U.S. patent application number 11/237076 was filed with the patent office on 2006-02-02 for thermal control interface coatings and pigments.
This patent application is currently assigned to JDS UNIPHASE CORPORATION. Invention is credited to Paul G. Coombs, Charles T. Markantes, Roger W. Phillips.
Application Number | 20060023327 11/237076 |
Document ID | / |
Family ID | 35731844 |
Filed Date | 2006-02-02 |
United States Patent
Application |
20060023327 |
Kind Code |
A1 |
Coombs; Paul G. ; et
al. |
February 2, 2006 |
Thermal control interface coatings and pigments
Abstract
The invention provides an optical structure with low chroma and
brightness in the visible region and low emissivity in the infrared
region. The optical structure includes an interference structure
having an infrared reflective layer and an infrared absorbing thin
film layer. These layers are in turn separated by a thin film
spacer of a dielectric or semiconductor material. The reflectivity
and transmission of the layers are selectively controlled through
the thickness of the layers such that the visual reflectivity and
color is independent of the infrared properties of the absorber and
reflector layers.
Inventors: |
Coombs; Paul G.; (Santa
Rosa, CA) ; Markantes; Charles T.; (Santa Rosa,
CA) ; Phillips; Roger W.; (Santa Rosa, CA) |
Correspondence
Address: |
ALLEN, DYER, DOPPELT, MILBRATH & GILCHRIST P.A.
1401 CITRUS CENTER 255 SOUTH ORANGE AVENUE
P.O. BOX 3791
ORLANDO
FL
32802-3791
US
|
Assignee: |
JDS UNIPHASE CORPORATION
Santa Rosa
CA
Flex Products, Inc., a corporation of the State of
California
|
Family ID: |
35731844 |
Appl. No.: |
11/237076 |
Filed: |
September 28, 2005 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
|
|
10152593 |
May 20, 2002 |
|
|
|
11237076 |
Sep 28, 2005 |
|
|
|
Current U.S.
Class: |
359/883 |
Current CPC
Class: |
G02B 5/0816 20130101;
Y10T 428/2993 20150115; Y10T 428/2991 20150115; G02B 5/0825
20130101; G02B 5/0858 20130101; G02B 5/281 20130101 |
Class at
Publication: |
359/883 |
International
Class: |
G02B 5/08 20060101
G02B005/08; G02B 7/182 20060101 G02B007/182 |
Claims
1-73. (canceled)
74. An optical structure comprising: a reflector; a spacer layer
with a spacer thickness disposed on the reflector; and an absorber
layer disposed on the spacer layer, the absorber layer having an
absorber thickness providing a transmittance through the absorber
layer between 5-85% wherein the reflector has a reflector
thickness, the spacer thickness and the absorber thickness are
selected to achieve an average first reflectivity of not more than
50% between 400-700 nanometers and an average second reflectivity
of not less than 50% between 4-40 microns.
75. The optical structure of claim 74 wherein the spacer thickness
is between 1 quarter-wave optical thickness at 200 nm and 2
quarter-wave optical thicknesses at 700 nm.
76. The optical structure of claim 74 wherein the spacer thickness
is selected to achieve a reflectivity minimum of the optical
interference structure between 200-1500 nm.
77. The optical structure of claim 74 wherein the spacer thickness
is less than one quarter-wave optical thickness at 700 nm and is
selected to achieve a reflectivity minimum of the optical structure
between 200-700 nm.
78. The optical structure of claim 74 wherein the reflector
comprises aluminum, the spacer layer comprises magnesium fluoride
and the absorber layer comprises chromium having an internal
transmittance of not more than 50%.
79. The optical structure of claim 74 wherein the spacer layer is
made of a selectively absorbing spacer material being more
absorptive in the visible range than in the infrared range.
80. The optical structure of claim 79 wherein the selectively
absorbing spacer material is selected from the group consisting of
iron oxide, tungsten oxide, copper oxide, and cobalt oxide.
81. The optical structure of claim 74 wherein the spacer layer
comprises a spacer material selected from the group consisting of
zinc sulfide, zinc oxide, zirconium oxide, titanium dioxide,
diamond-like carbon, indium oxide, indium-tin-oxide, tantalum
pentoxide), ceric oxide, yttrium oxide, europium oxide, iron oxide,
ferric oxide, hafnium nitride, hafnium carbide, hafnium oxide,
lanthanum oxide, magnesium oxide, neodymium oxide, praseodymium
oxide, samarium oxide, antimony trioxide, silicon, silicon
monoxide, germanium, selenium trioxide, tin oxide, tungsten
trioxide, and combinations thereof.
82. The optical structure of claim 74 wherein the spacer layer
comprises a spacer material selected from the group consisting of
silicon dioxide; aluminum oxide; metal fluoride, including
magnesium fluoride, aluminum fluoride, cerium fluoride, lanthanum
fluoride, sodium aluminum fluorides including Na.sub.3AlF.sub.6 and
Na.sub.5Al.sub.3F.sub.14, neodymium fluoride, samarium fluoride,
barium fluoride, calcium fluoride, and lithium fluoride; and
organic monomers and polymers, including dienes, alkenes, acrylates
including methacrylate, perfluoroalkenes, polytetrafluoroethylene,
and fluorinated ethylene propylene ("FEP").
83. The optical structure of claim 74 wherein the absorber
thickness is selected to achieve a reflectivity minimum of less
than 10% reflectivity of the optical interference structure between
200-1500 nm.
84. The optical structure of claim 74 wherein the absorber
thickness is selected to achieve a reflectivity minimum of the
optical interference structure between 200-1500 nm.
85. The optical structure of claim 74 disposed on a plurality of
pigment flakes in a paint vehicle to provide a paint
formulation.
86. The optical structure of claim 85 wherein the paint vehicle has
a low infrared emittance.
87. The optical structure of claim 85 disposed on a surface to
provide a solar absorber.
88. The optical structure of claim 85 disposed on a surface to
provide infrared camouflage.
89. The optical structure of claim 74 disposed on a plurality of
pigment flakes in an ink vehicle to provide an ink.
90. The optical structure of claim 74 disposed on a surface to
provide an infrared image.
91. The optical structure of claim 90 wherein the infrared image is
not discernible by an unaided human eye.
92. The optical structure of claim 90 wherein the infrared image is
incorporated in a heat-sensitive foil pressed onto a surface.
93. The optical structure of claim 74 wherein the optical structure
has indiscernible color shift when viewed by a human eye through a
viewing arc of 0-90 degrees measured from a normal to a major
surface of the optical structure with a fixed illumination
source.
94. The optical structure of claim 74 disposed on a plurality of
pigment flakes in a polymeric sheet.
95. The optical structure of claim 94 wherein the polymeric sheet
comprises a material selected from the group consisting of aqueous
polymer, polyvinyl alcohol, polyvinyl acetate polyvinylpyrrolidone,
poly(ethoxyethylene), poly(methoxyethylene), poly(acrylic) acid,
poly(acrylamide), poly(oxyethylene), poly(maleic anhydride),
hydroxyethyl cellulose, cellulose acetate and poly(sacchrides)
including gum arabic and pectin, poly(acetals) including
polyvinylbutyral, poly(vinyl halides) including polyvinyl chloride
and polyvinylene chloride, poly(dienes) including polybutadiene,
poly(alkenes) including polyethylene, poly(acrylates) including
polymethyl acrylate, poly(methacrylates) including poly
methylmethacrylate, poly(carbonates) including poly(oxycarbonyl
oxyhexamethylene, poly(esters) including polyethylene
terephthalate, poly(urethanes), poly(siloxanes), poly(suphides),
poly(sulphones), poly(vinylnitriles), poly(acrylonitriles),
poly(styrene), poly(phenylenes) including poly(2,5
dihydroxy-1,4-phenyleneethylene), poly(amides), natural rubbers,
formaldahyde resins, and combinations thereof.
96. The optical structure of claim 94 wherein the polymeric sheet
is an extruded sheet.
97. The optical structure of claim 94 wherein the polymeric sheet
is stretched.
98. The optical structure of claim 74 disposed on a plurality of
pigment flakes and mixed with a powder coating vehicle to provide a
powder coating formulation.
99. The optical structure of claim 98 wherein the powder coating
vehicle is clear at visible wavelengths.
100. The optical structure of claim 74 disposed on a film.
101. The optical structure of claim 100 wherein the film includes
an adhesive layer.
102. The optical structure of claim 74 disposed on a foil.
103. The optical structure of claim 102 wherein the foil comprises
aluminum or stainless steel.
104. The optical structure of claim 74 wherein the absorber
thickness is less than 3 times tabs.sub.min, the minimum visible
reflectance absorber thickness providing a minimum reflectivity of
the optical interference structure between 200-1500 nm.
105. The optical structure of claim 74 wherein the absorber layer
comprises an absorber material selected from the group consisting
of chromium, nickel, iron, titanium, aluminum, tungsten,
molybdenum, niobium, metal alloys, including Ni--Cr--Fe alloy,
metal dispersed in a dielectric matrix, iron oxide
(Fe.sub.2O.sub.3), silicon monoxide (SiO), chromium oxide
(Cr.sub.2O.sub.3), carbon, titanium nitride (TiN), and titanium
sub-oxide (TiO.sub.x where x is less than 2.0).
106. The optical structure of claim 74 wherein the reflector,
spacer layer, and absorber layer are chosen so as to achieve a
chroma of less than 20 for the optical interference structure.
107. The optical structure of claim 74 wherein the reflector layer
comprises a reflector material selected from the group consisting
of aluminum, silver, iron, tantalum, iridium, rhenium, copper,
silver, gold, platinum, palladium, nickel, cobalt, niobium,
chromium, tin, alloys, metal carbides, metal oxides, metal
nitrides, metal sulfides.
108. The optical structure of claim 74 wherein the reflector layer
comprises a reflector material selected from the group consisting
of indium oxide, indium tin oxide (ITO), europium oxide
(Eu.sub.2O.sub.3), vanadium pentoxide (V.sub.2O.sub.5), rhenium
oxide (ReO.sub.3), lanthanum boride (LaB.sub.6).
109. The optical structure of claim 74 wherein the spacer layer has
a spacer layer thickness of 1 quarter-wave optical thickness for
wavelengths between 100-500 nm and further comprising a second
spacer layer disposed on the absorber layer, the second spacer
layer having a second spacer layer thickness of 1 quarter-wave
optical thickness for wavelengths between 100-500 nm; and a second
absorber layer having an internal transmittance between 5% and 85%
disposed on the second spacer layer.
