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BEGIN:VEVENT
SUMMARY:Beam Condition Monitors and a Luminometer Based on Diamond Sensors
DTSTART;VALUE=DATE-TIME:20140225T024500Z
DTEND;VALUE=DATE-TIME:20140225T030500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-11@indico.inp.nsk.su
DESCRIPTION:Speakers: Wolfgang Lange (DESY Zeuthen)\nDetectors with diamon
 d sensors are used in the CMS experiment and along the LHC ring to monitor
  beam conditions. The fast system BCM1F in CMS using single crystal diamon
 d sensors allows bunch by bunch measurements with nanosecond time resoluti
 on. Operating right from the very first beams in CMS it was extended to de
 liver the online luminosity of the experiment. Similar detectors were also
  installed at critical positions of the LHC. The talk will review the perf
 ormance and give an outlook to the upgrade in the current shutdown.\n\nhtt
 ps://indico.inp.nsk.su/event/0/contributions/11/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/11/
END:VEVENT
BEGIN:VEVENT
SUMMARY:CMS Alignment and Calibration
DTSTART;VALUE=DATE-TIME:20140225T020000Z
DTEND;VALUE=DATE-TIME:20140225T022500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-27@indico.inp.nsk.su
DESCRIPTION:Speakers: Yuriy Pakhotin (Texas A and M University)\nDetermina
 tion of alignment and calibration constants plays one of the central role 
 in the operation of the CMS experiment. Prompt and accurate alignment and 
 calibration of the CMS components are crucial to achieve optimal performan
 ce of the detector and to allow the CMS physics program to reach its goals
 . Sophisticated algorithms and workflows are developed and routinely emplo
 yed to align and calibrate various systems of the CMS detector. Also dedic
 ated express streams of promptly reconstructed data events with reduced co
 ntent have been deployed to achieve fast access to data samples after coll
 ection and their efficient processing in alignment and calibration workflo
 ws. We discuss details of the alignment and calibration procedures for all
  CMS components\, results of the several years of CMS operation and achiev
 ed performance of the CMS detector for physics analyses. We also present p
 lans for upgrade and future development.\n\nhttps://indico.inp.nsk.su/even
 t/0/contributions/27/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/27/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Photon collider Higgs factories
DTSTART;VALUE=DATE-TIME:20140224T084000Z
DTEND;VALUE=DATE-TIME:20140224T090500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-87@indico.inp.nsk.su
DESCRIPTION:Speakers: Valery Telnov (Budker INP)\nAbstract is not provided
 .\n\nhttps://indico.inp.nsk.su/event/0/contributions/87/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/87/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Detector Challenges at CLIC
DTSTART;VALUE=DATE-TIME:20140224T100000Z
DTEND;VALUE=DATE-TIME:20140224T103000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-35@indico.inp.nsk.su
DESCRIPTION:Speakers: Strahinja Lukic (Vinca Institute of Nuclear Sciences
 )\nThe presentation reports on ongoing studies for general purpose detecto
 rs at a future TeV-scale e⁺e⁻ Compact LInear Collider (CLIC).\nThe CLI
 C physics goals impose stringent requirements on the detector.\nImprovemen
 ts on state-of-the-art track and jet energy resolutions are needed. At the
  same time\, the beam-induced backgrounds introduce challenging conditions
  for the event reconstruction. Under these circumstances\, satisfying the 
 physics goals is achieved by designing the detectors with high granularity
  particle flow in mind.\nIn the presentation\, several sub-detector system
 s are highlighted and it is shown how the detector requirements can be ach
 ieved.\n\nhttps://indico.inp.nsk.su/event/0/contributions/35/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/35/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Measurement of the integrated luminosity and the luminosity spectr
 um at the linear collider
DTSTART;VALUE=DATE-TIME:20140224T105000Z
DTEND;VALUE=DATE-TIME:20140224T111000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-40@indico.inp.nsk.su
DESCRIPTION:Speakers: Strahinja Lukic (Vinca Institute of Nuclear Sciences
 )\nThe high charge density and high energy at future linear colliders will
  present challenges to the luminosity measurement that have not been there
  in the past. The intense electromagnetic interaction between the electron
  bunches influences the luminosity measurement at the level of several per
