Topic 7: Photographic Process

Size: px
Start display at page:

Download "Topic 7: Photographic Process"

Transcription

1 V Topic 7: Photographic Process Aim: To cover the basics of the photographic process, and the properties of photographic material. Contents: asics of Photographic Process xposure and Transmittance urter and riffield Curve Characterisation of Photographic Process Two stage process Transmittance in coherent light. APPL PTC P PATMT of PYC Photographic Process -1- Autumn Term

2 V tructure of Photographic Material mulsion of ilver alide Crystals elatin Anti-halation layer ubstrate (acetate/glass) rain: mulsion of rains of ilver alide in elatin base. rain elatin 50! 500 nm (λ=10! λ=2) 3! 15 µm thick ach grain contains 10 11! ions, so large on atomic scale. ilver alide: Typically mixture of ilver romide, ilver odide and other ilver salts. ubstrate: sually acetate or polyester. lass use when flat stable material needed, (in holography and spectroscopy). Anti-halation layer: Light blocking layer to prevent internal reflections from substrate. ull details of photographic process is difficult chemistry, just supply an overview. APPL PTC P PATMT of PYC Photographic Process -2- Autumn Term

3 V asic Process xpose to Light 1. Quantum(s) of light free electron(s) in lattice. 2. lectron captured by silver ion (interstitial ion) 3. Migration of silver ions to neutralise local charge 4. eformation of lattice allows migrated silver ions to form form speck of silver in the grain. 5. pecks of silver known as Latent mage. ote: pecks much smaller than the grain, typically 50 to 100 silver atoms. Latent mage strength given by number of specks so proportional to incident number of photons (intensity) ormation of one latent image take about 10,4 s (limits film speed). n practice, need about 50 photons absorbed by a single grain to form Latent mage. This process results in the Latent mage recording the incident intensity pattern. APPL PTC P PATMT of PYC Photographic Process -3- Autumn Term

4 V evelopment Want to develop grains of silver halide exposed to light into solid (opaque) silver. Two basic processes, Chemical and Physical. Chemical evelopment: Treat film with weak reducing agent, 1. Add electrons to silver halide that liberates silver. 2. Liberated silver binds to latent image specks. 3. rains with strong latent image develop first. Process is highly temperature dependent, and slow (many minutes). (complex chemical process). Physical evelopment: asically same principle, but deposited silver mostly comes from silver salts in the developer rather than the silver salts in the film. (very little used due to cost of developer.) ixing emove remaining silver halide with stronger reducing agent. Typically also contains agents to harden the gelatin to prevent mechanical damage. APPL PTC P PATMT of PYC Photographic Process -4- Autumn Term

5 V xposure and Transmittance efine: xposure as nergy per nit Area incident. or incident intensity of g(x;y) for timeτ: (x;y)=g(x;y)τ We will typically imply (x;y) dependence, and write = gτ efine: ntensity Transmittance at a point (x;y) as T = Transmitted intensity at (x;y) ncident intensity at (x;y) T 0 T T = T 0 so 0 T 1 o in two dimensions we have T(x,y) f(x,y) g(x,y) g(x;y)= f(x;y)t(x;y) with g(x;y) f(x;y) APPL PTC P PATMT of PYC Photographic Process -5- Autumn Term

6 V xposure to Transmittance urter and riffield showed that 1 log 10 Mass of metallic silver T efine: ptical ensity as mass of metallic silver per unit area, so: = log 10 1 T =,log 10 (T) The film characteristics are then experimentally measured as plot of against. ote: ach film has a different characteristic plot. The shape of this plot can also be altered by different types of developer and by changing the development time. Most manufactured supply technical information on request. APPL PTC P PATMT of PYC Photographic Process -6- Autumn Term

7 V urter and riffield Curve s 3 houlder 2 f 1 Toe Linear egion 0-0 log () Low xposure: ptical ensity not dependent on. Constant og Level f. (Typically f 0:3) 2. Medium xposure: Linear region where log 10 () (seful region). 3. igh xposure: aturation (all grains developed into silver). Typically s 3:0 (0.01% transmittance) ynamic range of the file is = s, f 2:5 typical film APPL PTC P PATMT of PYC Photographic Process -7- Autumn Term

8 V ilm peed ilm peed: Measure of for given xposure. olographic materials measured in µjcm,2, to give a good holographic exposure. Photographic material subjective speed measure when developed in standard developer. Two typical measures: AA Linear with Linear with (log of exposure) Typical ilm peeds: AA Type 5 Lithographic film 25 Very slow portrait film 100 ormal b/w or colour film 400 ast b/w or colour 1000 astest normal film > 1000 pecial processing sed as a guide only: (eg: 400 AA film requires 1/4 xposure of 100 AA). ifficult to get quantative measure. (ee tutorial) Always get trade-off low speed mall rains igh esolution igh speed Large rains Low esolution APPL PTC P PATMT of PYC Photographic Process -8- Autumn Term

9 V n linear region we have Linear egion = γlog 10 (), 0 where γ is the gradient (Called ilm amma). We have that =,log 10 (T) & so that the intensity transmittance = gτ T = 10 0,γ = 10 0(gτ),γ elation between xposure and intensity transmittance T is - LA. Key esult Low Contrast: γ 1 igh speed lack/white file, (P-5, or Tri-X). mall changes in ptical ensity with Large change in exposure. ilms normally ast. igh Contrast: γ 2! 3 Lithogrphic copy film, very Large changes in ptical ensity with mall changes in exposure. utput often binary (black or white). ilms noramlly low. APPL PTC P PATMT of PYC Photographic Process -9- Autumn Term

