Documents Found!
As seen in
Less Work, Better Grades
Join
Course Hero
Access
best resources
Ace
your classes
Ace your courses with Course Hero!
|
|
|
Study Smarter, Score Higher
Here are the top 5 related documents
...FECO.nb
Optics 505 James C. Wyant
1
6.5 FECO (Fringes of Equal Chromatic Order)
FECO (Fringes of Equal Chromatic Order)
Ref: Born & Wolf, p. 359. The FECO interferometer is a multiple-beam interferometer in which the test sample is focused onto t...
...1.0 MEASUREMENT OF PARAXIAL PROPERTIES OF OPTICAL SYSTEMS
James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ 85721 jcwyant@u.arizona.edu
If we wish to completely characterize the paraxial properties of a lens, it is necessary to...
...8.2.15) Lateral Shear Test In a lateral shear interferometer the wavefront to be tested, W(x,y), is interfered with a shifted version of itself. Let the shift, or shear, between the two interfering wavefronts be x in the x direction, then a bright fr...
...Absolute Testing
Absolute measurement of flats Absolute measurement of flats Absolute measurement of spheres Absolute measurement of spheres Absolute measurement of surface roughness Absolute measurement of surface roughness
James C. Wyant
Abso...
Document Content (unformatted)
Course Hero has millions of student submitted documents similar to the one
below including study guides, homework solutions, papers, exam answer keys and textbook solutions.
513L Optics - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #3 - Refractive Index Measurement: Abbe Refractometer Goniometer Brewster's Angle The purpose of this lab is to become familiar with several methods of measuring refractive index. Procedure: Use the goniometer to measure the prism angle, angle of minimum deviation, and the refractive index of the prism provided. Use the Abbe refractometer to measure the refractive index and dispersion of a) the lens b) the prism c) a liquid sample. CAUTION: The illuminating and measuring prisms in the Abbe are made of glass with a high refractive index. They are inherently soft. Be careful not to add any more scratches. Do not touch the reference prism when applying the matching fluid. If too much fluid is used, the test piece will slide off. The manner in which the surface of the measuring prism is treated will determine the useful life of the instrument. Using the 633nm polarized HeNe laser, measure Brewster's angle and compute the refractive index from it. Optics 513L - James C. Wyant (2008) Questions: Goniometer 1) What is your measurement uncertainty in the a) Prism angle? b) Angle of minimum deviation? c) Refractive index? 2) What is the precision of the refractive index measurement? sets What the limits on precision? 3) What factors affect the accuracy of the measurement? Abbe Refractometer 1) What is the measurement uncertainty in the refractive index? Explain. 2) What is the precision of the refractive index measurement? What sets the limits on precision? What is the precision of the dispersion measurement? 3) 4) What factors affect the accuracy of the measurement? Why should the refractive index of the contact liquid used in measuring the index of a solid sample be higher than the index of the sample? How close should the index of the matching fluid be to the sample? should the index of the matching fluid be to the reference prism? How close 5) 6) 7) How do scratches on the reference prism affect the measurement and its accuracy? Describe in words the light path when a) the sample is illuminated. b) the scale is illuminated. How would you modify the model of the Abbe refractometer used in the lab to make the measurements either more accurate or easier to perform? 8) Brewster's Angle 1) What are the major sources of error in the measurement? 2) How do your measured values compare with tabulated data in the Schott glass catalog for BK7? Optics 513L - James C. Wyant (2008) 3) How would you propose to increase the accuracy of the measurements?
Find millions of documents here - Study Guides, Homework Solutions, Papers, Exam Answer Keys and more.
Course Hero has millions of course related materials that will enable you to learn better,
faster and get an A in all your courses.
Below is a small sample set of documents:
Below is a small sample set of documents:
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #11 - Laser Based Fizeau Interferometer The purpose of this lab is to become familiar with the use of a laser based Fizeau interferometer for testi...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #7 - Foucault, Wire, and Ronchi Tests The purpose of this lab is to obtain \"hands on\" experience with the Foucault (knife-edge), wire, and Ronchi te...
Arizona >> OPTICS >> 08 (Fall, 2008)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> OPTICS >> 513 (Fall, 2009)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> OPTICS >> 08 (Fall, 2008)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> OPTICS >> 513 (Fall, 2009)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> CHAPTER >> 513 (Fall, 2009)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> OPTICS >> 10 (Fall, 2009)
...
Arizona >> OPTICS >> 513 (Fall, 2009)
...
Arizona >> CHAPTER >> 513 (Fall, 2009)
...
Arizona >> OPTICS >> 513 (Fall, 2009)
LightDistributionNearFocus.nb 1 Light Distribution Near Focus Diagram showing notation for diffraction of a converging wave at a circular aperture y P 2a x z f Fresnel diffraction equation The amplitude can be written as u@x, yD = A kf Hx2 +y 2 ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
LightDistributionNearFocus.nb 1 Light Distribution Near Focus Diagram showing notation for diffraction of a converging wave at a circular aperture y P 2a x z f Fresnel diffraction equation The amplitude can be written as u@x, yD = A kf Hx2 +y 2 ...
