour physics experiment

     Probe new physics observables in wide range of decays

     Pattern of deviation from Standard Model can be used

    to identify structure of new physics.

     Clean experimental environment means clean signals in many modes

     Polarised e− beam benefit for τ LFV searches.

     Best capability for precision CKM constraints of any existing/proposed experiment

     Measure angles and sides of the Unitarity triangle

     Measure other CKM matrix elements at threshold and using τ data

     People willing to join this program are welcome in all areas

     Now is a good time, as we are starting to plan the physics TDR

     There will a Physics Book 1-2 years later

    The status
    The Status

    Superb approval in italy
    SuperB approval in Italy

     SuperB inserted in April 2010 among the Italian

    National Research Program (PNR) Flagship Projects

     Cooperation of INFN and IIT (Italian Institute of Technology)

     HEP experiment and light source

     In December 2010, funding of 19 M€ as first part of a pluriennal funding plan

     Internal to Ministry of Research

     In April 2011 approval of the PNR, including 250M€ for SuperB

     Press release

    PNR info

    Superb funding in infn 3 year plan
    SuperB Funding in INFN 3-year plan

    •  Funding for accelerator

    • and infrastructure

    •  Computing funding from

    • special funds for south

    • development

    •  Detector funding inside

    • ordinary funding agency

    • budget

    •  In addition, we reuse

    • parts of PEP-II and Babar

    • for a value of about

    • 135M€

    •  IIT contribution (100M€?) in addition, mainly for synchrotron light lines construction

    •  Brightness of light produced by bending magnets/ondulators competitive

    • w.r.t. existing machines on a wide range of photon energy


    Funding and management
    Funding and management

     MoUs for TDR work in place with Canada, France, UK, Russia and SLAC

     Negotiation with partner countries for construction MoUs started

     Expect that

     Important in-kind contribute by the re-use of parts of PEP-II

    and Babar, for a value of about 135M€

     For the accelerator and infrastructure, most funding will be Italian

     For the detector only half of the needed funding will come from Italy

     About 25M€

     The project will be managed through an

    European Research Infrastructure Consortium (ERIC)

    EMC barrel

    before installation

    in BaBar

    Front faces of DIRC quartz

    bars shining in the dark

    Site location
    Site location

     Preferred choice

     Tor Vergata

     Under review for technical compatibility

     Other possibilities

     North or south, in geologically stable areas

     Three sites identified

    Tor Vergata site




    Frascati laboratories

    200 m

    Next steps and timeline
    Next steps and timeline

     Choose the site asap!

     Foreseen for end of May 2011

     The preferred site is Tor Vergata close to LNF

     Complete the detector and accelerator Technical Design Reports

     End of 2011/Mid 2012

     Computing TDR about a year later

     Prepare the transition from TDR Phase to Construction

     Collaboration will start formally forming in Elba meeting, May 2011

     Start recruitment for the construction

     Mainly Accelerator Physicists and Engineers

     Completion of construction foreseen end of 2015

     First collisions mid 2016


     SuperB support by Italy is now confirmed – and firmly established

     Funding coming from a pluri-annual plan for the accelerator

     ~50 M€ to be found for the detector on a 5 years period (50% covered by INFN)

     Site to be defined soon

     Next step will be to start the civil engineering

     Collaboration formation process starting at the end of the month

     SuperB communities (detector, accelerator, computing, physics) are growing

     Yet: many opportunies at all levels for groups willing to join

     Achille Stocchi (SuperB France contact person) is open to any discussion

     Do not hesitate to contact us if you want to have more information!