10 V Variation of γ or filmable to modify γ by changing exposure and development conditions. ncrease amma: Low exposure plus long/hot development. Weak latent image, only brightest point developed to full darkness, high contrast. ecrease amma: igh exposure plus short/cold development. trong latent image. Latent image only partially developed, low contrast. or a typical /W white film (P-5), we get γ evelopment Time (minutes) so will careful development we can select the γ required. APPL PTC P PATMT of PYC Photographic Process -10- Autumn Term

11 V Two tage Process Consider two stage photographic process. 1) orm egative ncident intensity of f(x;y) for time τ with γ. egative with T = K ( f τ ),γ K = constant 2) orm Positive lluminate egative, project onto second film. T Photographic Material Constant g(x,y) = T n second film, intensity g(x;y)=t (x;y) econd film has γ P and exposure τ P, transmission T P = K P (gτ P ),γ P = K P (K τ P ),γ P( f τ ) γ γ P = K( f τ ) γ γ P o if we choose γ γ P = 1 then we have the original incident intensity. T P (x;y) f(x;y) ntensity Linearity possible APPL PTC P PATMT of PYC Photographic Process -11- Autumn Term

12 V egatives in Coherent Light orm a negative with intensity f(x;y), intensity transmittance T = K( f τ),γ where for coherent light f(x;y)=ju(x;y)j 2. lluminate negative with coherent light, want Amplitude Transmittance. lluminate with constant beam, transmitted amplitude is v(x;y)= p T(x;y) assuming that there is no optical path differences in the negative, (no phase effects). efine: Amplitude Transmittance, which we will usually write as: T a = p T = 10 0=2 ( f τ),γ=2 T a = p K( f τ),γ=2 K = constant Key esult This will be used in holography in the next lecture. APPL PTC P PATMT of PYC Photographic Process -12- Autumn Term

13 V Practical Problem elatin surface not flat after development elatin urface olid ilver ubstrate hrinks to cover solid silver, (also cracks). ips of up to 2µm common, so sever phase problem. olution: ptical ate: ptically lat lass ndex Matching fluid elatin film se oil/solvent with same refractive index as gelatin, (n = 1:53) Light silicon oil or xylene (both rather unpleasant). ptical gate required when critical optical measures are being made. APPL PTC P PATMT of PYC Photographic Process -13- Autumn Term

Radiology. Radiograph: Is the image of an object made with use of X- ray instead of light.

Radiology. Radiograph: Is the image of an object made with use of X- ray instead of light. Radiology د. اريج Lec. 3 X Ray Films Radiograph: Is the image of an object made with use of X- ray instead of light. Dental x- ray film: Is a recording media on which image of the object was made by exposing

More information

Holography (A13) Christopher Bronner, Frank Essenberger Freie Universität Berlin Tutor: Dr. Fidder. July 1, 2007 Experiment on July 2, 2007

Holography (A13) Christopher Bronner, Frank Essenberger Freie Universität Berlin Tutor: Dr. Fidder. July 1, 2007 Experiment on July 2, 2007 Holography (A13) Christopher Bronner, Frank Essenberger Freie Universität Berlin Tutor: Dr. Fidder July 1, 2007 Experiment on July 2, 2007 1 Preparation 1.1 Normal camera If we take a picture with a camera,

More information

Characterization of High Resolution Photographic Emulsion BB640 by Holographic Methods

Characterization of High Resolution Photographic Emulsion BB640 by Holographic Methods 24 International Symposium on Silver Halide Technology Characterization of High Resolution Photographic Emulsion BB64 by Holographic Methods M. Ulibarrena, L. Carretero, S. Blaya, R. Madrigal and A. Fimia

More information

Chapters 1-3. Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation. Chapter 3: Basic optics

Chapters 1-3. Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation. Chapter 3: Basic optics Chapters 1-3 Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation Radiation sources Classification of remote sensing systems (passive & active) Electromagnetic

More information

X-ray Imaging. PHYS Lecture. Carlos Vinhais. Departamento de Física Instituto Superior de Engenharia do Porto

X-ray Imaging. PHYS Lecture. Carlos Vinhais. Departamento de Física Instituto Superior de Engenharia do Porto X-ray Imaging PHYS Lecture Carlos Vinhais Departamento de Física Instituto Superior de Engenharia do Porto cav@isep.ipp.pt Overview Projection Radiography Anode Angle Focal Spot Magnification Blurring

More information

Seminar 8. Radiology S8 1

Seminar 8. Radiology S8 1 Seminar 8 Radiology Medical imaging. X-ray image formation. Energizing and controlling the X-ray tube. Image detectors. The acquisition of analog and digital images. Digital image processing. Selected

More information

Chapters 1-3. Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation. Chapter 3: Basic optics

Chapters 1-3. Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation. Chapter 3: Basic optics Chapters 1-3 Chapter 1: Introduction and applications of photogrammetry Chapter 2: Electro-magnetic radiation Radiation sources Classification of remote sensing systems (passive & active) Electromagnetic

More information

The Technology of Enhanced Color Saturation. KODAK EKTACHROME 100D Color Reversal Film/5285. David Long Eastman Kodak Company

The Technology of Enhanced Color Saturation. KODAK EKTACHROME 100D Color Reversal Film/5285. David Long Eastman Kodak Company The Technology of Enhanced Color Saturation KODAK EKTACHROME 100D Color Reversal Film/5285 David Long Eastman Kodak Company History of 100D Film Color Technology Initial Benefit Statement Research into

