Smart x-ray optics, focussing in on the next generation of x-ray telescopes Carolyn Atkins a *, Peter Doel a, Samantha Thompson a, Hongchang Wang a and.

Slides:



Advertisements
Similar presentations
Outline Curriculum (5 lectures) Each lecture  45 minutes
Advertisements

Chapter 6: Telescopes – Portals of Discovery. Visible light is only one type of electromagnetic radiation emitted by stars Each type of EM radiation travels.
Geiger-Muller detector and Ionization chamber
Machine Tools And Devices For Special Technologies Plasma machining Slovak University of Technology Faculty of Material Science and Technology in Trnava.
Light and Telescopes Please pick up your assigned transmitter
Introduction Secondary electron secondary electron detector The electron beam interaction with near surface specimen atoms will make a signal which results.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
SEM Magnification Calibration. Magnification Errors Proper calibration of the SEM scans (magnification) is primary to metrology. SEM Magnification requires.
2L 2aL s h T Introduction Zach Frye, University of Wisconsin-Eau Claire Faculty Advisors: Mohamed Elgindi, and John Drost, Department of Mathematics Funded.
Optics and Telescopes Chapter 5 Survey of Astronomy om astro1010-lee.com.
X Ray Astronomy Presented by:- Mohit Shashwat Ankit.
Telescopes (Chapter 6). Based on Chapter 6 This material will be useful for understanding Chapters 7 and 10 on “Our planetary system” and “Jovian planet.
Light and Telescopes Chapter 5. Radio Interferometry The Very Large Array (VLA): 27 dishes are combined to simulate a large dish of 36 km in diameter.
Ways of Seeing X-Rays By Myles Gray & Steve Dwyer.
1 Oxidation Effects on the Optical Constants of Heavy Metals in the Extreme Ultraviolet Amy Grigg R. Steven Turley Brigham Young University.
1 X-Ray Photoelectron Molecular By Amy Baker R. Steven Turley, David Allred, Matt Linford, Yi Lang, BYU Thin Special Thanks to R. Steven Turley, David.
Generation-X telescope: Measurement of On-Orbit Adjustment Data Dan Schwartz, R. J. Brissenden, M. Elvis, G. Fabbiano, T. Gaetz, D. Jerius, M. Juda, P.
Telescopes and Astronomical Instruments The 2 main points of telescopes are 1)To make images with as much angular information as possible 2)To gather as.
SWCX and the production of X-rays SWCX produces X-rays when heavy ions in the solar wind interact with neutrals in the Earth’s exosphere, cometary nebulae,
Optics and Telescopes Chapter Six.
Ch 25 1 Chapter 25 Optical Instruments © 2006, B.J. Lieb Some figures electronically reproduced by permission of Pearson Education, Inc., Upper Saddle.
GENERATING AND DETECTING OF ULTRASOUND
The X-ray Astronomy Imaging Chain. Pop quiz (1): which of these is the X-ray image?
Electrochemistry Chapter 20.
Unit 1 Physics Detailed Study 3.1 Chapter 10: Astronomy.
Theoretical Analysis of a Nanosensor based on WO 3 coated Carbon Nanotube for Ultra-high Sensitive Breath Acetone Sensing Ming Xia, Advisor: Prof. Xingguo.
Issues with the use of telescopes
Radiation & Telescopes ____________ radiation: Transmission of energy through space without physical connection through varying electric and magnetic fields.
Telescopes and the Atmosphere Our goals for learning How does Earth’s atmosphere affect ground-based observations? Why do we put telescopes into space?
Chapter 23 Mirrors and Lenses.
A diffraction grating with 10,000 lines/cm will exhibit the first order maximum for light of wavelength 510 nm at what angle? (1 nm = 10-9 m) 0.51° 0.62°
Compare refracting and reflecting telescopes. Have you ever bent or slowed down light? How?
Spin-Float production of thin paraboloidal segments in glass Piero Salinari Istituto Nazionale di Astrofisica (INAF) Florence, Italy.
Optics for Wide Field X-ray Imaging
© 2010 Pearson Education, Inc. Chapter 6 Telescopes: Portals of Discovery.
Introduction The traditional method for actuating microengineered structures using PZT has been to use bulk PZT bonded to the structure in question. Work.
Delft University of TechnologyDelft Centre for Mechatronics and Microsystems Introduction Adaptive optics (AO) is a technique to actively sense, estimate.
Telescope Technologies
Survey of the Universe Tom Burbine
1 X-Ray Photoelectron Spectroscopy to Examine Molecular Composition Amy Baker R. Steven Turley Brigham Young University.
Lecture Outlines Astronomy Today 7th Edition Chaisson/McMillan © 2011 Pearson Education, Inc. Chapter 5.
Chapter 6 Telescopes: Portals of Discovery. 6.1 Eyes and Cameras: Everyday Light Sensors Our goals for learning How does your eye form an image? How do.
