ESPRESSO. Preliminary Specifications for the Dichroic. VLT-SPE-ESP , Issue 5.0 October 17 th, 2013
|
|
- Rafe Shaw
- 5 years ago
- Views:
Transcription
1 Centro de Astrofísica da Universidade do Porto Universidade de Lisboa, CAAUL and LOLS INAF, Osservatorio Astronomico di Trieste INAF, Osservatorio Astronomico di Brera Observatory of the University of Geneva Physics Institute, University of Bern Instituto de Astrofísica de Canarias European Southern Observatory ESPRESSO Preliminary Specifications for the Dichroic VLT-SPE-ESP , Issue 5.0 October 17 th, 2013 Prepared Ana B. Fragoso October 17, 2013 Name Date Signature Approved Name Date Signature Released F. Pepe Name Date Signature
2
3 VLT-SPE-ESP , Issue 5.0 3/20 Change Record Issue/Rev. Date Section/Page affected Reason/Remarks /03/2013 First version /03/2013 Coating on the DC front face / 12 Coating on the DC rear face/ 12 Shape and size / 13 Transmission for the red range is specified Wavelength range is modified Misprint /07/2013 Optical figure / 10 Clear Aperture/12 Coating / 12 Wedge/13 Refractive Index/14 Environmental Requirements/15 Packaging, Handling, Storage and Transportation Requirements/16 Radii of curvature changed CA changed Details in coating design Wedge is included in new design Data of index is included /10/2013 Coating on the DC rear face/12 Material/14 Glass homogeneity/15 Homogeneity is relaxed /10/2013 Applicable Documents/7 Reference Documents/7 Table of Contents Chapter 1. Introduction Scope of the Document Documents Applicable Documents Reference Documents Acronyms and Abbreviations Acronyms...7 Chapter 2. Functional description...9 Chapter 3. Preliminary Specifications Functional Requirements Optical Requirements Optical figure Surface form tolerance of the optical surfaces Surface shape accuracy Surface slope error... 11
4 4/20 ESPRESSO Project Surface micro-roughness Surface Imperfections Coating Coating on the DC front face Transition profile (coating on front face) Coating on the DC rear face Resistance to cleaning Physical Requirements Clear Aperture Shape and size Central thickness Wedge Conic bevel finishing Material Refractive Index Bubble classification Striae grade Glass homogeneity Stress birrefringence Mechanical Performance Requirements Long term stability Reliability Requirement Lifetime guideline Environmental Requirements Packaging, Handling, Storage and Transportation Requirements Transport obligations Handling and storage requirements...16 Chapter 4. Cleanliness Requirements Cleanliness...17 Chapter 5. Appendix A Appendix B Verification at factory...17 : Descriptive drawing...19 : Opto-mechanical Concept...20
5 VLT-SPE-ESP , Issue 5.0 5/20 List of Figures Figure 1. Spectrograph optical layout (TBU)...9 Figure 2. Footprint onto DM (Blue Arm). Colour rays by wavelengths...9 Figure 3. Footprint onto DM (Red Arm). Colour rays by wavelengths...10 Figure 4. DC wedge. Vectors for each surface are indicated in red. YZ view...13 Figure 5. Direction of the reference axis...14 Figure 6. Mount concept...20 List of Tables Table 1. Refractive Index...14 Table 2. Environmental conditions (TBC)...16 Table 3. Handling and Storage Conditions at IAC facilities...16 Table 4. Handling and Storage Conditions at Geneve...16 Table 5. Handling and Storage Conditions at Paranal Observatory...17 Table 6. Verification Matrix...18
6
7 VLT-SPE-ESP , Issue 5.0 7/20 Chapter 1. Introduction 1.1 Scope of the Document Manufacturing specifications for the ESPRESO Dichroic are established in that document. They are mainly following the ISO Standards. If some other Standard were used, it will be explicitly mentioned. Comments from possible suppliers and expert people have been taken into account in the specification of the element. 1.2 Documents Applicable Documents AD-1 ESPRESSO DC Drawing VLT-DWG-ESP SP B Reference Documents RD Acronyms and Abbreviations Acronyms AD Applicable Document ADC Atmospheric Dispersion Corrector AOI Angle Of Incidence APSU Anamorphic Pupil Slicer Unit AR Anti-Reflective BC Blue Camera BDS Blue Detector System BTM Blue Transfer Mirror BXD Blue Cross Disperser CA Clear Aperture CCD Charge Coupled Device CCL Combined Coudé Laboratory CIU Calibration Injection Unit CR Coudé Room CT Coudé Train CU Calibration Unit DC Dichroic EE Exit End EG Echelle Grating EPT ESPRESSO Project Team at the IAC