More information

DEVELOPMENT PROCESS FOR PVCz HOLOGRAM

DEVELOPMENT PROCESS FOR PVCz HOLOGRAM Journal of Photopolymer Science and Technology Volume 4, Number 1(1991) 127-134 DEVELOPMENT PROCESS FOR PVCz HOLOGRAM Yasuo YAMAGISHI, Takeshi ISHITSUKA, and Yasuhiro YONEDA Fujitsu Laboratories Ltd. Morinosato

More information

Transmitting Light: Fiber-optic and Free-space Communications Holography

Transmitting Light: Fiber-optic and Free-space Communications Holography 1 Lecture 9 Transmitting Light: Fiber-optic and Free-space Communications Holography 2 Wireless Phone Calls http://havilandtelconews.com/2011/10/the-reality-behind-wireless-networks/ 3 Undersea Cable and

More information

Lithography. 3 rd. lecture: introduction. Prof. Yosi Shacham-Diamand. Fall 2004

Lithography. 3 rd. lecture: introduction. Prof. Yosi Shacham-Diamand. Fall 2004 Lithography 3 rd lecture: introduction Prof. Yosi Shacham-Diamand Fall 2004 1 List of content Fundamental principles Characteristics parameters Exposure systems 2 Fundamental principles Aerial Image Exposure

More information

SFR 406 Spring 2015 Lecture 7 Notes Film Types and Filters

SFR 406 Spring 2015 Lecture 7 Notes Film Types and Filters SFR 406 Spring 2015 Lecture 7 Notes Film Types and Filters 1. Film Resolution Introduction Resolution relates to the smallest size features that can be detected on the film. The resolving power is a related

More information

LECTURE 26: Interference

LECTURE 26: Interference ANNOUNCEMENT *Final: Thursday December 14, 2017, 1 PM 3 PM *Location: Elliot Hall of Music *Covers all readings, lectures, homework from Chapters 28.6 through 33. *The exam will be multiple choice. Be

More information

X-ray Tube and Generator Basic principles and construction

X-ray Tube and Generator Basic principles and construction X-ray Tube and Generator Basic principles and construction Dr Slavik Tabakov - Production of X-rays OBJECTIVES - X-ray tube construction - Anode - types, efficiency - X-ray tube working characteristics

More information

Achievement of Arbitrary Bandwidth of a Narrow Bandpass Filter

Achievement of Arbitrary Bandwidth of a Narrow Bandpass Filter Achievement of Arbitrary Bandwidth of a Narrow Bandpass Filter Cheng-Chung ee, Sheng-ui Chen, Chien-Cheng Kuo and Ching-Yi Wei 2 Department of Optics and Photonics/ Thin Film Technology Center, National

More information

Processing Film. How do I develop and fix the latent image on my film so I can make prints? By Marcine Linder

Processing Film. How do I develop and fix the latent image on my film so I can make prints? By Marcine Linder Processing Film How do I develop and fix the latent image on my film so I can make prints? By Marcine Linder The Structure of Film The emulsion layer of black and white film has light-sensitive silver

More information

Experimental Competition

Experimental Competition 37 th International Physics Olympiad Singapore 8 17 July 2006 Experimental Competition Wed 12 July 2006 Experimental Competition Page 2 List of apparatus and materials Label Component Quantity Label Component

More information

NPTEL NPTEL ONLINE COURSE. NPTEL Online Certification Course (NOC) NPTEL. Theory and Practice of Non Destructive Testing

NPTEL NPTEL ONLINE COURSE. NPTEL Online Certification Course (NOC) NPTEL. Theory and Practice of Non Destructive Testing NPTEL NPTEL ONLINE COURSE NPTEL Online Certification Course (NOC) NPTEL Theory and Practice of Non Destructive Testing Dr. Ranjit Bauri Dept. of Metallurgical & Materials Engineering IIT Madras, Chennai

More information

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2003 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency

Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency Fully depleted, thick, monolithic CMOS pixels with high quantum efficiency Andrew Clarke a*, Konstantin Stefanov a, Nicholas Johnston a and Andrew Holland a a Centre for Electronic Imaging, The Open University,

More information

Optical Requirements

Optical Requirements Optical Requirements Transmission vs. Film Thickness A pellicle needs a good light transmission and long term transmission stability. Transmission depends on the film thickness, film material and any anti-reflective

More information

Refractive Power of a Surface. Exposure Sources. Thin Lenses. Thick Lenses. High Pressure Hg Arc Lamp Spectrum

Refractive Power of a Surface. Exposure Sources. Thin Lenses. Thick Lenses. High Pressure Hg Arc Lamp Spectrum eractive Power o a Surace The reractive power P is measured in diopters when the radius is expressed in meters. n and n are the reractive indices o the two media. EE-57: icrofabrication n n P n n Exposure

More information

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. EE143 Ali Javey Slide 5-1

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. EE143 Ali Javey Slide 5-1 Section 2: Lithography Jaeger Chapter 2 Litho Reader EE143 Ali Javey Slide 5-1 The lithographic process EE143 Ali Javey Slide 5-2 Photolithographic Process (a) (b) (c) (d) (e) (f) (g) Substrate covered

More information

Supplementary information for Stretchable photonic crystal cavity with

Supplementary information for Stretchable photonic crystal cavity with Supplementary information for Stretchable photonic crystal cavity with wide frequency tunability Chun L. Yu, 1,, Hyunwoo Kim, 1, Nathalie de Leon, 1,2 Ian W. Frank, 3 Jacob T. Robinson, 1,! Murray McCutcheon,

More information

Basics of Holography

Basics of Holography Basics of Holography Basics of Holography is an introduction to the subject written by a leading worker in the field. The first part of the book covers the theory of holographic imaging, the characteristics