EUROPEAN EXTREMELY LARGE TELESCOPE WILL HAVE A 40 METER MIRROR AND WILL GATHER 13 TIMES MORE LIGHT THAT THE BEST CURRENT TELESCOPE – IMAGES WILL BE 16.
Introduction to Graphical Hardware Display Technologies
6.3 Telescopes and the Atmosphere 6.4 Eyes and Cameras: Everyday Light Sensors Our goals for learning How does Earth’s atmosphere affect ground-based observations?
X-ray Instruments Development of precision hard X-ray multilayer optics with sub-arcminute performance Optics Assembly Approach Graphite spacers are epoxied.
THE EARTH AS AN OBSERVATORY. Learning Outcomes To understand that the Earth’s atmosphere is transparent to some electromagnetic radiation and opaque to.
TOPIC 2: STRONGER EYES. Telescopes Telescopes allow us to see objects that are very distant in space. Optical Telescopes Lippershey made one of the first.
1 Development of Light Weight Replicated Integral Optics: An Innovative Approach Suzanne Romaine (SAO) R. Bruni, P. Gorenstein, R. Rosati (SAO) B. Ramsey.
“Adaptive optics is the most revolutionary technological breakthrough in astronomy since Galileo pointed his telescope skyward to explore the heavens 400.
Silicon Optics for Wide Field X-ray Imaging Dick Willingale et al. – SPIE August 2013 Silicon Optics for Wide Field X-ray Imaging Dick Willingale University.
Telescopes Lecture. Standards Understand how knowledge about the universe comes from evidence collected from advanced technology (e.g., telescopes, satellites,
1 Earth’s Atmosphere & Telescopes Whether light is absorbed by the atmosphere or not depends greatly on its wavelength. Earth’s atmosphere can absorb certain.
Telescopes Mr. Hibbetts Special thanks to Dr. Dan Bruton, Astronomy and Physics SFA.
14FEB2005/KWCAE2-UsersGroup Astro-E2 X-Ray Telescopes XRT Setup & Structure Performance Characteristics –Effective Area –Angular Resolution –Optical Axes.
Electroplating By: Matthew Nerhing. What is Electroplating? Electroplating- It is the deposition of a thin layer of metal on a surface by an electrical.
P. Friedrich, H. Bräuninger Extrapolation of the electroforming replication technique as it has been successfully applied to the XMM-Newton mirror systems.
Workshop on X-Ray Mission Concepts Brian Ramsey 1, Kiranmayee Kilaru 2, Carolyn Atkins 3, Mikhail V. Gubarev 1, Jessica A. Gaskin 1, Steve O’Dell 1, Martin.
Zhanshan Wang Institute of Precision Optical Engineering (IPOE) School of Physics Science and Engineering Tongji University, Shanghai , China Soft.
Before, you learned Objects in the universe are grouped together in different ways The motions of planets and other nearby objects are visible from Earth.
B.V.M. Engineering College MSM Level of structure & Structure Property correlationship : Adodariya Shyam : Amit Chaudhary
THE NUCLEAR MODEL OF THE ATOM. Lesson Objectives Distinguish between the three main subatomic particles. Understand the contributions of J. J. Thomson,
Optical configuration and optical tests of the HartRAO Lunar Laser Ranger N. Nkosi 1, 2, L. Combrinck 1, 2, M. Akombelwa 2 1. Hartebeesthoek Radio Astronomy.
Conclusion An ACF bonding system dedicated for curved substrates has been set up and bonding of polyimide flexcable to curved glass has been successfully.
Chapter 6 Telescopes: Portals of Discovery
Vladimer Chavchanidze Institute of Cybernetics
6.3 Telescopes and the Atmosphere
IR Telescopes Need relatively large objectives for reasonable resolution at infrared wavelengths. Need cooling to reduce thermal background “noise”
Chandra X-ray Observatory
Telescopes Lecture.
