A LEADER IN OPTICAL TECHNOLOGY. GRADIUM Lenses.

Size: px
Start display at page:

Download "A LEADER IN OPTICAL TECHNOLOGY. GRADIUM Lenses."

Transcription

1 A LEADER IN OPTICAL TECHNOLOGY GRADIUM Lenses

2 ABOUT LIGHTPATH TECHNOLOGIES LightPath Technologies makes quality and customer satisfaction a top priority. We value your business, and it is our goal to provide competitively priced, top quality products that satisfy your technical and time-to-market requirements. The quality management system at LightPath Technologies has been registered with TUV America and SGS China as ISO 9001:2008 compliant since August of 2001 and August of 2006 respectively. A range of environmental chambers are available in-house for reliability testing for Telcordia and other MIL The Corporate Headquarters in Orlando has 30,000 square feet of space including 8,000 square feet of class 10,000 Orlando facility also maintains a class 100 clean room for high performance projects, a precision machine shop with single point diamond turning capabilities for quick turn prototypes and complete metrology labs. programs hosting both Sales and Engineering teams. Our new manufacturing facility in Zhenjiang, China is approximately 26,000 square feet and is also wholly owned. It includes an impressive 11,000 square feet of clean room. OUR VISION Grow LightPath Technologies es into an optical solution company that is a fully integrated manufacturer and supplier of visible and infrared red optical components and sub-systems, based on world class optical manufacturing technology

3 TABLE OF CONTENTS About LightPath 02 Table of Contents 03 GRADIUM Lens Overview 04 GRADIUM Lens Specifications 05 GRADIUM Lens Specifications 06 GRADIUM Coatings 07 3

4 GRADIUM LENSES OVERVIEW ASPHERIC PERFORMANCE FOR HIGH POWER LASER DELIVERY Gradient index lenses for high power laser delivery Aspheric performance Smaller focused spot size Delivers single lens replacement for conventional doublets Provides high performance at a cost effective price Standard designs with diameters from 5 mm to 80 mm Ideal for high power applications, GRADIUM lenses and their gradient-index structure often allow a GRADIUM singlet to replace a conventional spherical doublet. GRADIUM lenses can be custom designed for visible or near infrared applications in diameters from 5 mm to over 100 mm. GRADIUM doublets are also available for better achromatic performance and can equal the performance of conventional triplets. GRADIUM lenses can be exploited to reduce spherical aberrations resulting in performance similar to single-term manufacturers incorporate GRADIUM optics in their laser delivery systems. GRADIUM lenses have been applied as simple singlets or doublets in complex multi-element systems. collimated, polychromatic light in the visible spectrum. The GRADIUM glass element is used to reduce the spherical aberration which is a common side effect of a cemented doublet design. The dispersion, as well as the optical index, varies in a controlled contiguous combination of many glass types. This continuous variation results in a transfer aberration correction not possible with homogeneous lenses. GRADIUM lenses should be used wherever small spot size, high numerical aperture (NA), increased beam energy, or excellent wavefront quality is important. A GRADIUM singlet does not have the limited laser damage threshold of a conventional cemented doublet, so laser power can be increased, leading to increased production throughout

5 GRADIUM LENS SPECIFICATIONS Plano-Convex (GPX) BFL EFL Bi-Convex (GBX) BFL EFL Meniscus (GMN) EFL BFL CA OD CA OD CA OD CT CT CT Lens Code Outer Diameter Clear Aperture F/# Effective Focal Center Thickness Back Focal GPX mm 4.00 mm mm 2.90 mm 3.09 mm GPX mm 4.50 mm mm 3.00 mm 8.23 mm GPX mm 4.00 mm mm 2.00 mm mm GPX mm 5.67 mm mm 2.60 mm 4.65 mm GPX mm 5.72 mm mm 2.00 mm mm GPX mm 9.00 mm mm 3.00 mm 8.00 mm GPX mm 9.00 mm mm 3.00 mm mm GPX mm 9.00 mm mm 2.50 mm mm GPX mm 9.00 mm mm 2.50 mm mm GPX mm 9.00 mm mm 2.50 mm mm GPX mm 9.00 mm mm 2.50 mm mm GPX mm 9.00 mm mm 2.00 mm mm GPX mm mm mm 4.20 mm mm Plano-Convex GPX mm mm mm 3.00 mm mm GPX mm mm mm 2.00 mm mm GPX mm mm mm 3.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 4.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 4.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm 5