8 8/20 ESPRESSO Project ESO European Southern Observatory ESPRESSO Echelle Spectrograph for Rocky Exoplanets and Stable Spectroscopic Observations ExpM Exposure Meter FEU Front End Unit FL Fiber Link, Field Lens FPCS Fabry-Perot Calibration Source FSU Field Stabilization Unit FT Feed Through GP Gerardo Periscope IAC Instituto de Astrofísica de Canarias IE Input End LDLS Laser Driven Light Source LFC Laser Frequency Comb MC Main Collimator OB Optical Bench PSU Pupil Stabilization Unit RC Red Camera RD Reference Document RDS Red Detector System RFM Red Folding Mirror RFU Refocusing Unit RTM Red Transfer Mirror RXD Red Cross Disperser SP Spectrograph SU Calibration Selector Unit TBC To Be Confirmed TBD To Be Defined/To Be Developed TBU To Be Updated ThAr Thorium Argon TS Toggling System, Thermal System UT Unit Telescope VLT Very Large Telescope VV Vacuum Vessel XD Cross Disperser
9 VLT-SPE-ESP , Issue 5.0 9/20 Chapter 2. Functional description ESPRESSO spectrograph optical design is based onto a white-pupil asymmetric configuration. A large off-axis parabolic mirror acts as main collimator and is used in double-pass: to illuminate a large mosaic echelle grating (ESPRESSO main disperser) and to collect dispersed light towards transfer optics. Once the light is dispersed by the echelle, a dichroic beam-splitter mirror, located near an intermediate focal plane, splits light into two optimized arms: Blue and Red. Each arm consists of re-imaging optics, specific cross-disperser VPH grism, and a refractive lens camera. The spectrograph optical layout is shown in figure below just as to give an idea of the orientation and position of the elements. The sketch is not representative of final dimensions or sizes. DC g Figure 1. Spectrograph optical layout (TBU) Scale: Millimeters Footprint onto DC is shown in figure below. Aperture Full X Width : Aperture Full Y Height: Figure 2. Footprint onto DM (Blue Arm). Colour rays by wavelengths
10 ESPRESSO Project Scale: Millimeters 10/20 Aperture Full X Width : Aperture Full Y Height: Figure 3. Footprint onto DM (Red Arm). Colour rays by wavelengths Chapter 3. Preliminary Specifications 3.1 Functional Requirements ESPRESSO Dichroic shall reflect wavelength in the blue range (from 380 nm to 515 nm) and transmit the red range (from 535 nm to 780 nm). It will be provided without any kind of cell or mounting. The corresponding Positioning Mechanism will be designed and provided by IAC (see the concept in Appendix B). Interface area with the mechanical parts (see drawing in Appendix A) shall be completely free of coating or any other material. 3.2 Optical Requirements Source: ESPRESSO Optical Group Optical figure The optical figure shall be: Surface Front face Back face 1 Test wavelength: nm Radii of Curvature Infinity mm Tolerance ± 1 fringes1 ± 50 mm Flat Spherical
11 VLT-SPE-ESP , Issue / Surface form tolerance of the optical surfaces The irregularities of the optical surface to which the requirements shall apply includes irregularities due to the following sources: Residuals of the polishing process. Gravitational deformation (see orientation in Figure 1). Thermal deformation within nominal environment conditions (see section 3.6 ) and for testing temperature to operation temperature. Temporal drift Surface shape accuracy The effect of the irregularity of the optical surface of DC on the reflected and transmitted wavefront shall be: < 150 nm P-V, over sub-apertures of 90 x 60 mm. < 40 nm rms, over sub-apertures of 90 x 60 mm Surface slope error 2 Surface slope error is specified for both optical surfaces. Maximum slope shall be: < 1.3 arcsec P-V, up to a spatial frequency of 2 mm. < 0.25 arcsec rms, up to a spatial frequency of 2 mm. NOTE: This requirement means that considering an integration lenght of 2 mm, the maximum P- V value of the slope error shall be < 1.3. arcsec (angle) and the rms value of the slope error shall be < 0.25 arcsec (angle). It complements the surface form tolerance requirement, being the first one for midspatial frequency errors Surface micro-roughness The optical surface shall be polished to a residual surface roughness of 2nm (rms) or better over the whole CA. The way in which the Micro-roughness is measured, shall be proposed by Contractor and approved by EPT. NOTE: Surface roughness of the non-optical surfaces shall be considered and agreed with EPT so as to assure the suitability for the Positioning Mechanism Surface Imperfections According to MIL-C-48497, the surface imperfections of the optical surfaces shall be 40/20. 2 Surface slope error is specified to control the non-uniform deviations in midspatial frequencies
