14FEB2005/KWCAE2-UsersGroup Astro-E2 X-Ray Telescopes XRT Setup & Structure Performance Characteristics –Effective Area –Angular Resolution –Optical Axes.

Slides:



Advertisements
Similar presentations
SVOM MXT Lobster Eye Telescope Breadboard Model Testing Preliminary Results Dick Willingale Adrian Martindale, Jim Pearson, Charly Feldman, Julian Osborne.
Advertisements

X-Ray Astronomy Lab X-rays Why look for X-rays? –High temperatures –Atomic lines –Non-thermal processes X-ray detectors X-ray telescopes The Lab.
November 20, 2003University of Colorado The Off-Plane Option Study Results Potential Capabilities Webster Cash University of Colorado.
Suzaku XRT Update Kai-Wing Chan, Yoshi Maeda & the XRT Team 3-MAY-2007.
A Narrow Field Lobster Eye Telescope Dick Willingale – AXRO December 2014 A Narrow Field Lobster Eye Telescope (for SVOM and similar) Dick Willingale Adrian.
Computed Tomography II
The HEROES Balloon- borne Hard X-ray Telescope Colleen A. Wilson-Hodge, J. Gaskin, S. Christe, A. Shih, K. Kilaru, D.A. Swartz, A. F. Tennant, B. Ramsey.
I. Parabolic Reflector Lab Background page__. A. Light at Boundaries 1. The Law of Reflection The diagram below illustrates the law of reflection.
Astro-H XRT system H.Awaki (Ehime University) + Astro-H XRT team (Nagoya Univ., NASA/GSFC, ISAS/JAXA, Ehime Univ., Chubu Univ., Osaka City Univ., Nara.
Multilayer Overview Current application Optimization of Multilayers Model Designs for GRI.
Astro-E2 and Japanese future space programs for high energy astrophysics Astro-E2 NeXT XEUS Small satellite programs Tadayasu Dotani (ISAS)
Types of Radiation Interactions All or Nothing Many Small There is a finite probability per unit length that the radiation is absorbed. If not, there is.
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.
Copyright © 2009 Pearson Education, Inc. Chapter 32 Light: Reflection and Refraction.
Wide-field, triple spectrograph with R=5000 for a fast 22 m telescope Roger Angel, Steward Observatory 1 st draft, December 4, 2002 Summary This wide-field,
Fiber Optics Defining Characteristics: Numerical Aperture Spectral Transmission Diameter.
On-Orbit Adjustment Calculation for the Generation-X X-ray mirror Figure D. A. Schwartz, R. J. Brissenden, M. Elvis, G. Fabbiano, D. Jerius, M. Juda, P.
September 19, 2002University of Colorado The Off-Plane Option for the Reflection Grating Spectrometer Webster Cash University of Colorado.
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.
R. M. Bionta SLAC November 14, 2005 UCRL-PRES-XXXXXX LCLS Beam-Based Undulator K Measurements Workshop Use of FEL Off-Axis Zone Plate.
Exploring the Hot Universe with the Coolest Instrument in Orbit Presented by Dr. James Lochner (USRA & NASA/GSFC) Sara Mitchell (SP Systems & NASA/GSFC)
 Design  Manufacturing  Recent X-Ray tests  Status Vadim Burwitz, Peter Friedrich on behalf of the eROSITA team.
Ch. 14 Light and Reflection. Flat Mirrors Simplest mirror Object’s image appears behind the mirror Object’s distance from the mirror is represented as.
Optical characteristics of the EUV spectrometer for the normal-incidence region L. Poletto, G. Tondello Istituto Nazionale per la Fisica della Materia.
Grazing-incidence design and others L. Poletto Istituto Nazionale per la Fisica della Materia (INFM) Department of Electronics and Informatics - Padova.
T. Horn, SHMS Optics Update SHMS Optics Update Tanja Horn Hall C Users Meeting 31 January 2009.
Optical characteristics of the EUV spectrometer (EUS) for SOLO L. Poletto, G. Tondello Istituto Nazionale per la Fisica della Materia (INFM) Department.
SXT Soft X-Ray Telescope Onboard the Yohkoh Satellite SXT.ppt.
Grazing Incidence X-ray Scattering from Patterned Nanoscale Dot Arrays D.S. Eastwood, D. Atkinson, B.K. Tanner and T.P.A. Hase Nanoscale Science and Technology.
X-ray Timing and Polarization mission & instrumentation DONG Yongwei Center for Particle Astrophysics Institute of High Energy Physics, Chinese Academy.
Visual Angle How large an object appears, and how much detail we can see on it, depends on the size of the image it makes on the retina. This, in turns,