6 GRADIUM LENS SPECIFICATIONS Plano-Convex Lens Code Outer Diameter Clear Aperture F/# Effective Focal Center Thickness Back Focal GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 6.00 mm mm GPX mm mm mm 8.00 mm mm GPX mm mm mm 8.00 mm mm GPX mm mm mm 8.00 mm mm GPX mm mm mm 8.00 mm mm GPX mm mm mm 8.00 mm mm GPX mm mm mm mm mm Bi-Convex Lens Code Outer Diameter Clear Aperture F/# Effective Focal Center Thickness Back Focal GBX mm mm mm 4.60 mm mm GBX mm mm mm 4.60 mm mm GBX mm mm mm 5.76 mm mm GBX mm mm mm 8.00 mm mm GBX mm mm mm mm mm ME GMN mm mm mm 5.00 mm mm STANDARD SPHERICAL LENS Standard spherical lenses suffer from spherical aberration, which artificially limits the focused spot size. GRADIUM LENS unique refractive index profile bends rays while traveling through the lens resulting in a better focused, smaller spot. General GRADIUM Design Wavelength Operating Temperature Storage Temperature Outer Diameter (OD) Tolerance Center Thickness (CT) Tolerance 546 nm -20ºC to +200ºC -40ºC to +300ºC ± mm ± mm Effective Focal (EFL) for GPX, GBX, and GMN Series ± 1% Working Distance (WD) for GPX, GBX, and GMN Series ± 1% Surface Quality 40/20 Scratch/Dig

7 GRADIUM COATINGS Standard Coating Curves BB1 BB2 DB3 DB5 VC8 Broad Band Dual Band VC Available Coatings* Wavelength Surface % -BB nm < 0.5 Average -BB nm < 0.5 Average -BB nm < 0.5 Average -DB1 633/1064 nm < 0.25 Maximum -DB2 532/1064 nm < 0.25 Maximum -DB4 530/670 nm < 0.25 Maximum -DB5 808/940 nm < 0.25 Maximum -DB6 1064/1550 nm < 0.25 Maximum -VC1 488 nm < 0.25 Maximum -VC2 532 nm < 0.25 Maximum -VC3 633 nm < 0.25 Maximum -VC4 670 nm < 0.25 Maximum -VC5 780 nm < 0.25 Maximum -VC6 830 nm < 0.25 Maximum -VC7 980 nm < 0.25 Maximum -VC nm < 0.25 Maximum -VC nm < 0.25 Maximum -VC nm < 0.25 Maximum Broad Band Dual Band VC Coating Code Wavelength Surface % -BB nm < 0.5 Average -DB3 1310/1550 nm < 0.25 Maximum -VC nm < 0.25 Maximum DID YOU KNOW? catalog, our engineering team will application. 7

8 DESIGNED PRODUCED DELIVERED Contact LightPath today for your custom quote or Challenger Tech Court Suite 100 Orlando, Florida 32826, USA Phone: Room 1608, No Yecheng RD Jiading Industry Park Shanghai China Phone: Fax: 埼玉県さいたま市南区南浦和 TEL: FAX: th Building, No. 99 Jing 15 RD Dingmao, Zhenjiang New District Jiangsu, China LPTHCORP-1510_B

Geltech Molded Aspheric Lenses

Geltech Molded Aspheric Lenses A LEADER IN OPTICAL TECHNOLOGY Geltech Molded Aspheric Lenses ABOUT LIGHTPATH TECHNOLOGIES LightPath Technologies makes quality and customer satisfaction a top priority. We value your business, and it

More information

ASPHERIC LENSES FOR OPTICS AND PHOTONICS

ASPHERIC LENSES FOR OPTICS AND PHOTONICS ASPHERIC LENSES FOR OPTICS AND PHOTONICS Products for Laser Guides, Measurement Systems, Metrology & Bio Medical Geltech Molded Glass Aspheres Infrared Optics Fiber Collimators GRADIUM Lenses OPTICAL TECHNOLOGIES

More information

LightPath. Infrared Optics. Leaders in aspheric optics and assemblies TECHNOLOGIES

LightPath. Infrared Optics. Leaders in aspheric optics and assemblies TECHNOLOGIES LightPath TECHNOLOGIES Infrared Optics Leaders in aspheric optics and assemblies Infrared Optics from the Experts in Molded Glass Optics Leaders in chalcogenide glass Molding Enhanced thermal performance

More information

Geltech Aspheric Lenses

Geltech Aspheric Lenses High quality optical glass lenses Custom designs available Numerical aperture up to 0.83 Diameters from 0.250 mm to 25.0 mm Diffraction-limited performance Available in standard and custom housings For

More information

The Optical Solutions Company

The Optical Solutions Company The Optical Solutions Company Company Overview Background & Core Competencies Company History 1985 - Integrated Solar Technologies Corp., formed in Taos to improve solar energy technology led to first

More information

CORPORATE PRESENTATION

CORPORATE PRESENTATION CORPORATE PRESENTATION WHO WE ARE Edmund Optics is a global OPTICS and IMAGING company that manufactures and supplies the worldwide technical community with precision optical components and subassemblies.

More information

Black Diamond Infrared Lenses 38

Black Diamond Infrared Lenses 38 Product Catalog LightPath Technologies Page Company Overview 2 Markets Served 3 LightPath s Capabilities 4 Custom Engineering 5 LightPath s Technology Portfolio 6 Geltech Aspheric Lenses 6 Molded Glass

More information

WELCOME TO EO ISRAEL EVENT

WELCOME TO EO ISRAEL EVENT WELCOME TO EO ISRAEL EVENT WHO WE ARE 2 Edmund Optics is a global OPTICS and IMAGING company that manufactures and supplies the worldwide technical community with precision optical components and subassemblies.

