WHITE PAPER. How to Include Detector Resolution in MTF Calculations. Zemax A Radiant Zemax Company

Similar documents
WHITE PAPER. Methods for Measuring Display Defects and Mura as Correlated to Human Visual Perception

WHITE PAPER. Guide to CCD-Based Imaging Colorimeters

Criteria for Optical Systems: Optical Path Difference How do we determine the quality of a lens system? Several criteria used in optical design

WHITE PAPER. Methods for Measuring Flat Panel Display Defects and Mura as Correlated to Human Visual Perception

Automated Solutions for SAE Standard HUD Measurement

Understanding Imaging System Specifications for Pixel-Level Measurement of Displays

Modulation Transfer Function

OCT Spectrometer Design Understanding roll-off to achieve the clearest images

Using Optics to Optimize Your Machine Vision Application

On spatial resolution

Fourier transforms, SIM

Tech Paper. Anti-Sparkle Film Distinctness of Image Characterization

Determining MTF with a Slant Edge Target ABSTRACT AND INTRODUCTION

Basic Resolution Testing using Test Charts

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS. GUI Simulation Diffraction: Focused Beams and Resolution for a lens system

Optical Design of an Off-axis Five-mirror-anastigmatic Telescope for Near Infrared Remote Sensing

Optics of Wavefront. Austin Roorda, Ph.D. University of Houston College of Optometry

High Contrast Imaging

WHITE PAPER. Five Signs that a Photometry-Based Imaging System is the Right Choice for Your Inspection Application

Image formation in the scanning optical microscope

GenePix Application Note

Chapter 36: diffraction

BIG PIXELS VS. SMALL PIXELS THE OPTICAL BOTTLENECK. Gregory Hollows Edmund Optics

6/3/15. The Anatomy of a Digital Image. Representative Intensities. Specimen: (molecular distribution)

Introduction. Chapter 16 Diagnostic Radiology. Primary radiological image. Primary radiological image

ISO INTERNATIONAL STANDARD. Photography Electronic still-picture cameras Resolution measurements

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Mechanical Engineering Department. 2.71/2.710 Final Exam. May 21, Duration: 3 hours (9 am-12 noon)

Modulation Transfer Function

Digital Detector Array Image Quality for Various GOS Scintillators

Binocular and Scope Performance 57. Diffraction Effects

2013 LMIC Imaging Workshop. Sidney L. Shaw Technical Director. - Light and the Image - Detectors - Signal and Noise

Today. next week. MIT 2.71/ /04/09 wk13-a- 1

Optical Performance of Nikon F-Mount Lenses. Landon Carter May 11, Measurement and Instrumentation

OPTICAL IMAGE FORMATION

MTF characteristics of a Scophony scene projector. Eric Schildwachter

Experiment 1: Fraunhofer Diffraction of Light by a Single Slit

Study on Imaging Quality of Water Ball Lens

FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION

DESIGN NOTE: DIFFRACTION EFFECTS

Opti 415/515. Introduction to Optical Systems. Copyright 2009, William P. Kuhn

VeraPath Optical Encoder Technology

Practice Problems for Chapter 25-26

Simulated validation and quantitative analysis of the blur of an integral image related to the pickup sampling effects

Performance of Image Intensifiers in Radiographic Systems

DECISION NUMBER FOURTEEN TO THE TREATY ON OPEN SKIES

Evaluating Commercial Scanners for Astronomical Images. The underlying technology of the scanners: Pixel sizes:

KODAK VISION Expression 500T Color Negative Film / 5284, 7284

Dario Cabib, Amir Gil, Moshe Lavi. Edinburgh April 11, 2011

Chapter 15 IC Photolithography

A Pin-Hole Projection System: Status

EASTMAN EXR 200T Film / 5293, 7293

Testing Aspherics Using Two-Wavelength Holography

Fast MTF measurement of CMOS imagers using ISO slantededge methodology

Ayaz Jhanorwala, Rishikesh Kumar, Satish Tilva. L & T MHPS Boilers Pvt Ltd., Hazira, Surat , India

