Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html

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Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
Computing at the
            Large Hadron Collider
           in the CMS experiment
www.iphc.cnrs.fr/-cms-.html

  Daniel Bloch
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
at the heart of matter

  électron : < ~10-20 m                         < ~10–20 m
                                     10–15 m
                    10–14 m
          10–10 m
>10–9 m

molecule   atom     nucleus   proton/neutron    quark
    chemistry                           particle physics
  electromagnetic interaction

                          strong interaction

                                      weak interaction

                                                             2
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
the standard model
§   Elaborated in years 1960-70
§   Describes both elementary particles (grouped in 3 families) and
     electroweak (unifies em and weak int.) and strong interactions
§   Relies on symetry properties
     (conservation laws)
§   Experimentally tested with great precision
     (~10-3 for em and weak unification)
§   Higgs mecanism: to explain the origin
     of particle masses
     => a new
     particle:
     Higgs boson:
     discovered
     at LHC
     in 2012

                                                                       3
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
beyond standard model: supersymetry ?
                                                                dark matter candidate
§   Supersymetry (Susy) is an
     elegant theory which                                                  ~
                                                                           χ01   ~χ0
     considers matter and                                                             2
     interaction particles on an
     equal footing:
                                                                          ~χ0     χ~0
                                                                             3          4
     § many new Susy particles                                                ~±
        are predicted,                                                         χ
        but not their mass !
        (+ many other parameters)
     § accessible at LHC ?

§   Susy would solve some of our fundamental questions:
     § the Higgs boson has been found, but why is it so light ?
     § the lightest Susy particle (neutral, weakly interacting) would be an
        excellent candidate for dark matter
     § electroweak and strong interactions can be unified in Susy models

§   But there are also known complications with Susy:
      §   not found yet ! It would be ``natural’’ to get it at TeV mass scale
      §   the minimal Susy model is (amost) ruled out => the number of free
           parameters may be large (between > 5 and up to 124 …)
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
proton collisions at LHC
                                 •   2800 bunches of protons
                                 •   energy of each proton : 6.5 TeV

                                 •   100 billions protons / bunch
                                 •   beam crossing rate: 40 MHz

                                 • in the experiments at each
bunches

                         crossing:
                                   ~ 20-50 proton-proton collisions
                                   ~ 1500 particles produced
protons

                       • 1 billion interactions / second

                                 • impossible to record everything !
constituents

(quarks, gluons)
                                 • a Higgs boson to find
                                   within 5 billions of

                                   collisions…

                                                                           5
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
proton collisions at LHC
                                 •   2800 bunches of protons
                                 •   energy of each proton : 6.5 TeV

                                 •   100 billions protons / bunch
                                 •   beam crossing rate: 40 MHz

                                 • In the experiments at each
bunches

                         crossing:
                                   ~ 20-50 proton-proton collisions
                                   ~ 1500 particules prodiuced
protons

                       • 1 billion interactions / second

constituents

                                 • A Higgs boson to find

(quarks, gluons)                   within 5 billions of
                                   collisions…

                                                                       6
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
the CMS collaboration

                 •   38 countries
                 •   183 institutes
                 •   ~3000 scientists
                     (permanent,
                     post-doc, students)
                 •   ~100 French people

                                       7
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
the CMS detector
as a 3D camera
of 14000 t, 29 m length, 15 m height
with 75 millions of pixels and taking
40 millions of pictures per second

                                        8
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
the CMS detector
concentric layers, each with well defined
detection purpose

                                 magnetic field 3.8 T
 Tracker
 reconstruct charged particles

 pixels : 100×150 µm2
 66M chanels, 1m2
 Silicon strips :
 9M chanels, 210 m2

                                                        9
Computing at the Large Hadron Collider in the CMS experiment - Daniel Bloch www.iphc.cnrs.fr/-cms.html
the CMS detector

Calorimeter(s)
Measure the energy of particles
(except muons and neutrinos)

em. (ECAL) :
76k cristals PbWO4
hadronic (HCAL) :
scintillators/Cu

                                     10
the CMS detector

            Muon Detectors

                             11
what happens during collisions ?