More information

The RSH Catalogue. CO2 Laser Optics/Consumables - Lenses

The RSH Catalogue. CO2 Laser Optics/Consumables - Lenses The RSH Catalogue CO2 Laser Optics/Consumables - Lenses 2014 2015 1 Company Profile RSH Optronics, Headquartered in Ajmer, Rajasthan, India, is the leading supplier & manufacturer for Photonics Products

More information

Optical Precision. Optimal Outcome.

Optical Precision. Optimal Outcome. Optical Precision. Optimal Outcome. 3402 Enterprise Drive Rowlett, TX 75088 USA Telephone: +1 (972) 463-8001 Fax: +1 (972) 463-8311 www.archeroptx.com PerfectLens Ultra Precision Glass Molded Aspheres

More information

Lenses Design Basics. Introduction. RONAR-SMITH Laser Optics. Optics for Medical. System. Laser. Semiconductor Spectroscopy.

Lenses Design Basics. Introduction. RONAR-SMITH Laser Optics. Optics for Medical. System. Laser. Semiconductor Spectroscopy. Introduction Optics Application Lenses Design Basics a) Convex lenses Convex lenses are optical imaging components with positive focus length. After going through the convex lens, parallel beam of light

More information

StockOptics. CATALOG 2018 Europe

StockOptics. CATALOG 2018 Europe StockOptics CATALOG 2018 Europe Dear asphericon customer Within the StockOptics product line, you can choose from an extensive portfolio of precision-polished aspheric lenses, cylinders and axicons. Benefit

More information

Aspheric Lenses. Contact us for a Stock or Custom Quote Today! Edmund Optics BROCHURE

Aspheric Lenses. Contact us for a Stock or Custom Quote Today!   Edmund Optics BROCHURE Edmund Optics BROCHURE Aspheric Lenses products & capabilities Contact us for a Stock or Custom Quote Today! USA: +1-856-547-3488 EUROPE: +44 (0) 1904 788600 ASIA: +65 6273 6644 JAPAN: +81-3-3944-6210

More information

LightPath. Geltech Molded Aspheric Lenses. Leaders in aspheric optics and assemblies TECHNOLOGIES

LightPath. Geltech Molded Aspheric Lenses. Leaders in aspheric optics and assemblies TECHNOLOGIES LightPath TECHNOLOGIES Geltech Molded Aspheric Lenses Leaders in aspheric optics and assemblies Geltech Precision Molded Aspheric Lenses Modern lenses for modern applications For today s most sophisticated

More information

StockOptics. CATALOG 2017 Europe

StockOptics. CATALOG 2017 Europe StockOptics CATALOG 2017 Europe a HighNA Page 05 Dear asphericon customer StockOptics Product Range a LowNA Page 07 Within the StockOptics product line, you can choose from an extensive portfolio of precisionpolished

More information

MULTI-ELEMENT LENSES. Don t see exactly what you are looking for? CVI Laser Optics specializes in prototype to volume production manufacturing!

MULTI-ELEMENT LENSES. Don t see exactly what you are looking for? CVI Laser Optics specializes in prototype to volume production manufacturing! MULTI-ELEMENT LENSES Mirrors Multi-element lenses are an ideal solution for applications requiring specialized performance and/or a high degree of aberration correction. Our line of multi-element lenses

More information

The LINOS Singlets. Our quality criteria:

The LINOS Singlets. Our quality criteria: The LINOS From convergent lenses and diffuse lenses to best form lenses and aspheres, our extensive selection of simple lenses, or singlets, with various focal lengths and diameters guarantees that you

More information

Telecentric Imaging Object space telecentricity stop source: edmund optics The 5 classical Seidel Aberrations First order aberrations Spherical Aberration (~r 4 ) Origin: different focal lengths for different

More information

COLLIMATORS AND FOCUSERS RECEPTACLE STYLE

COLLIMATORS AND FOCUSERS RECEPTACLE STYLE COLLIMATORS AND FOCUSERS RECEPTACLE STYLE FEATURES: High power handling Rugged and compact design Low insertion loss Wide wavelength range 200-2100 nm Wide range of beam diameters GRIN, aspheric, achromatic,

More information

Using molded chalcogenide glass technology to reduce cost in a compact wide-angle thermal imaging lens

Using molded chalcogenide glass technology to reduce cost in a compact wide-angle thermal imaging lens Using molded chalcogenide glass technology to reduce cost in a compact wide-angle thermal imaging lens George Curatu a, Brent Binkley a, David Tinch a, and Costin Curatu b a LightPath Technologies, 2603

More information

Beam expansion standard concepts re-interpreted

Beam expansion standard concepts re-interpreted Beam expansion standard concepts re-interpreted Ulrike Fuchs (Ph.D.), Sven R. Kiontke asphericon GmbH Stockholmer Str. 9 07743 Jena, Germany Tel: +49-3641-3100500 Introduction Everyday work in an optics