The Beam Characteristics of High Power Diode Laser Stack

Low Contrast Dielectric Metasurface Optics. Arka Majumdar 1,2,+ 8 pages, 4 figures S1-S4

06SurfaceQuality.nb Optics James C. Wyant (2012) 1

MTF and PSF measurements of the CCD detector for the Euclid visible channel

MEASURING HEAD-UP DISPLAYS FROM 2D TO AR: SYSTEM BENEFITS & DEMONSTRATION Presented By Matt Scholz November 28, 2018

IMAGING TECHNIQUES FOR MEASURING PARTICLE SIZE SSA AND GSV

Charged Coupled Device (CCD) S.Vidhya

Improved Fusing Infrared and Electro-Optic Signals for. High Resolution Night Images

TSBB09 Image Sensors 2018-HT2. Image Formation Part 1

CODE V Tolerancing: A Key to Product Cost Reduction

KODAK PRIMETIME 640T Teleproduction Film / 5620,7620

High-resolution ADC operation up to 19.6 GHz clock frequency

Optical Design of. Microscopes. George H. Seward. Tutorial Texts in Optical Engineering Volume TT88. SPIE PRESS Bellingham, Washington USA

CXCI. Optical design of a compact telescope for the next generation Earth Observation system CXCI. Vincent COSTES. Octobre 2012

arxiv:physics/ v1 [physics.optics] 12 May 2006

Sharpness, Resolution and Interpolation

OPTI 517 Image Quality. Richard Juergens

Spatial Resolution as an Iris Quality Metric

Lecture 8. Lecture 8. r 1

Sampling Efficiency in Digital Camera Performance Standards

Scanning and Recording of Motion Picture Film: CRT Film Recording

More on the Mask Error Enhancement Factor

Commercial Scanners and Science

Material analysis by infrared mapping: A case study using a multilayer

Optical Coherence: Recreation of the Experiment of Thompson and Wolf

Overview: Integration of Optical Systems Survey on current optical system design Case demo of optical system design

A Study of Slanted-Edge MTF Stability and Repeatability

The predicted performance of the ACS coronagraph

Optical Design & Analysis Paul Martini

Diffraction Single-slit Double-slit Diffraction grating Limit on resolution X-ray diffraction. Phys 2435: Chap. 36, Pg 1

Paper or poster submitted for Europto-SPIE / AFPAEC May Zurich, CH. Version 9-Apr-98 Printed on 05/15/98 3:49 PM

Adaptive Optics for LIGO

Improvements for determining the modulation transfer function of charge-coupled devices by the speckle method

FLIR K2. FLIR-DIRECT.ca

Amorphous Selenium Direct Radiography for Industrial Imaging

Stop Guessing, Start Seeing

Resolution. [from the New Merriam-Webster Dictionary, 1989 ed.]:

Intrinsic Camera Resolution Measurement Peter D. Burns a and Judit Martinez Bauza b a Burns Digital Imaging LLC, b Qualcomm Technologies Inc.

Post PDR Optical Design Study. Robert Barkhouser JHU/IDG January 6, 2014

White Paper. Machine Vision & Raman Spectroscopy - Application Example. by Kenneth W. Chapman, Senior Vision Engineer, Centice Corporation

Sensitive measurement of partial coherence using a pinhole array

Copyright is owned by the Author of the thesis. Permission is given for a copy to be downloaded by an individual for the purpose of research and

Thermography. White Paper: Understanding Infrared Camera Thermal Image Quality

IMAGE SENSOR SOLUTIONS. KAC-96-1/5" Lens Kit. KODAK KAC-96-1/5" Lens Kit. for use with the KODAK CMOS Image Sensors. November 2004 Revision 2

ADAPTIVE CORRECTION FOR ACOUSTIC IMAGING IN DIFFICULT MATERIALS

The Formation of an Aerial Image, part 3

Transcription:

How to Include Detector Resolution in MTF Calculations

How to Include Detector Resolution in MTF Calculations Introduction Modulation Transfer Function (MTF) is an important method of describing the performance of an optical system. A consequence of applying Fourier theory to image forming optical systems, MTF describes the contrast in the image of a spatial frequency presented in the scene being viewed. See this article for more information on what MTF is. MTF describes the imaging of the system, but an important system parameter is usually neglected: the resolution of the detector. If the detector s pixels are significantly bigger than the resolvable spot size, the optical system is said to be detector limited, and the overall system MTF is reduced compared to the MTF the optical system itself is capable of achieving. MTF is commonly used to describe the performance of an imaging system, but the fi nite resolution of the detection system is often ignored. This white paper describes how to account for detector pixel sizes and position shifts to give a full-system MTF measurement. Experimentally, MTF can be measured by imaging a small bar (or single-frequency sine) chart through the lens and onto the detector. The bar chart must be small because the optical transfer function of the lens should not vary significantly over the target pattern. Within we can use the same method: the partially coherent image analysis feature is used to image a small bar chart through the system onto a pixellated detector, and the MTF is computed directly from this. An Example The example file used here can be downloaded via this link. It is a derivative of the Cooke triplet sample file: 2 I, LLC

We image a bar chart through the system: The full width of the image is 0.5 mm, and the optical performance of the lens does not vary significantly over this field of view: 3 I, LLC

We will now look at the cross-section of the Partially Coherent Image Analysis, configured like so: so we use 500 1µ-wide pixels to view our image. The resulting image is like so: 4 I, LLC

The cross section of the false color map is shown above. Note we have ten cycles of the bar pattern over about a 200µ region: this corresponds to 50 cycles/mm. The MTF can then be estimated by determining the maximum and minimum relative intensity across the cross section. To reduce the effects of edges, the analysis parameters should be set to provide at least 5 well defined peaks across the cross section. The MTF is computed by looking for the minimum and maximum intensity at all points between the second and second-to-last local peaks in the intensity data. By considering only data within these two peaks, the effects of the edges is somewhat reduced. The estimated MTF is then given by the usual computation of (Imax-Imin)/(Imax+Imin). Finally, note that if a bar target is used, the resulting MTF is the square-wave, not sinewave modulation: Note there is excellent agreement between the two analysis features, with an estimated MTF of 0.68 from both the Partially Coherent Image Analysis and the FFT MTF plot at 50 cycles/mm (note that we are only approximately at 50 cycles/mm in the Partially Coherent Image Analysis). This is to be expected, as the 1µ detector pixel size is smaller than the 5µ RMS spot size and 3.5µ Airy disk radius. This combination of optical system and detector is optics limited, not detector limited. 5 I, LLC

Instead, repeat the Partially Coherent Image Analysis, but use an array of 100 x 100 pixels each of 5µ width. Now the MTF is 0.43: The MTF is clearly degraded by the coarser detector resolution. Equally important, consider what happens if the detector is shifted in the image plane. Because the pixel size is close to the resolution limit, the measured MTF will be sensitive to shifts of the detector array on the order of one pixel. If we decenter the detector by a half-pixel in x... 6 I, LLC

...the MTF improves to 0.59 because there is less cross-talk between light and dark regions of the image as they are integrated by the detector array: Summary If an optical system s minimum resolvable spot is comparable to or less than the detector size, it is important to consider the effects of integrating the spatial signal on the detector array when computing MTF. The Partially Coherent Image Analysis feature provides this capability. 7 I, LLC

MTF is commonly used to describe the performance of an imaging system, but the finite resolution of the detection system is often ignored. This white paper describes how to account for detector pixel sizes and position shifts to give a full-system MTF measurement. Contact Us Today Americas and Worldwide, LLC 22908 NE Alder Crest Drive, Suite 100 Redmond, WA 98053 T. +1 425 298-2145 Europe Europe, Ltd. 8 Riverside Business Park, Stoney Common Road Stansted, CM24 8PL, UK T. +44 1279 810911 Greater China China, Ltd. B301 SOHO ZhongShan Plaza No.1065 West ZhongShan Road ChangNing District Shanghai 200051 T. +86 21 5242-2288.com sales@zemax.com 2013 Radiant LLC. Radiant, ProMetric, TrueTest and are trademarks of Radiant LLC. All other marks are the property of their respective owners. 770-9004-01 1/13