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Water motions and orientations in nanotubes of various dimensions.

Water motions and orientations in nanotubes of various dimensions.

Water motions and orientations in nanotubes of various dimensions. (Simulations done by Jay Mashl, University of Illinois/NCSA/Beckman Institute Computational Biology/Nanoscience Group). System Setup. Carbon nanotube (fixed). 8 sizes of nanotubes ranging 5.4  -  16.3 Å dia.,

By aurorette
(234 views)

5x5 Pixel Array Status 3 Dec 2003

5x5 Pixel Array Status 3 Dec 2003

5x5 Pixel Array Status 3 Dec 2003. Sam Burke Sean Stromberg UCSB HEP Group. ASIC Progress. AMI CMOS 0.35 Design Kit 2 Received Design Manual C035MD Ver 5 Design Manual C035MA Ver 3 Core Cells, D Scan FF’s, LVDS Library Pad Limited and Core Limited I/O Cells

By kaden
(108 views)

ALVC

ALVC

Philips Semiconductors, Texas Instruments, tecnología integrada del dispositivo, Hitachi y Pericom abarca la gama más amplia de familias de baja tensión de la lógica. ALVC. CMOS de baja tension avanzada. Se realiza típicamente a las velocidades de 2.2ns en 3.3V.

By vail
(132 views)

Ladder Testing at IPHC and LBL

Ladder Testing at IPHC and LBL

Ladder Testing at IPHC and LBL. Outline. Synchronization of the ladder Ladder L1 operated in SYNC Ladder L2 (LBL) no SYNC Sensor with a faulty output Summary. Synchronization of the ladder.  As suggested by Gilles. Sync sequence: Stop the main CLK RSTB JTAG configuration

By sienna
(133 views)

Part IV Data Path and Control

Part IV Data Path and Control

Part IV Data Path and Control. Try to achieve CPI = 1 with clock that is as high as that for CPI > 1 designs; is CPI < 1 feasible? (Chap 15-16). Design hardware for CPI = 1; seek improvements with CPI > 1 (Chap 13-14). Define an instruction set; make it simple enough

By snow
(119 views)

RAL Site Report

RAL Site Report

RAL Site Report. Castor F2F, CERN Matthew Viljoen. Stuff to cover (at some point). General Operations report (Matthew) Database report (Rich) Tape report (Tim) Disk-only solution investigations (Shaun). Current group structure. Matt 70% mgnt /ops Chris 50% ops

By pegeen
(155 views)

Simulated real beam into simulated MICE

Simulated real beam into simulated MICE

Simulated real beam into simulated MICE. Mark Rayner CM26. Introduction. Various fancy reweighting schemes have been proposed But how would the raw beam fare in Stage 6? TOF0 measures p x and p y at TOF1 given quadrupole field maps

By angus
(109 views)

Monday 6 th

Monday 6 th

Monday 6 th. 07:39 Dump fill #1854, RQ6.L2 tripped, followed by access Piquet EL has changed the three fuses on electrical distribution. Piquet EPC has not found any fault on their power supplies. 9 minutes of stable beams…. 11:35 Injecting again, fill #1855, 1092 + 12 non colliding bunches

By andie
(79 views)

Use of Wavelength Shifter to Enhance Cerenkov Light Detection Art McDonald

Use of Wavelength Shifter to Enhance Cerenkov Light Detection Art McDonald

Use of Wavelength Shifter to Enhance Cerenkov Light Detection Art McDonald SNO Institute, Queen’s University Kingston, Ontario, Canada. D 2 O. D 2 O + WLS. How It Works - SNO. Acrylic Cutoff < 330 nm. 2. SNO OPTICS. H 2 N. O. O. O. HO 3 S. CH 2. C. O. N. CH 3. O. O. HO. O.

By moe
(84 views)

Neutron Spin Echo Spectroscopy (NSE)

Neutron Spin Echo Spectroscopy (NSE)

Neutron Spin Echo Spectroscopy (NSE). Group B. Ilir Zoto Tao Hong Yanmei Lan Nikolaos Daniilidis Sonoko Kanai Mitra Yoonesi Zhaohui Sun 2003 Summer School NCNR, NIST Gaithersburg, MD 20890. NSE Time scale ~ 1 - 10 ns Size scale 1-100 Å. shape fluctuations. Spontaneous curvature,

By roz
(78 views)

Monoenergetic proton backlighting for studying field evolution and areal density in HEDP

Monoenergetic proton backlighting for studying field evolution and areal density in HEDP

Detector. 3 MeV. 15 MeV. DD. D 3 He. 0.6 ns after laser on. Detector. Monoenergetic proton backlighting for studying field evolution and areal density in HEDP. Laser. Detector. R. D. Petrasso, MIT. Summary.

