Hyperspectral imaging of aurora and airglow at KHO Fred Sigernes 1,*, Yuriy Ivanov 2, Sergey Chernouss 3, Trond Trondsen 4, Alexey Roldugin 3, Yury Fedorenko.

Slides:



Advertisements
Similar presentations
THE AURORAL EMISSIONS AND THE ELECTRON PRECIPITATION UNDER DIFFERENT GEOMAGNETIC CONDITIONS DURING RECURRENT SOLAR WIND STREAM Guineva V. 1, Despirak I.
Advertisements

1 ATST Imager and Slit Viewer Optics Ming Liang. 2 Optical layout of the telescope, relay optics, beam reducer and imager. Optical Layouts.
Copyright © 2009 Pearson Education, Inc. Chapter 35 Diffraction and Polarization.
Chapter 35 Diffraction and Polarization
Status of the Kjell Henriksen Observatory (KHO) auroral forecast service F. Sigernes 1, S. E. Holmen 1, M. Dyrland 1, A. L. Bækken 2, P. Brekke 3, S. Chernouss.
Motivation Spectroscopy is most important analysis tool in all natural sciences Astrophysics, chemical/material sciences, biomedicine, geophysics,… Industry.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
1 Laser Beam Coherence Purpose: To determine the frequency separation between the axial modes of a He-Ne Laser All sources of light, including lasers,
Currently: 3 year ( ) NSF-supported UF/IAP collaborative project "Methods and Instruments for High-Precision Characterization of LIGO Optical Components"
SECCI/COR2 Status Report SECCHI CONSORTIUM MEETING D. Socker, S. Plunkett, A. Vourlidas.
An Introduction to mini-SONG Project Xiaojun Jiang Natioanl Astronomical Observatories Chinese Academy of Sciences.
Light & Optics: Making a Telescope Dr Lisa Jardine-Wright.
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,
Extracting the Mystery from the Red Rectangle Meghan Canning, Zoran Ninkov, and Robert Slawson Chester Carlson Center for Imaging Science Rochester Institute.
Astronomical Spectroscopy
Ch 25 1 Chapter 25 Optical Instruments © 2006, B.J. Lieb Some figures electronically reproduced by permission of Pearson Education, Inc., Upper Saddle.
The Camera Chapter 4.
1 The University Centre in Svalbard (UNIS), N-9171 Longyearbyen, Norway 2 The Norwegian Polar Institute, Ny-Ålesund, Norway 3 Norwegian Institute of Fisheries.
Near Infrared Tunable Filter System for ATST Big Bear Solar Observatory & Solar Research Center, NJIT Aug. 25, 2003.
1 The University Centre in Svalbard (UNIS), N-9171 Longyearbyen, Norway 2 Magnetosphere Ionosphere Research Lab, University of New Hampshire, USA 3 Keo.
Astronomical Instrumentation Often, astronomers use additional optics between the telescope optics and their detectors. This is called the instrumentation.
Chapter 6: The Tools of the Astronomer. Telescopes come in two general types Refractors use lenses to bend the light to a focus Reflectors use mirrors.
Diffraction: single slit How can we explain the pattern from light going through a single slit? w screen L x.
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley Reflected image Draw one ray from the object that enters the eye after reflecting.
LSC meeting, HLO, August 18, 2004 IAP/UF/LIGO Research Collaboration: Status and Prospectives Efim Khazanov, Ilya Kozhevatov, Anatoly Malshakov, Oleg Palashov,
The Kjell Henriksen Observatory (KHO) Fred Sigernes, Lisa Baddeley, Dag Lorentzen, Margit Dyrland, Silje Eriksen Holmen, Xiangcai Chen, Pål.
The Hard X-ray Modulation Telescope Mission
Astronomy & Astrophysics Advisory Committee (AAAC) May 11, 2006 Vladimir Papitashvili Antarctic Sciences Section Office of Polar Programs National Science.
© 2004 Pearson Education Inc., publishing as Addison-Wesley Telescopes.
PHYS 252 / 2021 PHYS 252 & PHYS 202 Polarization Scattering Absorption.
14 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
High Resolution Echelle Spectrograph for Chinese Weihai 1m Telescope. Leiwang, Yongtian Zhu, Zhongwen Hu Nanjing institute of Astronomical Optics Technology.
Astrophotography The Basics. Image Capture Devices Digital Compact cameras Webcams Digital SLR cameras Astronomical CCD cameras.
