New opportunities in optical testing given by photochromic materials - - PowerPoint PPT Presentation

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New opportunities in optical testing given by photochromic materials - - PowerPoint PPT Presentation

New opportunities in optical testing given by photochromic materials Giorgio Pariani, Martino Quintavalla, Rossella Castagna, Letizia Colella, Chiara Bertarelli, Frederic Zamkotsian, Andrea Bianco Photochromic materials F Change of: F 3 -


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SLIDE 1

New opportunities in optical testing given by photochromic materials

Giorgio Pariani, Martino Quintavalla, Rossella Castagna, Letizia Colella, Chiara Bertarelli, Frederic Zamkotsian, Andrea Bianco

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SLIDE 2

Photochromic materials

X X C H 3 C H 3 R 1 R 2 F F S S

COLORLESS FORM

A

X X R 1 R 2 F F S S

COLORED FORM

B

Change of: And:

  • Conductivity/charge mobility
  • Dipole moment
  • Redox potential.
  • Luminescence
  • No thermal switching
  • Good fatigue resistance
  • Fast responce

UV-Vis absorption spectra Polarizability/Refractive indices

300 400 500 600 700 800 1 2 3 l A 300 400 500 600 700 800 1 2 3 l A

Vis UV

Bertarelli, C., Bianco, A., Castagna, R., Pariani, G., J. Photochem. Photobiol. C: Photochemistry Reviews, 12(2), 106–125 (2011)

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SLIDE 3

Photochromic Focal Plane Masks

400 500 600 700 800 20 40 60 80 100

l (nm) T%

Filter1 Filter2 Mask opaque

  • Photochromic polymer (6%) in PMMA
  • 70 mm thick film
  • large contrast in a specific spectral

range of interest (Ha, Na,...)

  • filters are needed to cover the entire

spectral range

  • easy to produce (with direct laser

writing) and easy to use

S S F F F F F F m S S F F F F F F m

UV vis

20 40 60 80 100

l (nm) T %

400 500 600 700 800 0.2 0.4 0.6 0.8 1

Contrast

A B A B

Bianco, A., et al., Astron. Nachr., 326(5), 370-374 (2005)

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SLIDE 4

Photochromic FPM @ Asiago Telescope

Bianco, A., Bertarelli C., Gallazzi, M.C., Zerbi G., Giro, E., Molinari, E., Astron. Nachr., 326(5), 370-374 (2005)

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SLIDE 5

Process

make the element re-writable: it is a reconfigurable platform

DESIGN

CGH pattern

TESTING

Interferometry

PRINTING

Irradiation: Vis light

ERASING

Irradiation: UV light

POST PROCESS

Chemical development

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SLIDE 6

Interferometry

  • Amplitude Computer Generated Holograms for optical testing
  • Photochromic Point Diffraction Interferometer
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SLIDE 7
  • J. C. Wyant, 1971-72

CGH

aspherical mirror spherical wavefront aspherical wavefront

Null Test

INTERFEROGRAM

spherical reference surface

CGH: binary representation of the interferogram between the spherical and aspherical wavefront under test. Each line adds ml of OPD and changes the wavefront slope by sin(q) = ml/L, L is the local line spacing.

Computer Generated Holograms

REQs: Line period L = down to 1 micron Accuracy e = 50 nm PV Size D = 150 mm

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SLIDE 8

Writing strategies

Direct Laser Writing scanning mode Mask projection raster mode

Photochromic substrate Moving stages Objective

  • High pattern density/slow process
  • High accuracy
  • Compex system/very versatile
  • Fast process/stitching for large areas
  • Distorsions from projection
  • Very versatile (according to the mask)

Photochromic substrate Mask

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SLIDE 9

Amplitude Fresnel CGH – scanning mode

1 cm

Spot diameter: 4 mm Centering precision: 7 mm Translation precision: 15 mm Light density: 50 W/mm

2

film focusing lens focusing screen beam splitter He-Ne laser stages shutter mirror

Laser Plotter

f20

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SLIDE 10

Test results

Fresnel CGH spherical wavefront spherical mirror Plane reference surface

0 order

th

1 order

st

CGH Interference fringes Wavefront analysis

PV: 1680 nm RMS: 238 nm PV, /2 RMS 3l l

Fringes are well visible: the produced Fresnel CGH satisfies the basic requirements of optical quality and contrast Other aberrations: some errors are introduced by the film surface and by the accuracy of the written pattern

Pariani, G., Bertarelli, C., Dassa, G., Bianco, A., Zerbi, G., Optics Express, 19(5), 4536–4541 (2011)

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SLIDE 11

Production with standard DLW – scanning mode

Results:

  • High material resolution, up to the writing beam size
  • High beam power may affect the surface
  • Contrast low for the autofocus beam and wrong writing

beam (at the limit of the material sensitivity) A custom DLW machine is required! Production of photochromic CGHs at the Institut für Technische Optik - Universität Stuttgart

Pariani, G., Bertarelli, C., Bianco, A., Schaal, F., Pruss, C., Proc. of SPIE, 8450(1), (2012). Smallest feature sizes: < 1µm (binary)

  • Max. substrate size:

Ø 300 mm

  • Max. substrate thickn.:

25 mm Write speed (typ.):

  • n-axis: 9 mm/h
  • ff-axis: 4 mm/h

Wavelength: 457-488-514 nm Positioning increment: radial: 0.6 nm azimuthal: 1'' @ 600 rpm CLWS300M (Production System) 30 micron Autofocus beam in the visible

f1

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SLIDE 12

Photochromic Point Diffraction Interferometer

Linnik 1933, Smartt 1972

Diffraction from a pinhole in a semi-transparent film

  • Simple use: PDI is positioned in the focal plane of the optics under test
  • Common path: very low sensitivity to vibrations and turbulence

B A pinhole

  • uter region

Quintavalla et al., Opt. Laser Eng. 2014

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SLIDE 13

Why a photochromic PDI?

Optical writing of the substrate:

  • single step process, no post process required
  • tunable transparency with irradiation time to maximize the fringe visibility

50 100 150 200 250 300 350 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 Tempo di schiarimento (s) Visibilita

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SLIDE 14

Why a photochromic PDI?

Optical writing of the substrate:

  • single step process, no post process required
  • tunable transparency with irradiation time to maximize the fringe visibility
  • wide range of pinhole size to match the optics under test
  • Pinhole size tunable from 1 to 50 microns
  • The size depends on the photons dose
  • Auto-confinement of the beam inside the

photochromic substrate

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SLIDE 15

Why a photochromic PDI?

Optical writing of the substrate:

  • single step process, no post process required
  • tunable transparency with irradiation time to maximize the fringe visibility
  • wide range of pinhole size to match the optics under test
  • the pinhole may be written by the test optic!

no fine alignments required continous monitoring easily possible works properly for low aberrated optics

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SLIDE 16

Results

self-referencing test

mirror at 0° mirror at 180° 150mm dia., f# 2 spherical mirror 2.5mm pinhole dia.

  • rientation

(deg) PtV (nm) RMS (nm) 128±15 27±3 180 126±16 22±3

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SLIDE 17

Results

comparison with a standard Fizeau inteferometer

PDI Fizeau INT PtV (nm) RMS (nm) Fizeau 144±9 29±2 PDI 132±15 26±3 150mm dia., f# 2 spherical mirror Certified 150mm dia., f# 8, λ/8 PtV and λ/40 RMS spherical mirror

absolute accuracy

PtV (nm) RMS (nm) SPEC 40 8 PDI 56±17 8.5±2