MicroSpot FOCUSING OBJECTIVES

Similar documents
Multi-Element Overview

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

CVI LASER OPTICS ANTIREFLECTION COATINGS

why TECHSPEC? From Design to Prototype to Volume Production

Bandpass Edge Dichroic Notch & More

Index. A Analyzer, Polarization. FO-18 L Laser Beam Expanders OC-10,11 Laser Collimators. FO-31 Apodizer. K Kits, FiberBench

High Volume Stock optics

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

RMS roughness: < 1.5Å on plane surfaces and about 2Å on smoothly bended spherical surfaces

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

The RSH Catalogue. Laser Optics & Lenses

Photonics West Contact us for a Stock or Custom Quote Today! Edmund Optics BROCHURE

Optical Design Forms for DUV&VUV Microlithographic Processes

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

Using Stock Optics. ECE 5616 Curtis

ND:YAG/ND:YLF...T-26 TUNABLE LASER MIRRORS...T-28 MISCELLANEOUS MIRRORS...T-30 ANTI-REFLECTIVE OVERVIEW...T-31 0 DEGREE ANGLE OF INCIDENCE...

Immersion Lithography Micro-Objectives

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

Research Grade Xenon Arc Lamp Sources LH-Series 75 W - 300W

Beam Shaping in High-Power Laser Systems with Using Refractive Beam Shapers

Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:

Introduction to Light Microscopy. (Image: T. Wittman, Scripps)

DPMPHOTONICS. Precision Optics Catalog. P.O. Box 3002 Vernon, CT Tel: (860) Fax: (860)

End Capped High Power Assemblies

The LINOS Singlets. Our quality criteria:

TECHSPEC COMPACT FIXED FOCAL LENGTH LENS

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

EDMUND OPTICS ULTRAVIOLET OPTICS

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

- Optics Design - Lens - Mirror - Window - Filter - Prism

Supplementary Figure 1. Effect of the spacer thickness on the resonance properties of the gold and silver metasurface layers.

Absentee layer. A layer of dielectric material, transparent in the transmission region of

EUV Plasma Source with IR Power Recycling

Oriel Flood Exposure Sources

UV EXCIMER LASER BEAM HOMOGENIZATION FOR MICROMACHINING APPLICATIONS

Excimer laser projector for microelectronics applications

SELECTION GUIDE MULTIPLE-ORDER QUARTZ WAVEPLATES ZERO-ORDER QUARTZ WAVEPLATES DUAL-WAVELENGTH WAVEPLATES... 85

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

Optical System Design

Photolithography II ( Part 2 )

Diffractive Axicon application note

Optical Systems. Selection Guide. Simple Telescope Kit page 6.4. Variable Attenuators for linearly polarized laser beam page 6.

Will contain image distance after raytrace Will contain image height after raytrace

PELHAM RESEARCH OPTICAL L.L.C.

Performance Factors. Technical Assistance. Fundamental Optics

ASPHERIC LENSES FOR OPTICS AND PHOTONICS

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

Copyright 2000 by the Society of Photo-Optical Instrumentation Engineers.

COLOUR INSPECTION, INFRARED AND UV

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

Laser Induced Damage Threshold of Optical Coatings

StockOptics. CATALOG 2018 Europe

Laser Speckle Reducer LSR-3000 Series


Geltech Aspheric Lenses

Optical Design with Zemax

Applying of refractive beam shapers of circular symmetry to generate non-circular shapes of homogenized laser beams

Microscope anatomy, image formation and resolution

Flat Top, Ultra-Narrow Band Pass Optical Filters Using Plasma Deposited Hard Oxide Coatings

High power VCSEL array pumped Q-switched Nd:YAG lasers

PHY 431 Homework Set #5 Due Nov. 20 at the start of class

CCAM Microscope Objectives

Angela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy

EE-527: MicroFabrication

Vertical External Cavity Surface Emitting Laser

GRINTECH GmbH. product information.

Optics Glossary. Back Focal Length (BFL): The distance between the last surface of a lens to its image focal plane.

