Multi-Spectral Transparent Materials Technologies - The American ...
Multi-Spectral Transparent Materials Technologies - The American ...
Multi-Spectral Transparent Materials Technologies - The American ...
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<strong>American</strong> Ceramic Society – Baltimore, June 2010<br />
<strong>Multi</strong>-<strong>Spectral</strong><br />
<strong>Transparent</strong> <strong>Materials</strong> <strong>Technologies</strong><br />
Daniel C. Harris<br />
Naval Air Systems Command<br />
China Lake, California<br />
Daniel.Harris@navy.mil<br />
760-939-1649<br />
<strong>Multi</strong>spectral ZnS was discovered by<br />
Chuck Willingham at Raytheon in 1980<br />
1
UV Visible Near IR<br />
Atmospheric Transmission<br />
Microwave<br />
2
Magnesium Fluoride Dome on Sidewinder Missile Protects<br />
Delicate Seeker and Transmits Infrared Radiation<br />
MgF 2 dome<br />
3
Lockheed Martin SNIPER Targeting Pod<br />
Sapphire<br />
window<br />
SNIPER Pod<br />
4
LANTIRN Zinc Sulfide Infrared Window<br />
Lockheed<br />
Martin photos<br />
Joint Strike Fighter Electro-Optic Targeting System<br />
Faceted Sapphire Window<br />
ATFLIR<br />
Zinc<br />
Sulfide<br />
window<br />
Goodrich<br />
photo<br />
5
Germanium<br />
window<br />
Germanium Windows on SLAM-ER<br />
6
Generic Issues for Window and Dome <strong>Materials</strong><br />
•<br />
•<br />
•<br />
Transmission and emission at desired frequencies<br />
Resistance to rain and sand erosion<br />
Resistance to thermal shock<br />
Electromagnetic shielding<br />
Common External Window <strong>Materials</strong><br />
•<br />
Long Wave Infrared (8-12 μm)<br />
• Zinc sulfide (Dow, II-VI)<br />
Germanium (Umicore)<br />
•<br />
Midwave Infrared (3-5 μm)<br />
• Sapphire (Crystal Systems, Saint Gobain, Rubicon)<br />
• Silicon<br />
• Magnesium fluoride (France–Saint Gobain)<br />
• Spinel (TA&T [Armorline], Surmet, MER)<br />
ALON (aluminum oxynitride) (Surmet)<br />
•<br />
Visible and Near Infrared<br />
• Various glasses<br />
• Fused silica<br />
7
Early Maverick Dome (ZnS) Broken by Rain Impact in 1980s<br />
8
Sidewinder Dome (MgF 2 ) Pitted by Sand in Persian Gulf (1990)<br />
9
Splat!<br />
Bug Impact on ZnS/ZnSe Sandwich Window<br />
[N. Osborne, University of Dayton Research Institute] 10
Dust Storm Created by Helicopter<br />
[Aviation Week & Space Technology, 5 May 2008, page 34] 11
Candidate Midwave (3-5 μm) <strong>Materials</strong><br />
for High-Speed Systems<br />
Optical GaP, yttria, and lanthana-doped yttria are not commercially available<br />
12
Transmittance<br />
0.8<br />
0.7<br />
0.6<br />
0.5<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
“2-Color” (Midwave + Long Wave) <strong>Materials</strong><br />
0<br />
ms-ZnS<br />
Ge<br />
2 4 6 8 10 12 14 16<br />
•Ge – Great for aircraft. Operating<br />
temperature up to ~100°C<br />
•Si – Only midwave. Operating<br />
temperature up to ~250°C<br />
•GaP – Midwave, not long wave.<br />
Operating temperature up to<br />
~600°C (Mach 4). High dn/dT.<br />
Poor erosion resistance. Not<br />
commercially available.<br />
GaP<br />
Si<br />
3-5 μm 8-14 μm<br />
Wavelength (μm)<br />
GaAs<br />
ZnSe<br />
•GaAs – Excellent optical quality in both<br />
bands. Operating temperature up to<br />
~400°C (Mach 3). Erosion resistance is<br />
modest. Not commercially available.<br />
• ZnSe – Superb optical quality in both bands,<br />
but very poor erosion resistance<br />
• <strong>Multi</strong>spectral ZnS – <strong>The</strong> only contender for<br />
Mach 4. Poor erosion resistance could<br />
be improved by coatings<br />
13
II-VI, Inc.<br />
High Quality Zinc Sulfide is Grown in Large Areas<br />
by Chemical Vapor Deposition<br />
14
<strong>The</strong>re is no adequate erosion<br />
protection coating for zinc sulfide<br />
<strong>The</strong>re is no durable multispectral<br />
material that transmits from the<br />
visible through the long wave<br />
infrared region<br />
(multispectral ZnS is used)<br />
15