More information

FABRICATION OF CMOS INTEGRATED CIRCUITS. Dr. Mohammed M. Farag

FABRICATION OF CMOS INTEGRATED CIRCUITS. Dr. Mohammed M. Farag FABRICATION OF CMOS INTEGRATED CIRCUITS Dr. Mohammed M. Farag Outline Overview of CMOS Fabrication Processes The CMOS Fabrication Process Flow Design Rules Reference: Uyemura, John P. "Introduction to

More information

The Photorefractive Effect

The Photorefractive Effect The Photorefractive Effect Rabin Vincent Photonics and Optical Communication Spring 2005 1 Outline Photorefractive effect Steps involved in the photorefractive effect Photosensitive materials Fixing Holographic

More information

Digital Imaging Rochester Institute of Technology

Digital Imaging Rochester Institute of Technology Digital Imaging 1999 Rochester Institute of Technology So Far... camera AgX film processing image AgX photographic film captures image formed by the optical elements (lens). Unfortunately, the processing

More information

EE143 Fall 2016 Microfabrication Technologies. Lecture 3: Lithography Reading: Jaeger, Chap. 2

EE143 Fall 2016 Microfabrication Technologies. Lecture 3: Lithography Reading: Jaeger, Chap. 2 EE143 Fall 2016 Microfabrication Technologies Lecture 3: Lithography Reading: Jaeger, Chap. 2 Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1-1 The lithographic process 1-2 1 Photolithographic

More information

Chapter Ray and Wave Optics

Chapter Ray and Wave Optics 109 Chapter Ray and Wave Optics 1. An astronomical telescope has a large aperture to [2002] reduce spherical aberration have high resolution increase span of observation have low dispersion. 2. If two

More information

Module - 2 Lecture - 13 Lithography I

Module - 2 Lecture - 13 Lithography I Nano Structured Materials-Synthesis, Properties, Self Assembly and Applications Prof. Ashok. K.Ganguli Department of Chemistry Indian Institute of Technology, Delhi Module - 2 Lecture - 13 Lithography

More information

Tutorial Solutions. Show that for an image of a distant disc of constant intensity the intensity on the film plane is. 1 F No

Tutorial Solutions. Show that for an image of a distant disc of constant intensity the intensity on the film plane is. 1 F No 7 Photographic Properties Tutorial s Short set of questions on the photographic process all exploring the relation between exposure and transmittance. Questions 1, and 4 are essential to the course. 7.1

More information

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. The lithographic process

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. The lithographic process Section 2: Lithography Jaeger Chapter 2 Litho Reader The lithographic process Photolithographic Process (a) (b) (c) (d) (e) (f) (g) Substrate covered with silicon dioxide barrier layer Positive photoresist

More information

Design and Analysis of Resonant Leaky-mode Broadband Reflectors

Design and Analysis of Resonant Leaky-mode Broadband Reflectors 846 PIERS Proceedings, Cambridge, USA, July 6, 8 Design and Analysis of Resonant Leaky-mode Broadband Reflectors M. Shokooh-Saremi and R. Magnusson Department of Electrical and Computer Engineering, University

More information

Section 2: Lithography. Jaeger Chapter 2. EE143 Ali Javey Slide 5-1

Section 2: Lithography. Jaeger Chapter 2. EE143 Ali Javey Slide 5-1 Section 2: Lithography Jaeger Chapter 2 EE143 Ali Javey Slide 5-1 The lithographic process EE143 Ali Javey Slide 5-2 Photolithographic Process (a) (b) (c) (d) (e) (f) (g) Substrate covered with silicon

More information

Development of a Thin Double-sided Sensor Film EXCLEAR for Touch Panels via Silver Halide Photographic Technology

Development of a Thin Double-sided Sensor Film EXCLEAR for Touch Panels via Silver Halide Photographic Technology Development of a Thin Double-sided Sensor Film EXCLEAR for Touch Panels via Silver Halide Photographic Technology Akira ICHIKI* Yuichi SHIRASAKI* Tadashi ITO** Tadahiro SORORI*** and Tadahiro KEGASAWA****

More information

Panchromatic negative film for aerial photography

Panchromatic negative film for aerial photography AVIPHOT PAN 400S Panchromatic negative film for aerial photography Aviphot Pan 400S PE1/PE0 is a panchromatic aerial negative film with medium resolution. The emulsion is coated onto a transparent polyester

More information

Observing Microorganisms through a Microscope

Observing Microorganisms through a Microscope 2016/2/19 PowerPoint Lecture Presentations prepared by Bradley W. Christian, McLennan Community College CHAPTER 3 Observing Microorganisms through a Microscope 1 Figure 3.2 Microscopes and Magnification.

More information

ECEN 4606, UNDERGRADUATE OPTICS LAB

ECEN 4606, UNDERGRADUATE OPTICS LAB ECEN 4606, UNDERGRADUATE OPTICS LAB Lab 7: Holography Original version: Professor McLeod SUMMARY: In this lab you will record and develop your own holograms including a double-exposure hologram that will

More information

Recording and reconstruction of holograms

Recording and reconstruction of holograms Recording and reconstruction of holograms LEP Related topics Dispersion, reflection, object beam, reference beam, real and virtual image, volume hologram, Lippmann-Bragg hologram, Bragg reflection. Principle

More information

Kodak Thermal Print Microfilms

Kodak Thermal Print Microfilms Kodak Thermal Print Microfilms Kodak Premium 1000 Thermal Print Film 1323 Kodak Thermal Print Film KF 1353/2353 Vesicular films exposed to actinic radiation (UV/violet) generate nitrogen gas within the