More information

Laser Diode Mounting Kits

Laser Diode Mounting Kits Laser Diode Mounting Kits For Ø5.6mm and Ø9mm Laser Diodes Complete Mounting System with Collimating Lens If your work involves laser diodes, you ll appreciate the benefits of Optima s laser diode mounting

More information

Using Stock Optics. ECE 5616 Curtis

Using Stock Optics. ECE 5616 Curtis Using Stock Optics What shape to use X & Y parameters Please use achromatics Please use camera lens Please use 4F imaging systems Others things Data link Stock Optics Some comments Advantages Time and

More information

Multi-Element Overview

Multi-Element Overview Intro Lenses Overview........ 128 Windows Achromats 425-675nm Cemented Doublets. 132 425-675nm Fast Achromats..... 133 1064/633nm Air-Spaced...... 134 1064/532nm Air-Spaced...... 135 Aplanats Visible....................

More information

Chapter 3. Introduction to Zemax. 3.1 Introduction. 3.2 Zemax

Chapter 3. Introduction to Zemax. 3.1 Introduction. 3.2 Zemax Chapter 3 Introduction to Zemax 3.1 Introduction Ray tracing is practical only for paraxial analysis. Computing aberrations and diffraction effects are time consuming. Optical Designers need some popular

More information

Exercise 1 - Lens bending

Exercise 1 - Lens bending Exercise 1 - Lens bending Most of the aberrations change with the bending of a lens. This is demonstrated in this exercise. a) Establish a lens with focal length f = 100 mm made of BK7 with thickness 5

More information

capabilities Infrared Contact us for a Stock or Custom Quote Today!

capabilities Infrared Contact us for a Stock or Custom Quote Today! Infrared capabilities o 65+ Stock Components Available for Immediate Delivery o Design Expertise in SWIR, Mid-Wave, and Long-Wave Assemblies o Flat, Spherical, and Aspherical Manufacturing Expertise Edmund

More information

Evaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System

Evaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System Page 1 5/7/2007 Evaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System Vincent Kan May 7, 2007 University of Toronto Department of Physics Supervisor: Prof.

More information

Performance Factors. Technical Assistance. Fundamental Optics

Performance Factors.   Technical Assistance. Fundamental Optics Performance Factors After paraxial formulas have been used to select values for component focal length(s) and diameter(s), the final step is to select actual lenses. As in any engineering problem, this

More information

The Design, Fabrication, and Application of Diamond Machined Null Lenses for Testing Generalized Aspheric Surfaces

The Design, Fabrication, and Application of Diamond Machined Null Lenses for Testing Generalized Aspheric Surfaces The Design, Fabrication, and Application of Diamond Machined Null Lenses for Testing Generalized Aspheric Surfaces James T. McCann OFC - Diamond Turning Division 69T Island Street, Keene New Hampshire

More information

Tutorial Zemax 8: Correction II

Tutorial Zemax 8: Correction II Tutorial Zemax 8: Correction II 2012-10-11 8 Correction II 1 8.1 High-NA Collimator... 1 8.2 Zoom-System... 6 8.3 New Achromate and wide field system... 11 8 Correction II 8.1 High-NA Collimator An achromatic

More information

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term Lens Design I Lecture 3: Properties of optical systems II 205-04-8 Herbert Gross Summer term 206 www.iap.uni-jena.de 2 Preliminary Schedule 04.04. Basics 2.04. Properties of optical systrems I 3 8.04.

More information

Understanding Optical Specifications

Understanding Optical Specifications Understanding Optical Specifications Optics can be found virtually everywhere, from fiber optic couplings to machine vision imaging devices to cutting-edge biometric iris identification systems. Despite

More information

1.1 Singlet. Solution. a) Starting setup: The two radii and the image distance is chosen as variable.

1.1 Singlet. Solution. a) Starting setup: The two radii and the image distance is chosen as variable. 1 1.1 Singlet Optimize a single lens with the data λ = 546.07 nm, object in the distance 100 mm from the lens on axis only, focal length f = 45 mm and numerical aperture NA = 0.07 in the object space.

More information

Optical Design with Zemax for PhD

Optical Design with Zemax for PhD Optical Design with Zemax for PhD Lecture 7: Optimization II 26--2 Herbert Gross Winter term 25 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content.. Introduction 2 2.2. Basic Zemax

More information

Exam 4. Name: Class: Date: Multiple Choice Identify the choice that best completes the statement or answers the question.