 cent. Precise correction of the beam-beam effects\, based on experimentall
 y measurable quantities\, is described here. In addition\, a comprehensive
  list of systematic effects in luminosity measurement is given\, with thei
 r individual contributions to the final uncertainty of the luminosity figu
 re.\n\nhttps://indico.inp.nsk.su/event/0/contributions/40/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/40/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Beam energy determination in collider experiments using backscatte
 ring  of laser light
DTSTART;VALUE=DATE-TIME:20140225T030500Z
DTEND;VALUE=DATE-TIME:20140225T033000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-43@indico.inp.nsk.su
DESCRIPTION:Speakers: Mikhail Achasov (G.I.Budker Institute of Nuclear Phy
 sics SB RAS)\nThe review of using of compton backscattering method for ele
 ctron beam energy  determination is given.\n\nhttps://indico.inp.nsk.su/ev
 ent/0/contributions/43/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/43/
END:VEVENT
BEGIN:VEVENT
SUMMARY:A luminosity detector for the PANDA experiment at FAIR
DTSTART;VALUE=DATE-TIME:20140225T022500Z
DTEND;VALUE=DATE-TIME:20140225T024500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-65@indico.inp.nsk.su
DESCRIPTION:Speakers: Prometeusz Jasinski (Helmholtz Institute Mainz)\nThe
  PANDA experiment at FAIR (Darmstadt) is a fixed target experiment in a hi
 gh energy storage ring. Antiprotons with a momentum of 1.5 GeV/c up to 15 
 GeV/c collide with an atomic beam perpendicular to the interaction point (
 IP). The spectrometer consists of a solenoid magnet around the IP followed
  by a dipole magnet. The spectrometer stages are both equipped with variou
 s planes of detectors for charged and neutral channels.\nTo determine the 
 luminosity with a precision of better than 3%\, PANDA will implement a tra
 cking device to reconstruct elastically scattered antiprotons near the non
  interacting antiproton beam. Four planes equipped with retractable HV-MAP
 S placed inside vacuum around the beam pipe.\nIn this overview talk we wil
 l discuss topics such as cooling of CVD-diamonds used as heat conductors f
 or the active pixel sensors\, production of aluminum support frames with s
 tainless steep pipes melted inside\, the construction of a differentialy p
 umped vacuum system\, the corresponding feed throughs at the vacuum box an
 d the status of the sensors themselves. All topics are completed by existi
 ng prototype results.\n\nhttps://indico.inp.nsk.su/event/0/contributions/6
 5/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/65/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The Multi-Purpose Detector for JINR heavy-ion collider
DTSTART;VALUE=DATE-TIME:20140225T042000Z
DTEND;VALUE=DATE-TIME:20140225T044500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-79@indico.inp.nsk.su
DESCRIPTION:Speakers: Stepan Razin (Joint Institute for Nuclear Research)\
 nThe Multi-Purpose Detector (MPD) is designed as 4π spectrometer to study
  heavy-ion collisions at the Nuclotron-based heavy Ion Collider fAcility a
 t JINR. At the designed luminosity the event rate in the MPD is ~7kHz and 
 charge particle multiplicity ~1000. A superconducting 5m diameter solenoid
  is equiped with a inner tracking system based on silicon microstrip detec
 tor\, large volume time-projection chamber\, time-of-flight system based o
 n RPC\, electromagnetic calorimeter\, endcap tracker and a series of fast 
 trigger detectors.\n\nhttps://indico.inp.nsk.su/event/0/contributions/79/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/79/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The Mu2e Experiment at Fermilab
DTSTART;VALUE=DATE-TIME:20140225T035500Z
DTEND;VALUE=DATE-TIME:20140225T042000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-88@indico.inp.nsk.su
DESCRIPTION:Speakers: David Hitlin (California Institute of Technology)\nW
 e present the status of Mu2e experiment for the search of coherent\, neutr
 ino-less conversion of muons into electrons in the field of a nucleus to a
  few parts in 10⁻¹⁷\, a sensitivity improvement of a factor of 10⁴ 
 over existing limits. The Mu2e experiment will be hosted by Fermilab at a 
 new muon campus. It will use a complex of solenoids to collect and transpo
 rt the muons\, produced when the 8 GeV pulsed proton beam hits the tungste
 n production target. The last solenoid in the complex will allow for the m
 easurement of the momentum of the electrons produced by the muons trapped 