110. The optical structure of claim 74 wherein the spacer thickness
is one quarter-wave optical thickness between 200-800 nm, the
reflector comprises aluminum reflector and the absorber layer
comprises 20 nm of chromium.
111. The optical structure of claim 74 wherein the optical
structure is formed on a flake substrate.
112. The optical structure of claim 111 wherein at least one of the
reflector, the spacer layer, and the absorber layer surrounds the
flake substrate.
113. The optical structure of claim 74 wherein the optical
structure has an optical structure thickness not greater than 250
nm and is formed on a stiff flake substrate.
114. The optical structure of claim 74 further comprising a
stiffening layer.
115. The optical structure of claim 74 further comprising an
overcoat layer having an overcoat layer thickness.
116. The optical structure of claim 115 wherein the overcoat layer
thickness is at least eight times the spacer layer thickness.
117. The optical structure of claim 115 wherein the overcoat layer
thickness is less than eight times the spacer layer thickness.
118. The optical structure of claim 74 having a chroma less than
5.
119. The optical structure of claim 74 having an average
reflectance not greater than 20% between 400-700 nm.
120. An optical structure comprising: a reflector; a spacer layer
with a spacer thickness disposed on the reflector; and an absorber
layer disposed on the spacer layer, the absorber layer having an
absorber thickness providing a transmittance through the absorber
layer between 5-85%, the spacer thickness being selected so as to
provide an average reflectance of the optical interference
structure less than 50% reflectivity between 400-700 nm and a
chroma of the optical interference structure less than 20.
121. The optical structure of claim 120 wherein the spacer
thickness is between one quarter-wave optical thickness at 300 nm
and two quarter-wave optical thicknesses at 550 nm.
122. The optical structure of claim 120 wherein the spacer
thickness is between 2 quarter-wave optical thicknesses at a first
wavelength of 280 nm and 2 quarter-wave optical thicknesses at a
second wavelength of 450 nm.
123. The optical structure of claim 120 wherein the spacer
thickness is between 2 quarter-wave optical thickness at a first
wavelength of 450 nm and 2 quarter-wave optical thicknesses at a
second wavelength of 550 nm.
124. An optical interference structure comprising: a reflector
having a reflectivity of at least 50% over a wavelength range of
4-40 microns; a spacer layer disposed on the reflector having a
spacer layer thickness of between 1 quarter-wave optical thickness
at a first wavelength of 200 nm and 2 quarter-wave optical
thicknesses at a second wavelength of 500 nm, the spacer layer
having a refractive index less than 2; and an absorber layer with
an absorber layer thickness selected to provide an average
reflectance of the optical interference structure less than 20%
between 400-700 nm.
125. The optical interference structure of claim 124 wherein the
optical interference structure has a chroma less than 20.
126. The optical interference structure of claim 124 further
comprising: a second spacer layer with a second spacer thickness
disposed on the absorber layer; and a second absorber layer
disposed on the second spacer layer.
127. The optical interference structure of claim 126 wherein the
spacer layer thickness is less than one quarter-wave optical
thickness at a wavelength of 700 nm and the second spacer layer
thickness is less than one quarter-wave optical thickness at the
wavelength of 700 nm.
128. The optical interference structure of claim 124 wherein the
substrate is an aluminum flake comprising the aluminum reflector
and the second aluminum reflector.
129. The optical interference structure of claim 124 wherein the
substrate is a substantially rigid dielectric flake.
130. The optical interference structure of claim 129 wherein the
substantially rigid dielectric flake comprises glass, mica,
alumina, iron oxide, graphite, bismuth oxychloride, boron nitride,
or polymer.
131. An optical interference structure comprising: an aluminum
reflector; a first dielectric layer disposed on the aluminum
reflector, the first dielectric layer comprising MgF.sub.2 having a
first dielectric thickness of 55 nm; a first absorber layer
comprising 7 nm of chromium disposed on the first dielectric layer;
a second dielectric layer disposed on the first absorber layer, the
second dielectric layer comprising MgF.sub.2 having a second
dielectric thickness of 55 nm; and a second absorber layer
comprising 2.5 nm of chromium disposed on the second dielectric
layer, the second absorber layer.
132. The optical interference structure of claim 131 wherein the
aluminum reflector is an opaque reflector layer not less than 30 nm
thick.
133. The optical interference structure of claim 131 further
comprising: a substrate having a first surface and a second
surface, the aluminum reflector being disposed on the first surface
of the substrate; a second aluminum reflector disposed on the
second surface of the substrate; a third dielectric layer disposed
on the second aluminum reflector, the third dielectric layer
comprising MgF.sub.2 having a third dielectric thickness of 55 nm;
a third absorber layer disposed on the third dielectric layer
comprising 7 nm of chromium; a fourth dielectric layer disposed on
the third absorber layer, the fourth dielectric layer comprising
MgF.sub.2 having a fourth dielectric thickness of 55 nm; and a
fourth absorber layer disposed on the fourth dielectric layer, the
second absorber layer comprising 2.5 nm of chromium.
134. An optical interference structure comprising: a substantially
opaque aluminum reflector a dielectric layer comprising ZnS being 1
quarter-wavelength optical thickness at a wavelength between
200-1400 nm; and an absorber layer having an internal transmittance
between 5-85%.
135. An optical interference structure comprising: an aluminum
reflector a dielectric layer comprising MgF.sub.2 being 1
quarter-wavelength optical thickness at a wavelength of 500 nm; and
an absorber layer comprising 20 nm of chromium.
136. The optical interference structure of claim 135 having a
chroma less than 5.
Description
CROSS REFERENCE TO RELATED APPLICATIONS
[0001] Not applicable.
STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT
[0002] Not applicable
REFERENCE TO SEQUENCE LISTING
[0003] Not applicable
BACKGROUND OF THE INVENTION
[0004] This invention relates to partially reflective coatings
useful for controlling thermal radiation, that is infrared
reflective coatings that that have selectively controlled optical
properties in visual wavelengths permitting a wide variation in
perceived color and brightness having optimal infrared optical
properties.
[0005] Various methods have been used to achieve thermal radiation
control of objects by selectively controlling the object's
reflectivity to infrared radiation. Methods generally involve
either applying a coating to an object or forming its outer surface
of a material having high infrared reflectivity. Thermal radiation
controlled objects and surfaces have a number of uses, among which
are solar collector absorber panels, space vehicle surfaces, and
camouflaging military vehicles from detection by infrared scanning.
In many cases, it is desirable to selectively reflect specific
wavelengths of the infrared radiation while attenuating others by
absorption. For example, for solar energy collection it is
desirable that the surface coating absorb radiation corresponding
to the sun's solar emission spectrum, that is principally from 300
to 2,500 nanometers, while having a higher reflectivity at longer
(generally above about 4 microns) "thermal" wavelengths. This
allows the object to absorb and retain the sun's heat because the
increased reflectivity at the thermal wavelengths decreases
emittance of these wavelengths. The temperature of the object
generally determines the wavelength of the thermal emissions. For
an object in thermal equilibrium with its surroundings having a
given temperature, the term emmitance is defined at the ratio of
the energy emitted by such object divided by the energy that would
be emitted by a perfect black body at the same temperature. For an
object at room temperature (27 degrees Celsius, 300 degrees
Kelvin), emittance can be written as: 300 .times. K = .intg. 4 40
.times. ( 1 - R .function. ( .lamda. ) - T .function. ( .lamda. ) )
.times. BB .function. ( .lamda. , 300 .times. K ) .times. .times. d
.lamda. .intg. 4 40 .times. BB .function. ( .lamda. , 300 .times. K
) .times. .times. d .lamda. ##EQU1## where R(.lamda.) and
T(.lamda.) are the reflectance and transmittance of the object at
each wavelength, respectively, BB(.lamda., 300 K) is shorthand for
the so-called black-body function predicting the amount of energy
emitted by a 300.degree. K. perfect black body at each wavelength,
and the limits of integration are 4 micrometers to 40 micrometers.
For an opaque object, the transmittance is zero and hence the
higher the IR reflectance of the object, the lower the IR
emittance. Conversely, for opaque objects, the lower the IR
reflectance of the object, the higher the IR emittance.
[0006] Differential absorption and reflectivity of solar and
thermal wavelengths, can be achieved by first metallizing a surface
with highly polished or reflective metal foils or coatings, as many
metals are highly reflective in the solar and far-infrared
(thermal) regions of the spectrum. Selective absorption in the
solar wavelengths can be achieved by over coating the reflective
metallic surface with materials that selectively absorb solar
wavelengths. The most common methods for forming such surfaces are
by electrochemical deposition techniques followed by chemical
oxidation of the deposit and by "paint" technology using organic
based coatings.
[0007] In the former case, a suitable substrate, such as aluminum,
is electroplated with copper. The copper surface is then chemically
oxidized to form a surface layer of cupric oxide. One objection to
this method is the high cost of the combined
electrochemical/chemical oxidation process to obtain the desired
surface. Another disadvantage is that one cannot select the visible
color or appearance of the composite structure, which is the color
of cupric oxide.
[0008] Paint technology has been used to give objects selective
radiation properties. Some paints use organic solvents and organic
binders with an additive. A particular example is a lead
sulfide/silicone resin binder in xylene. However, organic-based
paints typically release volatile organic compounds, which may be
controlled or even prohibited in some areas because of
environmental concerns. Further, such organic paints may not
provide sufficient radiation control properties for some
applications.
[0009] Water-based paints have also been investigated. Black
silicate paint has been developed that uses a suitable pigment
bound in an alkali metal silicate, such as sodium silicate. Such a
formulation is sprayable and achieves an effect similar to that of
the electrochemical process or by organic binder paint technology.
Unfortunately, the pigments can react chemically with the silicate
binders in some instances to form pigment silicate salts or
complexes. These compounds alter the properties of absorptance and
emittance of the coating to such an extent that the performance of
the coating may degrade to an unacceptable level.
[0010] Another approach is to use two water-based coatings in which
a layer of a semiconductor pigment is first deposited upon a
thermally reflective substrate and then this pigment layer is
overcoated with an alkali metal silicate binder. The silicate layer
is heat cured at above ambient temperatures to form a protective
coating over the pigment.