Exam 4. Name: Class: Date: Multiple Choice Identify the choice that best completes the statement or answers the question. Name: Class: Date: Exam 4 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. Mirages are a result of which physical phenomena a. interference c. reflection

More information

MicroSpot FOCUSING OBJECTIVES

MicroSpot FOCUSING OBJECTIVES OFR P R E C I S I O N O P T I C A L P R O D U C T S MicroSpot FOCUSING OBJECTIVES APPLICATIONS Micromachining Microlithography Laser scribing Photoablation MAJOR FEATURES For UV excimer & high-power YAG

More information

Tutorial Zemax Introduction 1

Tutorial Zemax Introduction 1 Tutorial Zemax Introduction 1 2012-07-17 1 Introduction 1 1.1 Exercise 1-1: Stair-mirror-setup... 1 1.2 Exercise 1-2: Symmetrical 4f-system... 5 1 Introduction 1.1 Exercise 1-1: Stair-mirror-setup Setup

More information

GEOMETRICAL OPTICS AND OPTICAL DESIGN

GEOMETRICAL OPTICS AND OPTICAL DESIGN GEOMETRICAL OPTICS AND OPTICAL DESIGN Pantazis Mouroulis Associate Professor Center for Imaging Science Rochester Institute of Technology John Macdonald Senior Lecturer Physics Department University of

More information

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons

More information

Aberrations of a lens

Aberrations of a lens Aberrations of a lens 1. What are aberrations? A lens made of a uniform glass with spherical surfaces cannot form perfect images. Spherical aberration is a prominent image defect for a point source on

More information

Applied Optics. , Physics Department (Room #36-401) , ,

Applied Optics. , Physics Department (Room #36-401) , , Applied Optics Professor, Physics Department (Room #36-401) 2290-0923, 019-539-0923, shsong@hanyang.ac.kr Office Hours Mondays 15:00-16:30, Wednesdays 15:00-16:30 TA (Ph.D. student, Room #36-415) 2290-0921,

More information

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term Lens Design I Lecture 3: Properties of optical systems II 207-04-20 Herbert Gross Summer term 207 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 207 06.04. Basics 2 3.04. Properties of optical

More information

Tutorial Zemax 9: Physical optical modelling I

Tutorial Zemax 9: Physical optical modelling I Tutorial Zemax 9: Physical optical modelling I 2012-11-04 9 Physical optical modelling I 1 9.1 Gaussian Beams... 1 9.2 Physical Beam Propagation... 3 9.3 Polarization... 7 9.4 Polarization II... 11 9 Physical

More information

INDEX OF REFRACTION index of refraction n = c/v material index of refraction n

INDEX OF REFRACTION index of refraction n = c/v material index of refraction n INDEX OF REFRACTION The index of refraction (n) of a material is the ratio of the speed of light in vacuuo (c) to the speed of light in the material (v). n = c/v Indices of refraction for any materials

More information

Robert Huang, CEO. Our Vision: To Be Major Player in Global Opto-Electronic Industry. Our Mission: To Broaden Wavelength

Robert Huang, CEO. Our Vision: To Be Major Player in Global Opto-Electronic Industry. Our Mission: To Broaden Wavelength Dear Customer: Over the past 14 years, Wavelength Opto-Electronic Singapore has grown from a small optics company to a global supplier in laser optics industry. Today, we have nearly 250 Wavelength employees

More information

PHY170: OPTICS. Things to do in the lab INTRODUCTORY REMARKS OPTICS SIMULATIONS

PHY170: OPTICS. Things to do in the lab INTRODUCTORY REMARKS OPTICS SIMULATIONS INTRODUCTORY REMARKS PHY170: OPTICS The optics experiments consist of two major parts. Setting up various components and performing the experiments described below. Computer simulation of images generated

More information

Optical System Design

Optical System Design Phys 531 Lecture 12 14 October 2004 Optical System Design Last time: Surveyed examples of optical systems Today, discuss system design Lens design = course of its own (not taught by me!) Try to give some

More information

PRODUCT BROCHURE PRECITEC LR. Optical sensor for ultra-precision surfaces

PRODUCT BROCHURE PRECITEC LR. Optical sensor for ultra-precision surfaces PRODUCT BROCHURE PRECITEC LR Optical sensor for ultra-precision surfaces 2 PRECITEC LR Optical sensor for ultra-precision surfaces PRODUCT HIGHLIGHTS PUSHING THE LIMITS WITH OPTICAL MEASUREMENT The PRECITEC

More information

Optical Design with Zemax

Optical Design with Zemax Optical Design with Zemax Lecture : Correction II 3--9 Herbert Gross Summer term www.iap.uni-jena.de Correction II Preliminary time schedule 6.. Introduction Introduction, Zemax interface, menues, file

More information

Sequential Ray Tracing. Lecture 2

Sequential Ray Tracing. Lecture 2 Sequential Ray Tracing Lecture 2 Sequential Ray Tracing Rays are traced through a pre-defined sequence of surfaces while travelling from the object surface to the image surface. Rays hit each surface once

More information

Optical Engineering 421/521 Sample Questions for Midterm 1

Optical Engineering 421/521 Sample Questions for Midterm 1 Optical Engineering 421/521 Sample Questions for Midterm 1 Short answer 1.) Sketch a pechan prism. Name a possible application of this prism., write the mirror matrix for this prism (or any other common

More information

Introduction to Optical Modeling. Friedrich-Schiller-University Jena Institute of Applied Physics. Lecturer: Prof. U.D. Zeitner

Introduction to Optical Modeling. Friedrich-Schiller-University Jena Institute of Applied Physics. Lecturer: Prof. U.D. Zeitner Introduction to Optical Modeling Friedrich-Schiller-University Jena Institute of Applied Physics Lecturer: Prof. U.D. Zeitner The Nature of Light Fundamental Question: What is Light? Newton Huygens / Maxwell