Beam Expander (4) Substituting Equation (1) into Equation (5), the following expression can be obtained

30 MM CAGE CUBE MOUNTED TURNING PRISM MIRRORS

Lens Design I Seminar 5

CREATING ROUND AND SQUARE FLATTOP LASER SPOTS IN MICROPROCESSING SYSTEMS WITH SCANNING OPTICS Paper M305

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

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Optical Isolator Tutorial (Page 1 of 2) νlh, where ν, L, and H are as defined below. ν: the Verdet Constant, a property of the

Fiber Optic Communications

Reflection! Reflection and Virtual Image!

A LEADER IN OPTICAL TECHNOLOGY. GRADIUM Lenses.

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

WJM Technologies excellence in material joining

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

The Importance of Wavelengths on Optical Designs

P r i s m s I N D E X

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

Transferring wavefront measurements to ablation profiles. Michael Mrochen PhD Swiss Federal Institut of Technology, Zurich IROC Zurich

Optical Components. Table of Contents. Mirrors. Windows & Filters

Design Description Document

WELCOME TO EO ISRAEL EVENT

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Practical Flatness Tech Note

PREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES

X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope

Mirrors. Plano and Spherical. Mirrors. Published on II-VI Infrared

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)

High-speed Fabrication of Micro-channels using Line-based Laser Induced Plasma Micromachining (L-LIPMM)

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

Flatness of Dichroic Beamsplitters Affects Focus and Image Quality

Gentec Electro-Optics, Inc

Filters for Dual Band Infrared Imagers

PREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES

Transcription:

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 Long working distance All refractive models UV achromatic models Video monitoring

Table of Contents Contents Pages Introduction 2-3 UV Refractive Objectives (LMU, LMUL) 3 AR Coatings for UV Excimer Lasers 4 YAG Refractive Objectives (LMH) 5 45 Max Reflectors/Beamsplitters 6 Reflective Objectives 7 MicroSpot Focusing Objectives, manufactured in USA by OFR. Classical Microscope Objectives versus OFR MicroSpot Focusing Objectives Modern industrial laser applications impose stringent demands on the microscope objective. Cemented elements and oil-immersed lenses severely limit the utility of the traditional objective with high-power UV and IR lasers. With lens elements made in excimergrade materials (fused silica and CaF2), OFR's MicroSpot Focusing Objectives are designed for use with UV, Visible, IR or high-power YAG lasers. Micro- Spot Objectives are increasingly used for micromachining, laser scribing and microlithography. An important feature of OFR MicroSpot Objectives is long working distance, the advantage of which is to minimize vapor deposition on the first lens surface resulting from ablated material. Also, this extra space allows insertion of protective windows, tools and other devices. OFR MicroSpot Classical Microscope Focusing Objectives Objective Application Spectrum UV, Visible or IR Visible only Optical Power Low or High Power Low Power only Object Target to be focused upon To be viewed Conjugates Infinite Finite Video Monitoring Yes Yes MicroSpot Focusing Objectives MS-1

MicroSpot Focusing Objectives, designed and manufactured by OFR since 1988... DESIGNED FOR UV AND HIGH POWER Traditional microscope objectives are designed for direct imaging by the eye. Because they contain high-index flint glasses, cemented interfaces or oilimmersed lenses, they are limited to low-power, visible spectrum applications. In contrast, OFR MicroSpot Focusing Objectives do not use cemented interfaces, and thus are well suited for high-power UV and YAG lasers. EXCIMER-GRADE OPTICAL MATERIALS The lens elements in OFR LMU and LMUL Series UV Achromatic Objectives are made of excimer-grade fused silica and CaF2, resulting in superior performance with high-power excimer lasers. All lenses are air-spaced. YAG LASER APPLICATIONS Lenses in the LMH Series YAG Laser Objectives are made of the same fused silica as OFR high-power YAG Laser Lenses (See PRECISION OPTICAL COMPONENTS catalog). With highenergy damage resistant AR coatings, LMH Objectives are designed for use with high power YAG lasers. AR-COATED FOR OPERATING WAVELENGTH Unlike traditional microscope objectives that are AR coated only for the visible spectrum, all OFR MicroSpot Objectives are coated for the wavelength of operation. LONG WORKING DISTANCE Short working distances of traditional objectives create problems in ablative applications (such as laser trimming or semi-conductor circuit shaping). OFR LMU UV Achromatic Objectives have long working distances that help to minimize vapor deposition on the front lens surface. For extreme cases, the LMUL Ultra-Long Objective has the longest working distance for its magnification. All OFR MicroSpot Objectives are designed for use with a collimated laser beam, that is, they are infinite conjugate objectives. OFR MicroSpot Focusing Objectives HIGH NA, LONG WORKING DISTANCE, HIGH-POWER CAPABILITY. In order to meet modern requirements for high NA, with long working distance and high-power capability, OFR designed the MicroSpot Focusing Objective product line. LMU and LMUL Series UV ACHROMATIC OBJECTIVES are designed for long working distance, diffraction limited performance with high-power, UV excimer lasers. LMH Series HIGH POWER Nd:YAG LASER OBJECTIVES are designed for diffraction limited performance and maximum power handling capability when used with industrial Nd:YAG lasers. LMU and LMUL MicroSpot Focusing Objectives All OFR MicroSpot Focusing Objectives... Consist of air-spaced components, with no cemented interfaces to limit usable laser power. Designed for use with lasers (infinite conjugate). Can be used with video monitoring. Equipped with the universal standard Royal Microscope Society (RMS) thread (Whitworth 0.8" x 36 TPI). MS-2