 into the muon stopping targets. To this goal\, Mu2e will adopt a challengi
 ng detector system. We present a detailed description and the expected per
 formance. The central part of the detector is a low-mass straw tube tracke
 r immersed in a 1 Tesla uniform magnetic field and placed in vacuum (10⁻
 ⁴ torr) to efficiently identify 105 MeV/c electrons\, with a resolution 
 of the order of 100 KeV/c\, and to reject a large amount of background hit
 s (average hit rate of ~15 kHz/cm²) within a high radiation environment (
 peak hit rate of ~3 MHz/cm²). A BaF₂ crystal calorimeter\, downstream o
 f the tracker\, will provide particle ID\, to further reduce backgrounds\,
  energy and time measurements. The large detector area will be extensively
  covered by multi-layer scintillation counters to reject\, at the level of
  10⁻⁴\, cosmic rays that could mimic signal tracks.\n\nhttps://indico.
 inp.nsk.su/event/0/contributions/88/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/88/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Detectors for Muon-to-Electron Conversion at the COMET Experiment
DTSTART;VALUE=DATE-TIME:20140227T031500Z
DTEND;VALUE=DATE-TIME:20140227T033500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-92@indico.inp.nsk.su
DESCRIPTION:Speakers: Yoshi Uchida (Imperial College London)\nCOMET is a m
 uon-to-electron conversion experiment at the J-PARC laboratory\, the first
  of two phases of which is scheduled to start running in 2016. Its final s
 ingle-event sensitivity to this rare muon decay process is expected to be 
 2.6 × 10⁻¹⁷. This experiment places very specific requirements on it
 s particle detectors\, which arise from the high background rates and the 
 need to find single electrons in the kinetic energy region of 100 MeV. We 
 describe the challenges posed by this experiment and the solutions that ar
 e being developed for the two phases.\n\nhttps://indico.inp.nsk.su/event/0
 /contributions/92/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/92/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Polarisation and beam energy measurement at linear e+e- colllider
DTSTART;VALUE=DATE-TIME:20140224T103000Z
DTEND;VALUE=DATE-TIME:20140224T105000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-93@indico.inp.nsk.su
DESCRIPTION:Speakers: Benedikt Vormwald (DESY)\nThe International Linear C
 ollider (ILC) is a future e⁺e⁻ collider at the energy frontier. Its ph
 ysics goals are clearly focused on precision measurements at the electrowe
 ak scale and beyond. Beam polarisation and beam energy are two important p
 arameters\, which need to be measured and monitored to unprecedented possi
 ble precision. In this talk we will present the concepts of polarisation a
 nd energy measurement according to the baseline design of the Technical De
 sign Report of the ILC.\nTwo Compton polarimeters per beam line will deter
 mine the beam polarisation. The anticipated precision of this measurement 
 of ∆P/P = 2.5 × 10⁻³ puts highest demands on detector alignment and 
 linearity. We will comment on recent detector developments as well as dete
 ctor calibration\, which allows for meeting this challenging design goal.\
 nThe beam energy will be measured before and after the interaction point t
 o a targeted precision of ∆E/E = O(10⁻⁴). We will discuss both plann
 ed independent concepts in this talk: A noninvasive energy spectrometer ba
 sed on beam position monitors is planned to be operated before the interac
 tion region. Behind the interaction region\, a synchrotron radiation imagi
 ng detector will allow not only for measuring the beam energy\, but also g
 ives access to the beam energy spread of the beam after collision.\n\nhttp
 s://indico.inp.nsk.su/event/0/contributions/93/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/93/
END:VEVENT
BEGIN:VEVENT
SUMMARY:The superconducting magnet of the Multipurpose Detector
DTSTART;VALUE=DATE-TIME:20140225T044500Z
DTEND;VALUE=DATE-TIME:20140225T050500Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-103@indico.inp.nsk.su
DESCRIPTION:Speakers: Evgeny Koshurnikov (Joint Institute for Nuclear Rese
 arch)\nThe multipurpose detector (MPD) is a 4π spectrometer to be used fo
 r studying charged hadrons\, electrons\, and photons generated in heavy io
 n collisions at energies provided by the NICA collider of the Joint Instit
 ute for Nuclear Research (Dubna).\nA constituent part of the MPD is a sole
 noid magnet with a superconducting NbTi coil and a steel flux return yoke.