[0011] The technology of thermal radiation control surfaces is
based on the need to obtain a surface that absorbs radiation in the
range of 300 to 2,500 nanometers while at the same time suppressing
emission of thermal energy. This basic principle accounts for the
operation of solar collector absorber panels, infrared transparent
coatings used on military equipment and the like. The general
approach is to start with a substrate material that has high
reflectance (low absorbance) over the entire spectral range
including the incident radiation and potential emission (300 to
40,000 nanometers, for example). Examples of such useful substrates
include metals such as aluminum, copper, steel and the like, and
non-metallic substrates, such as plastics and glass, which can be
metallized to provide a highly reflective surface.
[0012] In order to obtain the desired properties of opaqueness to
ultraviolet and visible light and transparency to infrared
radiation, it is desirable to form a coating on the highly
reflective substrate that absorbs in the visible and ultraviolet
region while transmitting infrared. The combination of the coating
on the substrate is preferably highly absorbing in the visible
range and highly reflecting (low emitting) in the thermal range.
This makes semiconductor pigments highly desirable, as these
compounds are highly transparent in the infrared, but absorb in the
visible region. Not all semiconductor pigments are useful, as those
having a high refractive index and thus a high surface reflection
coefficient give rise to unacceptable reflection losses. Thus, only
those semiconductor pigments having low enough refractive indices
to keep surface reflectivity at a minimum are acceptable. Among
such useful semiconductor pigments are copper oxide, iron oxides,
both naturally-occurring and synthetically made, chromium oxides,
nickel oxide, complexes of nickel-zinc-sulfide, lead sulfide and so
forth. Since thermal and photochemical stability is required of the
semiconductor, organic dyes would not be very useful and the
preferred semiconductors are, therefore, the inorganic pigments
already enumerated.
[0013] Such thermal control surfaces have undesirable visual
appearances for many applications because the broadband reflectors
are very bright or metallic in appearance, while selective
absorbers have a black appearance in the visible.
[0014] One approach uses a paint composition to achieve a diffused
visual blue-gray coating of non-metallic texture for use on metal
surfaces that provides reduced infrared emittance. Previous
camouflage coatings and paints used on hulls of naval vessels often
exhibited relatively high solar absorption because of the dark
colors and diffused finishes that are characteristic of the
coatings. This high solar absorption resulted in high surface
temperatures that increase cooling requirements and more
importantly increased infrared radiation. In modern warfare,
infrared detection techniques have become highly developed and
means for counter-detection techniques are accordingly required.
Artificial cooling of hot exposed surfaces is effective to reduce
infrared emission. However, this method increases electrical power
requirements aboard ship as well as adding parasitic weight and
volume to equipment aboard the ship.
[0015] This low infrared emittance coating is applied as a paint to
provide a durable opaque coating suitable for use on exposed
surfaces of naval vessels or on hot surfaces of a gas turbine
exhaust. Ideally, such coated surfaces exhibit low reflectance in
the visual portion of the light wavelengths and high reflectance in
the infrared portion. The paint is a mixture of colorant and
emitance control pigments such as aluminum, zinc sulfide, antimony
trisulfide, and blue pigments; aluminum oxide filler; silicon alkyd
resin binder; polarized montmorillite clay; and a diluent. Like
traditional military paints, it utilizes some fraction of visually
absorptive pigments, that do not have wavelength specific or
optimized infrared properties; their reflectance tends to be
constant over different wavelength bands, which compromises its
infrared performance.
[0016] Various flakes or pigments have been made that have
optically selective or optically variable properties. Some
optically selective pigments have interference structures that
enhance or suppress a portion of the visible spectrum to achieve a
desired color, and are generally used in colorful paints, inks,
plastics, and other carriers. Some optically variable pigments are
similarly directed at the visible spectrum and shift color as the
location of the observer changes. The interference structures
typically include thin film layers of spacer (dielectric) and
absorber materials over a reflector. Similar flakes utilize optical
coating structures to selectively absorb solar radiation in paint
intended for passive solar energy systems; however, the thermal
emittance characteristics of the paint appears to be influenced by
the infrared absorption spectra of the paint vehicle.
[0017] Prior technology for thermal control of visually opaque
objects resulted in either a highly reflective metallic appearance,
in the case of broadband visual IR reflectors, or a black color, in
that materials selectively absorbing in the solar IR region are
also absorbing in visual wavelengths. Other attempts at reducing
the chroma of coatings often include adding a darkening agent to
the carrier or binder. This often detracts from the IR performance
of the coating. Attempts to achieve other visual colors resulted in
some compromise of the thermal control properties
[0018] Accordingly, it would be desirable to provide flake-like
pigments that have low reflection in visible light in a range of
colors, with selectable visible color characteristics being
independent from their IR characteristics.
[0019] Another object of the present invention is to provide
thermal control of visually opaque objects, especially those having
arbitrary or irregular shape by application of a coating or foil
that allows selective absorption of light at visible wavelengths,
and reflection of light at IR wavelengths. It is further desirable
that thermal control coatings have a range of independently
selected color and chroma in the visible wavelengths.
[0020] Another objective of the present invention to provide
efficient solar energy collection absorbing material with low
thermal emittance, and that solar energy collection absorbing
material be available in a selection of colors.
BRIEF SUMMARY OF THE INVENTION
[0021] The present invention provides optical interference
structures that appear dark or have low chroma in the visible
portion of the spectrum and relatively high reflectivity in the
infrared portion of the spectrum. In one embodiment the optical
interference structure includes a reflector, spacer layer, and
absorber layer. The absorber layer has a thickness that provides a
transmittance of between about 5-85%. In other embodiments the
thickness of the absorber layer and spacer layer are selected
according to the reflectivity of the reflective layer. In some
embodiments, the optical interference structures have a chroma of
less than 50 and a reflectivity in the infra-red portion of the
spectrum of more than 50%, and in some cases greater than 80%.
[0022] In some embodiments the optical interference structures are
used in pigments, such as by forming the optical interference
structure on one or both sides of a pigment flake, or forming the
structures on a roll of polymer film, and then separating and
processing the deposited film structure into pigment flakes. In
other embodiments, the optical interference structures are
deposited onto a substrate, such as a sheet of foil, that is than
attached to an object, or directly onto an object, such as a panel.
The foil or object can be reflective and serve as the reflector in
the resulting interference structure.
BRIEF DESCRIPTION OF THE DRAWINGS
[0023] FIG. 1A is a simplified cross section diagram of a
multi-layer interference structure according to an embodiment of
the present invention.
[0024] FIG. 1B shows the calculated performance of two different
structures as a function of absorber thickness.
[0025] FIG. 1C shows the calculated performance of two different
structures as a function of absorber thickness.
[0026] FIG. 2A is a simplified cross section diagram of a portion
of a pigment flake according to an embodiment of the present
invention.
[0027] FIG. 2B is a simplified cross section diagram of a pigment
flake according to an embodiment of the present invention.
[0028] FIG. 2C is a simplified cross section of a pigment flake
according to another embodiment of the present invention.
[0029] FIG. 2D is a simplified cross section of a pigment flake
according to another embodiment of the present invention.
[0030] FIG. 2E is a simplified cross section of a pigment flake
according to another embodiment of the present invention.
[0031] FIG. 3A is a simplified cross section diagram of a
multi-layer interference structure with a center thickening layer
according to an embodiment of the present invention.
[0032] FIG. 3B is a simplified cross section of a pigment particle
according to another embodiment of the present invention.
[0033] FIG. 3C is a simplified cross section of a portion of a
pigment particle according to another embodiment of the present
invention.
[0034] FIGS. 4A and 4B are graphs of the predicted reflectance
versus wavelength for an embodiment of the present invention.
[0035] FIGS. 5A and 5B are graphs of the measured reflectance
versus wavelength for an embodiment of the present invention.
[0036] FIGS. 6A and 6B are graphs of the predicted reflectance
versus wavelength for another embodiment of the present
invention.
[0037] FIGS. 7A and 7B are graphs of the predicted reflectance
versus wavelength for another embodiment of the present
invention.
[0038] FIGS. 8A-8C are simplified cross sections of films and foils
according to embodiments of the present invention.
[0039] FIGS. 9A and 9B are simplified cross sections of polymeric
sheets according to embodiments of the present invention.
[0040] FIG. 10 is a simplified cross section of a paint layer
applied to a surface according to an embodiment of the present
invention.
[0041] FIG. 11 is a simplified plan view of an image according to
an embodiment of the present invention.
DETAILED DESCRIPTION OF THE INVENTION
[0042] The present invention relates to optical thin film
structures that provide low perceived color and relatively high IR
reflectivity. Embodiments of the invention may be embodied as
pigment flakes for use in paints, inks, plastic sheets (films),
plastic objects, and powder coatings, as foils that are attached to
objects, or coatings that are formed directly on objects. In some
embodiments, the optical thin film structures appear very dark or
even black. Objects coated with pigments, foils, or coatings
according to these embodiments of the invention have low perceived
color because of the low lightness, even though the measured chroma
may be fairly high. In other embodiments, a pigment, foil, or
coating appears gray, which may have high lightness in combination
with relatively low chroma. In yet other embodiments, the optical
thin film structures can be selected to provide a low level of
color. Typically, such optical thin film structures exhibit little
goniometric color shifting, unlike what are commonly known as
optically variable pigments.
[0043] Table 1 briefly outlines some of the various embodiments of
the present invention. The average reflectance from 400-700 nm is
basically a measure of the lightness (L*) in the visible region.
The average reflectance between 4-40 micrometers is basically an
indication of the IR reflectance, and the chroma (C*.sub.ab
according to CIE.TM. colormetric conventions) is basically an
indication of the visible color characteristic of the surface or
object. A high IR reflectance is desirable to reduce IR emissivity,
such as for solar energy collectors or IR camouflage.
TABLE-US-00001 TABLE 1 Comparison of Optical Attributes Between
Some Embodiments of the Present Invention Ave. Reflectance Ave.
Reflectance Appearance 400-700 nm 4-40 microns Chroma (C*.sub.ab)
Black <20% >50% up to 50 Gray <50% >50% <5 Low Color
<50% >50% <20
[0044] Other types of pigments are designed to provide high chroma
and a high degree of optical variance, i.e. color change, with
viewing angle. However, in certain embodiments of the invention a
relatively neutral color of the pigment flakes arises from a
substantially constant reflectivity as a function of wavelength
within the visible spectral region. A change in viewing angle does
not produce a significant color change because the spectral
response remains relatively flat at shorter wavelengths.
[0045] Black, gray, and low-color optical thin film structures
according to some embodiments of the present invention are
relatively thin, compared to multi-layer high-chroma optical
thin-film stacks, for example. When depositing thin designs (e.g.
optical thin film stacks having a total thickness less than 250 nm)
onto flakes, it may be desirable to provide a stiffening layer(s)
or to form the optical design on stiff flakes, such as glass
flakes, which are discussed in further detail below.