18 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
Optical Aeronomy Calibration Facility CEDAR WORKSHOP JUNE, 2007 Jeff Baumgardner, Center for Space Physics Boston University.
EoI#118 Auroral Optical Network International Network for Auroral Optical Studies of the Polar Ionosphere Ingrid Sandahl Swedish Institute of Space Physics,
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
NCKU UCB Tohoku ISUAL / ROCSAT-2 August 2001 Sprites observation by ISUAL on the ROCSAT-2 satellite J. L. Chern, R. R. Hsu, H. T. Su, A. B. Chen, and L.
Calibration of the Polarization Property of SOT K.Ichimoto, Y.Suematsu, T.Shimizu, Y.Katsukawa, M.Noguchi, M.Nakagiri, M.Miyashita, S.Tsuneta (National.
SITE PARAMETERS RELEVANT FOR HIGH RESOLUTION IMAGING Marc Sarazin European Southern Observatory.
1 Optical observations of asteroids – and the same for space debris… Dr. D. Koschny European Space Agency Chair of Astronautics, TU Munich Stardust school.
Telescopes. Light Hitting a Telescope Mirror huge mirror near a star * * * small mirror far from 2 stars In the second case (reality), light rays from.
Multi-colour sctintillator-based ion beam profiler James Green, Oliver Ettlinger, David Neely (CLF / STFC) 2 nd Ion diagnostic workshop June 7-8 th.
1 Access and Use of Auroral Imaging Data Harald U. Frey Space Sciences Laboratory University of California at Berkeley Credit: D. Hutchinson.
Hyperspectral remote sensing
Sensitivity Calibration of Narrow Field of View Optical Instruments F. Sigernes 1, T. Svenøe 2, J. Holmes 1, M. Dyrland 1, D.A. Lorentzen 1, J. Moen 3,
Student of the Week. Essential Idea:  Resolution places an absolute limit on the extent to which an optical or other system can separate images of.
Telescopes….. Telescopes are helpful to astronomers because they…. Collect more light Separate distant objects…. Magnify the image Detect other wavelengths…
1 Progress of the Thomson Scattering Experiment on HSX K. Zhai, F.S.B. Anderson, D.T. Anderson HSX Plasma Laboratory, UW-Madison Bill Mason PSL, UW-Madison,
The Field Camera Unit Results from technical meeting S. Scuderi INAF – Catania.
ISUAL Design Concept S. Mende. SDR 7 Jun NCKU UCB Tohoku ISUAL Design Concept S. Mende Sprite Example Sprite Image obtained by Berkeley/NCKU 1999.
Auto-stereoscopic Light-Field Display By: Jesus Caban George Landon.
F. Pepe Observatoire de Genève Optical astronomical spectroscopy at the VLT (Part 2)
Spectrometer The instrument used for the astronomers MinGyu Kim
Astronomical Spectroscopic Techniques. Contents 1.Optics (1): Stops, Pupils, Field Optics and Cameras 2.Basic Electromagnetics –Math –Maxwell's equations.
LSC meeting, Hanford, 2002 LIGO-G Z Remote in situ monitoring of weak distortions Ilya Kozhevatov, Efim Khazanov, Anatoly Poteomkin, Anatoly Mal’shakov,
Solid-state Laser Crystal and Device Laboratory Yen-Yin Li Speaker : Yen-Yin Li Adviser : Sheng-Lung Huang Topic Report Graduate Institute of Photonics.
ANGWIN, Cambridge, 2016 Space physics research infrastructure at Svalbard, Norway D. A. Lorentzen (1,2), L. J. Baddeley (1,2) (1) Birkeland Centre for.
Astronomical Spectroscopic Techniques
Optical Non-Invasive Approaches to Diagnosis of Skin Diseases
F. Sigernes 1,2,3 1 The University Centre in Svalbard (UNIS), N-9171 Longyearbyen, Norway 2 The Birkeland Centre for Space Science (BCSS) 3 The Kjell Henriksen.
LOW COST HYPERSPECTRAL
UiO Allsky Imagers Imagers equivalent to Keo Sentry 3i/TEC from Keo Scientific LTD Fast 3-inch telecentric all-sky optics, 180 deg FoV 5 position temperature.
BASIC HYPER SPECTRAL IMAGING
What Is Spectral Imaging? An Introduction
BASIC HYPER SPECTRAL IMAGING
Optical Non-Invasive Approaches to Diagnosis of Skin Diseases
BASIC HYPER SPECTRAL IMAGING
BASIC HYPER SPECTRAL IMAGING
Meeting 11 Polarimetry: Beamsplitter; data formats Ken Nordsieck
Presentation transcript:

Hyperspectral imaging of aurora and airglow at KHO Fred Sigernes 1,*, Yuriy Ivanov 2, Sergey Chernouss 3, Trond Trondsen 4, Alexey Roldugin 3, Yury Fedorenko 3, Boris Kozelov 3, Andrey Kirillov 3, Ilia Kornilov 3, Vladimir Safargaleev 3, Silje Holmen 1, Margit Dyrland 1, Dag Lorentzen 1 and Lisa Baddeley 1 1 The University Centre in Svalbard (UNIS), N-9171 Longyearbyen, Norway 2 Main Astronomical Observatory, National Academy of Sciences, Ukraine 3 Polar Geophysical Institute, Murmansk Region, Apatity, Russia 4 Keo Scientific Ltd., Calgary, Alberta, Canada MLTI Waves and Dynamics at Polar Latitudes Workshop, Utah State University, 9-11 October 2012

THE KJELL HENRIKSEN OBSERVATORY – KHO Prof. Dr 2 K. Henriksen KHO 1) Instrumental module (30x) 2) Service Section 3) Platform Summer view Location More info at:

KHO TELESCOPE IN ADDITION a)Magnetometers b)Scintillation receivers (GPS) c)Riometer d)Weather station e)Web cameras

KHO 1.University Centre in Svalbard 2.University of Oslo 3.University of Tromsø 4.University of Alaska, Fairbanks 5.University College London 6.University of Wales Aberystwyth 7.University of Southampton 8.University of New Hampshire 9.Augsburg College 10.Tohoku University 11.National Institute of Polar Research Japan 12. Finnish Meteorological Institute 13.Embry Riddle Aeronautical University 14.Danish Meteorological Institute * 15.Air Force Research Laboratory * 16.Laboratoire de Planétologie de Grenoble 17.Institute of Radio Astronomy 18.AVINOR 19.The Polar Institute of China 20.The University of Electro-Communications Tokyo The 10 KHO … & excellent students!

LYR INTERNET KHO - UNIS – ARS - MINE 7

HYPERSPECTRAL IMAGING AT KHO Picture of the assembled Spextube Imagers. M is rotary table, T front surface mirror, L1 front lens, A 35mm camera lens adapter, O laser pointer, B barrel contains spectroscope, L3 camera lens, CCD camera head, I lift table, and E two steel bars. Inspired by SP3 (1993). Fiskeriforskning (1997) The FishTube spectrograph

1th Samples

(a)Airspex 1 Imager (b)(b) video camera (c)(c) tripod (d)(d) dome Airspex 2 Imager – Swedish version! AGF331 Remote Sensing and Advanced Spectroscopy ( ) The Oriel FICS spectral imager Experimental setup Dornier Dronespex I-IV

Samples

Electronic Machine Shops ~14 days Purchase optics and mounts FS-IKEA ? AURORAL LOW LIGHT HYPERSPECTRAL IMAGING?