Diamond Could be an Excellent Long Wave Infared Window<br />
(But Not a Midwave Window) if it Were Affordable and<br />
Could be Made in Desired Sizes and Shapes<br />
Transmittance<br />
0.8<br />
0.7<br />
0.6<br />
0.5<br />
0.4<br />
0.3<br />
0.2<br />
0.1<br />
0.0<br />
<strong>The</strong>oretical reflection limit<br />
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14<br />
Wavelength (μm)<br />
Chemical vapor<br />
deposited diamond<br />
1.74 mm thick<br />
Midwave Long wave<br />
16
•<br />
•<br />
Windows emit radiation at the wavelengths they absorb<br />
Emission from the Window Creates Noise at a Sensor<br />
17
•<br />
•<br />
Most Infrared Transmitting <strong>Materials</strong> are Highly<br />
Reflective at Radio Frequencies<br />
Dome thickness should be multiple of λ/2 to minimize reflection<br />
Hemispheric geometry is the only practical one for IR/RF dome<br />
so that angle of incidence is always the same<br />
Radome thickness is optimized<br />
to minimize reflection at one<br />
angle of incidence<br />
Hemispheric dome minimizes<br />
reflection of all rays that pass<br />
through the center of the dome<br />
Penalty is severe drag<br />
18
Shielding Effectiveness (dB)<br />
RF Shielding by Square Gold Grid on Sapphire<br />
Observed<br />
Predicted<br />
Frequency (GHz)<br />
Grid spacing is much less than wavelength in this example<br />
If wavelength approaches grid spacing, more leakage occurs<br />
K. T. Jacoby, M. W. Pieratt, J. I. Halman, and K. A. Ramsey, Proc. SPIE 2009, 7302, 73020X<br />
<strong>The</strong>ory for transmission: S.-W. Lee, G. Zarillo, and C.-L. Law IEEE Transactions Antennas &<br />
Propagation 1982, AP-30, 904<br />
5 µm wide lines<br />
50 µm center to<br />
center
<strong>The</strong>re is a Strong Need for Infrared-<strong>Transparent</strong><br />
Electrically Conductive Coatings for<br />
Electromagnetic Shielding<br />
h<br />
P o<br />
P<br />
Conductive coating<br />
Sheet resistance = R s<br />
For example, indium tin oxide has visible transparency and electrical conductivity<br />
<strong>The</strong>re is no known material with adequate infrared transparency and adequate<br />
electrical conductivity<br />
d<br />
Infrared window<br />
Dielectric constant = ε<br />
20
DARPA/ONR Nano-Composite Optical Ceramics Program<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
2µm<br />
Raytheon Y 2 O 3 -MgO composite<br />
Transmittance (%)<br />
0 2 4 6 8 10<br />
Wavelength (µm)<br />
Objectives (2007-2011)<br />
•<br />
•<br />
•<br />
2 Compositions<br />
50:50 YM<br />
70:30 MY<br />
of Y2O3-MgO 2 mm thick<br />
Midwave infrared (3-5 μm) transmission<br />
> spinel<br />
<strong>The</strong>rmal shock resistance > sapphire<br />
Fabricate windows and domes<br />
Raytheon<br />
Nanocerox<br />
CeraNova<br />
University of California,<br />
Davis<br />
Rutgers University<br />
University of Connecticut<br />
21
Raytheon Nanograin Yttria-Magnesia Composite<br />
Provides Mechanical Properties Superior to<br />
Those of Either End Member<br />
Photographed<br />
with visible light<br />
Photographed<br />
with infrared light<br />
22
Aerodynamic Domes and Conformal Windows<br />
Navy SBIR Program (Small Business Innovation Research)<br />
Toroidal glass window made at Penn State<br />
University with OptiPro UltraForm Finishing –<br />
2009<br />
ALON ogive dome made at OptiPro – 2009<br />
23
Example of conformal window: spinel toroid made at Penn State<br />
University with OptiPro UltraForm Finishing – Jan 2010<br />
24
Alumina Dome blank<br />
CeraNova<br />
Final finishing<br />
QED<br />
Aerodynamic Dome Program Elements<br />
Grinding and polishing:<br />
OptiPro, Optimax, CeraNova, Penn State Univ, Univ. Rochester<br />
Metrology<br />
OptiPro<br />
ASE Optics<br />
Breault<br />
Appl. Science Innov.<br />
Applied Science Innovations<br />
OptiPro & ASE Optics<br />
Breault<br />
25
Aerodynamic Dome Program Elements (continued)<br />
Corrective optics<br />
OptiPro (fabrication)<br />
ASE Optics (metrology)<br />
Coating deep concave surfaces<br />