12 12/20 ESPRESSO Project Coating Source: ESPRESSO PI Coating design will be provided by the supplier to be revised and approved by the EPT before manufacturing Coating on the DC front face DC front face (flat) shall be dichroic coated ensuring: Reflectivity over 97% (goal 99%) from 380 nm to 515 nm. Transmission over 98% (goal 99%) from 535 nm to 780 nm Maximum AOI is 14 degrees. (TBC) Transition profile (coating on front face) Nominal transition wavelength is 525 nm. A sharp transition from reflection to transmission is required. Transition shall be < 10 nm (goal 6 nm) from 95%R to 0.5%R, and < 20 nm (goal 10 nm) from 98%R to 0.2%R (TBC) Ripples shall be minimized in amplitude and frequency. They shall be < ±0.5% of average efficiency (reflexion or transmission) and < 1% per Angstrom (TBC) Coating on the DC rear face DC rear face (spherical) shall be AR coated. AR coating transmission shall be over 99% (goal 99.5%) from 380 nm to 780 nm. NOTE: All coating imperfections shall be included in the allowable general surface imperfections and roughness indication Resistance to cleaning The DC coating shall not be adversely affected by materials and procedures used when cleaning the surfaces with: CO2 snow, peel off methods and wet cleaning methods. If some special procedure is required it shall be indicated by DC supplier. 3.3 Physical Requirements Clear Aperture Source: ESPRESSO Optical Group DC Clear Aperture dimensions shall be: 455 x 80 mm 2 (centered)
13 VLT-SPE-ESP , Issue / Shape and size Source: ESPRESSO Optical Group Shape and size of the optical surface shall be rectangular. Dimensions: 460 x 90 mm 2. Tolerance: ±0.010 mm Central thickness Source: ESPRESSO Optical Group DC central thickness shall be 30 mm. ±1 mm. NOTE: DC thickness shall assure the optical and mechanical requirements. EPT shall be informed if any requirement is compromised by this small thickness Wedge Source: ESPRESSO Optical Group DC shall have a wedge of 0.5 degrees in YZ section (see Figure 4). That means that the angle between the curvature radius of the rear surface and the flat surface shall be βx=95degrees (rotation around X axis). (See Figure 4 and Figure 5) Y Z Figure 4. DC wedge. Vectors for each surface are indicated in red. YZ view
14 14/20 ESPRESSO Project Y X Figure 5. Direction of the reference axis Tolerance in wedge shall be < 60 arcsec (in any direction) Conic bevel finishing Source: EPT All the edges shall have protective chamfers from 1 to 1.5 mm width; the angle to axis shall temper the transition from the optical surface to the edge surface Material Source: ESPRESSO Optical Group Ohara BSL7Y or equivalent (Schott BK7HT). NOTE: Glass selection shall be proposed by supplier and approved by EPT Refractive Index Source: ESPRESSO Optical Group. Refractive index of the glass shall be measured and reported. Data shall be taken at 22ºC at nm. and nm. (see table below) Wavelength BSL7Y Refractive Index nm nm Table 1. Refractive Index Bubble classification Source: EPT Bubble classification of Ohara BSL7Y: According to Ohara Bubble Group B.1.
15 VLT-SPE-ESP , Issue / Striae grade Source: EPT Striae grade of Ohara BSL7Y shall be A per MIL-G-174B (no visible striae) Glass homogeneity Source: EPT Optical homogeneity of Ohara BSL7Y shall be < 1 x 10-5 (TBC). Grade Special A10 in OHARA standards. It shall be guaranteed through thickness (460 x 90 face) Stress birrefringence Source: EPT Stress birefringence of Ohara BSL7Y shall be better than 10 nm/cm. 3.4 Mechanical Performance Requirements Long term stability The optical surfaces shall be stable during lifetime. If temporal drift is produced due to the coating material, the effect shall be considered as an additional source of irregularity of the optical surface, which shall be limited. 3.5 Reliability Requirement Lifetime guideline Source: EPT DC should be designed for a minimum lifetime of 15 years under the environment conditions specified in Table 2. This lifetime start at first integration on ESPRESSO spectrograph. 3.6 Environmental Requirements Source: ESPRESSO Team The DC will operate inside a vacuum chamber. It shall survive under the environmental conditions stated in Table 2 (TBC). The DC requirements shall be fulfilled under the operation conditions.