More information

Invited Paper. recording. Yuri N. Denisyuk, Nina M. Ganzherli and Irma A. Maurer

Invited Paper. recording. Yuri N. Denisyuk, Nina M. Ganzherli and Irma A. Maurer Invited Paper Thick-layered light-sensitive dichromated gelatin for 3D hologram recording Yuri N. Denisyuk, Nina M. Ganzherli and Irma A. Maurer loffe Physico-Technical Institute of the Academy of Sciences

More information

AVIPHOT ASP 400 S PE1/PE0

AVIPHOT ASP 400 S PE1/PE0 AVIPHOT ASP 400 S PE1/PE0 Panchromatic negative B/W film for traffic infringement camera ASP 400 S is a panchromatic halftone aerial negative film with near IR sensitivity. The emulsion is coated onto

More information

ECEN 4606, UNDERGRADUATE OPTICS LAB

ECEN 4606, UNDERGRADUATE OPTICS LAB ECEN 4606, UNDERGRADUATE OPTICS LAB Lab 7: Holography Original version: Professor McLeod SUMMARY: In this lab you will record and develop your own holograms including a double-exposure hologram that will

More information

Photons interaction with matter

Photons interaction with matter ب س م هللا الر ح من الر حیم Photons interaction with matter Ionization Ionization is the process of removing an electron from an electrically neutral atom to produce an ion pair. An ion is an atom or subatomic

More information

LECTURE 1 The Radiographic Image

LECTURE 1 The Radiographic Image LECTURE 1 The Radiographic Image Prepared by:- KAMARUL AMIN ABDULLAH @ ABU BAKAR UiTM Faculty of Health Sciences Medical Imaging Department 11/23/2011 KAMARUL AMIN (C) 1 Lesson Objectives At the end of

More information

Supplementary Figure 1. GO thin film thickness characterization. The thickness of the prepared GO thin

Supplementary Figure 1. GO thin film thickness characterization. The thickness of the prepared GO thin Supplementary Figure 1. GO thin film thickness characterization. The thickness of the prepared GO thin film is characterized by using an optical profiler (Bruker ContourGT InMotion). Inset: 3D optical

More information

Resolution. Diffraction from apertures limits resolution. Rayleigh criterion θ Rayleigh = 1.22 λ/d 1 peak at 2 nd minimum. θ f D

Resolution. Diffraction from apertures limits resolution. Rayleigh criterion θ Rayleigh = 1.22 λ/d 1 peak at 2 nd minimum. θ f D Microscopy Outline 1. Resolution and Simple Optical Microscope 2. Contrast enhancement: Dark field, Fluorescence (Chelsea & Peter), Phase Contrast, DIC 3. Newer Methods: Scanning Tunneling microscopy (STM),

More information

Computer Generated Holograms for Optical Testing

Computer Generated Holograms for Optical Testing Computer Generated Holograms for Optical Testing Dr. Jim Burge Associate Professor Optical Sciences and Astronomy University of Arizona jburge@optics.arizona.edu 520-621-8182 Computer Generated Holograms

More information

Photonics and Optical Communication

Photonics and Optical Communication Photonics and Optical Communication (Course Number 300352) Spring 2007 Dr. Dietmar Knipp Assistant Professor of Electrical Engineering http://www.faculty.iu-bremen.de/dknipp/ 1 Photonics and Optical Communication

More information

Physics 1C Lecture 27B

Physics 1C Lecture 27B Physics 1C Lecture 27B Single Slit Interference! Example! Light of wavelength 750nm passes through a slit 1.00μm wide. How wide is the central maximum in centimeters, in a Fraunhofer diffraction pattern

More information

Lab in a Box Microwave Interferometer

Lab in a Box Microwave Interferometer In 1887 Michelson and Morley used an optical interferometer (a device invented by Michelson to accurately detect aether flow) to try and detect the relative motion of light through the luminous either.

More information

Using double-exposure holographic techniques to evaluate the deformation of an aluminum can under stress

Using double-exposure holographic techniques to evaluate the deformation of an aluminum can under stress Using double-exposure holographic techniques to evaluate the deformation of an aluminum can under stress Maggie Lankford Physics Department, The College of Wooster, Wooster, Ohio 44691, USA (Dated: December

More information

Atmospheric interactions; Aerial Photography; Imaging systems; Intro to Spectroscopy Week #3: September 12, 2018

Atmospheric interactions; Aerial Photography; Imaging systems; Intro to Spectroscopy Week #3: September 12, 2018 GEOL 1460/2461 Ramsey Introduction/Advanced Remote Sensing Fall, 2018 Atmospheric interactions; Aerial Photography; Imaging systems; Intro to Spectroscopy Week #3: September 12, 2018 I. Quick Review from

More information

Integrated Photonics based on Planar Holographic Bragg Reflectors

Integrated Photonics based on Planar Holographic Bragg Reflectors Integrated Photonics based on Planar Holographic Bragg Reflectors C. Greiner *, D. Iazikov and T. W. Mossberg LightSmyth Technologies, Inc., 86 W. Park St., Ste 25, Eugene, OR 9741 ABSTRACT Integrated

More information

Ti/Au TESs as photon number resolving detectors

Ti/Au TESs as photon number resolving detectors Ti/Au TESs as photon number resolving detectors LAPO LOLLI, E. MONTICONE, C. PORTESI, M. RAJTERI, E. TARALLI SIF XCVI National Congress, Bologna 20 24 September 2010 1 Introduction: What are TES? TESs

More information

The range of applications which can potentially take advantage of CGH is very wide. Some of the

