'Proton beam' diaporamas de présentation

Target concepts for future high power proton beams

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SEU protection methods in ASICs (+ 1 word on TID)

SEU protection methods in ASICs (+ 1 word on TID). Sandro Bonacini sandro.bonacini@cern.ch. A word on Total Ionizing Dose (TID). Modern CMOS deep-submicron technologies like 130 nm require a limited effort in order to make TID-hard circuits Core logic only thin oxide transistors

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First Concepts for an Detector

First Concepts for an Detector. Requirements from Physics. ep -physics the detector needs to cover inclusive ? semi-inclusive ? exclusive reactions large acceptance absolutely crucial particle identification ( p ,K,p,n ) over wide momentum range excellent vertex resolution (charm)

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Quark *) Distributions with the LHeC

Project Scenarios Statistics Systematics Light Quarks Heavy Quarks. Quark *) Distributions with the LHeC. Max Klein DESY , 7.4.2010 Meeting on QCD at the LHeC. *) For the gluon see p revious talks by E. Perez at DIS07 C. Gwenlan at DIS09. Some plots old, s ome plots new.

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Proton Driven Plasma Wakefield Accelerator FNAL 27-10-2009

Proton Driven Plasma Wakefield Accelerator FNAL 27-10-2009. Lasers: Centimeters instead of Kilometers ?. If we take a Petawatt laser pulse, I=10 21 W/cm 2 then the electric field is as high as E =10 14 eV/m =100 TeV/m.

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Calculation of detector acceptance for measuring muon lifetime in MuSIC beam test by GEANT4

Kuno -Group D1 Nguyen Duy Thong . Calculation of detector acceptance for measuring muon lifetime in MuSIC beam test by GEANT4. Introduction Results Summary. Outline. Introduction. MuSIC facility. The process in MuSIC facility:

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HiRadMat Window Design report v1.0

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Development of a camera for imaging of prompt gamma rays in measurements of proton beam range

Development of a camera for imaging of prompt gamma rays in measurements of proton beam range. P.Busca 1,2 , C.Fiorini 1,2 , R.Peloso 1,2 , M.Basilavecchia 3 , T.Frizzi 3 , D. Prieels 4 , J. Smeets 5 * , F. Stichelbaut 4 , A. Benilov 4 , F. Roellinghoff 4

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Collimator and beamline heating

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Particle Physics Software aids Medicine

Precise physics models for radiation interactions with matter. Open source code providing advanced technologies to developing countries at no cost. Accurate geometry and material modeling. Powerful data analysis tools. The GRID for fast and cheap processing on distributed computing resources.

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Neutron Spectrometry with H e -3 proportional counters

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T riple GEM detector at CERN n_TOF facility

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Using Akka Platform in Unidentified Falling Object Detection on the LHC

Using Akka Platform in Unidentified Falling Object Detection on the LHC. An Example Use Case Scenario. Evangelos Motesnitsalis Magnet Powering Interlocks & Software Machine Protection and Electrical Integrity Group Technology Department

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LHC Injector Synchrotrons 2012

LHC Injector Synchrotrons 2012. LHC Injectors: SPS Q20 operational. Operational since September 2012 Remove or ease intensity limitations in the SPS No hardware change Very smooth transition, allowing brighter beams at LHC injection

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reporter A.V. Shchagin

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MERIT Beam Collimator Design

MERIT Beam Collimator Design. Nicholas Olesen 9 August 2006. Contents. Collimator Role Requirement Specifications Proposed Design Additional Information. Collimator Role. Beam of ~30 x 10 12 protons per pulse, integrated power of ~140kW Align the proton beam with the mercury target

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Meson Productions for Hg Jet with Disk Shape

Meson Productions for Hg Jet with Disk Shape. X. Ding BNL-AAG Meeting March 15, 2012. IDS120h Configuration. Meson Production with IDS120h. Why the meson productions are lower at KE<5 GeV ? . The mercury jet target geometry. The proton beam and mercury jet cross at z =-37.5 cm.

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What is Plasma Wakefield Acceleration?

Novel particle acceleration technique. Short beam enters plasma. Free e- pulled towards beam. e- reach beam, and overshoot. What is Plasma Wakefield Acceleration?. Ion region is left behind beam. e- pulled back towards axis by ions. +. +. -. -. +. -. +. +.

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MICE TARGET OPERATION

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The Self-Modulation I nstability

Affects long drive beams. Long beam enters plasma. Free e- pulled towards proton beam. E- overshoot the proton beam. Ion region left behind head of proton beam. E- pulled back on axis by ions Impinge on proton beam. The Self-Modulation I nstability. +. +. -. -.

186 views • 1 slides