More information

APPLICATION NOTE

APPLICATION NOTE THE PHYSICS BEHIND TAG OPTICS TECHNOLOGY AND THE MECHANISM OF ACTION OF APPLICATION NOTE 12-001 USING SOUND TO SHAPE LIGHT Page 1 of 6 Tutorial on How the TAG Lens Works This brief tutorial explains the

More information

Lens Design Optimization/ Estimator Product Requirements Document University of Rochester, Institute of Optics OPT 310 Senior Design

Lens Design Optimization/ Estimator Product Requirements Document University of Rochester, Institute of Optics OPT 310 Senior Design Lens Design Optimization/ Estimator Product Requirements Document University of Rochester, Institute of Optics OPT 310 Senior Design Joe Centurelli & Natalie Pastuszka Document Number 001 Revisions Level

More information

PHYSICS OPTICS. Mr Rishi Gopie

PHYSICS OPTICS. Mr Rishi Gopie OPTICS Mr Rishi Gopie Ray Optics II Images formed by lens maybe real or virtual and may have different characteristics and locations that depend on: i) The type of lens involved, whether converging or

More information

why TECHSPEC? From Design to Prototype to Volume Production

why TECHSPEC? From Design to Prototype to Volume Production high volume stock optics Lenses From Design to Prototype to Volume Production Prisms Filters why TECHSPEC? Volume Discounts from 6 to 100,000 Pieces Certified Edmund Optics Quality Continual Availability

More information

PRECISION LENS MOLDING OF CHALCOGENIDE OPTICS. Jayson J. Nelson 22 Apr 2015

PRECISION LENS MOLDING OF CHALCOGENIDE OPTICS. Jayson J. Nelson 22 Apr 2015 PRECISION LENS MOLDING OF CHALCOGENIDE OPTICS Jayson J. Nelson 22 Apr 2015 PRECISION LENS MOLDING OF CHALCOGENIDE OPTICS 2 Global markets are looking for low cost materials that satisfy infrared imaging

More information

GRINTECH GmbH. product information.

GRINTECH GmbH. product information. GRINTECH GmbH product information www.grintech.de GRIN rod lenses Gradient index lenses for fiber coupling and beam shaping of laser diodes z l d s f Order example: GT-LFRL-100-025-50-CC (670) Design wavelength

More information

Ch 24. Geometric Optics

Ch 24. Geometric Optics text concept Ch 24. Geometric Optics Fig. 24 3 A point source of light P and its image P, in a plane mirror. Angle of incidence =angle of reflection. text. Fig. 24 4 The blue dashed line through object

More information

Some of the important topics needed to be addressed in a successful lens design project (R.R. Shannon: The Art and Science of Optical Design)

Some of the important topics needed to be addressed in a successful lens design project (R.R. Shannon: The Art and Science of Optical Design) Lens design Some of the important topics needed to be addressed in a successful lens design project (R.R. Shannon: The Art and Science of Optical Design) Focal length (f) Field angle or field size F/number

More information

a) How big will that physical image of the cells be your camera sensor?

a) How big will that physical image of the cells be your camera sensor? 1. Consider a regular wide-field microscope set up with a 60x, NA = 1.4 objective and a monochromatic digital camera with 8 um pixels, properly positioned in the primary image plane. This microscope is

More information

High Volume Stock optics

High Volume Stock optics High Volume Stock optics From Design to Prototype to Volume Production TECHSPEC Lenses TECHSPEC prisms TECHSPEC filters COPYRIGHT COPYRIGHT 2011 EDMUND 2014 EDMUND OPTICS, OPTICS, INC. ALL INC. RIGHTS

More information

OPTICS DIVISION B. School/#: Names:

OPTICS DIVISION B. School/#: Names: OPTICS DIVISION B School/#: Names: Directions: Fill in your response for each question in the space provided. All questions are worth two points. Multiple Choice (2 points each question) 1. Which of the

More information

Lens Design I Seminar 5

Lens Design I Seminar 5 Y. Sekman, X. Lu, H. Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 5 Exercise 5-1: PSF scaling (Homework) To check the Airy

More information

Industrial quality control HASO for ensuring the quality of NIR optical components

Industrial quality control HASO for ensuring the quality of NIR optical components Industrial quality control HASO for ensuring the quality of NIR optical components In the sector of industrial detection, the ability to massproduce reliable, high-quality optical components is synonymous

More information

Exercises Advanced Optical Design Part 5 Solutions

Exercises Advanced Optical Design Part 5 Solutions 2014-12-09 Manuel Tessmer M.Tessmer@uni-jena.dee Minyi Zhong minyi.zhong@uni-jena.de Herbert Gross herbert.gross@uni-jena.de Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str.

More information

Lens Design II. Lecture 2: Structural modifications Herbert Gross. Winter term

Lens Design II. Lecture 2: Structural modifications Herbert Gross. Winter term Lens Design II Lecture 2: Structural modifications 26--26 Herbert Gross Winter term 26 www.iap.uni-jena.de 2 Preliminary Schedule 9.. Aberrations and optimization Repetition 2 26.. Structural modifications

More information

Converging Lenses. Parallel rays are brought to a focus by a converging lens (one that is thicker in the center than it is at the edge).