[0046] I. General Description of Optical Thin Film Structures
According to Embodiments of the Present Invention
[0047] FIG. 1A is a simplified cross section of a multi-layer
interference structure 10 according to an embodiment of the present
invention. The structure includes an optical thin film stack 15
deposited on a substrate 11. The substrate could be a flake, such
as a glass or metal flake, a foil or film, or an object, such as a
structural panel. Only one side of the substrate is shown with an
optical thin film stack, but the opposing side of the substrate
could also have an optical stack, being the same as or different
from the one illustrated. Flakes are often coated symmetrically on
both sides, as further discussed in relation to FIGS. 2A and 2B,
below.
[0048] The first layer 12 of optical stack 15 is reflective in at
least the infrared wavelength range of interest. A spacer layer 13
overlies the IR-reflective layer 12. The spacer layer can be either
a dielectric or semiconductor material, but in this embodiment is a
dielectric material. A layer of absorber material 14 is coated onto
the spacer layer 13. The spacer and absorber layers are in optical
communication with each other and the underlying reflective layer
in the sense that they form an optical interference coating in
which the incident light is selectively attenuated by destructive
interference and/or induced absorption. It will be recognized by
those skilled in the art of optical coating design that a single
layer can be replaced by a plurality of multiple layers without
substantially affecting the function, that is the optical
communication of the aforementioned layers as set forth above.
Similarly, the substrate itself may be reflecting and act as a
reflector. In that case the separate reflective layer might then be
omitted. Thus, the recitation of a single layer in optical
communication with adjacent layers is intended to encompass such
replacements and substitutions.
[0049] The optical stack 15 may comprise additional layers of
dielectric-absorber (D-A) layer pairs. The D-A layer pairs may
comprise the same sets of materials or different materials; for
example layer sequence R/D.sub.1/A.sub.1/D.sub.2/A.sub.2, where R
is the reflector layer and the subscripts 1 and 2 denote different
materials in the classes of spacers and absorbers. The stack can
have other structures, for example a layer sequence
R/D.sub.1/A.sub.1/D.sub.2 in which the absorber layer is overcoated
or in optical communication with a second dielectric layer D.sub.2.
When the thickness of D.sub.2 is less than about 8 times that of
layer D.sub.1, layer D.sub.2 affects and can enhance the
performance of the optical stack 15, and act as an anti-reflective
coating in some instances. At thicknesses above about 8 times layer
D.sub.1, layer D.sub.2 is used primarily as a protective
overcoat.
[0050] The thickness of the overcoat may be selected according to
the intended application. For example, if the optical thin film
structure is formed on a pigment flake, the overcoat might be
relatively thick for use in a paint formulation, and relatively
thin for use in an extruded plastic sheet. The thickness of the
overcoat may be selected according to the improved rigidity it
provides so that the pigment flakes can withstand high-stress
processes, and/or according to the desired protection from the
environment. A flake intended for use in a carrier that provides a
high degree of protection from the environment, or for use in a
relatively benign environment, might have a thinner overcoat or no
overcoat, while a flake intended for use in a harsh environment
might have a more substantial overcoat.
[0051] The design of the optical stack, which is primarily the
thicknesses and compositions of the reflector, dielectric and
absorber layers, can be varied according to the teachings of the
invention to selectively control the visible color and the infrared
properties. The thickness of these layers may be characterized by a
physical thickness, t, in for example micrometers, or by the
quarterwave optical thickness ("QWOT") with respect to light of a
particular wavelength, .lamda., wherein n is the refractive index
of the layer at designated wavelength: QWOT=t/4.times.n(.lamda.)
(Eq. 1)
[0052] While the optimized thickness of these layers will depend on
their optical properties, such as refractive index and extinction
coefficient at visible and infrared wavelengths, the thickness of
the absorber material is generally selected to control the visible
reflectivity of the stack based on the desired visible and infrared
performance. As the thickness (t.sub.a) of the absorber material
increases from zero thickness, the optical stack reflectivity
decreases from a value characteristic of the reflective layer,
R.sub.r (.lamda..sub.vis) to a minimum value. This reflectance drop
is due to increasing levels of destructive interference between
light beams leaving the reflector layer and those leaving the
partially-reflecting absorber layer. Further increases in absorber
thickness cause the device's visible reflectance to increase from
the minimum value to a higher value consistent with the inherent
reflectivity of the absorber material. In some embodiments, the
substrate can be reflective, and the separate reflective layer can
be omitted. Similarly, in some embodiments the reflective minimum
lies outside the visible range, such as at 850 nm in the near IR or
at 300 nm in the near ultraviolet ("UV"). These wavelengths are
merely exemplary.
[0053] FIGS. 1B and 1C illustrate the calculated performance of
different structures as a function of absorber thickness for an
optical stack using an aluminum reflector, which is relatively
bright, and an optical stack using a chromium reflector, which is
not as reflective as aluminum. The curve 26 shown as a dotted line
represents the predicted reflectance at 510 nm of an aluminum
reflector with one quarter-wave (at 470 .mu.m) thickness of
magnesium fluoride, and a chromium absorber. The curve 28 shown as
a solid line represents the predicted reflectance at 510 nm of a
chromium reflector with one quarter-wave (at 460 nm) thickness of
magnesium fluoride, and a chromium absorber. The spacer thickness
may be greater or less than the examples, and a change in the
spacer thickness sometimes results in an adjustment to the
thickness of the absorber layer to achieve minimum reflectance in
the visible spectrum.
[0054] FIG. 1C illustrates that as the absorber layer gets thicker,
the reflectivity of the stacks rises from the minimum until it
reaches the reflectivity of the absorber material itself. Stated
differently, devices with infinitely thick absorbers no longer act
as interference devices but instead have the appearance and
performance of the absorber material across both the visible and
infrared portions of the spectrum. Although a reflectivity minimum
of about zero is attained with each stack, the optimum value of the
absorber layer thickness for an optical stack using a relatively
dark reflector is less than the optimum absorber thickness for an
optical stack with a brighter reflector. Similarly, the optimum
thickness of the spacer layer used with the darker reflector also
decreased slightly.
[0055] The absorber thickness depends upon the desired levels of
visible reflectance and infrared reflectance. For the device to
have a dark appearance and a high far-infrared reflectance, the
thickness of the absorber should provide the minimum or
near-minimum reflectance in the visible region. This value will be
called tabs.sub.min (see FIG. 1B, ref. num. 29) for the optical
stack with the aluminum reflector. When an infrared reflectance
more like the opaque absorber material (generally lower) is
desired, the thickness of the absorber should be greater than
tabs.sub.min. Conversely, when the visible reflectance of the
device is desired to be closer to that of the bare reflector, the
thickness of the absorber should be less than tabs.sub.min. In the
range of about 0-3.times.tabs.sub.min the visible performance of
the device can be selected without significantly degrading the
far-infrared thermal performance of the device. The optimal
absorber thickness for other optical stacks may be different
depending on the type of reflector and spacer thickness.
[0056] The materials for the reflector layers are selected to have
the reflective characteristics suitable for the intended use of the
foil or pigment. A preferred reflector material is aluminum, which
has good reflectance characteristics, inexpensive, and is easy to
form into a thin layer. It will be appreciated in view of the
teachings herein, however, that other reflective materials may be
used in place of aluminum, such as silver, iron, tantalum, iridium,
rhenium, copper, silver, gold, platinum, palladium, nickel, cobalt,
niobium, chromium, tin, and combinations or alloys of these or
other metals or other materials that reflect in the infrared
spectrum of interest. Other useful reflective materials include,
but are not limited to, the transition and lanthanide metals and
combinations thereof; as well as metal carbides, metal oxides,
metal nitrides, metal sulfides, combinations thereof, or mixtures
of metals and one or more of these materials. Accordingly, specific
examples of suitable IR reflecting materials include indium oxide,
indium tin oxide (ITO), europium oxide (Eu.sub.2O.sub.3), vanadium
pentoxide (V.sub.2O.sub.5), rhenium oxide (ReO.sub.3), lanthanum
boride (LaB.sub.6), combinations thereof, and the like. The
thickness of the reflective layer is selected so that it is at
least semi-reflective, but preferably opaque at infrared
wavelengths. The reflectivity of the reflective layer is preferably
greater than 50% over the wavelength range of 4 to 40 micrometers,
and the thickness of the reflective layer can be increased to
improve the stiffness of pigment particles or improve handling.
[0057] The spacer layers 23a and 23b are typically made of
materials having indices of refraction in the range from about
1.2-4.5. The spacer layers can be composed of various materials
such as those having a "high" refractive index, i.e. greater than
about 1.65. Nonlimiting examples of suitable high index materials
include zinc sulfide (ZnS), zinc oxide (ZnO), zirconium oxide
(ZrO.sub.2), titanium dioxide (TiO.sub.2), diamond-like carbon,
indium oxide (In.sub.2O.sub.3), indium-tin-oxide ("ITO"), tantalum
pentoxide (Ta.sub.2O.sub.5), ceric oxide (CeO.sub.2), yttrium oxide
(Y.sub.2O.sub.3), europium oxide (Eu.sub.2O.sub.3), iron oxides
such as (II)diiron(III) oxide (Fe.sub.3O.sub.4) and ferric oxide
(Fe.sub.2O.sub.3), hafnium nitride (HfN), hafnium carbide (HfC),
hafnium oxide (HfO.sub.2), lanthanum oxide (La.sub.2O.sub.3),
magnesium oxide (MgO), neodymium oxide (Nd.sub.2O.sub.3),
praseodymium oxide (Pr.sub.6O.sub.11), samarium oxide
(Sm.sub.2O.sub.3), antimony trioxide (Sb.sub.2O.sub.3), silicon
(Si), silicon monoxide (SiO), germanium (Ge), selenium trioxide
(Se.sub.2O.sub.3), tin oxide (SnO.sub.2), tungsten trioxide
(WO.sub.3), combinations thereof, and the like. Other suitable high
index materials include mixed oxides. When used as spacer layers,
materials are most commonly oxidized to their stoichiometric state,
such as ZrTiO.sub.4, but may be sub- or super-oxidized.
Non-limiting examples of such mixed oxides include zirconium
titanium oxide and niobium titanium oxide.