16 16/20 ESPRESSO Project Lab conditions Vacuum conditions (alignment) (operation) Survival limit Temperature +20 C +17 C +35 C Thermal variation 2 C 1 mk 1 C/h Relative humidity ~40% (controlled) N/A 0% to 100% with condensation Atmospheric pressure ~1 atm ~10-3 mbar (TBC) N/A Table 2. Environmental conditions (TBC) 3.7 Packaging, Handling, Storage and Transportation Requirements Source: EPT Transport obligations The Contractor shall be responsible, in cost and risk, to transport the equipment manufactured from its facilities to the IAC facilities. The package shall be designed to support normal air and sea transport condition. The package shall be also designed to be used for preventive maintenance tasks and in case of reparation. So, the package shall be designed to support at least 10 packing and 10 unpacking operation keeping all its performances Handling and storage requirements The design of the items and packages shall prevent them from being damaged under the conditions shown in tables below. Condition Requirement Altitude 500 m Temperature +15 C to +30 C Relative humidity 0% to 100% with condensation Atmospheric pressure ~ 1atm Gravity orientation All orientations Shock Peak acceleration 10g all axes Table 3. Handling and Storage Conditions at IAC facilities Condition Requirement Altitude 400 m Temperature +20 C ± 3 C Relative humidity 20% to 100% Atmospheric pressure ~720 mbar Gravity orientation All orientations Shock Peak acceleration 10g all axes Table 4. Handling and Storage Conditions at Geneve
17 VLT-SPE-ESP , Issue /20 Condition Requirement Altitude 2600 m Temperature -8 to 25 C Temperature gradient during night -0.4 C/h Relative humidity 5-20% Atmospheric pressure 750 mbar Gravity orientation All orientations Moderate earthquakes (some times per year) Mg < 7.75 Shock Peak acceleration 10g all axes Table 5. Handling and Storage Conditions at Paranal Observatory Chapter 4. Cleanliness Requirements 4.1 Cleanliness Source: EPT DC shall be delivered clean: surface cleanliness (according to MIL-STD-1246). The optical surface shall be able to be cleaned at the surface cleanliness level cited above, without damaging the coating applied. The contractor shall provide a procedure for cleaning the grisms. Chapter 5. Verification at factory Source: EPT Verification shall be accomplished by one or more of the following verification methods: Test (T): When requirements have to be verified by measuring product performance and functionality. The analysis of data derived from test shall be considered an integral part of the test. Demonstration (D): Can be considered as test where qualitative operational performance and requirements are demonstrated. Analysis (A): When verification is achieved by performing theoretical o empirical evaluation by accepted techniques, the method shall be referred to as Analysis. An example is the modelling and computational simulation. Inspection (I): When verification is achieved by visual determination of physical characteristics (such as construction features, hardware conformance to document drawings, etc) the method shall be referred to as Inspection. The Verification Matrix (VM) shows the methods that shall be used to accept each one of the critical requirements. NV means No Verification is needed.
18 18/20 ESPRESSO Project Code Header Ver. Method Remarks 3.1 Functional Requirements I 3.2 Optical Requirements Optical figure T Surface form tolerance of the optical T surfaces Surface shape accuracy T Surface slope error T Surface micro-roughness T Surface Imperfections T Coating T Coating on the DC front face T Coating on the DC rear face T Transition profile T Resistance to cleaning T 3.3 Physical Requirements Clear Aperture T Shape and size T Central thickness T Wedge T Conic bevel finishing I Material T Refractive Index T Bubble classification T Striae grade T Glass homogeneity T Stress birrefringence T 3.4 Mechanical Performance Requirements Long term stability NV 3.5 Reliability Requirement Lifetime guideline NV 3.6 Environmental Requirements T 3.7 Packaging, Handling, Storage and Transportation Requirements Transport obligations I Handling and storage requirements I 4.1 Cleanliness D Table 6. Verification Matrix Information on material properties shall be provided by the glass supplier
19 VLT-SPE-ESP , Issue /20 Appendix A : Descriptive drawing NOTE: Wedge is not indicated in this drawing. It will be explicitly included in final version of the specifications.
20 20/20 ESPRESSO Project Appendix B : Opto-mechanical Concept The optics is hold onto a structural steel frame by 3 points in a kinematic and athermal way. At the same time each frame is fixed by 3 points to the OB in a quasi-kinematic way. Figure 6. Mount concept
Spectrograph Lens Fabrication RFQ 22 Jan, 2003
Spectrograph Lens Fabrication RFQ 22 Jan, 2003 1 Scope of Project This document describes the specifications for the fabrication of 18 optical elements to be used in the Prime Focus Imaging Spectrograph
More informationCORRECTOR LENS FOR THE PRIME FOCUS OF THE WHT
IAC TECHNOLOGY DIVISION DM/SR-WEA/023 AD1. Procurement technical specifications for L4.doc 17 de junio de 2015 PROJECT / DESTINATION: CORRECTOR LENS FOR THE PRIME FOCUS OF THE WHT TITLE: PROCUREMENT TECHNICAL
More informationSection 5 ISO Drawings ISO 10110
Section 5 ISO 10110 Drawings Optical Drawings provide a precise Definition of your optic for fabrication. Standards allow for a common language to be used between you and the optician so there is no confusion
More informationUnderstanding 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 informationAVOIDING TO TRADE SENSITIVITY FOR LINEARITY IN A REAL WORLD WFS
Florence, Italy. Adaptive May 2013 Optics for Extremely Large Telescopes III ISBN: 978-88-908876-0-4 DOI: 10.12839/AO4ELT3.13259 AVOIDING TO TRADE SENSITIVITY FOR LINEARITY IN A REAL WORLD WFS D. Greggio
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 30 LIGHTMACHINERY TEST REPORT LQT 30.11-1 TITLE: HMI Michelson Interferometer Test Report Serial Number 1 - Wideband FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
More informationOptical design of the ESPRESSO spectrograph at VLT
Optical design of the ESPRESSO spectrograph at VLT P. Spanò* a, D. Mégevand b, J.M. Herreros c, F.M. Zerbi a, A. Cabral d, P. Di Marcantonio e, C. Lovis b, S. Cristiani e, R. Rebolo c, N. Santos f, F.