The range of applications which can potentially take advantage of CGH is very wide. Some of the CGH fabrication techniques and facilities J.N. Cederquist, J.R. Fienup, and A.M. Tai Optical Science Laboratory, Advanced Concepts Division Environmental Research Institute of Michigan P.O. Box 8618, Ann

More information

CHAPTER 7. Components of Optical Instruments

CHAPTER 7. Components of Optical Instruments CHAPTER 7 Components of Optical Instruments From: Principles of Instrumental Analysis, 6 th Edition, Holler, Skoog and Crouch. CMY 383 Dr Tim Laurens NB Optical in this case refers not only to the visible

More information

Astronomical Detectors. Lecture 3 Astronomy & Astrophysics Fall 2011

Astronomical Detectors. Lecture 3 Astronomy & Astrophysics Fall 2011 Astronomical Detectors Lecture 3 Astronomy & Astrophysics Fall 2011 Detector Requirements Record incident photons that have been captured by the telescope. Intensity, Phase, Frequency, Polarization Difficulty

More information

Supplementary Figure 1 Reflective and refractive behaviors of light with normal

Supplementary Figure 1 Reflective and refractive behaviors of light with normal Supplementary Figures Supplementary Figure 1 Reflective and refractive behaviors of light with normal incidence in a three layer system. E 1 and E r are the complex amplitudes of the incident wave and

More information

Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane

Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane Swapnajit Chakravarty 1, Wei-Cheng Lai 2, Xiaolong (Alan) Wang 1, Che-Yun Lin 2, Ray T. Chen 1,2 1 Omega Optics, 10306 Sausalito Drive,

More information

32nm High-K/Metal Gate Version Including 2nd Generation Intel Core processor family

32nm High-K/Metal Gate Version Including 2nd Generation Intel Core processor family From Sand to Silicon Making of a Chip Illustrations 32nm High-K/Metal Gate Version Including 2nd Generation Intel Core processor family April 2011 1 The illustrations on the following foils are low resolution

More information

Micro-sensors - what happens when you make "classical" devices "small": MEMS devices and integrated bolometric IR detectors

Micro-sensors - what happens when you make classical devices small: MEMS devices and integrated bolometric IR detectors Micro-sensors - what happens when you make "classical" devices "small": MEMS devices and integrated bolometric IR detectors Dean P. Neikirk 1 MURI bio-ir sensors kick-off 6/16/98 Where are the targets

More information

Robert Magnusson, Ph.D.

Robert Magnusson, Ph.D. Robert Magnusson, Ph.D. Texas Instruments Distinguished University Chair in Nanoelectronics Director of the Nanophotonics Device Group Co-founder and Chief Technical Officer of Resonant Sensors Incorporated

More information

ILFORD FACT SHEET ILFORD NUCLEAR EMULSIONS. HARMAN technology Limited TECHNICAL INFORMATION FOR PARTICLE PHYSICS APPLICATIONS

ILFORD FACT SHEET ILFORD NUCLEAR EMULSIONS. HARMAN technology Limited TECHNICAL INFORMATION FOR PARTICLE PHYSICS APPLICATIONS ILFORD HARMAN technology Limited FACT SHEET ILFORD NUCLEAR EMULSIONS TECHNICAL INFORMATION FOR PARTICLE PHYSICS APPLICATIONS 1 INTRODUCTION Nuclear research emulsions were first developed in the 1940s

More information

arxiv: v2 [astro-ph.im] 22 Sep 2011

arxiv: v2 [astro-ph.im] 22 Sep 2011 Title : will be set by the publisher Editors : will be set by the publisher EAS Publications Series, Vol.?, 2018 arxiv:1109.4485v2 [astro-ph.im] 22 Sep 2011 R&D STATUS OF NUCLEAR EMULSION FOR DIRECTIONAL

More information

AST 443 / PHY 517. Photon Detectors

AST 443 / PHY 517. Photon Detectors AST 443 / PHY 517 Photon Detectors Photons Light is electro- magne>c radia>on Crossed electric and magne>c vectors Self- propaga>ng Travels at speed of light c c=2.99792 x 10 8 m/s (vacuum) λν = c n=c/v

More information

CCD Analogy BUCKETS (PIXELS) HORIZONTAL CONVEYOR BELT (SERIAL REGISTER) VERTICAL CONVEYOR BELTS (CCD COLUMNS) RAIN (PHOTONS)

CCD Analogy BUCKETS (PIXELS) HORIZONTAL CONVEYOR BELT (SERIAL REGISTER) VERTICAL CONVEYOR BELTS (CCD COLUMNS) RAIN (PHOTONS) CCD Analogy RAIN (PHOTONS) VERTICAL CONVEYOR BELTS (CCD COLUMNS) BUCKETS (PIXELS) HORIZONTAL CONVEYOR BELT (SERIAL REGISTER) MEASURING CYLINDER (OUTPUT AMPLIFIER) Exposure finished, buckets now contain

More information

GAFCHROMIC HD-810 Radiochromic Dosimetry Film Configuration, Specifications and Performance Data

GAFCHROMIC HD-810 Radiochromic Dosimetry Film Configuration, Specifications and Performance Data GAFCHROMIC HD-810 Radiochromic Dosimetry Film Configuration, Specifications and Performance Data Description GAFCHROMIC HD-810 dosimetry film is designed for the measurement of absorbed dose of high-energy

More information

PHOTOPOLYMER FOR RECORDING HOLOGRAMS. Hideo Tanigawa, Taichi Ichihashi, and Takashi Matsuo*