Arizona >> OPTICS >> 11 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> OPTICS >> 513 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> OPTICS >> 06 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> OPTICS >> 513 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> CHAPTER >> 513 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> OPTICS >> 06 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> OPTICS >> 513 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> OPTICS >> 08 (Fall, 2008)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> OPTICS >> 513 (Fall, 2009)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> CHAPTER >> 513 (Fall, 2009)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> OPTICS >> 05 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> OPTICS >> 513 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> CHAPTER >> 513 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> OPTICS >> 05 (Fall, 2009)
White Light Interferometry Eliminates ambiguities in heights present with monochromatic interferometry Techniques old, but use of modern electronics and computers enhance capabilities and applications 1998 - James C. Wyant Page 1 of 24 How High...
Arizona >> OPTICS >> 513 (Fall, 2009)
White Light Interferometry Eliminates ambiguities in heights present with monochromatic interferometry Techniques old, but use of modern electronics and computers enhance capabilities and applications 1998 - James C. Wyant Page 1 of 24 How High...
Arizona >> OPTICS >> 08 (Fall, 2008)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> OPTICS >> 513 (Fall, 2009)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> CHAPTER >> 513 (Fall, 2009)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> OPTICS >> 04 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> OPTICS >> 513 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> OPTICS >> 05 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> OPTICS >> 513 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> CHAPTER >> 513 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> OPTICS >> 07 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> OPTICS >> 513 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> OPTICS >> 04 (Fall, 2009)
4.8 Classical Interferogram Analysis Elementary analysis of interferograms Elementary analysis of interferograms Computer analysis of interferograms Computer analysis of interferograms Typical Interferogram Surface Error = (/2) (/S) Classical...
Arizona >> OPTICS >> 513 (Fall, 2009)
4.8 Classical Interferogram Analysis Elementary analysis of interferograms Elementary analysis of interferograms Computer analysis of interferograms Computer analysis of interferograms Typical Interferogram Surface Error = (/2) (/S) Classical...
Arizona >> OPTICS >> 05 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> OPTICS >> 513 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> CHAPTER >> 513 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> OPTI >> 510 (Fall, 2009)
Fall 2008 OPTI 510L Fundamentals of Applied Optics Lab Instructor: Jim Burge Optical Sciences 733 (520) 621-8182 jburge@optics.arizona.edu Teaching Assistant: Rene Zehnder Optical Sciences 300 (520) 626-7302 rzehnder@optics.arizona.edu Class: Mein...
Arizona >> OPTI >> 510 (Fall, 2009)
Error Analysis Error analysis is an extremely important part of any measurement. All the uncertainties in a measurement conspire to give the incorrect result. It is important that you understand the limitations of your measurements and that you alway...
Arizona >> OPTI >> 510 (Fall, 2009)
510L LAB 7 Coma Set-up Equipment: o o o o o o Fiber Light Source (it\'s good to have a bright source when using small pinholes) 50 m Pinhole (or any small pinhole) Two slow, plano-convex lenses for collimating and focusing Two fast lenses of matchin...
Arizona >> HW >> 10 (Fall, 2009)
Two Part Epoxy Adhesives A Technical Memo Prepared for Opti 521 Introduction to Opto-Mechanical Engineering By Scott Gibb November 24, 2006 Description and Basic Characteristics Two-part epoxy adhesive is a type of thermosetting polymer. A thermoset,...
Arizona >> HW >> 521 (Fall, 2009)
Two Part Epoxy Adhesives A Technical Memo Prepared for Opti 521 Introduction to Opto-Mechanical Engineering By Scott Gibb November 24, 2006 Description and Basic Characteristics Two-part epoxy adhesive is a type of thermosetting polymer. A thermoset,...
Arizona >> HW >> 10 (Fall, 2009)
Optomechanical Epoxy Adhesives Mark T. Sullivan Lockheed Martin Space Systems Advanced Technology Center, 3251 Hanover Street, Palo Alto, CA 94304 mark.t.sullivan@lmco.com 650/424-2722 SUMMARY This report summarizes the basic characteristics and pro...
Arizona >> HW >> 521 (Fall, 2009)
Optomechanical Epoxy Adhesives Mark T. Sullivan Lockheed Martin Space Systems Advanced Technology Center, 3251 Hanover Street, Palo Alto, CA 94304 mark.t.sullivan@lmco.com 650/424-2722 SUMMARY This report summarizes the basic characteristics and pro...
Arizona >> HW >> 10 (Fall, 2009)
Manual Linear Stages Dathon Golish OPTI 521 HW #10b University of Arizona 520-626-9230 dgolish@u.arizona.edu November 29, 2006 This report will compare and contrast the characteristics of various manual linear stages of moderate travel distance (~10 ...