More informationCOS NCM2 Mirror Substrate Specification
Date: Document Number: Revision: Contract No.: NAS5-98043 CDRL No.: N/A Prepared By: E. Wilkinson 2-18-99 E. Wilkinson, COS Instrument Scientist, CU/CASA Date Reviewed By: R. Cahill 2-18-99 R. Cahill,
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 30 LIGHTMACHINERY TEST REPORT LQT 30.11-2 TITLE: HMI Michelson Interferometer Test Report Serial Number 2 - Narrowband FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 34 LIGHTMACHINERY TEST REPORT LQT 30.11-3 TITLE: HMI Michelson Interferometer Test Report Serial Number 3 wide band FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
More informationAlex Lyubarsky OPTI 521 December 8, 2013
Alex Lyubarsky OPTI 521 December 8, 2013 Introduction to Optical Specification Standards (Section 1) Sections 2-13 of ISO 10110 Standard Specification ISO 10110 Drawings Q & A ISO 10110 standard created
More informationPractical 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 informationObservational Astronomy
Observational Astronomy Instruments The telescope- instruments combination forms a tightly coupled system: Telescope = collecting photons and forming an image Instruments = registering and analyzing the
More informationDesign and Manufacture of 8.4 m Primary Mirror Segments and Supports for the GMT
Design and Manufacture of 8.4 m Primary Mirror Segments and Supports for the GMT Introduction The primary mirror for the Giant Magellan telescope is made up an 8.4 meter symmetric central segment surrounded
More informationEE119 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 informationOptical Design of the SuMIRe PFS Spectrograph
Optical Design of the SuMIRe PFS Spectrograph Sandrine Pascal* a, Sébastien Vives a, Robert H. Barkhouser b, James E. Gunn c a Aix Marseille Université - CNRS, LAM (Laboratoire d'astrophysique de Marseille),
More informationCOS FUV Grating Substrate Specification
COS FUV Grating Substrate Specification Date: Document Number: Revision: Contract No.: NAS5-98043 CDRL No.: N/A Prepared By: Reviewed By: Approved By: Approved By: Approved By: E. Wilkinson, COS Instrument
More informationMAORY E-ELT MCAO module project overview
MAORY E-ELT MCAO module project overview Emiliano Diolaiti Istituto Nazionale di Astrofisica Osservatorio Astronomico di Bologna On behalf of the MAORY Consortium AO4ELT3, Firenze, 27-31 May 2013 MAORY
More information2.2 Wavefront Sensor Design. Lauren H. Schatz, Oli Durney, Jared Males
Page: 1 of 8 Lauren H. Schatz, Oli Durney, Jared Males 1 Pyramid Wavefront Sensor Overview The MagAO-X system uses a pyramid wavefront sensor (PWFS) for high order wavefront sensing. The wavefront sensor
More informationEE119 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 informationStatement of Work for the procurement of the Collimator and Camera mirrors of the GTCAO WFC. Gran Telescopio de Canarias, S.A.
OAPs SOW TITLE Statement of Work for the procurement of the Collimator and Camera mirrors of the GTCAO WFC Code : Issue : Date : No. of pages : 8 Gran Telescopio de Canarias, S.A. Instituto de Astrofísica
More informationAn integral eld spectrograph for the 4-m European Solar Telescope
Mem. S.A.It. Vol. 84, 416 c SAIt 2013 Memorie della An integral eld spectrograph for the 4-m European Solar Telescope A. Calcines 1,2, M. Collados 1,2, and R. L. López 1 1 Instituto de Astrofísica de Canarias
More informationGMT Instruments and AO. GMT Science Meeting - March
GMT Instruments and AO GMT Science Meeting - March 2008 1 Instrument Status Scientific priorities have been defined Emphasis on: Wide-field survey science (cosmology) High resolution spectroscopy (abundances,
More informationOptical 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 informationPhysics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:
Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: PID: Signature: CLOSED BOOK. TWO 8 1/2 X 11 SHEET OF NOTES (double sided is allowed), AND SCIENTIFIC POCKET CALCULATOR
More informationDesign parameters Summary
634 Entrance pupil diameter 100-m Entrance pupil location Primary mirror Exit pupil location On M6 Focal ratio 6.03 Plate scale 2.924 mm / arc second (on-axis) Total field of view 10 arc minutes (unvignetted)
More informationCHARA AO Calibration Process
CHARA AO Calibration Process Judit Sturmann CHARA AO Project Overview Phase I. Under way WFS on telescopes used as tip-tilt detector Phase II. Not yet funded WFS and large DM in place of M4 on telescopes
More informationSystem/Prescription Data
System/Prescription Data File : U:\alpi's designs\1.0 Meter\1.0 meter optical design\old Lenses- Design Stuff\LCOGT 1.0meter Telescope Design for UCSB.zmx Title: LCOGT 1.0 Meter Telescope Date : THU NOV
More informationOptimization of coupling between Adaptive Optics and Single Mode Fibers ---
Optimization of coupling between Adaptive Optics and Single Mode Fibers --- Non common path aberrations compensation through dithering K. Saab 1, V. Michau 1, C. Petit 1, N. Vedrenne 1, P. Bério 2, M.
