'Normal incidence' presentation slideshows

KEK layout

KEK layout. k. ito 1 JASS2002 Oct 21, 2002. PF-AR. PF-2.5GeV. ?. k. ito 2 JASS2002 Oct 21, 2002. Layout of the Photon Factory. Synchrotron radiation beamlines in the vacuum ultraviolet and soft X-ray region. k. ito 3 JASS2002 Oct 21, 2002.

811 views • 60 slides

Extreme UV (EUV) lithography

Extreme UV (EUV) lithography. Overview, why EUV lithography? EUV source (hot and dense plasma). Optics (reflection mirrors). Mask (absorber on mirrors). Resist (sensitivity, LER, out-gassing). Contamination control.

2.57k views • 51 slides

GG 450 April 3, 2008

GG 450 April 3, 2008. Refraction, Diffraction, Energy, Sources, and Sensors. Critical Angle: Recall: (Snell's law)

698 views • 46 slides

PHY 712 Electrodynamics 9-9:50 & 10-10:50 AM Olin 107 Plan for Lecture 16-17: Read Chapter 7

591 views • 45 slides

Data from IPP Garching

Data from IPP Garching. W. Eckstein, MPIPP Garching, Germany. Book: Sputtering by Particle Bombardment Editors: R. Behrisch, W. Eckstein. Introduction and Overview (Behrisch, Eckstein) Computer Simulation of the Sputtering Process (Eckstein, Urbassek) Sputtering Yields (Eckstein)

552 views • 37 slides

Electrolytic Etching

Electrolytic Etching. It is a simple way to reveal microstructure of metallic alloys Purpose of etching is to reveale the microstructure of metals and alloys by creating an image contrast. Electrolytic etching ensues right after an electropolishing operation is completed,

1.19k views • 35 slides

Electron-hole pair excitations in the dissociative adsorption

411 views • 23 slides

Photon Transport Monte Carlo

Photon Transport Monte Carlo. Matthew Jones/Riei Ishiziki. Purdue University. Overview Physical processes PMT and electronics response Some results Plans. September 27, 2004. Overview. A photon transport Monte Carlo was developed to interpret TOF results from Run-Ic.

353 views • 20 slides

Announcements 11/12/12

312 views • 19 slides

Unbound States

482 views • 18 slides

R@D work for PID in Novosibirsk

R@D work for PID in Novosibirsk. E.A.Kravchenko Budker INP, Novosibirsk. Outline. MC simulation of RICH with aerogel and NaF radiators R@D on MCP PMTs Life-time tests 3 MCP PMTs Status of multilayer aerogel production and characterization Conclusion. ? 2. Sodium fluoride radiator.

333 views • 18 slides

Motivation General rule for muon triggers:

267 views • 18 slides

Announcements 11/14/11

236 views • 16 slides

Reflectance Models

250 views • 15 slides

Medium effects on waves Geometrical spreading

Medium effects on waves Geometrical spreading. Wave spreads over a larger surface as it travels through the medium. For a spherical wave, the wave energy falls off as the square of the distance. Its effect is to weaken the later arrivals in the seismic section.

295 views • 13 slides

ACCURACY OF DFT CALCULATIONS IN THE DISSOCIATION OF N 2 /W(110) ?

240 views • 12 slides

Improvements in the QE of photocathodes

Improvements in the QE of photocathodes. Peter Townsend University of Sussex Brighton BN1 9QH, UK. The basic steps. Optical absorption Strongly dependent on composition, but predictable from the wavelength dependence of the optical constants

111 views • 11 slides

Diamond detectors: a few facts, test beams and summer plans

159 views • 7 slides

Reflection coefficients

S r. P r. P i. f r. q i. q r. a 1 , b 1 a 2 , b 2. q t. f t. P t. S t. Sin q i Sin q r Sin q t Sin f r Sin f t a 1 a 1 a 2 b 1 b 2. Reflection coefficients. r. -. r. V. V. 2. 2. 1.

153 views • 5 slides

MAE 5495: Launch Vehicle Analysis Lesson 4: Introduction to Thermodynamics

MAE 5495: Launch Vehicle Analysis Lesson 4: Introduction to Thermodynamics. Dr. Andrew Ketsdever UCCS. Rockets of the Day. Laser Propulsion Laser Pointer: 5 mW, Spot size 3-4 mm diameter For normal incidence and r = 1 F = 33 picoNewtons Isp = ? (almost)

111 views • 3 slides