[0058] Some spacer materials exhibit absorption in the far
infrared. Because the spacer layers are relatively thin, generally
only one or two quarter-waves in optical thickness in the visible
spectrum, inclusion of spacer layers with IR absorbing material
does not unduly affect the IR emittance of devices.
[0059] Spacer layers can be either selective or non-selective in
the visible region. When selectively absorbing in the visible, the
spacer works together with the absorber layer via optical
interference to modify the reflected color, generally attenuating
the reflection over the wavelengths where the spacer absorbs. This
combinatory effect provides color shades that are not otherwise
available with optical interference structures having non-selective
spacer layers. At the same time, the structures can provide high
infrared reflectance. Examples of selectively absorbing spacer
materials include iron oxide, tungsten oxide, copper oxide, and
cobalt oxide.
[0060] The spacer layers can each be composed of the same material
or different materials, and can have the same or different optical
or physical thickness for each layer. It will be appreciated that
when the spacer layers are composed of different materials or have
different thicknesses the pigment flakes exhibit different colors
on each side, and the resulting mix of flakes in a pigment or paint
mixture would show a new color that is the combination of the two
colors. The resulting color would be based on additive color theory
of the two colors coming from the two sides of the flakes. In a
multiplicity of flakes, the resulting color would be the additive
sum of the two colors resulting from the random distribution of
flakes having different sides oriented toward the observer.
[0061] When a high level of visible absorption (dark appearance) is
desired, the spacer layer preferably has an optical thickness of
about 1.0 QWOT at 200 nm to about 2.0 QWOT at 500 nm, and most
preferably about 1.0 QWOT at 300 nm to about 1.0 QWOT at 700 nm.
For maximum solar absorbance, the refractive index of the spacer
layer is more preferably less than 2.0, most preferably less than
about 1.65. Use of a low index dielectric material broadens the
wavelength region of low reflectance, thus increasing the level of
solar absorption. Examples of low-index materials include silicon
dioxide (SiO.sub.2), aluminum oxide (Al.sub.2O.sub.3), metal
fluorides such as magnesium fluoride (MgF.sub.2), aluminum fluoride
(AlF.sub.3), cerium fluoride (CeF.sub.3), lanthanum fluoride
(LaF.sub.3), sodium aluminum fluorides (e.g., Na.sub.3AlF.sub.6 or
Na.sub.5Al.sub.3F.sub.14), neodymium fluoride (NdF.sub.3), samarium
fluoride (SmF.sub.3), barium fluoride (BaF.sub.2), calcium fluoride
(CaF.sub.2), lithium fluoride (LiF), combinations thereof, or any
other low index material, i.e. a material having an index of
refraction of about 1.65 or less. For example, organic monomers and
polymers can be utilized as low index materials, including dienes
or alkenes such as acrylates (e.g., methacrylate),
perfluoroalkenes, polytetrafluoroethylene (e.g. TEFLON.RTM.),
fluorinated ethylene propylene ("FEP"), combinations thereof, and
the like.
[0062] It should be appreciated that several of the above-listed
dielectric materials are typically present in non-stoichiometric
forms, often depending upon the specific method used to deposit the
dielectric material as a coating layer, and that the above-listed
compound names indicate the approximate stoichiometry. For example,
silicon monoxide and silicon dioxide have nominal 1:1 and 1:2
silicon:oxygen ratios, respectively, but the actual silicon:oxygen
ratio of a particular dielectric coating layer varies somewhat from
these nominal values. Such non-stoichiometric dielectric materials
are also within the scope of the present invention.
[0063] Suitable materials for the absorber layer include metals,
alloys, and compounds that can be reliably deposited at a thickness
at which they are semi-transparent at visible wavelengths. The
semi-transparent layer may have either uniform absorption, i.e.
neutral density, or selective absorption across the wavelengths of
the visible spectrum, or selective absorption between the visible
and IR regions, depending on the desired coloration and the color
of the native reflector layer. It should be understood that the
absorber coating at this thickness does not need to be continuous
to still work as an optical absorber. For example, a plurality of
islands or dots of absorber material can suffice as an absorber.
Examples of suitable metals include chromium, nickel, iron,
titanium, aluminum, tungsten, molybdenum, niobium, combinations,
compounds or alloys thereof, such as INCONEL.TM. (Ni--Cr--Fe),
metals mixed in a dielectric matrix, or other substances that are
capable of acting as a uniform or selective absorber in the visible
spectrum. Alternatively, the absorber can also be a dielectric
material such as an iron oxide (e.g., Fe.sub.2O.sub.3), silicon
monoxide (SiO), chromium oxide (Cr.sub.2O.sub.3), carbon, titanium
nitride (TiN), titanium sub-oxide (TiO.sub.x where x is less than
2.0), combinations thereof, and the like.
[0064] FIG. 2A is a simplified cross section of a pigment particle
20 with a symmetrical multi-layer interference structure according
to another embodiment of the present invention. The spacer layers
23a, 23b, and absorber layers 24a, 24b, are symmetrical about the
reflector 22. The diameter of the pigment particle (parallel to the
plane of the layers) is typically about 5 microns to about 100
microns, but preferably from about 10 microns to about 40 microns,
and may be any of a variety of shapes, including irregular shapes.
Although the particle is shown as an essentially planar stack, flat
layers are not required. In some instances, the particle can take
on an irregular shape, either as seen in a plan view, or cross
section. In a particular embodiment, the particle is shaped
similarly to a lima bean. The deposited layers are generally
locally parallel to the surface on which they are deposited. Some
techniques of layer formation on flakes, such as sol-gel
techniques, tend to create rounded particles.
[0065] The pigment particle 20 has a central reflective layer 22.
The reflective layer has dielectric or other spacer layers 23a and
23b on each major surface, with absorber layers 24a and 24b
deposited on the spacer layers. Pigment particles according to
embodiments of the present invention may include additional layers
of dielectric-absorber pairs. For example, layer sequence
A.sub.2/D.sub.2/A.sub.1/D.sub.1/R/D.sub.1/A.sub.1/D.sub.2/A.sub.2
uses two dielectric-absorber pairs D.sub.1-A.sub.1 and
D.sub.2-A.sub.2. The D-A layer pairs may have the same materials or
different materials on each side of the reflective layer. One side
of the pigment particle might have a different number of layers
than the other, for example
A.sub.1/D.sub.1/R/D.sub.1/A.sub.1/D.sub.2/A.sub.2. Similarly, the
layers may be of different materials, such as
A.sub.1/D.sub.1/R/D.sub.2/A.sub.2 or A/D.sub.1/R/D.sub.1/A.sub.2,
etc., or corresponding layers on opposite sides of the reflective
layer might be of different thicknesses. The pigment particle 20
may have other structures, for example layer sequence
D.sub.2/A.sub.1/D.sub.1/R/D.sub.1/A.sub.1/D.sub.2 in which the
absorber layers 24a and 24b would be overcoated with additional
dielectric layers (not shown). In some instances, it may be
desirable to overcoat an optical stack with a dielectric layer that
does not significantly alter the optical properties of the stack,
but provides environmental protection to the stack.
[0066] When the thickness of such an overcoat dielectric layer is
less than about 8 times that of layer of the first dielectric layer
23a, the overcoat dielectric layer affects and can enhance the
performance of the pigment particle, in some cases acting as
anti-reflective layer. At thicknesses above about 8 times the
thickness of the first dielectric layer, the overcoat dielectric
layer is used primarily as a protective overcoat.
[0067] FIG. 2B is a simplified cross section of a pigment flake 21
according to an embodiment of the present invention showing the
central reflective layer 22 surrounded by a spacer layer 33 and an
absorber layer 34. The central reflective layer could be a rigid
flake with a reflective thin film layer deposited on both sides, or
a metal flake, for example.
[0068] FIG. 2C is a simplified cross section of a pigment particle
110 according to another embodiment of the present invention. The
pigment particle has improved rigidity and handling characteristics
achieved by the addition of one or more central stiffening or
thickening layers 112. The particle also includes reflector layers
114a and 114b that form part of the optical stacks 116a and 116b,
which include spacer and absorber layers (not individually shown).
The stiffening layer can be made from a wide variety of different
materials including metals, alloys, dielectrics, and
semiconductors.
[0069] Stiffer particles are desirable because they better survive
higher-shear processes used in spray painting and because their
stiffness allows for easier size-reduction processes (i.e. milling
or grinding), while maintaining the flatness of the particle.
Maintaining flatness is desirable so that the aggregate effect of
the particles applied to a surface is similar to the optical
characteristics of a foil with a similar optical thin film stack
applied to the surface. The stiffening layer typically has a
thickness in the range of 10 nm to 101m, preferably between 200 nm
and 2 .mu.m, which can improve handling, such as sizing and
dispersing, in addition to stiffening the particles. The reflector
layers 114a and 114b can be of the same types as reflector layers
12 and 22 described above. Similarly, it should be appreciated that
optical stacks 116a and 116b can be of the same types as optical
stacks described above in relation to FIGS. 1A and 2A, and can be
symmetrical or non-symmetrical.
[0070] FIG. 2D is a simplified cross section of a pigment flake 60
according to another embodiment of the present invention. The
pigment flake 60 has a central pre-flake 61. The pre-flake 61 has a
central layer or core 61a formed of a reflective material onto
which are disposed layers of transparent material 61b, 61 b' having
a sufficiently high stiffness to reinforce the reflecting layer and
make the pre-flake 61 substantially rigid. The core 61 is aluminum
about 30 nm thick, which is generally opaque, but could be other
materials or thicknesses. The transparent layers 61b, 61b' are
SiO.sub.x, (where x is less than 2.0) about 10-50 nm thick, but
could be other materials. These silicon oxide layers are
transparent and provide stiffness in conjunction with the aluminum
reflective layer.
[0071] A dielectric layer 62 is then coated on the preflake 61,
followed by deposition of an absorber layer 63. The dielectric and
absorber layers are coated on all sides of the preflake, including
its ends. The thickness and material of the dielectric layer 62 is
selected taking into account the optical thickness of transparent
layers 61b and 61b' to provide low chroma.