By yannis
(90 views)

Protein « photos » with ultrafast lasers

Protein « photos » with ultrafast lasers

Protein « photos » with ultrafast lasers. Goran Zgrablic Institut de Physique de la Mati è re Condens é e Universit é de Lausanne. Summer School of Science, Vi šnjan Observatory , 27 th july 2003. Proteins: Nano-machines of living cell.

By caraf
(162 views)

Status of the V0 electronics

Status of the V0 electronics

V0C. V0A. Status of the V0 electronics. Tests of photomultipliers Signal treatment Electronics Milestones. Photo-multiplier. 16. 19. 16. 19. 15. Charge, gain, time resolution. Signal x 10 + 25 m cable. Signal amplitude. 75 mV – 1.5 V. ( 125 mV – 1.5 V). Signal amplitude.

By morela
(142 views)

Propagation of HI Beams in Chamber Metal Vapor Atmosphere

Propagation of HI Beams in Chamber Metal Vapor Atmosphere

Propagation of HI Beams in Chamber Metal Vapor Atmosphere. C. Olson, Sandia National Laboratories D. Welch, D. Rose, B. Oliver, T. Genoni, and R. Clark, Mission Research Corporation S. Yu, Lawrence Berkeley National Laboratories ARIES Electronic Project Meeting 10-24-01. Outline.

By eros
(68 views)

Approaches to Turbulence in High-Energy-Density Experiments R. Paul Drake University of Michigan

Approaches to Turbulence in High-Energy-Density Experiments R. Paul Drake University of Michigan

Approaches to Turbulence in High-Energy-Density Experiments R. Paul Drake University of Michigan. 2007 TMBW, Trieste.

By loring
(51 views)

ECAL Design Studies and Scintillator/W/Silicon Hybrid

ECAL Design Studies and Scintillator/W/Silicon Hybrid

ECAL Design Studies and Scintillator/W/Silicon Hybrid. (Quite a lot of this talk overlaps with my (poor audio) talk from Dec 8 th – but there’s a fair amount of new material – and for several of you most of the material is new). Graham W. Wilson Univ. of Kansas Jan 8 th 2004.

By kasie
(136 views)

Status of the LHCb experiment

Status of the LHCb experiment

Status of the LHCb experiment. Andrei Golutvin ( Imperial & CERN & ITEP ) on behalf of the LHCb Collaboration. Outline: Introduction Detector Subsystems Trigger/Online/Computing First Look at the data Cost and funding issues Collaboration matters

By vic
(113 views)

Neutron detection

Neutron detection

Neutron detection. DEMON. present time : DEMON, TONNERRE, EDEN, HENDES, LAND, ORION, … neutron wall.  good neutron detection arrays but. - often compromise (intrinsic efficiency, energy range, angular resolution,...). - become old. - incompatible with safety rules.

By amadis
(186 views)

Fundamental Limits of Timing Resolution for Scintillation Detectors

Fundamental Limits of Timing Resolution for Scintillation Detectors

Outline: Basic Theory Real World Effects Optical Photon Propagation. Fundamental Limits of Timing Resolution for Scintillation Detectors. W. W. Moses, W. S. Choong , & S. E. Derenzo Lawrence Berkeley National Laboratory March 13, 2013.

By vachel
(123 views)

Test Beam 2003 Data Analysis and MonteCarlo Studies

Test Beam 2003 Data Analysis and MonteCarlo Studies

Test Beam 2003 Data Analysis and MonteCarlo Studies. M. Barone Software and Analysis Meeting ATLAS/Frascati. Outline. H8 Test Beam 2003 setup data analysis Results MonteCarlo simulation Garfield Results Work in progress Conclusions. 2003 H8 setup. BML2. BOL2. BIL2. BIL1. BML1.

By burke
(159 views)

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