LMU-Series UV Achromatic Objectives OFR's all-refractive UV Achromatic MicroSpot Focusing Objectives are designed for use with high power, UV excimer lasers and other ultraviolet sources. SPECIFICATIONS Materials Excimer-Grade Fused Silica Excimer-Grade Calcium Fluoride Design Spectrum 193 nm to 450 nm Energy Throughput 96-98% 5 mm RMS thread 5 mm RMS thread 25 mm dia. 29 mm dia. L D 92 mm 38 mm dia. WD LMU-Series 29 mm dia. Lens elements comprising the LMU Objectives are made from the highest quality, lowest absorption excimer grade fused silica and CaF2 available. For information on material testing under high power UV radiation, the following are recommended: "Optical Materials for Excimer Laser Applications" M. Rothschild, Optics & Photonics News, May, 1993 "Long-Term Effects of Pulsed KrF Laser Radiation on Crystalline and Amorphous SiO2". D.J. Krajnovich, I.K. Pour, SPIE Vol. 2114, Proceedings, 1993 Boulder Damage Symposium "Excimer Lasers: Applications, Beam Delivery Systems and Laser Design" SPIE Vol. 1835, Proceedings, Nov. 1992 Boston Conference "Improvements in Crystal Optics for Excimer Lasers" Toepke, D. Cope, Harshaw/Bicron Crystal Products Group 19 mm LMUL-20X Ultra Long-Working Distance (λ>240 nm, no NUV) UV MicroSpot FOCUSING OBJECTIVES Theoretical Catalog Working Effective Numerical Focal Spot Entrance Number Distance Focal Length Aperture Diameter Aperture D L LMU-3X-λ 49 mm 60 mm 0.08 5 µm* 10 mm 21 mm 28 mm LMU-5X-λ 35 mm 40 mm 0.13 3 µm* 10 mm 21 mm 28 mm LMU-10X-λ 15 mm 20 mm 0.25 2 µm* 10 mm 21 mm 42 mm LMU-15X-λ 8.5 mm 13 mm 0.32 1 µm* 8.5 mm 21 mm 40 mm LMU-20X-λ 4 mm 10 mm 0.40 1 µm* 8 mm 21 mm 39 mm LMU-40X-λ 1 mm 5 mm 0.50 1 µm* 5 mm 21 mm 38 mm LMUL-20X-λ 19 mm 10 mm 0.40 Discuss 8 mm see drawing When ordering, specify coating according to wavelength and power rating by adding the appropriate coating code, for example, LMUL-20X-266 or LMU-10X-UVB. * Note that Theoretical Focal Spot Diameter values are based on a Gaussian profile input beam at Design Wavelength which fills the Entrance Aperture at the 1/e 2 limits. ZERO-POWER ACHROMATIZER available, See page 7. MS-3