Arizona >> HW >> 521 (Fall, 2009)
Manual Linear Stages Dathon Golish OPTI 521 HW #10b University of Arizona 520-626-9230 dgolish@u.arizona.edu November 29, 2006 This report will compare and contrast the characteristics of various manual linear stages of moderate travel distance (~10 ...
Arizona >> HW >> 10 (Fall, 2009)
OPTI 521 HW 10 ADHESIVES TALIAFERRO Summers Optical Type RD3-74 2-Part Optical Epoxy with Plasticizer for Low Curing-Stress Applications http:/www.emsdiasum.com/summers/optical/cements/default.htm SUMMARY AND BASIC CHARACTERISTICS Summers Optical s...
Arizona >> HW >> 521 (Fall, 2009)
OPTI 521 HW 10 ADHESIVES TALIAFERRO Summers Optical Type RD3-74 2-Part Optical Epoxy with Plasticizer for Low Curing-Stress Applications http:/www.emsdiasum.com/summers/optical/cements/default.htm SUMMARY AND BASIC CHARACTERISTICS Summers Optical s...
Arizona >> HW >> 10 (Fall, 2009)
Milbond Structural Adhesive A Technical Memo for OPTI521 Tim Williams Nov. 30, 2006 Introduction and Basic Characteristics Basic characteristics, strengths, applications and usage information are given for Milbond Structural Adhesive. Milbond is a st...
Arizona >> HW >> 521 (Fall, 2009)
Milbond Structural Adhesive A Technical Memo for OPTI521 Tim Williams Nov. 30, 2006 Introduction and Basic Characteristics Basic characteristics, strengths, applications and usage information are given for Milbond Structural Adhesive. Milbond is a st...
Arizona >> HW >> 10 (Fall, 2009)
UV Curing Adhesives Jay Vizgaitis, Opti 521 Homework 10 Properties: UV curing adhesive are one part adhesives that cure within seconds when UV light is applied. They are used for bonding glasses to glass, metals, and plastics for applications such as...
Arizona >> HW >> 521 (Fall, 2009)
UV Curing Adhesives Jay Vizgaitis, Opti 521 Homework 10 Properties: UV curing adhesive are one part adhesives that cure within seconds when UV light is applied. They are used for bonding glasses to glass, metals, and plastics for applications such as...
Arizona >> WORKSHOP >> 2009 (Fall, 2009)
Co-Sponsor: http:/spie.org U of AZ College of Optical Sciences Computer Generated Holography (CGH) and Diffractive Optical Element (DOE) Workshop Introduction From the early work of Lohmann to present day, applications such as multi-spectral disper...
Arizona >> OPTI >> 696 (Fall, 2009)
Fluorescence Spectral Characteristics of Fiber Optic Imaging Bundles Josh Udovich November 30, 2005 Outline Why fiber bundles? Current uses of fiber optic imaging bundles Autofluorescence of these bundles really is an issue Testing setup Fiber fluo...
Arizona >> OPTI >> 696 (Fall, 2009)
The Axicon Proteep Mallik OPTI 696bx 12/7/05 Outline What is an axicon? Its history Its many uses Optical alignment Generation of diffraction free beams Corneal surgery OCT Atom traps Acoustic testing . the list is endless! Modeling an axicon- ZEM...
Arizona >> OPTI >> 696 (Fall, 2009)
Ultrathin Fiberscope Utilizing a Single Channel for Both Illumination and Imaging Angelique Kano, Arthur Gmitro College of Optical Sciences and Radiology Research University of Arizona Part I: Numerical Aperture Sharing to Achieve Single Channel Fi...
Arizona >> OPTI >> 696 (Fall, 2009)
Liquid Crystal Displays Heather Durko Practical Optics Seminar 30 November 2005 Overview LC basics LC types and applications Grayscale LCD Color LCD \"reverse engineering\" Conclusion Liquid crystals 1888Friedrich Reinitzer discovered two melt...
Arizona >> OPTI >> 696 (Fall, 2009)
Organic Devices Mir F. Salek Optics Seminars Final Presentation Goals Introducing organic light emitting diodes and organic solar cells Describing the process of developing these devices in Lab Summary Organic semiconductors OLEDs Organic solar cel...
Arizona >> OPTI >> 696 (Fall, 2009)
Design of a CTIS for use in the long-wave infrared Riley Aumiller 11-07-05 Outline Introduction to new device Describe how it is different Layout Details about components Go into detail about the design of a specific component. Review Questio...
Arizona >> ISTA >> 6 (Fall, 2009)
COMPARATIVE ASSESSMENT OF ROSELLE (Hibiscus sabdariffa var. sabdariffa) SEED MEAL AND KENAF (Hibiscus sabdariffa var. altissima) SEED MEAL AS REPLACEMENT FOR SOYBEAN MEAL IN PRACTICAL DIETS FOR FINGERLINGS OF NILE TILAPIA, Oreochromis niloticus O. A....
What are you waiting for?