Converging Lenses. Parallel rays are brought to a focus by a converging lens (one that is thicker in the center than it is at the edge). Chapter 30: Lenses Types of Lenses Piece of glass or transparent material that bends parallel rays of light so they cross and form an image Two types: Converging Diverging Converging Lenses Parallel rays

More information

A broadband achromatic metalens for focusing and imaging in the visible

A broadband achromatic metalens for focusing and imaging in the visible SUPPLEMENTARY INFORMATION Articles https://doi.org/10.1038/s41565-017-0034-6 In the format provided by the authors and unedited. A broadband achromatic metalens for focusing and imaging in the visible

More information

Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California

Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Modern Optical Engineering The Design of Optical Systems Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Fourth Edition Me Graw Hill New York Chicago San Francisco

More information

Why is There a Black Dot when Defocus = 1λ?

Why is There a Black Dot when Defocus = 1λ? Why is There a Black Dot when Defocus = 1λ? W = W 020 = a 020 ρ 2 When a 020 = 1λ Sag of the wavefront at full aperture (ρ = 1) = 1λ Sag of the wavefront at ρ = 0.707 = 0.5λ Area of the pupil from ρ =

More information

COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR)

COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR) COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR) PAPER TITLE: BASIC PHOTOGRAPHIC UNIT - 3 : SIMPLE LENS TOPIC: LENS PROPERTIES AND DEFECTS OBJECTIVES By

More information

Optical Design Forms for DUV&VUV Microlithographic Processes

Optical Design Forms for DUV&VUV Microlithographic Processes Optical Design Forms for DUV&VUV Microlithographic Processes James Webb, Julie Bentley, Paul Michaloski, Anthony Phillips, Ted Tienvieri Tropel Corporation, 60 O Connor Road, Fairport, NY 14450 USA, jwebb@tropel.com

More information

CHAPTER 18 REFRACTION & LENSES

CHAPTER 18 REFRACTION & LENSES Physics Approximate Timeline Students are expected to keep up with class work when absent. CHAPTER 18 REFRACTION & LENSES Day Plans for the day Assignments for the day 1 18.1 Refraction of Light o Snell

More information

Optical Theory Simplified: 9 Fundamentals To Becoming An Optical Genius

Optical Theory Simplified: 9 Fundamentals To Becoming An Optical Genius LEARNING UNDERSTANDING INTRODUCING APPLYING Optical Theory Simplified: 9 Fundamentals To Becoming An Optical Genius A P P L I C A T I O N N O T E S Optics Application Examples Understanding Optical Specifications

More information

The New Standard in Lightfastness Testing

The New Standard in Lightfastness Testing The New Standard in Lightfastness Testing Xenon Lightfastness Tester Model B02 s The New Standard in Lightfastness Testing Designed specifically to meet ISO 105 B02, the new rotating rack Q-Sun Model

More information

Lens Design I Seminar 1

Lens Design I Seminar 1 Xiang Lu, Ralf Hambach Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 1 Warm-Up (20min) Setup a single, symmetric, biconvex lens

More information

Average: Standard Deviation: Max: 99 Min: 40

Average: Standard Deviation: Max: 99 Min: 40 1 st Midterm Exam Average: 83.1 Standard Deviation: 12.0 Max: 99 Min: 40 Please contact me to fix an appointment, if you took less than 65. Chapter 33 Lenses and Op/cal Instruments Units of Chapter 33

More information

Chapter 29/30. Wave Fronts and Rays. Refraction of Sound. Dispersion in a Prism. Index of Refraction. Refraction and Lenses

Chapter 29/30. Wave Fronts and Rays. Refraction of Sound. Dispersion in a Prism. Index of Refraction. Refraction and Lenses Chapter 29/30 Refraction and Lenses Refraction Refraction the bending of waves as they pass from one medium into another. Caused by a change in the average speed of light. Analogy A car that drives off

More information

YAG LASER OPTICS - COVERSLIDES / LENSES / MIRRORS / LASER RODS / FLASH LAMPS / FIBER OPTIC CABLES

YAG LASER OPTICS - COVERSLIDES / LENSES / MIRRORS / LASER RODS / FLASH LAMPS / FIBER OPTIC CABLES Clear Beam Company PH: 864-898-0702 115 Pine Lane FAX: 864-898-0078 Pickens, SC 29671 YAG LASER OPTICS - COVERSLIDES / LENSES / MIRRORS / LASER RODS / FLASH LAMPS / FIBER OPTIC CABLES CTA8061 Cotton Tip

More information

Some lens design methods. Dave Shafer David Shafer Optical Design Fairfield, CT #

Some lens design methods. Dave Shafer David Shafer Optical Design Fairfield, CT # Some lens design methods Dave Shafer David Shafer Optical Design Fairfield, CT 06824 #203-259-1431 shaferlens@sbcglobal.net Where do we find our ideas about how to do optical design? You probably won t