  The magnet weighs eight hundred tons and is intended for providing a high
 ly homogeneous magnetic field of 0.5 T in an aperture 4596 mm in diameter 
 to ensure the transverse momentum resolution within the range of 0.1-3 GeV
 /c at NICA.\nStructurally\, the MPD magnet yoke is a cylindrical barrel-li
 ke structure\, which consists of 24 beams that return the magnetic flux of
  the coil\, two support rings\, two poles\, and two support cradles that c
 arry the total weight of the detector. The stainless cryostat with the sup
 erconducting coil is rigidly fixed inside the yoke barrel. The adopted str
 uctural arrangement of the yoke guarantees high rigidity of the whole magn
 et and will ensure the required field homogeneity (integral of the radial 
 magnetic induction component) in the TPC region after subsequent withdrawa
 ls of the poles and multiple movements of the magnet to the assembly site 
 for updating or repair.\nThe coil is a one-layer solenoid made of a superc
 onducting NbTi cable in the aluminum matrix. The conductor is wound onto i
 nside the aluminium support cylinder. The cooling method chosen for the MP
 D magnet is based on the forced two-phase helium flow using a helium refri
 gerator. The coil conductor is cooled indirectly via the thermal contact w
 ith the aluminum cylinder and heat removal through the cylinder to the alu
 minum tube with circulated liquid helium.\n\nhttps://indico.inp.nsk.su/eve
 nt/0/contributions/103/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/103/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Detector Systems at the International Linear Collider
DTSTART;VALUE=DATE-TIME:20140224T093500Z
DTEND;VALUE=DATE-TIME:20140224T100000Z
DTSTAMP;VALUE=DATE-TIME:20260610T145259Z
UID:indico-contribution-1-110@indico.inp.nsk.su
DESCRIPTION:Speakers: Frank Simon (Max-Planck-Institute for Physics)\nThe 
 International Linear Collider is a planned energy frontier electron-positr
 on collider which will cover the energy range from 250 GeV to 1 TeV in sev
 eral stages. This machine will precisely study the Higgs and Top sectors\,
  perform electroweak precision measurements and will explore New Physics b
 oth directly and indirectly. This ambitious program requires highly perfor
 mant detector systems. Two detector concepts are being developed for this 
 future collider: The International Large Detector ILD and the Silicon Dete
 ctor SiD. Both are optimized for precise event reconstruction based on par
 ticle flow in a hermetic detector\, with high precision main trackers\, hi
 ghly granular imaging electromagnetic and hadronic calorimeters and high-r
 esolution low-mass vertex detectors. The two detector concepts adopted dif
 ferent technology choices to achieve the physics goals\, with SiD based on
  an all-silicon tracker in a compact detector with a 5T magnetic field\, a
 nd ILD based on a large TPC favoring a highly redundant pattern recognitio
 n over single-point resolution in a more moderate 3.5 T to 4 T field.  Thi
 s presentation will motivate the designs of both detectors based on the ma
 in physics objectives of ILC\, will give an overview over the different de
 tector subsystems and will show selected results from performance studies 
 based on realistic detector simulations.\n\nhttps://indico.inp.nsk.su/even
 t/0/contributions/110/
LOCATION:
URL:https://indico.inp.nsk.su/event/0/contributions/110/
END:VEVENT
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