More informationEric B. Burgh University of Wisconsin. 1. Scope
Southern African Large Telescope Prime Focus Imaging Spectrograph Optical Integration and Testing Plan Document Number: SALT-3160BP0001 Revision 5.0 2007 July 3 Eric B. Burgh University of Wisconsin 1.
More informationOptics and photonics Preparation of drawings for optical elements and systems. Part 5: Surface form tolerances
Provläsningsexemplar / Preview INTERNATIONAL STANDARD ISO 10110-5 Third edition 2015-08-01 Optics and photonics Preparation of drawings for optical elements and systems Part 5: Surface form tolerances
More informationThe optical design of X-Shooter for the VLT
The optical design of X-Shooter for the VLT P. Spanò *a,b, B. Delabre c, A. Norup Sørensen d, F. Rigal e, A. de Ugarte Postigo f, R. Mazzoleni c, G. Sacco b, P. Conconi a, V. De Caprio a, N. Michaelsen
More information4DAD, a device to align angularly and laterally a high power laser using a conventional sighting telescope as metrology
4DAD, a device to align angularly and laterally a high power laser using a conventional sighting telescope as metrology Christophe DUPUY, Thomas PFROMMER, Domenico BONACCINI CALIA European Southern Observatory,
More informationInverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter
Inverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter OATo Technical Report Nr. 119 Date 19-05-2009 by: Silvano Fineschi Release Date Sheet: 1 of 1 REV/ VER LEVEL DOCUMENT CHANGE RECORD DESCRIPTION
More informationHigh Resolution Optical Spectroscopy in the ELT Era. Cynthia S. Froning University of Texas at Austin May 25, 2016
High Resolution Optical Spectroscopy in the ELT Era Cynthia S. Froning University of Texas at Austin May 25, 2016 Background Feasibility studies in 2005-2006: UC Santa Cruz, U. Colorado Not selected as
More informationDifrotec Product & Services. Ultra high accuracy interferometry & custom optical solutions
Difrotec Product & Services Ultra high accuracy interferometry & custom optical solutions Content 1. Overview 2. Interferometer D7 3. Benefits 4. Measurements 5. Specifications 6. Applications 7. Cases
More informationChapter 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!!! DELIVERABLE!D60.2!
www.solarnet-east.eu This project is supported by the European Commission s FP7 Capacities Programme for the period April 2013 - March 2017 under the Grant Agreement number 312495. DELIVERABLED60.2 Image
More informationSOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals
Published on SOAR (http://www.ctio.noao.edu/soar) Home > SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals SOAR Integral Field Spectrograph (SIFS): Call for Science Verification
More informationComputer 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 informationUsing 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 informationIMAGE 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
KODAK for use with the KODAK CMOS Image Sensors November 2004 Revision 2 1.1 Introduction Choosing the right lens is a critical aspect of designing an imaging system. Typically the trade off between image
More informationX-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope
X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope Kenichi Ikeda 1, Hideyuki Kotaki 1 ' 2 and Kazuhisa Nakajima 1 ' 2 ' 3 1 Graduate University for Advanced
More informationFigure 1. The Feros ber link (for details cf. text). the bers' entrance-surface diameter resulting in an eective f/4.6 feed which is well-suited to mi
A two-beam two-slice image slicer for ber-linked spectrographs A. Kaufer Landessternwarte Heidelberg, Konigstuhl 12, D-69117 Heidelberg, Germany Abstract. For the Feros ber-linked high-resolution echelle
More informationOctober 7, Peter Cheimets Smithsonian Astrophysical Observatory 60 Garden Street, MS 5 Cambridge, MA Dear Peter:
October 7, 1997 Peter Cheimets Smithsonian Astrophysical Observatory 60 Garden Street, MS 5 Cambridge, MA 02138 Dear Peter: This is the report on all of the HIREX analysis done to date, with corrections
More informationSolution 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 information3.0 Alignment Equipment and Diagnostic Tools:
3.0 Alignment Equipment and Diagnostic Tools: Alignment equipment The alignment telescope and its use The laser autostigmatic cube (LACI) interferometer A pin -- and how to find the center of curvature
More informationThe performance of the CHEOPS On-Ground calibration system
The performance of the CHEOPS On-Ground calibration system B. Chazelas a*, F. P. Wildi a, M. Sarajlic a, M. Sordet a, A. Deline a a University of Geneva, Astonomy dpt., 51 ch. des Maillettes, CH-1290 Sauverny,
More informationSouthern African Large Telescope. Prime Focus Imaging Spectrograph. Polarimetric Optics Design Study
Southern African Large Telescope Prime Focus Imaging Spectrograph Polarimetric Optics Design Study Kenneth Nordsieck University of Wisconsin Revision 1.1 5 Oct 2001 SALT PFIS/IMPALAS Polarimetric Optics
More informationLens 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 informationCollimation Tester Instructions
Description Use shear-plate collimation testers to examine and adjust the collimation of laser light, or to measure the wavefront curvature and divergence/convergence magnitude of large-radius optical
More informationsimulations, tests and production