GWADW 2010 in Kyoto, May 19, Development for Observation and Reduction of Radiation Pressure Noise T. Mori, S. Ballmer, K. Agatsuma, S. Sakata,
Chapter 23 Light. Chapter Ray Model of Light Light travels in straight lines Ray model of light - light travels in straight line paths called.
Optics for Wide Field X-ray Imaging
The Hard X-ray Modulation Telescope Mission
PACS IIDR 01/02 Mar 2001 FPFPU Alignment1 D. Kampf KAYSER-THREDE.
Laue lenses for hard X-rays (> 60 keV) F. Frontera and A. Pisa on behalf of a Large Collaboration Rome, 18 March 2005.
SPIE Optics for EUV, X-Ray, and Gamma-Ray Astronomy VI
PHYSICS DEPARTMENT.
K-D-PR Fabrication and testing of KGMT FSM prototype Oct Ho-Soon Yang, Hak-Yong Kihm, Il-Kwon Moon, Jae-Bong Song, Yun-Woo Lee Korea.
Optical Subsystem Roy Esplin Dave McLain. Internal Optics Bench Subassembly 2 Gut Ray Dichroic Beamsplitter (MWIR reflected, LWIR transmitted) LWIR Lens.
LHC Phase II Collimator Compact jaw simulations New FLUKA => ANSYS mapping scheme New 136mm x 950mm jaw –60cm primary collimator –Helical cooling channel.
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
X-ray Instruments Development of precision hard X-ray multilayer optics with sub-arcminute performance Optics Assembly Approach Graphite spacers are epoxied.
1 Development of Light Weight Replicated Integral Optics: An Innovative Approach Suzanne Romaine (SAO) R. Bruni, P. Gorenstein, R. Rosati (SAO) B. Ramsey.
Apr 17-22, NAOJ External alignment with X-Ray Telescope (XRT) and EUV Imaging Spectrometer (EIS) Y. Katsukawa (NAOJ) and SOT team.
Light Reflection and Mirrors.  The Law of Reflection  When a wave traveling in two dimensions encounters a barrier, the angle of incidence is equal.
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.
Image at:
Optical characteristics of the EUV spectrometer for the grazing-incidence region L. Poletto, G. Tondello Istituto Nazionale per la Fisica della Materia.
Solar orbiter_______________________________________________.
“The SIMBOL-X optics”, Bologna, 14 May 2007 SIMBOL-X SIMBOL-X OPTICS SIMBOL-X OPTICS Giovanni Pareschi INAF - Osservatorio Astronomico di Brera Lower Spider.
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.
MPI Semiconductor Laboratory, The XEUS Instrument Working Group, PNSensor The X-ray Evolving-Universe Spectroscopy (XEUS) mission is under study by the.
Jason Koglin, SPIE, August 2002 Development and production of hard X-ray multilayer optics for HEFT Caltech Space Radiation Laboratory Hubert Chen, Fiona.
PACS IIDR 01/02 Mar 2001 Optical System Design1 N. Geis MPE.
Zhanshan Wang Institute of Precision Optical Engineering (IPOE) School of Physics Science and Engineering Tongji University, Shanghai , China Soft.
Copyright © 2009 Pearson Education, Inc. Chapter 35-Diffraction.
Zhanshan Wang, Zhenxiang Shen, Qiushi Huang, ZhongZhang, Bin Ma Institute of Precision Optics and Engineering (IPOE), Tongji University Institute of Precision.
Date of download: 6/28/2016 The Association for Research in Vision and Ophthalmology Copyright © All rights reserved. From: A Novel, Real-Time, In.
Development of Micro-Pore Optics at NAOC MPO research group X-ray Imaging Laboratory, NAOC Presented by Chen Zhang.
1 Radiation Environment at Final Optics of HAPL Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI HAPL Meeting ORNL March.
Phys102 Lecture 26, 27, 28 Diffraction of Light Key Points Diffraction by a Single Slit Diffraction in the Double-Slit Experiment Limits of Resolution.
Chapter 35-Diffraction Chapter 35 opener. Parallel coherent light from a laser, which acts as nearly a point source, illuminates these shears. Instead.
Wave Optics Chapter 27.
Observational Astronomy
Chapter 35-Diffraction Chapter 35 opener. Parallel coherent light from a laser, which acts as nearly a point source, illuminates these shears. Instead.
XRT Performance Update
Hall C Users Meeting 31 January 2009
Optics Alan Title, HMI-LMSAL Lead,
Presentation transcript:

14FEB2005/KWCAE2-UsersGroup Astro-E2 X-Ray Telescopes XRT Setup & Structure Performance Characteristics –Effective Area –Angular Resolution –Optical Axes –Field of View

14FEB2005/KWCAE2-UsersGroup XRT Set up 5 XRT’s on extended bench –4 on imagers with f=4.75m –1 on spectrometer with f=4.50m Same external dimension for XRT-I & XRT-S –~ 40 cm diameter, ~25 cm height

14FEB2005/KWCAE2-UsersGroup Structure Optic –Reflective optics –Grazing incidence –Conical approximation to Wolter type I –2 reflections in 2 stages –Collimation 1 stage –Gold surface –Nested shells of segmented “cylinder” Angle of incidence (on-axis) varies from inner (smaller) to outer (larger) spectral response: Critical angle ~ 1/E

14FEB2005/KWCAE2-UsersGroup Geometry and Mechanics –Segmented circular elements –Reflectors positioned in slots –(Almost) all constructed out of Al –Sandwiched elements: Gold surface / epoxy adhesion layer / aluminum substrate Thermal properties –Operational T: 20 +/- 7.5 C –Sun shields –Heating elements –Thermal Shields Quadrant construction: 4- fold symmetry in image Sandwiched structure: dependence on temperature from CTE mismatch On ground, slight resolution dependence on orientation: displacement & gravity sag

14FEB2005/KWCAE2-UsersGroup Astro-E2 XRT-IAstro-E2 XRT-SASCA Number of telescope 414 Focal length 4.75 m4.5 m3.5 m Inner Diameter 118 mm119 mm120 mm Outer Diameter 399 mm400 mm345 mm Height 279 mm Mass/Telescope 19.5 kg18.5 kg9.8 kg Number of nested shells Reflectors/Telescope Geometric area/Telescope 873 cm cm cm 2 Reflecting surface Gold Substrate material Aluminum Substrate thickness 155  m 127  m Reflector slant height mm Basic parameters of XRT

14FEB2005/KWCAE2-UsersGroup XRT Characterization from ISAS Measurements ISAS 30 m pencil beam ISAS pencil beam Full illumination Data from JAXA/ISAS Y.Maeda

14FEB2005/KWCAE2-UsersGroup Full XRT Images I0 I1I2 I3S

14FEB2005/KWCAE2-UsersGroup Effective Area Full Telescope Effective Area at 4.51 keV: XRT-I: I0-I3: 340 / 334 / 331 / 335 cm 2 XRT-I average 335 cm 2 XRT-S: 332 cm 2 X-ray W D C U (Configuration) ~ 4% up from E1 ~ 9% down from E1

14FEB2005/KWCAE2-UsersGroup Effective Areas Rough numbers, for each XRT –~ 450 cm 2 at 1.5 keV –~ 335 cm 2 at 4.5 keV –~ 245 cm 2 at 8.0 keV (smaller ~ 90% for XRT-S at higher E) –~ 175 cm 2 at 9.4 keV Au M edge at ~ 2 keV Efficiency slight improved (a few %) from Astro-E1 For XRT-S, difference is mainly due to Pt  Au –Especially at higher energy due to larger critical angle of Pt

14FEB2005/KWCAE2-UsersGroup Point Spread and Encircled Energy Functions Angular Resolution

14FEB2005/KWCAE2-UsersGroup Angular Resolution: HPD

14FEB2005/KWCAE2-UsersGroup Angular Resolution Measured with Half-Power Diameter from Encircled Energy Function No dependence of angular resolution on energy –Indirect energy dependence on radial position of responsible reflectors –Errors in angular resolution (axial figure errors, positioning errors, etc.) are largely radius independent HPD ~1.8’ –Focal length errors absorbed Sharp core: inner r ~ 0.1’: sharply rising (~ linear) EEF ; no flat PSD (c.f. ASCA mirrors) 90% encircled power within 4’ diameter

14FEB2005/KWCAE2-UsersGroup Focal Lengths & Orientation Dependence Focal Length variation – as large as 50 mm – all errors due to focal length deviation are absorbed (measurement done at nominal f) Dependence on orientation Hope (optimistic) that resolution will be better in space: – no displacement – no gravity sag

14FEB2005/KWCAE2-UsersGroup Optical Axes

14FEB2005/KWCAE2-UsersGroup Optical Axis Optical axes defined as the direction of maximum output –Not the bore sites (which are well sub-arc- minutes) Optical axes of quadrants are located within +/-1 arcmin from the nominal telescope axes Do not contribute to angular resolution (double reflection) Lower throughput by <~5% at 1 arc minute

14FEB2005/KWCAE2-UsersGroup Field of View X-ray W D C U Q3 (Configuration)  F.O.V. (FWHM) 0’ 45’ 90’ Al-K Ti-K Cu-K Pt-L (arcmin.) (XRT-I) FOV of full XRT at 4.51 keV

14FEB2005/KWCAE2-UsersGroup Field of View Collimator limits stray light, but not significantly restricts the aperture Full XRT Field of View ~ 20’ at 4.5 keV Energy dependence via radial dependence of responsible reflectors –Smaller FOV for higher energy x-ray (smaller critical angle of reflection)

14FEB2005/KWCAE2-UsersGroup Parameters for the Pre-collimator XRT-IXRT-S Number of Collimators41 Height32 mm Blade substrateAluminum Blade Thickness 120  m Blade Height22 mm Height from Blade Top to Reflector Top30 mm Number of nested shells Blade/Telescope Mass/Collimator2.7 kg

14FEB2005/KWCAE2-UsersGroup Satellite Alignment