[0072] FIG. 2E is a simplified cross section of a pigment flake 70
according to another embodiment of the present invention. The
dielectric layer 72 is less than about 250 nm in thickness. A
reflective layer 71a is deposited on a stiff flake 71, which may be
desirable in combination with the relatively thin dielectric layer
to provide a stiff pigment particle. Rather than incorporating a
central vacuum-deposited stiffening layer or forming a multi-layer
pre-flake by a vacuum deposition method (and subsequent stripping
and grinding to produce appropriately sized flakes) the thin film
layers are deposited in sequence on a relatively flat and
substantially rigid particle, such as glass, mica, alumina, iron
oxide, graphite, bismuth oxychloride, boron nitride, polymer or
metal or similar particle. By coating a relatively flat flake 71
with a reflective layer 71a, one creates a pre-formed platelet-like
flake suitable for further coating, similar to the preflake 61
discussed in accordance with FIG. 6. In this case, the reflective
layer surrounds the stiff flake. Examples of methods for coating
such relatively flat and substantially rigid particles are chemical
vapor deposition (CVD), physical vapor deposition (PVD), including
sputtering, and electroplating. A spacer layer 72 is deposited to
surround the reflective layer 71a, and an absorber layer 73 is
deposited to surround the spacer layer.
[0073] FIG. 3A is a simplified cross section of a pigment flake 80
according to another embodiment of the present invention. The
relative thicknesses of the layers are not shown to scale. A
reflective preflake 81 includes reflective layers 81b, 81b',
separated by a rigid layer 81a. The reflector layers 81b, 81b' are
typically opaque or nearly opaque; therefore, the optical
properties of the rigid layer are not important. The material and
thickness of the rigid layer are selected according to the overall
thickness and mechanical properties of the other thin film
materials in the multi-layer pigment, which include a spacer layer
82 and an absorber layer 83. The rigid layer could be made of
metal, dielectric material, semiconductor material, or organic
material.
[0074] The thickness of the rigid layer is typically between about
10 nm to 10 .mu.m, more preferably from about 100 nm to about 2.0
.mu.m and most preferably from about 200 nm to about 500 nm,
depending on the material of the rigid layer and the intended
deposited layers.
[0075] In a particular embodiment, the rigid layer 81a is a layer
of silicon monoxide (SiO or SiO.sub.x where x<2) about 250 nm
thick covered on both sides with reflector layers 81b, 81b' of
opaque iridium. Increasing the total thickness of the thin film
structure in this manner aids in stripping the materials off a
plastic web substrate, such as is used in roll-coating techniques,
to form preflakes or platelets for pigments according to
embodiments of the invention. Additionally, thicker pigment
particles were found to be easier to sort (size) and handle
compared to optically equivalent, yet physically thinner
designs.
[0076] When such a multilayer thin film interference coating is
stripped from a supporting substrate or web, the flakes or
platelets typically range in size (distance across the face) from
2-200 .mu.m. The platelets can be further reduced in size as
desired. For example, the flakes can be subjected to an air grind
to reduce their size to a size ranging typically from about 2-50
micrometers without adversely affecting their optical
characteristics. The flakes or platelets are produced to have an
aspect ratio of at least 2:1 and preferably about 5:1 to about
15:1, with a narrow particle size distribution. The aspect ratio is
ascertained by taking the ratio of the largest dimension of a
surface of the flake parallel to the planes of the layers forming
the thin film to the thickness dimension of the platelet.
[0077] FIG. 3B is a simplified cross section of a pigment particle
84 according to another embodiment of the present invention. In
this case the preflake includes a rigid layer 81a, reflector layers
81b, 81b', and spacer layers 85, 85'. The thin film layers can be
roll-coated onto a film and then removed and processed into
platelets of desired size, as discussed in conjunction with FIG.
3A, above. The absorber layer 86 surrounds the preflake.
[0078] FIG. 3C is a simplified cross section of a pigment particle
88 according to another embodiment of the present invention. A
rigid layer 81a, reflective layers 81b, 81b', spacer layers 85, 85'
and absorber layers 87, 87' have all been formed on film and then
removed and processed into platelets of desired size. The rigid
layer is sufficiently thick to provide the desired handling
characteristics.
[0079] In order to impart additional durability to interference
pigment flakes according to embodiments of the present invention,
it is sometimes desirable to anneal or heat treat the platelets at
a temperature ranging from about 200.degree. C. to about
300.degree. C., preferably from about 250.degree. C. to about
275.degree. C., for a period of time ranging from 10 minutes to 24
hours, preferably about 15-30 minutes in air or an inert
atmosphere, such as N.sub.2 or Ar.
[0080] It should be appreciated that although FIGS. 2A, 2B, and 2E
show structures in which each layer completely surrounds the layer
underneath, devices with essentially equivalent performance can be
achieved with layers that do not surround those layers underneath,
such as shown in FIGS. 2C, 2D, and 3A-3C. Similarly, while optical
stacks according to the invention have been illustrated with single
spacer-absorber layers, multiple spacer-absorber layer pairs could
be used. In some embodiments, a functional layer may be made up of
more than one material. For example, a thin, non-opaque highly
reflective layer might be formed on a less-reflective particle, or
the spacer layer might be made up of multiple layers of dielectric
material, as discussed above in conjunction with FIG. 6A.
[0081] The pigment flakes described in accordance with FIGS. 1A,
2A-2E, and 3A-3C can also be manufactured using a PVD process to
deposit the layers. A collection of flakes can be produced by
forming a symmetrical multi-layer thin film structure on a flexible
web of material and separating the thin film structure from the web
to provide a collection of platelets. While some pigment flakes
made according to embodiments of the present invention using roll
coating techniques, particularly relatively thin flakes, perform
well optically, they can be difficult to strip from the plastic web
and to process down to size desirable for use in paints and inks
without a stiffening layer. Other embodiments are easily stripped
from the plastic web. In some applications, the desired particle
size is about 20 .mu.m. In other applications, it may be desirable
to use particles in the range of about 5 microns to about 100
microns across.
[0082] Although highly reflective particles according to some
embodiments of the present invention can have low chroma, it is
generally desirable that optical stacks according to the present
invention have an average reflectance less than about 50% in the
visible spectrum. Chroma (C*.sub.ab) is generally the degree of
perceived color of an object compared to a gray object having the
same lightness (L*) and is further defined according to the CIE
1976 L*a*b* color system by the formula
C*.sub.ab=(a*.sup.2+b*.sup.2).sup.0.5. Even objects with low
average reflectivity can at the same time have a non-uniform
reflectivity imparting color, i.e. chroma, to the object. Thus it
is further desirable that the chroma of an optical stack, or
pigment particles or foils incorporating optical stacks according
to embodiments of the present invention have a chroma less than
about 20. Other embodiments, such as foils, surfaces, or pigment
particles that appear black, may have higher chroma because the
lightness is so low, typically less than about 5. In these
embodiments chroma may be as high as 50 without imparting
significant perceived color.
[0083] II. An Optical Thin Film Structure with a Black
Appearance
[0084] In a multilayer interference structure of an embodiment,
performance factors such as infrared emittance, solar absorbance,
and visible color values are determined by the choice of number of
layers, the materials and their thicknesses. When a black visible
appearance is desired, the absorber thickness is chosen in
combination with the reflector according to the absorber material
to reduce the reflectance of the optical stack in the visible
spectrum. For example, if the reflector layer is aluminum, a
preferred absorber has a visible transmittance of about 50%, which
is considered moderate transmittance, to reduce the average
resulting visible reflectance of the optical stack to less than
about 20%. In contrast, if the reflector is chromium, tantalum, or
another material having a lower reflectivity than aluminum, the
absorber layer transmittance may be increased in correspondence to
the lower visible reflectivity of the reflector layer.
[0085] FIG. 2B represents one type of pigment flake configuration
that could be used for embodiments of the present invention. This
type of flake is symmetrical, in other words, the coating layers
are essentially the same on all sides. Such symmetry is not
required. For example, flakes might have symmetry only with regards
to the layers on the major surfaces, or might have different thin
film layers on different surfaces.
[0086] In one embodiment, a pigment flake in accordance with FIG.
2B has a central reflector layer of aluminum about 100 nm thick, a
dielectric layer of MgF.sub.2 having a thickness of about 1.0 QWOT
@ 480 nm to provide minimum reflectance in the visible region, and
an absorber layer of chromium with a thickness of about 6 nm to
provide about 50% transmission through the as-deposited chromium
layer.
[0087] The absorber thickness is chosen to give the minimum
reflectance over the visible spectrum, with the minimum reflectance
centered around 510 nm. The design appears black to the human eye,
with an anticipated lightness (L*) of about 6 and a chroma
(C.sub.ab*) of about 50.
[0088] A flake-like pigment according to such a design is
preferably mixed into a low emittance polymer binder and applied
like paint, turning surfaces into a high efficiency solar absorber.
FIG. 4A illustrates the predicted visible performance of the device
described above, while FIG. 4B shows the predicted performance of
the same design over the visible and infrared wavelengths.
[0089] When used as a pigment, this design has several possible
advantages over traditional absorptive black pigments. For example,
decorative black paints according to embodiments of the present
invention can achieve a black metallic ("sparkly") effect. It is
believed that the sides of the flakes provide relatively strong
localized reflection in the visible region, thus providing the
sparkle. Alternatively the black pigment flakes could be mixed with
bright (reflective) flakes in a clear carrier (paint base) to
provide a gray sparkle finish. In conventional paint systems, a
black color is typically obtained by mixing fine carbon black or
similar pigment into the paint, which dulls reflectivity occurring
from reflective flakes.
[0090] One can achieve dark colors by changing the dielectric
thickness of the interference design. Increasing the dielectric
thickness gives colors of indigo and dark blue; decreasing the
thickness gives dark brown. The wavelength of minimum reflectance
decreases (toward blue/UV to values in the range of 200-510 .mu.m)
with decreasing dielectric thickness and increases (toward red/IR
to values in the range of 510-1500 nm) with increasing dielectric
thickness.
[0091] The design's reflectance is higher in the infrared than in
the visible portion of the spectrum, thus able to provide a covert
feature in a security device. When placed in outer space or in
outdoor locations, the design provides simultaneous high absorption
of solar wavelengths (0.2-2.5 .mu.m) and low emittance of thermal
wavelengths (4-40 .mu.m) making it an excellent solar absorber.
[0092] An optical design as described above for the pigment flake
discussed in conjunction with FIGS. 4A and 4B can be adapted for
deposition onto a foil. The foil can be laminated, glued, or
otherwise applied to another object, such as a solar absorber
module, to provide that object with enhanced optical absorption and
thermal retention.
[0093] III. An Optical Thin Film Structure with a Gray
Appearance
[0094] When a gray appearance is to be coupled with a moderate
infrared emittance (moderate infrared reflectance), the
transmittance of the absorber is chosen to be lower than for the
black case. For example, when the reflector is aluminum, a
preferred absorber has a visible transmittance of about 15% to
about 50% depending on the desired lightness, while the visible
transmittance can be as low as 5% and still function in this
manner. So now we have a desired absorber thickness providing
between 15-85% transmittance for a reflector with not less than 80%
reflectance, depending upon the degree of infrared emittance that
is desired. This selection allows one to create optical stacks with
similar visual characteristics, yet different IR
characteristics.