Precision Photonics<br />
26
Transmittance (%)<br />
100<br />
80<br />
60<br />
40<br />
20<br />
0<br />
<strong>Transparent</strong> Polycrystalline Alumina Could Replace<br />
Sapphire in Some Infrared-Only Applications<br />
• Krell et al, Fraunhofer Institute,<br />
reported infrared transparent Al2 with 0.5 μm grain size in 2003<br />
• Properties similar to sapphire<br />
• Can be made into shapes ―<br />
impractical for sapphire<br />
Sapphire 2.6 mm thick<br />
O 3<br />
Alumina<br />
1.02 mm thick<br />
5.00 mm thick<br />
CeraNova<br />
0.0 0.5 1.0 1.5 2.0 2.5<br />
Wavelength (μm)<br />
(1 mm thick)<br />
Alumina<br />
CeraNova [M. V. Parish & M. R. Pascucci, Proc. SPIE 2009, 7302, 730205]<br />
Polished Hemisphere<br />
(2 mm thick)<br />
Unfinished Dome<br />
27
“Coarse” Metrology with OptiPro UltraSurf Instrument<br />
can Measure a Workpiece During Grinding and<br />
Polishing Before Interferometry Applies<br />
Light Pen:<br />
•<br />
•<br />
Commercial pen from<br />
STIL<br />
Quad Probe from ASE<br />
Optics SBIR contract<br />
28
OptiPro 2009<br />
UltraSurf Measurement of ALON Ogive Dome<br />
with ASE Quad Probe<br />
29
“Fine” Metrology of Free-Form Optics by Interferometry<br />
Applied Science Innovations<br />
• Modular attachment to<br />
commercial interferometer<br />
• Wavefront and surface metrology<br />
• <strong>Multi</strong>ple double-pass transmittedwavefront<br />
maps cover entire<br />
surface<br />
• Solve system of equations to<br />
produce maps of both surfaces<br />
• Reference spherical mirror<br />
• Resolution better than 100 nm<br />
• Sample size limited by size of<br />
spherical mirror only<br />
• Patent 7,545,511 - 2009<br />
Resolved fringes<br />
Unresolved<br />
fringes<br />
Map of broken<br />
wine glass<br />
As reference mirror<br />
is moved, fringes are<br />
produced by limited<br />
regions. Hundreds<br />
of images stitched<br />
together produce<br />
map of both surfaces<br />
and transmitted<br />
wavefront<br />
30
QED <strong>Technologies</strong><br />
Rochester NY<br />
Magnetorheological Fluid Jet (MR Jet) Prototype<br />
Jet with<br />
magnet off<br />
Jet with<br />
magnet on<br />
Spindle<br />
Work piece<br />
Nozzle<br />
Fluid collection<br />
Polycrystalline Alumina Dome Concave Surface<br />
Initial figure 1.74 μm P-V Final figure 0.3 μm P-V 31
Airplanes and Ships could use Sensor Windows<br />
Much Larger than Anything Available Today<br />
Sensor windows<br />
Reconnaissance pod<br />
32
Two Approaches to Large Sensor Windows:<br />
1. Scale up size of monolithic window<br />
2. Edge bond windows to make larger windows<br />
TA&T 11 x 18”<br />
spinel<br />
window Surmet<br />
19 x 25” ALON window<br />
33
Adhesive-Free Bonding of Sapphire or Laser Crystals<br />
at Onyx Optics<br />
Bond<br />
line<br />
Fracture<br />
line<br />
H.-C. Lee, H. E. Meissner, X. Mu, C. Liu, and W. Qiu, Proc. SPIE 2009, 7302, 73020A<br />
Polish surfaces to be contacted<br />
to near-atomic flatness<br />
When surfaces are brought into<br />
contact, they stick together<br />
Heat to drive out adsorbed molecules<br />
and increase strength of bond<br />
Sapphire flexure bars joined at the center do<br />
not fracture on the bond line -- indicating that<br />
bond is stronger than sapphire<br />
Disadvantage is difficulty of preparing<br />
optically flat mating surfaces<br />
34
Resonant Cavity Approach to Tri-Mode Seeker Dome<br />
Performance objectives:<br />
• Transmit midwave infrared<br />
• Transmit near-infrared laser<br />
• Transmit millimeter wavelength λ o<br />
• Reject out-of-band radio frequencies<br />
• Durable to survive rain and sand erosion<br />
Dielectric 1<br />
Dielectric 2<br />
Conductive<br />
grid<br />
Gridded, bonded<br />
ALON dome<br />
from Surmet<br />
37
Summary<br />
Generic window problems<br />
• Transparency over all desired wavelengths<br />
• Optical emission<br />
• Rain and sand erosion<br />
• <strong>The</strong>rmal shock<br />
Infrared materials problems<br />