Antireflection Coatings MicroSpot Objectives are supplied with high energy-resistant, multilayer antireflection coatings optimized for either a specific excimer laser wavelength or a broadband range of wavelengths within the design spectrum. Standard coatings are shown below. When ordering, replace the "λ" at the end of the part number with the appropriate wavelength (nm) or coating code. Transmission is more than adequate for video monitoring in the visible. For use outside the UV design spectrum, discuss with OFR. Contact OFR for information concerning direct and remote monitoring, and individual model performance at other wavelengths. ANTIREFLECTION COATINGS NARROWBAND AR COATINGS Per surface Center Maximum Power Wavelength Bandwidth Reflectance Rating 193 nm (ArF) 192-194 nm <1.5% 100 MW/cm 2 248 nm (KrF) 240-260 nm <0.5% 200 MW/cm 2 257 nm 266 nm (Nd:YAG) 255-280 nm <0.35% 500 MW/cm 2 308 nm (XeCI) 288-319 nm <0.25% 500 MW/cm 2 351 nm (XeF) 340-370 nm <0.25% 500 MW/cm 2 354 nm (Nd:YAG) 340-370 nm <0.25% 500 MW/cm 2 BROADBAND AR COATINGS Per surface Coating Maximum Power Code Bandwidth Reflectance Rating UVB 240-360 nm 1.5% 50 MW/cm 2 NUV* 325-500 nm 1 % 50 MW/cm 2 *Not available on LMUL-20X. NOTE: Power rating based upon 20 n-s pulses, 20 Hz. TRANSMISSION OF LMU SERIES OBJECTIVES HIGH POWER AR COATINGS Objective Transmission Note LMU-5X-193 90% LMU-40X-193 80% LMU-5X-248 94% LMU-40X-248 86% LMU-5X-266 94% LMU-40X-266 86% Transmission depends on beam diameter and characteristics, and therefore is not completely predictable. Please inquire. BROADBAND AR COATINGS (LOW POWER ONLY) 240-360 nm 325-500 nm LMU-5X-UVB >90% LMU-5X-NUV >92% LMU-40X-UVB >80% LMU-40X-NUV >86% MS-4

LMH-Series High Power YAG Laser Objectives OFR High Power Nd:YAG MicroSpot Focusing Objectives are designed to transmit and focus the high power radiation emitted by industrial Nd:YAG lasers. Energy Damage Materials Throughput Coating Threshold Fused Silica >96-98% within High power damage-resistant, 500 MW/cm 2 design spectrum multilayer antireflection coating optimized for 532 nm or 1064 nm. Other coatings available upon request. NOTE: Power rating based upon 20 n-s pulses, 20 Hz, 532nm or 1064 nm. Use Outside the Design Spectrum The High Power Nd:YAG Objectives are designed for diffraction-limited performance at 1064 nm. Near-diffraction limited performance can be achieved outside the design spectrum, including the visible spectrum. Inquire. Focal length at 532 nm is 2% shorter than at 1064 µm. Contact OFR for information concerning direct and remote monitoring and individual model performance at other wavelengths. 5 mm L RMS thread 25 mm dia. D LMH-5X WD LMH-Series LMH-20X HIGH POWER Nd:YAG LASER MicroSpot FOCUSING OBJECTIVES Theoretical Catalog Working Effective Numerical Focal Spot Entrance Number Distance Focal Length Aperture Diameter Aperture D L LMH-5X-532 or 1064 35 mm 40 mm 0.13 12 µm* 10 mm 21 mm 28 mm LMH-10X-532 or 1064 15 mm 20 mm 0.25 6 µm* 10 mm 21 mm 28 mm LMH-20X-532 or 1064 6 mm 10 mm 0.40 4 µm* 8 mm 21 mm 38 mm * Note that Theoretical Focal Spot Diameter values are based on a Gaussian profile input beam at Design Wavelength which fills the Entrance Aperture at the 1/e 2 limits. MS-5