PHOTOPOLYMER FOR RECORDING HOLOGRAMS. Hideo Tanigawa, Taichi Ichihashi, and Takashi Matsuo* PHOTOPOLYMER FOR RECORDING HOLOGRAMS Hideo Tanigawa, Taichi Ichihashi, and Takashi Matsuo* MY0001406 Osaka National Research Institute, AIST 1-8-31, Midorigaoka, Ikeda, Osaka 563-8577, Japan Phone: +81-727-51-9537,

More information

plasmonic nanoblock pair

plasmonic nanoblock pair Nanostructured potential of optical trapping using a plasmonic nanoblock pair Yoshito Tanaka, Shogo Kaneda and Keiji Sasaki* Research Institute for Electronic Science, Hokkaido University, Sapporo 1-2,

More information

The 34th International Physics Olympiad

The 34th International Physics Olympiad The 34th International Physics Olympiad Taipei, Taiwan Experimental Competition Wednesday, August 6, 2003 Time Available : 5 hours Please Read This First: 1. Use only the pen provided. 2. Use only the

More information

Chapter 1. Basic Electron Optics (Lecture 2)

Chapter 1. Basic Electron Optics (Lecture 2) Chapter 1. Basic Electron Optics (Lecture 2) Basic concepts of microscope (Cont ) Fundamental properties of electrons Electron Scattering Instrumentation Basic conceptions of microscope (Cont ) Ray diagram

More information

Chapter 17: Wave Optics. What is Light? The Models of Light 1/11/13

Chapter 17: Wave Optics. What is Light? The Models of Light 1/11/13 Chapter 17: Wave Optics Key Terms Wave model Ray model Diffraction Refraction Fringe spacing Diffraction grating Thin-film interference What is Light? Light is the chameleon of the physical world. Under

More information

light sensing & sensors Mo: Tu:04 light sensing & sensors 167+1

light sensing & sensors Mo: Tu:04 light sensing & sensors 167+1 light sensing & sensors 16722 mws@cmu.edu Mo:20090302+Tu:04 light sensing & sensors 167+1 reading Fraden Section 3.13, Light, and Chapter 14, Light Detectors 16722 mws@cmu.edu Mo:20090302+Tu:04 light sensing

More information

CHIRPED FIBER BRAGG GRATING (CFBG) BY ETCHING TECHNIQUE FOR SIMULTANEOUS TEMPERATURE AND REFRACTIVE INDEX SENSING

CHIRPED FIBER BRAGG GRATING (CFBG) BY ETCHING TECHNIQUE FOR SIMULTANEOUS TEMPERATURE AND REFRACTIVE INDEX SENSING CHIRPED FIBER BRAGG GRATING (CFBG) BY ETCHING TECHNIQUE FOR SIMULTANEOUS TEMPERATURE AND REFRACTIVE INDEX SENSING Siti Aisyah bt. Ibrahim and Chong Wu Yi Photonics Research Center Department of Physics,

More information

Synthesis of projection lithography for low k1 via interferometry

Synthesis of projection lithography for low k1 via interferometry Synthesis of projection lithography for low k1 via interferometry Frank Cropanese *, Anatoly Bourov, Yongfa Fan, Andrew Estroff, Lena Zavyalova, Bruce W. Smith Center for Nanolithography Research, Rochester

More information

Introduction Visible light is an electromagnetic wave, characterized by a wavelength, an amplitude

Introduction Visible light is an electromagnetic wave, characterized by a wavelength, an amplitude Thin Film Interferences of SiO2 and TiO2 : Thickness and Iridescence Eman Mousa Alhajji North Carolina State University Department of Materials Science and Engineering MSE 355 Lab Report 201 A Matthew

More information

The Silver Gelatin Photographic Print

The Silver Gelatin Photographic Print The Silver Gelatin Photographic Print How to create a properly exposed, in focus, properly developed and fixed photographic print from a black and white negative By Marcine Linder Darkroom Triangle of

More information

Unit thickness. Unit area. σ = NΔX = ΔI / I 0

Unit thickness. Unit area. σ = NΔX = ΔI / I 0 Unit thickness I 0 ΔI I σ = ΔI I 0 NΔX = ΔI / I 0 NΔX Unit area Δx Average probability of reaction with atom for the incident photons at unit area with the thickness of Delta-X Atom number at unit area

More information

Physical Optics. Diffraction.

Physical Optics. Diffraction. Physical Optics. Diffraction. Interference Young s interference experiment Thin films Coherence and incoherence Michelson interferometer Wave-like characteristics of light Huygens-Fresnel principle Interference.

More information

Properties of a Detector

Properties of a Detector Properties of a Detector Quantum Efficiency fraction of photons detected wavelength and spatially dependent Dynamic Range difference between lowest and highest measurable flux Linearity detection rate

More information

Organic Antireflective Coatings for Photomask Fabrication using Optical Pattern Generators

Organic Antireflective Coatings for Photomask Fabrication using Optical Pattern Generators Organic Antireflective Coatings for Photomask Fabrication using Optical Pattern Generators Benjamen M. Rathsack 1, Cyrus E. Tabery 1, Cece Philbin 2, and C. Grant Willson 1 September 15, 1999 1 Department

More information

HUYGENS PRINCIPLE AND INTERFERENCE

HUYGENS PRINCIPLE AND INTERFERENCE HUYGENS PRINCIPLE AND INTERFERENCE VERY SHORT ANSWER QUESTIONS Q-1. Can we perform Double slit experiment with ultraviolet light? Q-2. If no particular colour of light or wavelength is specified, then

More information

Physics Laboratory Scattering of Photons from Electrons: Compton Scattering

Physics Laboratory Scattering of Photons from Electrons: Compton Scattering RR Oct 2001 SS Dec 2001 MJ Oct 2009 Physics 34000 Laboratory Scattering of Photons from Electrons: Compton Scattering Objective: To measure the energy of high energy photons scattered from electrons in