                                   12
trigger and data acquisition

1rst level trigger: 100 kHz   high level trigger: 1 kHz (100 ms / event)
    660 000 MB/s                         600 MB/s
                                                     600
    from all sub-detectors                raw data

                                                                           13
first data reconstruction at CERN

  7
                      800

                             30

                600
                                    14
The World LHC Computing Grid
a worldwide net of many computing sites:

                              CERN	
  

  CERN çè national centers çè academic centers
    Tier 0     Tiear 1 : 12 sites        Tier 2 : 140 sites   15	
  
the grid in France and at Strasbourg

CERN     çè   CC IN2P3              çè       8 sites
Tier 0          Tier 1                           Tier 2
                                      at IPHC Strasbourg:
                                      • Tier 2 for CMS and Alice
                                      • 15% of ressources for other
                                         local usage (subatomic
                                         physics, protéomic, bio-
                                         informatics, …)
                                      20M h of computing/year,
                                      2000 slots,
                           CERN	
     1400 TB disk space

                                                                      16	
  
event size and reconstruction time
• depends on the intensity of the beams:
      •   superimposed interactions ~ 20 to 50
      •   => affects the size of the events and their reconstruction time !
•   event size ~0.2 to 0.9 MB
•   reconstruction time per event ~15-80 s
•   need also to generate and simulate data: ~50 s / events
•   total number of events per year (real data + simulated): 5 Billions

                                                                              17
CPU and disk needs
                  CPU                        DISK
TIER 0
  CMS      6k cores               15 PB (+35 PB tape)
  2015

TIER 1
  CMS     25k cores               30 PB (+70 PB tape)
  2015

TIER 2
   CMS    60k cores               30 PB
   2015

                                                        18
event reconstruction
§   What we look for:                  §   What we observe in the detector…
§   example of the production of a
     Susy-top pair
§   experimental signature:
     top-quark pair +MET

                                χ0

         χ0

                                        §   Information in calorimeters: ECAL,HCAL.
                                        §   Trajectories of charged particles.
                                        §   Muons (red line).
                                        §   Missing Transverse Energy (MET: arrow).
event reconstruction (cont)

                                 • Jets of particles with
point of decay                     the trajectograph and
of a jet from b quark              calorimeters
            (accuracy ~100 µm)
                                 • Identification of jet
                                   from b decay
                                   (« b-tagging ») with
                                   pixel detector: distance
                                   of decay flight

                                 • Missing Tranverse
     pp collision                  Energy (MET) :
     point                         hermetic detectors =>
                                   allows one to measure
                                   the energy and
                                   direction of invisible
                                   particles (neutrino,
                                   dark mater if any) in
                                   the plane transverse to
                                   the beam axis
                                                             20
event reconstruction (cont)

    Reconstruction
        of jets

                                Rejection of
                                events from
                               pile-up pp int.

   Identification      Selection of jets
    of the event
need to reject the large background

§   from different processes, but giving a similar signature
§   can be :
     § Physical background (irreductible), with same final state
     § Instrumental background: due to badly reconstructed particles

                                                                  jet     electron
                                                                          + MET
                                                                  jet

                                                                  jet
                                                                  jet

                                                                  jet

§   need to define the sensitive variables to enhance the signal:
     § production rate (cross section).
     § invariant mass (or related quantities) of the initial particles
processing flow for a typical analysis
§ trigger: electron+jets or muon+jets or ee, eµ, µµ
        rate ~200 Hz at 8 TeV (about 1/3 of all recorded events)

§ selection of the reconstructed events
  and writing of reduced size information (Ttrees)

§ input, read on the Grid:
  §   data: 500M events
  §   simulation: Susy signal = 150M events, backgrounds = 150M events
  §   overall size: 0.4 MB × 500M + 0.7 × 300M ~ 400 TB
  §   processing time: 2 s / event
         repeated 2-3 times after each new version of the data reconstruction
         total: 1M hours of computing time

§ output, stored at IPHC on the Grid (can be used worldwide):
  §   100M data events, 150M simulated events
  §   overall size: 30 TB with full information, 5 TB with reduced information
  §   processing time (fast) : 2.5 ms / event on local cluster
          => ~200 hours for all data and simulation
              but repeated many times (~10)
search for the Susy-top
§ no Susy-top observed so far (at 8 TeV collision energy):
  set limits on its mass and on dark matter particle

§ need to go higher in energy: 13 TeV collisions from this year
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