More information

Optical design of Dark Matter Telescope: improving manufacturability of telescope

Optical design of Dark Matter Telescope: improving manufacturability of telescope Optical design of Dark Matter Telescope: improving manufacturability of telescope Lynn G. Seppala November 5, 2001 The attached slides contain some talking point that could be useful during discussions

More information

Study on Imaging Quality of Water Ball Lens

Study on Imaging Quality of Water Ball Lens 2017 2nd International Conference on Mechatronics and Information Technology (ICMIT 2017) Study on Imaging Quality of Water Ball Lens Haiyan Yang1,a,*, Xiaopan Li 1,b, 1,c Hao Kong, 1,d Guangyang Xu and1,eyan

More information

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name: EE119 Introduction to Optical Engineering Fall 2009 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

Practical Guide to Specifying Optical Components

Practical Guide to Specifying Optical Components Practical Guide to Specifying Optical Components OPTI 521 Introduction to Opto-Mechanical Engineering Fall 2012 December 10, 2012 Brian Parris Introduction This paper is intended to serve as a practical

More information

Optimisation. Lecture 3

Optimisation. Lecture 3 Optimisation Lecture 3 Objectives: Lecture 3 At the end of this lecture you should: 1. Understand the use of Petzval curvature to balance lens components 2. Know how different aberrations depend on field

More information

Solution of Exercises Lecture Optical design with Zemax Part 6

Solution of Exercises Lecture Optical design with Zemax Part 6 2013-06-17 Prof. Herbert Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Solution of Exercises Lecture Optical design with Zemax Part 6 6 Illumination

More information

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term Lens Design I Lecture : Optimization II 5-6- Herbert Gross Summer term 5 www.iap.uni-jena.de Preliminary Schedule 3.. Basics.. Properties of optical systrems I 3 7.5..5. Properties of optical systrems

More information

Bandpass Edge Dichroic Notch & More

Bandpass Edge Dichroic Notch & More Edmund Optics BROCHURE Filters COPYRIGHT 217 EDMUND OPTICS, INC. ALL RIGHTS RESERVED 1/17 Bandpass Edge Dichroic Notch & More Contact us for a Stock or Custom Quote Today! USA: +1-856-547-3488 EUROPE:

More information

OPAC 202 Optical Design and Inst.

OPAC 202 Optical Design and Inst. OPAC 202 Optical Design and Inst. Topic 9 Aberrations Department of http://www.gantep.edu.tr/~bingul/opac202 Optical & Acustical Engineering Gaziantep University Apr 2018 Sayfa 1 Introduction The influences

More information

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2002 Final Exam Name: SID: CLOSED BOOK. FOUR 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

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

Chapter 18 Optical Elements

Chapter 18 Optical Elements Chapter 18 Optical Elements GOALS When you have mastered the content of this chapter, you will be able to achieve the following goals: Definitions Define each of the following terms and use it in an operational

More information

TECHNICAL QUICK REFERENCE GUIDE MANUFACTURING CAPABILITIES GLASS PROPERTIES COATING CURVES REFERENCE MATERIALS

TECHNICAL QUICK REFERENCE GUIDE MANUFACTURING CAPABILITIES GLASS PROPERTIES COATING CURVES REFERENCE MATERIALS TECHNICAL QUICK REFERENCE GUIDE COATING CURVES GLASS PROPERTIES MANUFACTURING CAPABILITIES REFERENCE MATERIALS TABLE OF CONTENTS Why Edmund Optics?... 3 Anti-Reflective (AR) Coatings... 4-16 Metallic Mirror

More information

Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging

Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging Wei Ting Chen 1,, Alexander Y. Zhu 1,, Mohammadreza Khorasaninejad 1, Zhujun Shi 2, Vyshakh Sanjeev 1,3

More information

LASER BEAM COLLIMATOR FOR FIBER AND DIRECT DIODE LASERS

LASER BEAM COLLIMATOR FOR FIBER AND DIRECT DIODE LASERS 0 FOR FIBER AND DIRECT DIODE LASERS 1 GENERAL INFORMATION 2017 OPI Photonics S.R.L. All rights reserved. OPI Photonics S.R.L. reserves the right to make changes to this document at any time without prior

More information

Micro-Optic Solar Concentration and Next-Generation Prototypes

Micro-Optic Solar Concentration and Next-Generation Prototypes Micro-Optic Solar Concentration and Next-Generation Prototypes Jason H. Karp, Eric J. Tremblay and Joseph E. Ford Photonics Systems Integration Lab University of California San Diego Jacobs School of Engineering

More information

Lens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term

Lens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term Lens Design I Lecture 5: Advanced handling I 2018-05-17 Herbert Gross Summer term 2018 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 2018 1 12.04. Basics 2 19.04. Properties of optical systems

More information

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term Lens Design I Lecture : Optimization II 8-6- Herbert Gross Summer term 8 www.iap.uni-jena.de Preliminary Schedule - Lens Design I 8.4. Basics 9.4. Properties of optical systems I 3 6.4. Properties of optical

More information