Presentation transcript:

Smart x-ray optics, focussing in on the next generation of x-ray telescopes Carolyn Atkins a *, Peter Doel a, Samantha Thompson a, Hongchang Wang a and David Brooks a a Department of Physics and Astronomy, University College London, Gower Street, London, WC1E 6BT, UK Collaborators logos Introduction The Smart X-ray Optics (SXO) Project is a UK based consortium consisting of several institutions investigating the application of adaptive optics to both large scale (telescopes) and small scale (microscopes) x-ray optics. Work is presented regarding the large scale optics; it is hoped that via the combination of two current astronomical optic techniques that the resolution can be improved from 0.5 arc seconds to 0.1 arc seconds. Figure 1 shows the development of x-ray telescopes through the past decades and how the resolution of an image has improved from 4 arc seconds to 0.5 arc seconds, our work is hoping to improve this even further. Acknowledgements This work has been funded by a Basic Technologies Grant from the UK Engineering and Physical Sciences Research Council (EPSRC). The author appreciates the help and advice offered by the SXO consortium, and would like to thank EPSRC for her PhD studentship. Status Update and Future Work Currently the SXO project is investigating and testing the production of the nickel shells, one problem with electroforming is attaining an even deposition as nickel ions favour the edges of the mould and therefore creating a stiffer overall shell. This problem is being researched and it is hoped that a satisfactory solution will be found. The support structure is currently in production and this will prove invaluable in the initial testing of the optic. X-ray Telescopes The first x-ray telescopes were launched in the 1970’s and the basic theory remains the same today, all x-ray telescopes are space borne, as x-rays from space do not penetrate the Earth’s atmosphere. An x-ray telescope works on the principle of external reflection, essentially an x-ray is ‘bounced’ off a mirror surface, very much like a bullet ricocheting off a wall. The telescope consists of two sets of nested cylinders, where the x-rays reflect twice before coming to a focus (Figure 2). The cylinders are nested to increase the surface area seen by the x-rays, they are also coated in a heavy element metal like: gold, iridium, platinum or nickel, to ensure that the x-ray reflection can occur. Crab Nebula Chandra Adaptive Optics These sophisticated optics correct a ground based telescope image for the distortions caused by the Earth’s atmosphere, these distortions are the same as those that cause stars in the night sky to appear to twinkle. Removing the affect of the atmosphere vastly increases the resolution and therefore the quality of the image, as shown in Figure 3. Adaptive optics work by having a deformable mirror and by constantly monitoring the atmosphere, the mirror is actively deformed to correct for the atmosphere at any particular point in time. Smart X-ray Optics: Prototype Design The SXO project is combining both the classical x-ray telescope design with the theory of adaptive optics, with the goal of achieving a resolution of 0.1 arc seconds. A prototype will be produced consisting of a segment of cylindrical shell, on the back of which will be bonded a series of piezoelectric actuators. A piezoelectric material is one that changes shape in an electric field. The prototype will be tested in the x-ray beam facility at The University of Leicester. The proposed final prototype is based on an elliptical segment that is capable of focussing of an x-ray beam. However prior to that a second prototype has been designed to allow various production methods to be investigated. The second prototype is a cylindrical segment (length 200mm, width 100mm, radius of curvature 154mm, thickness 1mm), Figure 4a displays the design for the cylindrical prototype mould. Prototype Manufacture Following the same production methods as previous x-ray telescopes, the process of shell replication will be used, replication is a process by which several shells can be made from a single mould (Figure 4b). The mould is submerged in an electroforming bath (Figure 4c) where a nickel layer will be deposited. The solution of the bath is made up of positive nickel ions, these ions become attracted to the surface of the mould when a electric field is present, as under these conditions the mould becomes negatively charged. When the nickel ions come into contact with the mould they gain two electrons and become neutral nickel atoms. Once the required deposition thickness has been attained the mould is removed from the bath and the pure nickel shell removed. The actuators will be bonded to the back of the nickel shell using a low shrinkage glue to ensure that distortions caused by the glue shrinking will be kept to a minimum. The actuators will be wired to a drive system, which will control the voltage output of each of the actuators and therefore the final resolution capable of the optic. Testing and Support Structure The x-ray beam facility consists of a long tube, approximately 29m in length, at one end is situated an x-ray point source and at the other end a detector. It is intended that the prototype will be situated approximately 4m from the detector. A support structure was designed to ensure that distortions due to gravity would be kept to a minimum. Figure 5 shows the proposed aluminium support structure and on top of two foam strips the prototype will be placed. Figure 6 highlights the effect due to gravity experienced by the prototype. Figure 2: a) The incoming x-rays reflecting off the mirror’s surface and coming to a focus, b) the form of the x-ray mirrors. (a) (b) Figure 3a: The Cat’s Eye Nebula taken by the Palomar Telescope with no adaptive optics present (courtesy of The Institute of Astronomy Cambridge) Figure 3b: The Cat’s Eye Nebula taken by the Palomar Telescope using adaptive optics (courtesy of The Institute of Astronomy Cambridge) Figure 5: The aluminium support structure Figure 6: The prototype resting on the support structure under the effect of gravity Red indicates a downward displacement of 2 x m Blue indicates a downward displacement of 5 x m Figure 1: The Crab Nebula as imaged by three different x-ray telescopes, a) The Einstein Observatory (courtesy of NASA), b) ROSAT (courtesy of S. L. Snowden USRA, NASA/GSFC) and c) Chandra (courtesy of NASA/CXC/SAO) Resolution 4 arc secondsResolution 3 arc secondsResolution 0.5 arc seconds Chandra X-ray Observatory (a)(b)(c) (a) (b) (c) Figure 4a: The cylindrical prototype mould showing dimensions, the material of the mould is stainless steel and it is polished to a high surface quality. Figure 4b: The finished cylindrical mould, only the curved surface of the mould will be used for nickel deposition. Figure 4c: The electroforming bath (0.6 x 0.6 x 0.6 m³), the mould will be suspended in the solution from the central brass bar facing the anode that supplies the positive nickel ions. central brass bar anode