Video Beamsplitters For Visual Monitoring with Camera UV/ VIDEO BEAMSPLITTERS OFR high-power damage resistant 45 MAX Reflectors/Dichroic Beamsplitters serve a dual purpose, and are used in applications requiring visual monitoring of action on an object in the focal plane of a MicroSpot Objective. The substrates are 6.3 mm thick fused silica. Transmit more than 60% of the visible, with maximum reflection 96-99% of the specified excimer wavelength. Transmittance of the visible is more then 60%. Wavelengths ZERO-POWER ACHROMATIZER (Correction Triplet) Although our LMU Objectives are achromatized for the UV, disparity between the visible (video monitoring) and UV tends to diminish the "sharpness" of the video image. This condition is corrected by our "zero-power" Achromatizer, a correction triplet that compensates for this disparity, thus producing a sharply focused video image. For this function, the Achromatizer is positioned between the camera and the beamsplitter. Note that at this time, the Achromatizer is compatible only with LMU-3X, LMU-10X and LMU-15X. LASER CAMERA OFR VIDEO ACHROMATIZER DICHROIC BEAMSPLITTER MicroSpot OBJECTIVE 193 nm (ArF) 308 nm (XeCI) 248 nm (KrF) 351 nm (XeF) 266 nm (Nd:YAG) 354 nm (Nd:YAG) Catalog Barrel Barrel Number Diameter Length Aperture LACU-20-λ Inquire Inquire 15 mm When ordering, specify λ for AR coatings. FOCAL PLANE UV MAX REFLECTORS/ DICHROIC BEAMSPLITTERS Catalog UV λ Visible UV Power Number Dimensions Reflectance* Transmittance Bandwidth Rating*** MYU-25-193 1" dia. x 1/4" 96% 80% 2% 300 MW/cm2 MYU-51-193 2" dia. x 1/4" 96% 80% 2% 300 MW/cm2 MYU-25-λ 248 1" dia. x 1/4" 99.5% 60-80% 6% 300 MW/cm2 MYU-51-λ 248 2" dia. x 1/4" 99.5% 60-80% 6% 300 MW/cm2 NOTE: When ordering, specify coating according to wavelength. For example, MYU-51-248. Reflectance shown is for random polarization. Bandwidth shown is at ±3% of peak. Power rating based upon 20 n-sec pulses, 20 Hz YAG/VIDEO BEAMSPLITTERS Transmission in the mid-visible more than 60% (color monitoring will appear greenish), while reflection > 99% at 1064 nm. YAG LASER MAX REFLECTORS/ DICHROIC BEAMSPLITTERS Catalog Visible Power Number Dimensions Reflectance* Transmittance Bandwidth Rating*** MYQ-25-532 or 1064 1" dia. x 1/4" 99.5% > 60% 6% 500 MW/cm2 MYQ-51-532 or 1064 2" dia. x 1/4" 99.5% > 60% 6% 500 MW/cm2 * Reflectance shown is for random polarization. ** Bandwidth shown is at ± 3% of peak. *** Power rating based upon 20 n-sec pulses, 20 Hz. MS-6

LMM-Series Reflective Objectives OFR MicroSpot Reflective Objectives consist of multiple reflecting elements, and therefore are achromatic. Spectral characteristics are dependent on the choice of coating. They are based on the classical Schwarzschild design. This design is corrected for third-order spherical aberration, coma and astigmatism at a specific conjugate ratio. Fifth-order aberrations are greatly reduced. OFR MicroSpot Reflective Objectives are designed for infinite conjugate applications that require longer working distances than the provided by refractive objectives. OFR MicroSpot Reflective Objectives are mounted in finely machined bodies with the universal standard, RMS thread. The convex mirror is rigidly held in place by traditional spider vane support. Central Obscuration The convex primary mirror, which acts to diverge the input laser beam, represents an obscuration in the center of the system. It is important to consider this obscuration when designing the complete imaging system. The most evident effect is a reduction of cross-sectional area in the clear aperture of the system. In consideration of a typical Gaussian beam, the obscuration can be an important factor in reducing total energy throughput. The aperture ratios listed below for each model represent the ratio of obscured to unobscured areas. Measurements are based on uniform, cross-sectional energy density. LMM Reflective Objectives Each Objective achieves optimum performance when the input laser beam fills its Design Aperture. Underfilling the aperture can result in decreased total transmission and can affect the focal spot diameter. 5mm 57mm WD LMM- Series RMS thread 26mm 48mm 44mm 42mm MicroSpot Focusing Objectives Theoretical Catalog Working Effective Numerical Focal Spot Design Aperture Number Distance Focal Length Aperture Diameter Aperture Ratio LMM-15X-λ-MU 22 mm 13.3 mm 0.25 3 µm* 6.7 mm 21% * Note that Theoretical Focal Spot Diameter values are based on a Gaussian profile input beam at Design Wavelength which fills the Entrance Aperture at the 1/e 2 limits METALLIC MIRROR COATINGS Coating Design Average Damage Code Bandwith Reflectance Threshold -MU (AI-MgF2 190 nm-400 nm 86% Low Power MS-7