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Very Large Space Optics for an Very Large Space Optics for an Investigation of the Extreme Universe Presented by Jim Adams for the Super EUSO Collaboration* for the Super EUSO Collaboration *Eberhard Karls Universität Tübingen; MPI für Physik, München; Universidad de Alcalá; APC (France); Swedish Institute of Space Physics; LIP (Portugal); Università di Genova; INAF (Palermo Italy); Physics; LIP (Portugal); Università di Genova; INAF (Palermo, Italy); INFN and INOA, (Florence, Italy); Università di Roma Tor Vergata; Università di Perugia; Observatoire de Neuchâtel; Skobeltsyn Institute; UNAM, Mexico; RIKEN, Japan; Univ, of Ala., Huntsville; Vanderbilt Univ ; Sp Sci Lab UCB; UCLA; Univ of Utah; NASA 8/25/08 1 Vanderbilt Univ.; Sp. Sci. Lab., UCB; UCLA; Univ. of Utah; NASA- MSFC and NASA-GSFC https://ntrs.nasa.gov/search.jsp?R=20090002566 2018-07-11T17:43:42+00:00Z

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Page 1: Very Large Space Optics for anVery Large Space Optics for ... · Very Large Space Optics for anVery Large Space Optics for an ... •Free Flyer Variable orbit ... PRESENTATION.ppt

Very Large Space Optics for anVery Large Space Optics for an Investigation of the Extreme

Universe

Presented by Jim Adams for the Super EUSO Collaboration*for the Super EUSO Collaboration

*Eberhard Karls Universität Tübingen; MPI für Physik, München; Universidad de Alcalá; APC (France); Swedish Institute of Space Physics; LIP (Portugal); Università di Genova; INAF (Palermo Italy);Physics; LIP (Portugal); Università di Genova; INAF (Palermo, Italy); INFN and INOA, (Florence, Italy); Università di Roma Tor Vergata; Università di Perugia; Observatoire de Neuchâtel; Skobeltsyn Institute; UNAM, Mexico; RIKEN, Japan; Univ, of Ala., Huntsville; Vanderbilt Univ ; Sp Sci Lab UCB; UCLA; Univ of Utah; NASA

8/25/08 1

Vanderbilt Univ.; Sp. Sci. Lab., UCB; UCLA; Univ. of Utah; NASA-MSFC and NASA-GSFC

https://ntrs.nasa.gov/search.jsp?R=20090002566 2018-07-11T17:43:42+00:00Z

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8/25/08 2

(cosmic rays); X (active galactic nuclei); blue shading (exposure)

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Event Arrival Direction Reconstruction

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Extreme Energy Cosmic Rays (EECR )(EECRs)

• Energies extending to at least 50 Joules/particleg g p• Fluxes of 1 particle/(km2∗century)

8/25/08 4http://www.astroparticlephysics.nl/cosmic_rays.jpg

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Shower Time Profile

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Hybrid Ground-based ArrayHybrid Ground based Array

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Fluorescence Detector

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Super-EUSO

•Variable orbit 1000 km

•Free Flyer•Variable orbit 1000 km

• FOV

• yr5Life ≈sr km104.2A 26inst

aper ⋅×≈

25° y5ife% 2010cycle ÷≈η

( ) yrsrkm104221A 26×≈

25

( ) yrsrkm104.22.1Aexp ×−≈

Tilted mode (?)

8/25/08 9(?) L10A 7

exp →

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Super EUSO Instrument R iRequirements

• Very large wide-angle telescope with high optical th h t d 1 illi di l l tithroughput and ~1 milliradian angular resolution

• High efficiency pixelated photo-detectors with single photon sensitivity– Photomultiplier tubes with ultra-bialkali photocathodes or– Silicon photomultipliers

• Optics Design Options– Reflective optics:

• Schmidt or Maksutov optics– Convex focal surface

– Refractive optics (the JEM-EUSO concept)Refractive optics (the JEM EUSO concept)• Very large and light-weight Fresnel lenses • Diffractive lens for chromatic correction

– Antireflective coatings needed in either case

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Photomultiplier Tubesp• Hamamatsu Ultra-Bialkali photocathodes

40 45% Q E f 330 400– 40-45% Q.E. from 330-400 nm– Off the shelf (Hamamatsu)

L i t t b f– Large inter-tube gaps on a convex surface• Back-illuminated Silicon Photomultipliers

– 90% Q.E. from 330-400 nm– Requires cooling– Developmental (Siemens)– Small inter-device gaps on a convex surface

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g p

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Optics Design ConceptsOptics Design Concepts

Maksutov optical design with an Schmidt design with an f/# of 0.7 and a

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f/# of 0.66, CAO at UAH, Huntsvilleg

50° field of view, CNR- INOA, Firenze

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Optics Throughput

Obscuration due to focal surfaceObscuration due to focal surface

+ Mirror reflectivity + transmission of Schmidt corrector reduce of ~ 0.9

Filt t id d f !!

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Filters not considered so far!!

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Refractive Opticsp

500.00 MM Diffractive/Fresnel

Focal Surface

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Achromatic Fresnel- Diffractive, f/1.0 Scale: 0.05 AZ 28-Apr-04

Throughput is less than with reflective systems

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Shower Imaging and ReconstructionSuper-EUSO functions like a high-speed and wide angle video camera• Frame rate: ~3 μsec/frameFrame rate: 3 μsec/frame

• Pixel Size: 4×4 mm2 on the focal surface or 1×1 km2 on Earth

R t ti i 1 1 1 k 3 l• Reconstruction in 1×1×1 km3 voxels

• Arrival direction reconstruction to <0.2°

• Energy reconstructed from fitted e gy eco st ucted o ttedintensity at shower maximum

For those events with a detected Cherenkov reflection at a knownCherenkov reflection at a known altitude:• Shower profile versus atmospheric depth will be reconstructed

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depth will be reconstructed.

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Optics Manufacturing R iRequirements

• Surface RoughnessSurface Roughness– 20 nm RMS on refractive elements

5 nm RMS on reflective elements– 5 nm RMS on reflective elements• Tilt errors

– <0.5 milliradian• Anti-reflective Coatings on refractive

elements– >90% transmission in the 330-400 nm band

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Super EUSO Spacecraft Concepts

These folding concepts were developed to fit Super-EUSO into an existing faring.

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ARES V OptionARES V Option• Launch Super p

EUSO as a rigid unit– Spherical mirror

constructed from regular hexagonalregular hexagonal zones

– Segmented corrector plate in the style of a lighthouse lens

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lighthouse lens

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Notional Designg

Segmented Corrector Plate Mirror constructed from

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hexagonal spherical segments

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Summaryy• Super EUSO is needed to find out how the

most energetic cosmic accelerators workmost energetic cosmic accelerators work and what they are accelerating?

• The Super-EUSO instrument must be aThe Super EUSO instrument must be a very large high-speed and wide-angle video camera in space.p

• We are open to suggestions for improvements in design and also concepts p g pfor manufacturing such an instrument.

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The End

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