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Published byKristopher Ezra Dixon Modified over 8 years ago
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SMART, Hida and next NAGATA, SHIN’ICHI
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Solar Magnetic Activity Research Telescope (SMART) The telescope was built at the Hida Observatory Kyoto University 2003 (Ueno et al. 2004) Bundle of Four telescopes T1:full disk H-alpha imaging ( 20cm) T2:full disk magnetograph ( 20cm) T3:partial disk H-alpha ( 25cm) T4:partial disk magnetograph( 25cm) Data archive http://www.hida.kyoto-u.ac.jp/SMART/ Project status: H-alpha observations keeps going well. On the other hand, precise vector magnetic field measurements are not realised yet. FeI 630.2nm 2
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SMART Publications Refereed – Nagashima et al. ApJ (2007) – Narukage et al. ApJL (2008) – Asai et al. JGR (2009) Proceedings – UeNo et al. SPIE (2003) – Ishii et al. ASPC (2004) – Nagata et al. ASCP (2004) – Ueno et al. ASPC (2004) – Nagata et al. SPIE (2009) The list is incomplete but the products of 7 years operations is not so large ~0.4 refreed papers /year ~0.7 proceedings papers /year Scientific contribution from core team members is not enough (Nagata, Ueno, PDs). What is the matter? We still have to spend most of our time for instrumentation: (a) Magnetic field measurement system improvement for T4. (b) Automated operations to save our time for science. (Problem 1) (Problem 2)
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SMART Narrow band filters タイプ口径 (mm) 波長 FWHM (mA) 用途現状 Lyot326563+/-2250SMART T1 休止中 Lyot406563+/-2250SMART T1 稼働中(調整中) Lyot506563+/-2250SMART T3 休止中(改修中) Lyot326302+/-2125SMART T2 稼働中 FP(tandem)606302100SMART T4 準備中 FP606302100-125SMART T4 休止中 FP606563150-250SMART T4 休止中 We have a lot of narrow band filters, and the experience, including human resources, with those filters are precious heritage of us for the future missions.
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Lyot Filter
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Fabry-Perot filters 9
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1 2 3 3 4 4 6 8 7 5 9 10 5 TCE specification TCE110 Thickness: 0.427mm FSR: 0.19nm FWHM: 0.0133nm Finess: 14.3 Tilt mechanism: no Pre-filter: installed Clear aperture: 60mm TCE114 Thickness: 0.303mm FSR: 0.27nm FWHM: 0.0172nm Finess: 15.5 Tilt mechanism: installed Pre-filter: no Clear aperture: 60mm 1.Etalon cell 2.Linear actuator for tilting 3.Heater for temperature control 4.Windows x 2 5.Window retaining rings x 2 6.Pre-filter mounting location 7.Pre-filter retaining ring 8.Manual screwdriver tilt adjust 9.High Voltage connectors x 2 10.Control cable connectors x 2
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Distance and optical index are changed by applying voltage Multiple reflection between the two surfaces.
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Fabry-perot filters characterization FWHM(nm)0.0170.013 FSR0.2660.189 Finnese15.514.3 FWHM(nm)0.0190.017 FSR0.260.19 Finnese13.611.2 FWHM ~0.017nm 12 Calibrated at the Domeless Solar Telescope Hida Observatory
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SMART T1 Objective lens collimator lens Narrow band filter Imaging lens CCD Camera
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SMART T2 Objective lens collimator lens Narrow band filter Imaging lens CCD Camera
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SMART T3 Objective lens collimator lens Narrow band filter Imaging lens CCD Camera
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SMART T4 Objective lens Relay Lens Narrow band filter Relay lens CCD Camera
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SMART Lyot Filter problems Damesage on optical element – Some of calcites were broken into pieces due to mechanical stress? Degradation of transmittance – Transmittance degrades along with time mechanical Supperior spatial resolution – Due to wave front errors, spatial resolution is significantly degraged? Observation system – Operation is affected by electro-magnetic noise from other instrument
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The dark features on 50mm H-alpha filter(2009.02.28) 8Aブロックを構成する4枚の方解石のうち3枚が割れているのを 確認。 この4枚を交換した(2010.03)
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Transmittance degradation
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T3 spatial resolution problem example (2007.12.06) T1(32mm) T3(50mm)
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SMART FP Filter issues The filter has not been mounted on the telescope Optical performance verification – Transmittance map across the clear aparture Some of the key parameters to be confirmed : 1.Central wavelength: 630.2 nm 2.FWHM: 0.01 nm 3.Overall Finesse of each etalon based on Reflectance of coatings: ~ 14 4.FWHM stability/variation over the aperture : target < 4.9 % of FWHM 5.Central wavelength stability/variation over the aperture : target < 0.002 nm
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Test configuration He-Ne Laser Spatial filter Collimator lensimaging lensCCD camera (Prosilica GE1650) FP filter
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Test configuration He-Ne 光 Φ0.48mm BS 05-STP-910 Collimator lensImaging lens Fabry-Perot FilterPupil Camera (GE1650-100246) Camera(GE1650-24004) The light through filter Calibration light path Test 4 mirror
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Without FP filterWith FP filter
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“Transmittance” map “transmittance” is observed to be larger tan 100%
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Test configuration He-Ne 光 Φ0.48mm BS 05-STP-910 Collimator lensImaging lens Fabry-Perot FilterPupil Camera (GE1650-100246) Camera(GE1650-24004) The light through filter Calibration light path Test 4 mirror The FP filter works as lens? The FP filter work as wave-plae?
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What is next? Classical three problems in the solar physics. What is the break through for the next? – Solar Flares (Non-thermal particle acceleration) – Solar Coronal heating Chromospheric fields – Solar Dynamo Precise surface velocity field measurement Projects (globalization should be taken into account) – SOLAR-C project with ISAS/JAXA – Ground-based telescopes Hida heritage – Narrow band filters development?
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