More information

Holographic Bragg Reflectors: Designs and Applications

Holographic Bragg Reflectors: Designs and Applications OTuP1.pdf 2009 OSA/OFC/NFOEC 2009 Holographic Bragg Reflectors: Designs and Applications T. W. Mossberg, C. Greiner, D. Iazikov LightSmyth Technologies OFC 2009 Review - Volume Holograms (mode-selective

More information

MICRO AND NANOPROCESSING TECHNOLOGIES

MICRO AND NANOPROCESSING TECHNOLOGIES MICRO AND NANOPROCESSING TECHNOLOGIES LECTURE 4 Optical lithography Concepts and processes Lithography systems Fundamental limitations and other issues Photoresists Photolithography process Process parameter

More information

PAPER No. 7: Criminalistics & Forensic Physics MODULE No. 31: Black & White & Colour Film Processing and Printing. and Printing

PAPER No. 7: Criminalistics & Forensic Physics MODULE No. 31: Black & White & Colour Film Processing and Printing. and Printing SUBJECT Paper No. and Title Module No. and Title Module Tag FSC_P7_M31 TABLE OF CONTENTS 1. Learning Outcomes 2. Introduction 3. Formation of Black and White Films 4. Black and White structure and forms

More information

Chapter 4 Imaging Lecture 17

Chapter 4 Imaging Lecture 17 Chapter 4 Imaging Lecture 17 d (110) Imaging Imaging in the TEM Diffraction Contrast in TEM Image HRTEM (High Resolution Transmission Electron Microscopy) Imaging STEM imaging Imaging in the TEM What is

More information

SPRAY DROPLET SIZE MEASUREMENT

SPRAY DROPLET SIZE MEASUREMENT SPRAY DROPLET SIZE MEASUREMENT In this study, the PDA was used to characterize diesel and different blends of palm biofuel spray. The PDA is state of the art apparatus that needs no calibration. It is

More information

Name Class Date. Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used.

Name Class Date. Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used. Assessment Chapter Test B Light and Our World USING KEY TERMS Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used. concave

More information

Chapter 23 Study Questions Name: Class:

Chapter 23 Study Questions Name: Class: Chapter 23 Study Questions Name: Class: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. When you look at yourself in a plane mirror, you

More information

Surface Topography and Alignment Effects in UV-Modified Polyimide Films with Micron Size Patterns

Surface Topography and Alignment Effects in UV-Modified Polyimide Films with Micron Size Patterns CHINESE JOURNAL OF PHYSICS VOL. 41, NO. 2 APRIL 2003 Surface Topography and Alignment Effects in UV-Modified Polyimide Films with Micron Size Patterns Ru-Pin Pan 1, Hua-Yu Chiu 1,Yea-FengLin 1,andJ.Y.Huang

More information

Tunable Color Filters Based on Metal-Insulator-Metal Resonators

Tunable Color Filters Based on Metal-Insulator-Metal Resonators Chapter 6 Tunable Color Filters Based on Metal-Insulator-Metal Resonators 6.1 Introduction In this chapter, we discuss the culmination of Chapters 3, 4, and 5. We report a method for filtering white light

More information

Testing Aspherics Using Two-Wavelength Holography

Testing Aspherics Using Two-Wavelength Holography Reprinted from APPLIED OPTICS. Vol. 10, page 2113, September 1971 Copyright 1971 by the Optical Society of America and reprinted by permission of the copyright owner Testing Aspherics Using Two-Wavelength

More information

Confocal Imaging Through Scattering Media with a Volume Holographic Filter

Confocal Imaging Through Scattering Media with a Volume Holographic Filter Confocal Imaging Through Scattering Media with a Volume Holographic Filter Michal Balberg +, George Barbastathis*, Sergio Fantini % and David J. Brady University of Illinois at Urbana-Champaign, Urbana,

More information

attosnom I: Topography and Force Images NANOSCOPY APPLICATION NOTE M06 RELATED PRODUCTS G

attosnom I: Topography and Force Images NANOSCOPY APPLICATION NOTE M06 RELATED PRODUCTS G APPLICATION NOTE M06 attosnom I: Topography and Force Images Scanning near-field optical microscopy is the outstanding technique to simultaneously measure the topography and the optical contrast of a sample.

More information

Spectroscopy of Ruby Fluorescence Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018

Spectroscopy of Ruby Fluorescence Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 1 Spectroscopy of Ruby Fluorescence Physics 3600 - Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 I. INTRODUCTION The laser was invented in May 1960 by Theodor Maiman.

More information

Project Staff: Timothy A. Savas, Michael E. Walsh, Thomas B. O'Reilly, Dr. Mark L. Schattenburg, and Professor Henry I. Smith

Project Staff: Timothy A. Savas, Michael E. Walsh, Thomas B. O'Reilly, Dr. Mark L. Schattenburg, and Professor Henry I. Smith 9. Interference Lithography Sponsors: National Science Foundation, DMR-0210321; Dupont Agreement 12/10/99 Project Staff: Timothy A. Savas, Michael E. Walsh, Thomas B. O'Reilly, Dr. Mark L. Schattenburg,

More information

BLACKBODY RADIATION PHYSICS 359E

BLACKBODY RADIATION PHYSICS 359E BLACKBODY RADIATION PHYSICS 359E INTRODUCTION In this laboratory, you will make measurements intended to illustrate the Stefan-Boltzmann Law for the total radiated power per unit area I tot (in W m 2 )

More information