• Few materials are used: ZnS, Ge, sapphire, MgF2, Si, spinel, ALON<br />
• No long wave infrared material is sufficiently durable<br />
• No multispectral (visible to long wave) material is sufficiently durable<br />
• Good infrared transmitting materials are highly reflective at radio<br />
frequencies<br />
Some Current Technology Development<br />
• Nanocomposite materials with new combinations of properties<br />
• Aerodynamic infrared dome<br />
• Conformal sensor window<br />
• Large area window<br />
• Monolithic<br />
• Edge bonded<br />
Daniel.Harris@navy.mil<br />
38
<strong>Multi</strong>-<strong>Spectral</strong> <strong>Transparent</strong> <strong>Materials</strong> <strong>Technologies</strong><br />
Daniel C. Harris<br />
Naval Air Systems Command, China Lake, California<br />
Ceramic windows and domes protect delicate sensors from harsh environments<br />
while transmitting electromagnetic radiation in one or more spectral<br />
regions. Window material deficiencies that have existed for half a century<br />
include window durability, thermal shock resistance, and optical emission.<br />
<strong>The</strong>re are no very durable materials that transmit both midwave<br />
55 minutes<br />
(3-5 micron)<br />
and long wave (8-12 micron) infrared radiation. Some current thrusts in<br />
window research and development include the fabrication of nanocomposites<br />
with properties not attained by monolithic materials, making conformal<br />
shapes that extend the state of the art in machining and metrology, and<br />
scaling up transparent ceramics to make meter-class windows.<br />
Biographical information: Dan Harris is a Senior Scientist and Esteemed<br />
Fellow at the Naval Air Systems Command in China Lake, California, where he<br />
manages research and development programs in infrared window materials. He<br />
is the author of the monograph "<strong>Materials</strong> for Infrared Windows and Domes"<br />
and holds degrees in chemistry from MIT and Caltech.
Program Components: Small Business Contracts<br />
N02-155: Nano-Grain Infrared Window <strong>Materials</strong><br />
Phase II CeraNova (completed 2006)<br />
N03-009: Nanopowders for IR Window <strong>Materials</strong><br />
Phase II MetaMateria (completed 2006)<br />
N04-172: Aerodynamic dome finishing<br />
Phase II + enhancement + Ph II.5 OptiPro<br />
Phase II Creare (completed 2008)<br />
N04-234: Aerodynamic dome blank fabrication<br />
Phase II + enhancement + Ph II.5 CeraNova<br />
Phase II QED (completed Dec 08)<br />
– continues as subcontractor<br />
N06-069: Metrology for Ogive Infrared Dome<br />
Phase II OptiPro + Ph II.5 OptiPro 2010<br />
Phase II Breault<br />
Phase II MetroLaser (completed May 09)<br />
N07-181: Conformal Sensor Window<br />
Phase II OptiPro<br />
Phase II Third Wave Systems<br />
Phase II Applied Science Innovations<br />
+ enhancement 2009<br />
N07-182: Aerodynamic Infrared Dome<br />
Phase II Optimax<br />
Phase II CeraNova<br />
N08-029: Corrective Optics for Conformal<br />
Windows and Domes<br />
Phase II OptiPro<br />
Phase II ASE Optics – Working with OptiPro<br />
metrology<br />
N03-082: Tactical Reconnaissance Window<br />
(Rob Borland technical monitor)<br />
Phase II + enhancement TA&T(completed<br />
Phase II QED (completed 2008)<br />
N08-134: Edge-Bonded Infrared Windows<br />
Phase II Onyx Optics<br />
Phase II MER/Onyx Optics<br />
N04-T009: Nanocomposite optical materials<br />
Phase II Synkera with Raytheon/DARPA<br />
on<br />
2009)<br />
N08-T003: Low-Expansion, <strong>The</strong>rmal-Shock-Resistant<br />
Dome Material<br />
Phase II <strong>Materials</strong> and Systems Research<br />
N09-028: Optical Coatings for Deep Concave Surfaces<br />
(Mark Moran technical monitor)<br />
Phase II Precision Photonics<br />
N10-163 High-Strength, Optical Quality Spinel<br />
N10-164 Large-Area, Monolithic Infrared Sensor Window<br />
N10-165 Optically Precise Conformal Sensor Window<br />
40
Planned DDG-1000 Zumwalt-Class Destroyer<br />
Large sensor windows on deckhouse<br />
Wikimedia commons graphic<br />
41