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513L Optics - James C. Wyant (2008) Optics 513L - Optical Testing and Testing Instrumentation Lab Lab #1 - Orientation Lab The purpose of this lab experiment is to become familiar with some elementary aspects of optical alignment and interferometry. First, a laser beam will be aligned with respect to an optical bench, spatially filtered, and collimated. Then, a Twyman-Green interferometer will be set up to observe interference fringes. Each student should align the spatial filter, collimate the beam using the shearing plate, and fine-tune the TwymanGreen to obtain fringes at least once. The techniques you learn today will be needed throughout the semester in order to do the lab experiments. Collimating a Laser Beam 1) Adjust the height and angle of laser beam to align it parallel to the optical bench. 2) Place the spatial filter assembly in front of the laser without the pinhole. 3) Adjust height and tilt of components so the reflections off the optical surfaces are reflected back on themselves. 4) Align the microscope objective so that the beam comes out in the proper orientation. 5) Replace the pinhole into the spatial filter assembly and defocus the microscope objective until light comes through the pinhole. 6) Adjust pinhole position for maximum throughput, bring microscope objective slightly back into focus, and adjust pinhole again. 7) Repeat step 6 until the pinhole is at the microscope objective's focus. 8) Insert collimating lens. height Adjust if necessary. 9) Use plane (nearly) parallel (shearing) plate to check for collimation by placing it in the expanded beam and observing fringes. The shearing plate should be oriented with the wedge going from top to bottom. When the beam is collimated, equally spaced straight horizontal fringes will be seen. Note that if the collimating lens is backwards, the fringes from the shearing plate will not be straight. Optics 513L - James C. Wyant (2008) Twyman-Green Interferometer 1) Setup a Twyman-Green interferometer with equal path lengths. 2) To obtain fringes, look at the focal plane of the lens and tilt the reference mirror to place the foci of both beams on top of one another. Then observe fringes in some other plane. You should get straight equally spaced fringes. 3) Tap the table and observe what happens to the fringes. 4) Increase the path length of one beam and try to obtain fringes. Questions 1) What is the effect of pinhole size on the spatial filter output? 2) How do you determine the optimum pinhole size? 3) Would it be easier or harder to align with the wrong size pinhole? 4) If the collimating lens is in backwards, what aberration is present? 5) How does the fringe stability of the shearing plate compare to that of the TwymanGreen? Why? 6) How large can the path difference be before the fringes are degraded? 7) What properties of the light source limit the fringe contrast as the path difference is increased?
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Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #5 - Twyman-Green Interferometer The purpose of this lab is to Become familiar with the use of a Twyman-Green interferometer for the testing of sph...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - 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 method...
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)
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Arizona >> OPTICS >> 513 (Fall, 2009)
...
Arizona >> CHAPTER >> 513 (Fall, 2009)
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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...
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