LIGHT FUNNELS: simulations, tests and production J.A. Aguilar, A. Basili, V. Boccone, A. Christov, M. della Volpe, T. Montaruli, M. Rameez University of Geneva, Switzerland 17/07/2013 alessandro.basili@cern.ch
More informationImage Formation. Light from distant things. Geometrical optics. Pinhole camera. Chapter 36
Light from distant things Chapter 36 We learn about a distant thing from the light it generates or redirects. The lenses in our eyes create images of objects our brains can process. This chapter concerns
More informationSouthern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan
Southern African Large Telescope Prime Focus Imaging Spectrograph Instrument Acceptance Testing Plan Eric B. Burgh University of Wisconsin Document Number: SALT-3160AP0003 Revision 2.2 29 April 2004 1
More informationA fast F-number 10.6-micron interferometer arm for transmitted wavefront measurement of optical domes
A fast F-number 10.6-micron interferometer arm for transmitted wavefront measurement of optical domes Doug S. Peterson, Tom E. Fenton, Teddi A. von Der Ahe * Exotic Electro-Optics, Inc., 36570 Briggs Road,
More informationDepartment of Electrical Engineering and Computer Science
MASSACHUSETTS INSTITUTE of TECHNOLOGY Department of Electrical Engineering and Computer Science 6.161/6637 Practice Quiz 2 Issued X:XXpm 4/XX/2004 Spring Term, 2004 Due X:XX+1:30pm 4/XX/2004 Please utilize
More informationPHYS 3153 Methods of Experimental Physics II O2. Applications of Interferometry
Purpose PHYS 3153 Methods of Experimental Physics II O2. Applications of Interferometry In this experiment, you will study the principles and applications of interferometry. Equipment and components PASCO
More informationA Thermal Compensation System for the gravitational wave detector Virgo
A Thermal Compensation System for the gravitational wave detector Virgo M. Di Paolo Emilio University of L Aquila and INFN Roma Tor Vergata On behalf of the Virgo Collaboration Index: 1) Thermal Lensing
More informationMirrors. Plano and Spherical. Mirrors. Published on II-VI Infrared
Page 1 of 13 Published on II-VI Infrared Plano and Spherical or total reflectors are used in laser cavities as rear reflectors and fold mirrors, and externally as beam benders in beam delivery systems.
More informationCharacteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy
Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy Qiyuan Song (M2) and Aoi Nakamura (B4) Abstracts: We theoretically and experimentally
More informationCascaded holographic spectrographs for astronomical applications
Cascaded holographic spectrographs for astronomical applications advanced modelling and experimental proof Eduard Muslimov Postdoc, group RnD, LAM RnD seminars, September 28 th 2017 Outline of the talk
More informationDevices & Services Company
Devices & Services Company 10290 Monroe Drive, Suite 202 - Dallas, Texas 75229 USA - Tel. 214-902-8337 - Fax 214-902-8303 Web: www.devicesandservices.com Email: sales@devicesandservices.com D&S Technical
More informationUsing 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 informationEE119 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 informationINTERFEROMETER VI-direct
Universal Interferometers for Quality Control Ideal for Production and Quality Control INTERFEROMETER VI-direct Typical Applications Interferometers are an indispensable measurement tool for optical production
More informationDesign of the cryo-optical test of the Planck reflectors
Design of the cryo-optical test of the Planck reflectors S. Roose, A. Cucchiaro & D. de Chambure* Centre Spatial de Liège, Avenue du Pré-Aily, B-4031 Angleur-Liège, Belgium *ESTEC, Planck project, Keplerlaan
More informationCHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT
CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element
More informationBandpass 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 informationMAURO GHIGO & GABRIELE VECCHI. ADONI Firenze,
MAURO GHIGO & GABRIELE VECCHI ADONI Firenze, 13-04-2016 The Polishing brings the workpiece from ground quality to optical quality. ZEEKO POLISHING In traditional optical polishing the tool is forced against
More informationAspheric 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 informationLens 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 informationDesign and test of a high-contrast imaging coronagraph based on two. 50-step transmission filters
Design and test of a high-contrast imaging coronagraph based on two 50-step transmission filters Jiangpei Dou *a,b, Deqing Ren a,b,c, Yongtian Zhu a,b, Xi Zhang a,b,d, Xue Wang a,b,d a. National Astronomical
More informationClassical Optical Solutions
Petzval Lens Enter Petzval, a Hungarian mathematician. To pursue a prize being offered for the development of a wide-field fast lens system he enlisted Hungarian army members seeing a distraction from
More informationAPPLICATION 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 informationPHY 431 Homework Set #5 Due Nov. 20 at the start of class
PHY 431 Homework Set #5 Due Nov. 0 at the start of class 1) Newton s rings (10%) The radius of curvature of the convex surface of a plano-convex lens is 30 cm. The lens is placed with its convex side down
More informationBEAM HALO OBSERVATION BY CORONAGRAPH
BEAM HALO OBSERVATION BY CORONAGRAPH T. Mitsuhashi, KEK, TSUKUBA, Japan Abstract We have developed a coronagraph for the observation of the beam halo surrounding a beam. An opaque disk is set in the beam
More informationAgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%.
