'Beam time' diaporamas de présentation

Radiation damage effects in Monolithic Active Pixel Sensors

726 views • 54 slides

Malte Hildebrandt

631 views • 50 slides

AGATA Performance C ommissioning @ PRESPEC

AGATA Performance C ommissioning @ PRESPEC. AGATA Commissioning WG. Demonstrate the performance of AGATA in a RIB facility at relativistic beam energies .

435 views • 30 slides

Time-like Compton Scattering with CLAS12

Time-like Compton Scattering with CLAS12. S. Stepanyan (JLAB) CLAS12 European Workshop  February 25-28, 2009, Genova, Italy. GPDs and nucleon structure Extraction of GPDs from Experimental Data TCS phenomenology and observables Quasi-real Photoproduction of lepton pairs in CLAS

448 views • 28 slides

A new m ? e g experiment at PSI

A new m ? e g experiment at PSI. For the MUEGAMMA collaboration Stefan Ritt (Paul Scherrer Institute, Switzerland). Introduction Experimental Technique Current status. Physics Motivation. SUSY theories generically predict LFV LFV forbidden by Standard Model

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User Program Models Worldwide

User Program Models Worldwide. Lessons Learned. Gopal Shenoy. Outline of Presentation. DOE /BES Synchrotron Radiation Facility Models SNS Model ESRF Model CCLRC Model ILL Model An Assessment: Lessons Learned. User Access and Demographics at DOE/BES Facilities.

348 views • 25 slides

0801 Group meeting

0801 Group meeting. Shiuan-Hal. Content. 1. How to measure the muon lifetime? 2. The previous measurements. 3. The MuLan experiment. 4. What is muon capture? 5. The MuCap experiment. How to measure the muon lifetime?. The muon lifetime is :. How is the muon lifetime measured?. N=1.

372 views • 24 slides

An AGATA @ GANIL Proposal P.H.Regan 1,10 , J.Nyberg 2 , J.Simpson 3 ,

Precision Determinations of the Transition Quadrupole Moments Approaching the N p N n Valence Maximum: Lifetimes of Yrast States in 166,168 Dy. An AGATA @ GANIL Proposal P.H.Regan 1,10 , J.Nyberg 2 , J.Simpson 3 ,

351 views • 22 slides

CERN Neutrino Project

CERN Neutrino Project. 26 th November , 2013 M.Nessi. DG N eutrino P roject mandate and recent P5-DG presentation. More recent Extended D irectorate notes on the R&D short-term plans. short-term objectives :

367 views • 22 slides

The Institut Laue-Langevin

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Commissioning status and plans

Commissioning status and plans. Shinji Machida o n behalf of the beam commissioning team ASTeC /STFC/RAL 12 August 2010. Beam time. Run #1: 20-23 June 2010 Run #2: 12-15 July 2010 Run #3: 27-29 July 2010 Run #4: 3-6 August 2010 end of 4 sector Run #5: 13-15 August 2010 full ring

412 views • 18 slides

260 views • 15 slides

Do you believe in Operation Statistics? Presented at the Accelerator Reliability Workshop 2011

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248 views • 13 slides

N ew detectors for meson spectroscopy in Hall B at JLab

N ew detectors for meson spectroscopy in Hall B at JLab. Baryons2013, June 27 2013. Gabriel Charles. New detectors for meson spectroscopy in hall-B at Jefferson Lab . 1) Meson spectroscopy at CLAS12 2) Feasibility 3) Detector development and time schedule.

219 views • 12 slides

KaoS meeting

KaoS meeting. T.Gogami 20/May/2011. Contents. Experimental setup Fiducialization of KaoS Works. Experimental setup. Pre- c hicane. SPECROMETER-C. Target ( 7 Li, 9 Be). KAOS. Experimental setup. Experimental parameters of this beam time. Pre- c hicane. SPECROMETER-C.

254 views • 11 slides

NUSTAR-5 Design and construction of a superfluid-helium stopping cell

195 views • 7 slides

T-506 REPORT FOR 6-22-13

T-506 REPORT FOR 6-22-13. Start at 5.88 GeV; 150 pC; 5 Hz 9:50 Complete 1 st of four 5-MRad runs 12:30 Complete 2 nd of four 5-Mrad runs 15:10 Complete 3 rd of four 5-Mrad runs 16:40 Begin 1 st of four 23-MRad runs 18:10 Beam down to change energy after 9.7 MRad

150 views • 4 slides

Measurement of the Ratio R = s L / s T in Semi-Inclusive Deep-Inelastic Scattering

Measurement of the Ratio R = s L / s T in Semi-Inclusive Deep-Inelastic Scattering. E12-06-104: Spokespersons Rolf Ent and Hamlet Mkrtchyan (30 days at 6.6 GeV , 6 days at 8.8 GeV , 4 days at 11.0 GeV ). Knowledge on R = s L / s T in SIDIS is essentially non-existing !.

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BLIP operations 06-21-11

119 views • 2 slides