[0095] In another embodiment of the present invention, a pigment
flake in accordance with FIG. 2B has a central reflector layer of
aluminum about 80 nm thick, a dielectric layer of MgF.sub.2 with an
optical thickness of about 1.0 QWOT @ 500 nm, and an absorber layer
of chromium with a physical thickness of about 20 nm. In this
design, the absorber and dielectric thicknesses are chosen to give
a medium level of lightness (L*), with nominally uniform
reflectance over a range of wavelengths, or in other words, a gray
visible appearance. This embodiment provides a high level of
reflectance in the infrared. Devices of this type are useful in
several applications. For example, if some but not all of the sun's
energy is to be absorbed and retained. Another example is when both
visible and IR camouflage is desired for objects in the sky or on
the sea. A gray color is useful for the visible camouflage, while
the high IR reflectance prevents high emission of thermal energy
that could be observed by IR detectors.
[0096] This embodiment can provide advantages for military
applications, where night vision type thermal imaging scanners are
used to detect articles or objects warmer than their surroundings.
An article coated with either a foil or pigment-containing coating
according to embodiments of the present invention will emit less
thermal infrared energy than its uncoated counterparts, rendering
it less distinguishable from surrounding objects at night, as well
as providing visible coloration compatible with daytime camouflage.
Articles painted with traditional gray paints pigmented with
mixtures of carbon black and white TiO.sub.2, generally do not have
significantly suppressed IR emissions.
[0097] In general, simultaneous visual and IR camouflage of objects
from human and artificial surveillance and tracking devices can be
obtained with an opaque exterior coating having a low luminous
reflectance, low solar absorption, and low infrared emittance. In
other embodiments, a dark or moderately dark exterior coating
having a low luminous reflectance and high infrared reflectance is
desired. The exterior may serve as visual camouflage, either as a
solid color or as patterned colors.
[0098] FIGS. 5A and 5B are graphs illustrating the measured
reflectivity versus wavelength for an optical stack in accordance
with the example of the gray optical structure discussed above. The
reflectance of the device reaches a minimum value around 1.3 .mu.m
in the near infrared and then increases in the mid and far-infrared
regions. The dielectric thickness can vary from a low value such as
1.0 QWOT @ 200 nm to a higher value such as 1.0 QWOT @ 800 nm while
still providing a nominally gray appearance.
[0099] Varying the thickness of the absorber layer can modify the
reflectance profile. When the absorber thickness is decreased from
the thickness of the absorber layer that provides the minimum
reflectance (tabs.sub.min, which is about 50% transmittance for an
aluminum reflector), the pigment appears gray, rather than black.
For example, with an optical stack having a minimum reflectance at
510 nm, decreasing the absorber thickness increases the
transmittance through the absorber layer, resulting in a
progressive change in appearance from black to dark gray to medium
gray to light gray and finally to silver, at about 85%
transmittance through the absorber layer. Thus, the lightness
value, L*, is selectable based on the absorber thickness going from
a value near zero when ta=tabs.sub.min, increasing steadily to the
value of the bare reflector as ta approaches zero. All this while
the mid- and far-IR reflectance remains high. The choice of the
reflector can determine the final color or shade of gray. Foils or
pigments with highly reflecting (>80%) metal as the reflector
layer, such as aluminum or silver, approach their native
appearance, i.e. a silver color, with very thin absorber layers.
The use of metals or other materials with lower reflectivity, such
as iron, silicon or tantalum, as the reflector layer limits the
color to grays, even with very thin absorber layers.
[0100] When the absorber thickness is increased from the thickness
of the absorber layer that provides the minimum reflectance, the
pigment also appears grayish. However, as the absorber
transmittance is decreased from about 50% to 0% (increasing
absorber thickness) the optical stack progressively ceases to act
as an interference structure. The appearance of the optical stack
approaches that of the absorber layer, changing from black through
dark gray to medium gray, as the absorber layer becomes
substantially opaque. As the transmittance of the absorber layer
decreases from about 50% to 0%, the infrared emittance is also
affected and progressively approaches that of the opaque absorber
material. Devices in this range are very useful when it is
desirable to have both a moderate level of solar absorbance along
with a moderate level of emittance.
[0101] IV. Low-Color Optical Thin-Film Structures
[0102] When a neutral appearance is desired such as in the gray and
black examples above, the optical design of layer construction,
materials, and thicknesses is chosen to minimize the absolute
chroma. There are other optical designs that provide low color
purity and chroma but have some perceived color. For example, the
optical design that gives the maximum solar absorbance is not
always the design that provides a black appearance. In other cases,
a pigment or foil with a slightly, typically dull, colored
appearance might be desired for aesthetic reasons. Some of these
dull colors are variants of gray such as gray-green, gray-blue, and
steel gray. The low-chroma blue design, for example, is suitable
for applications where it is desirable to avoid visible detection.
Other colors can be considered variants of black such as dark
brown, dark blue, deep burgundy, dark green, and indigo. These
colors can be obtained using variations of the asymmetrical and
symmetrical embodiments above and at the same time provide the
desired levels of solar absorbance and infrared emittance.
[0103] Typically, to obtain thermal control structures with a dull
but colored appearance, the dielectric (spacer) thickness is
increased or decreased from that which gives neutrality (i.e. no
perceptible color). Starting from a neutral black, as the
dielectric thickness increases, the color typically changes from
black to indigo to dull blue to dull green. As the dielectric
thickness decreases, the color usually moves from black to dark
brown.
[0104] The dielectric or spacer layer for colored low-chroma
optical stacks preferably comprises materials having indices of
refraction in the range from about 1.2 up to 4.5 and preferably has
an optical thickness of between about 1 QWOT at 200 nm and 2 QWOT
at 700 nm, and more preferably about 1 QWOT at 300 nm to about 2
QWOT at 500 nm. The refractive index of the dielectric layers is
more preferably greater than 1.65, most preferably greater than
about 2.0. Selection of a high refractive dielectric material is
one way to minimize the variation in interference color with angle
incidence, that is, a shift in observed color as the observer
changes his position with respect to the coated object, or views a
plane or portion of the objected disposed at a non-parallel
orientation with respect to other portions of the object or article
(assuming a fixed light source). In comparison, optical stacks used
in applications where color shifting is desirable typically use
spacer layers made of materials with a refractive index less than
1.65, and more preferably less than about 1.5.
[0105] The color shifting tendencies of optical stacks according to
embodiments of the present invention can also be reduced by
reducing the thickness of a low-index dielectric layer. This
reduces the interference color and chroma as well as the color
shift in visible wavelengths. As the dielectric layers serve to
make the flake mechanically rigid, when the dielectric layers are
reduced in thickness, it is may be preferable to increase the
thickness and/or rigidity of the reflective layer or to provide a
stiffening layer.
[0106] In another embodiment of the invention, a pigment flake in
accordance with FIG. 2B has a central reflector layer 22 of
aluminum about 40 nm thick and a dielectric layer 33 about 1.0 QWOT
at 300 nm to about 2.0 QWOT at 550 nm in optical communication with
the reflector layer. The absorber layer 34 has a thickness
sufficient to reduce the internal transmission of the absorber
layer to about 50% across the visible spectrum. The overall average
reflectivity of the pigment flake is less than about 50% over the
visible spectrum.
[0107] The visible appearance of the pigment and resultant coatings
can be progressively modified from dark brown to black to indigo to
a dull blue to a dull green by adjusting the thickness of the
dielectric layer 33. For example, when a dull blue color with low
chroma is desired, the dielectric layer thickness is in the range
of about 2.0 QWOT @ 280 nm to 2.0 QWOT @ 450 nm. Alternatively, a
device having a dull green color with low chroma results when the
dielectric layer thickness increases to a range of about 2 QWOT @
450 nm to 2 QWOT @ 550 nm. When using a low-index dielectric,
increasing the dielectric thickness to greater than about 2 QWOT @
700 nm results in unstable chroma. Unstable chroma is a condition
where the perceived color depends on the angle of incident light.
For blue and green devices, the reflectance of the device reaches a
local minimum value in the near infrared, and then increases in the
mid- and far-infrared regions. By providing generally low
reflectance in the visible and near IR regions, while at the same
time achieving high reflectance in the mid- and far-IR regions,
this embodiment performs as a good solar absorber.
[0108] FIGS. 6A and 6B illustrate the calculated performance of
another embodiment of the present invention. Optical designs
according to this embodiment can incorporated into both foils and
pigments, such as a thermal control flake with a structure of
A/D/R/D/A. The approximate layer materials and thicknesses for this
example device are as follows: [0109] R=80 nm aluminum [0110] D=1.0
QWOT ZnS @ 200 nm [0111] A=27 nm carbon.
[0112] For this example, the absorber thickness is chosen to
provide about 45% internal transmittance (i.e. transmittance
in/through the absorber layer) in the visible region. The design
provides a dark (low lightness) burgundy color appearance and a
high infrared reflectance. The dielectric ZnS has a high refractive
index, so the reflectance in the mid infrared region is generally
higher than designs utilizing lower index dielectrics, which is an
advantage for applications requiring better performance in this
region. At the same time, the reflectance minimum in the solar
region is not as broad as the design described in association with
the black optical design. When utilized as a foil, the design can
be simplified to S/R/D/A, where S is an optional substrate.
[0113] FIGS. 7A and 7B are graphical illustrations of the
calculated (modeled) optical performance of a multi-layer
interference structure according to an embodiment of the present
invention over visible wavelengths and infrared wavelengths. The
multi-layer interference structure can be incorporated into both
foils and pigments. Rather than utilizing one dielectric-absorber
pair, the optical stack has two dielectric-absorber pairs. In a
further embodiment, a pigment flake with layer order:
A.sub.2/D.sub.2/A.sub.1/D.sub.1/R/D.sub.1/A.sub.1/D.sub.2/A.sub.2
is used. The approximate layer materials and thicknesses for this
example device are as follows: [0114] R=80 nm aluminum [0115]
D.sub.1=D.sub.2=1.0 QWOT MgF.sub.2 @ 300 nm [0116] A.sub.1=7 nm
chromium [0117] A.sub.2=2.5 nm chromium
[0118] The device achieves a uniform low reflectance across the
visible spectrum but achieves a high reflectance level (low
emittance) in the far infrared. Instead of two dielectric-absorber
pairs, three and four pairs can be used; however, this increases
cost and complexity. When utilized as a foil, the design can be
simplified to S/R/D.sub.1/A.sub.1/D.sub.2/A.sub.2 where S is an
optional substrate. In some embodiments, the reflector is
substantially thicker than necessary to provide the desired
reflectance, and serves as a substrate to deposit the other layers
on, such as aluminum foil or stainless steel foil.