The NORUSCA All-sky cameras Two NORUSCA II 1st Generation all-sky cameras (A) and (B). (1) Front element of all-sky lens, (2) 24 x 4 inch2 mount plate, (3) collimator lens tube, (4) lens mount, (5) ring holders, (6) filter box, (7) camera lens, and (8) EMCCD detector. Instrumental volume is ~ 65 x 18 x 16 cm3. Total mass is 8.9 kg. NORUSCA II-E fish-eye lens specifications Spectral range 430 – 750 nm Paraxial focal length3.5 mm F-numberf/1.1 Number of lens elements12 Field of view 180 º (circular) Filter diameter35 mm Angle of incident on filter   7 º Dimensions Ø 110 × 320 mm Camera lens mountC-mount EMCCD detector: - PI ProEM 512B x 8.2 mm deg. air cooled - Back-illuminated; 90% QE

Optical layout and design of the NORUSCA II Camera Lens mechanics and optical diagram of the NORUSCA II all-sky lens: (1)focusing mechanism and collimator lenses, (2) filter box - chamber, (2)(3) camera lens, and (4) camera head.

The NORUSCA II Point Spread function Resolution: ~ 60 lp/mm

Filter: Liquid Crystal Tunable Filter (LCTF) (Cambridge Research & Instrumentation, Inc.). *P. J. Miller, “Use of Tunable Liquid Crystal Filters to Link Radiometric and Photometric Standards”, Metrologia 28, 145 – 149 (1991). Spectral tuning is obtained by using electronically controlled liquid crystal wave plates to a Lyot filter design*. The wave plates behave as optical birefringent elements with an electrically variable retardance. Retardance is termed the optical path difference between the ordinary and extraordinary rays passing through a birefringent element. The latter is controllable due the effect that the liquid crystal molecules are orientation sensitive to electric fields applied between the plates. Since the retardance is directly linked to wavelength, the filters are tunable. Our filter: 400–720nm 550nm

System performance 1. Focus tests Crossed scatter plots work best Source: 1 mm diameter 1m

System performance 2. Mapping function Mapping function coefficients NORUSCAII all-sky lens R in units of[PIXELS][mm] A0A A1A A2A Source: -1 mm diameter pinhole -Schott NG9 -Distance = 1m -Rotation in steps of 10 deg. 2nd order polynomial fit: R is for  > 30º in-between the mapping functions of an equal area and an orthographic fisheye lens, and its maximum R max = 4.08 mm at  = 90 º matches the size of the EMCCD. Note:

System performance 3. Spectral characteristics - center pixel! [mW m -2 nm -1 ] [R s CTS -1 ]

System performance 3. Spectral characteristics – auroral emissions Channel # Wavelength [nm] Emission species FWHM [nm] Calibration factor [R s CTS -1 ] N2+N [OI] [OI] N2+N Background HH NII NII NaI [OI] HH N 2 1P(6-3) N 2 1P(5-2) N2N Background The minimum detection threshold signal is assumed to be 3 times the dark noise level, or 3  = 150 CTS/s. For the green [OI] nm emission, the minimum detection limit then becomes 550 R.

First Samples Screen dump of raw data from the camera at 630 nm. View from authors office desk at UNIS. Exposure time 10 ms at gain 40. Composite RGB color image. Red (R) nm, green (G) nm and blue (B) nm. Or …

Samples H Y P E R S P E C T R A L

Raw data January :15:03 UT

Nightside aurora Media 1 Panel (A): Color composite image from the NORUSCA II camera 24th of January 2012 at 15:15 UT. Location is the Kjell Henriksen Observatory (KHO). The Red color component of the image is at center wavelength 630 nm, Green at nm and Blue at nm

Dayside aurora Panel (A): Color composite image from the NORUSCA II camera 29 th of December 2011 at 08:55:00UT. Location is the Kjell Henriksen Observatory (KHO). The Red color component of the image is at center wavelength 630 nm, Green at nm and Blue at nm. Media 2

Concluding remarks (preliminary) NORUSCA II: New hyperspectral all-sky camera (430 – 720 nm). Wavelength element (filter): LCTF with FWHM = nm. Novel C-mount NORUSCA II–E All-sky lens f/value=1.1. Detects ~1/2 kR of auroral emissions in just 1 sec. No moving mechanical parts to swap center wavelength. It uses 50 ms to swap between 41 available center wavelengths. Opens for new processing methods such as classification The major disadvantage of the system is the low transmission of the LCTF, especially in the blue part of the spectrum.

Acknowledgement We wish to thank The Research Council of Norway through the project named: Norwegian and Russian Upper Atmosphere Co-operation On Svalbard part 2 # /S30 (NORUSCA2).