Application Note AN004: Fiber Coupling Improvement Introduction AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%. Industrial lasers used for cutting, welding, drilling,
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science
Student Name Date MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.161 Modern Optics Project Laboratory Laboratory Exercise No. 3 Fall 2005 Diffraction
More informationCOS FUV Grating Holographic Recording Specification
COS FUV Grating Holographic Recording Specification Date: Document Number: Revision: Contract No.: NAS5-98043 CDRL No.: N/A Prepared By: E. Wilkinson 11-12-98 E. Wilkinson, COS Instrument Scientist, CU/CASA
More informationECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the
ECEN 4606 Lab 8 Spectroscopy SUMMARY: ROBLEM 1: Pedrotti 3 12-10. In this lab, you will design, build and test an optical spectrum analyzer and use it for both absorption and emission spectroscopy. The
More informationSCHOTT Shaped Fiber Rods
SCHOTT Shaped Fiber Rods Precisely Shaped Illumination for Dental Handpieces Examples of end configurations of shaped fiber rods High transmission and high numerical aperture in combination with excellent
More informationSystems Biology. Optical Train, Köhler Illumination
McGill University Life Sciences Complex Imaging Facility Systems Biology Microscopy Workshop Tuesday December 7 th, 2010 Simple Lenses, Transmitted Light Optical Train, Köhler Illumination What Does a
More informationTutorial 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 informationIndustrial 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 informationOptical 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 informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationContent. Instrumentation Programmes at ESO Mark Casali. Instrumentation at ESO. Future Instrument Programmes
Instrumentation Programmes at ESO Mark Casali Content Instrumentation at ESO Introduction Instruments in Construction Technologies Future Instrument Programmes La Silla Paranal Programme E-ELT programme
More informationOptical 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 informationPractical Flatness Tech Note
Practical Flatness Tech Note Understanding Laser Dichroic Performance BrightLine laser dichroic beamsplitters set a new standard for super-resolution microscopy with λ/10 flatness per inch, P-V. We ll
More informationPotential benefits of freeform optics for the ELT instruments. J. Kosmalski
Potential benefits of freeform optics for the ELT instruments J. Kosmalski Freeform Days, 12-13 th October 2017 Summary Introduction to E-ELT intruments Freeform design for MAORY LGS Free form design for
More informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationExercise 8: Interference and diffraction
Physics 223 Name: Exercise 8: Interference and diffraction 1. In a two-slit Young s interference experiment, the aperture (the mask with the two slits) to screen distance is 2.0 m, and a red light of wavelength
More informationDesign for a new Prime Focus Corrector on the Wyoming InfraRed Observatory (WIRO) 2.3 m Telescope Final Pre-fabrication design of 12 January, 2004
Design for a new Prime Focus Corrector on the Wyoming InfraRed Observatory (WIRO) 2.3 m Telescope Final Pre-fabrication design of 12 January, 2004 PI: Chip Kobulnicky Department of Physics & Astronomy
More informationUV/Optical/IR Astronomy Part 2: Spectroscopy
UV/Optical/IR Astronomy Part 2: Spectroscopy Introduction We now turn to spectroscopy. Much of what you need to know about this is the same as for imaging I ll concentrate on the differences. Slicing the
More informationOptical 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 informationRequirements for Polarizing Grid
Requirements for Polarizing Grid Document: ARO-340570-A-REQ Version A Status: DRAFT Prepared by: Names(s) and Signature(s) Robert W. Freund Date 11-Mar-2005 Approved by: Name and Signature Date Released
More informationThe SIDE dual VIS-NIR fiber fed spectrograph for the 10.4 m Gran Telescopio Canarias
The SIDE dual VIS-NIR fiber fed spectrograph for the 10.4 m Gran Telescopio Canarias O. Rabaza* a, H.W. Epps b, M. Ubierna a, J. Sánchez a, M. Azzaro a, F. Prada a a Institute of Astrophysics of Andalucia
More informationPHYS 160 Astronomy. When analyzing light s behavior in a mirror or lens, it is helpful to use a technique called ray tracing.
Optics Introduction In this lab, we will be exploring several properties of light including diffraction, reflection, geometric optics, and interference. There are two sections to this lab and they may
More informationSouthern African Large Telescope. Prime Focus Imaging Spectrograph. Grating and Filter Specification Document
Southern African Large Telescope Prime Focus Imaging Spectrograph Grating and Filter Specification Document Chip Kobulnicky University of Wisconsin Kenneth Nordsieck University of Wisconsin Revision 2.1
More informationSouthern African Large Telescope. Prime Focus Imaging Spectrograph. Optics Design
Southern African Large Telescope Prime Focus Imaging Spectrograph Optics Design Kenneth Nordsieck University of Wisconsin Revision 1.1 5 Oct 2001 SALT PFIS/IMPALAS Optics Design Oct 5, 2001 i Table of
More information