[0119] V. Forms and Applications of Embodiments of the
Invention
[0120] Optical thin film structures according to embodiments can be
formed on pigment particles, films, foils, and other objects. For
example, a optical thin film structure might be deposited directly
on a piece of glass, metal, plastic, ceramic, or composite
material, or on a film or foil that is applied to a piece of wood,
fabric, plastic, glass, metal, ceramic, or composite material.
[0121] FIG. 8A is a simplified cross section of a portion of a film
or foil 90 according to an embodiment of the present invention. An
optical thin film structure 91 according to an embodiment of the
present invention is deposited on a substrate 89, such as a polymer
film, e.g. a film of polyethylene terephthalate ("PET") or a metal
foil, such as aluminum or stainless steel foil. An optional top
coating 92 is applied over the optical thin film structure to
provide protection from the environment, or to enhance the optical
properties of the film or foil. In an alternative embodiment, a
polymer cover sheet is attached to the top of the optical thin film
structure with a layer of laminating adhesive. An optional mounting
adhesive layer 93 is provided on the opposite side of the
substrate, and a release liner 94 is provided to facilitate
handling of the assembly. The release liner is removed to expose
the mounting adhesive layer so the film or foil can be conveniently
applied to a surface.
[0122] FIG. 8B is a simplified cross section of a foil 95
as-described in accordance with FIG. 8A, above, attached to a panel
96. The release liner is removed to expose the mounting adhesive,
and the film is applied to the panel. Films according to
embodiments of the present invention provide thermal control by
having low IR emittance (high IR reflectivity) while transmitting
or absorbing higher wavelength light.
[0123] FIG. 8C is a simplified cross section of an optical thin
film transfer foil 111 for application to a surface. The optical
thin film stack 91' may be deposited "backwards" onto the substrate
89', such as a plastic film. In other words, the absorber is
deposited first, then the spacer layer, and finally the reflector.
An optional adhesive layer 93' and release liner 94 may be included
for attaching the transfer foil to a surface, or the surface may be
coated with the adhesive before attaching the foil. An optional
release layer 110 may be included between the substrate and the
thin film layer to facilitate removal of the substrate from the
transfer foil after it has been attached to the surface. An
optional overcoat layer (not shown) may be applied between the
optical thin film stack and the release layer before applying the
transfer foil to the surface, or may be applied after the transfer
foil has been attached to the surface.
[0124] Pigment flakes according to embodiments of the present
invention can be incorporated into any number of liquid or solid
media and used as ink, paint, extruded plastic film, plastic part,
or powder coatings, for example. The optical designs have
advantages where a low chroma and/or relatively neutral color
effect is desired along with low infrared emittance. The dielectric
and absorber thicknesses of the design are chosen to meet the
desired color, lightness, reflectance, solar absorptance, and
infrared emittance properties. Embodiments of the present invention
allow one to design a foil, pigment, or other structure
incorporating an optical stack to give a wide range of solar
absorptance, infrared emittance, lightness, and color values.
Designs with thin absorbers, i.e. with absorber layers that are
thinner than the absorber thickness that would provide the minimum
reflectance in the visible spectrum, will have higher mid-infrared
reflectance than will designs with thicker absorbers. The optical
design of the pigment flakes may be optimized according to the type
of carrier or vehicle ("matrix") the pigment flakes will be
dispersed in. In some instances, the matrix has a relatively low
refractive index, and optical designs derived for air can be used
in the carrier with little degradation of the optical performance
of the pigment dispersed in the matrix.
[0125] FIG. 9A is a simplified cross section of a polymeric sheet
97 with pigment flakes 98 according to an embodiment of the present
invention. Such a polymeric sheet can be formed by casting or by
extrusion. The film forming the sheet should have a thickness of at
least two times the thickness of the multi-layer interference thin
film flakes, which typically have a thickness of approximately 0.5
micrometer, so that the sheet should have a thickness of about 1
.mu.m or more.
[0126] In general, the polymeric sheet comprises a layer of polymer
material having first and second parallel surfaces 99, 100. A
plurality of pigments flakes according to an embodiment of the
present invention are disposed within the layer of polymeric
material. The flakes generally have an aspect ratio not less than
about 2:1 and first and second parallel surfaces that generally
align themselves to the first and second parallel surfaces of the
polymeric sheet so that the aggregate effect of the particles is
similar to the effect that might be obtained by a foil or film as
described above in relation to FIG. 8A. Alignment of the flakes can
be achieved during extrusion or casting, or by stretching the
polymer sheet, for example. An adhesive layer and release liner may
be further added to one or both sides of the polymeric sheet.
Similarly, the sheet may be laminated to additional polymeric
sheets or other objects. Alternatively, a multiple layer polymeric
sheet can be formed by co-extruding films in which the outermost,
and preferably thinner layer, comprises the pigments of the instant
invention.
[0127] FIG. 9B is a simplified cross section of a co-extruded
polymer sheet 101 with pigment flakes according to another
embodiment of the present invention. The a first film layer 102 in
such a co-extruded film may provide structural support or
protection to the film layer 103 containing the pigment flakes,
serve as an adhesion or bonding layer to the article or housing
requiring thermal control or serve as the structural housing
itself. In other embodiments, a central film layer may be extruded
with pigment-containing layers on either side, or a pigment
containing layer may be sandwiched between two film layers, such as
clear or dyed PET.
[0128] In connection with the present invention, various types of
polymers can be used. For example, with an aqueous polymer, a
polyvinyl alcohol, polyvinyl acetate polyvinylpyrrolidone,
poly(ethoxyethylene), poly(methoxyethylene), poly(acrylic) acid,
poly(acrylamide), poly(oxyethylene), poly(maleic anhydride),
hydroxyethyl cellulose, cellulose acetate and poly(sacchrides) such
as gum arabic and pectin may be used. If an organic solvent base is
to be utilized, almost any polymer system that is dissolvable may
be used. This may include those polymers listed in the aqueous
examples above but will also include the additional polymers of
poly(acetals), such as polyvinylbutyral, poly(vinyl halides), such
as polyvinyl chloride and polyvinylene chloride, poly(dienes) such
as polybutadiene, poly(alkenes) such as polyethylene,
poly(acrylates) such as polymethyl acrylate, poly(methacrylates)
such as poly methylmethacrylate, poly(carbonates) such as
poly(oxycarbonyl oxyhexamethylene, poly(esters) such as
polyethylene terephthalate, poly(urethanes), poly(siloxanes),
poly(suphides), poly(sulphones), poly(vinylnitriles),
poly(acrylonitriles), poly(styrene), poly(phenylenes) such as
poly(2,5 dihydroxy-1,4-phenyleneethylene), poly(amides), natural
rubbers, formaldahyde resins and other polymers.
[0129] FIG. 10 is a simplified cross section of a layer of paint
104 containing pigment flakes 98 according to an embodiment of the
present invention applied to a surface 105. The paint includes a
paint vehicle 106 that is fluid when the paint is applied. As the
paint dries or hardens, the pigment flakes generally align
themselves with the surface. Thus, the aggregate effect of the
pigment particles is similar to the surface being covered with a
foil or film, or being directly coated with the thin film layers
having a similar optical thin film structure. In a particular
embodiment, the paint matrix is a polymer with a low infrared
emittance, such as a silicon-based paint. In a particular
embodiment, it is desirable that the vehicle or matrix of the
pigment flakes has an IR emittance less than about 0.5.
[0130] The current invention offers the advantages listed in the
previous section in that one can provide a portable thin film
applicable as a paint, ink, plastic, or other form that has
substantially lower reflectance values in the visible portion of
the optical spectrum compared to the infrared portion of the
spectrum. Thus, one can provide a variety of brightness and colors
with low infrared emittance. The reflectance characteristics can be
further selected between the near- and far-infrared regions. Paints
according to embodiments of the invention may be indigo, blue,
green, brown, and burgundy, as well as black and various shades of
gray.
[0131] In the energy control field, this invention allows for solar
control paints with high absorptance and low emittance that can be
applied to a variety of surfaces and materials. In addition, it
allows thermal control paints with specified absorptance/emittance
ratios. Pigments made according to the teachings of the invention
to have a dark or black appearance are useful in decorative,
military, or solar energy markets.
[0132] Pigments made according to embodiments of the present
invention are also useful in anti-counterfeiting applications.
Pigments having a neutral or near neutral appearance (low chroma or
very low chroma) and high IR reflectivity can be used to impart an
IR image to an object. In further embodiments, neutral or low
chroma ink, paint, foil, or similar material having high IR
reflectivity is patterned in conjunction with similar neutral or
low chroma with lower IR reflectivity. For example, an image could
be printed on a bill, certificate, passport, or other article that
has one image visible to the eye, and another image visible in the
infrared, such as overprinting an IR image with black pigment
according to the present invention in a black field printed with
conventional black ink.
[0133] FIG. 11 is a simplified plan view of an image 107 printed
with ink according to an embodiment of the present invention. The
image has a first field 108 and a second field 109. For simplicity
of illustrations, both fields are shown without color or shading,
but would generally be black, gray, or low-color, at least for one
field of the image. For example, the first field could be printed
with conventional black ink, and the second field printed with
black ink according to an embodiment of the present invention. The
second field could have relatively high IR reflectivity and be
easily viewed with an IR detector, but essentially be invisible to
a human. Such techniques may be used to superimpose IR images on
visual images, or to embed IR images on or in objects, such as for
security or anti-counterfeiting purposes. Similarly, the entire
image could be printed with ink according to the present invention,
which would not be obvious by casual inspection, yet be verifiable
with IR inspection techniques, and would be much more involved for
the counterfeiter to make.
[0134] The present invention may be embodied in other specific
forms without departing from its spirit or essential
characteristics. The described embodiments are to be considered in
all respects only as illustrative and not restrictive. The scope of
the invention is, therefore, indicated by the appended claims
rather than by the foregoing description. All changes that come
within the meaning and range of equivalency of the claims are to be
embraced within their scope.
* * * * *