U.S. patent application number 13/963607 was filed with the patent office on 2013-12-12 for microcavity oleds for lighting.
This patent application is currently assigned to University of Florida Research Foundation, Inc.. The applicant listed for this patent is University of Florida Research Foundation, Inc.. Invention is credited to Franky So.
Application Number | 20130328029 13/963607 |
Document ID | / |
Family ID | 44507525 |
Filed Date | 2013-12-12 |
United States Patent
Application |
20130328029 |
Kind Code |
A1 |
So; Franky |
December 12, 2013 |
Microcavity OLEDS for Lighting
Abstract
Various methods and systems are provided for related to organic
light emitting diodes (OLEDs) having a microcavity. In one
embodiment, a white-light source includes a first microcavity
organic light emitting diode (OLED) configured to emit a narrow
spectrum of blue light; a second microcavity OLED configured to
emit a narrow spectrum of green light, and a third microcavity OLED
configured to emit a narrow spectrum of red light. In another
embodiment, a light source includes a plurality of OLEDs disposed
on a glass substrate. Each of the OLEDs is configured to emit light
in substantially orthogonal to the glass substrate in a predefined
spectrum. Each of the OLEDs includes a semi-reflecting mirror; and
an emitting layer, where the emitting layer in each OLED
corresponds to a respective color of light emitted by the OLED.
Inventors: |
So; Franky; (Gainesville,
FL) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
University of Florida Research Foundation, Inc. |
Gainesville |
FL |
US |
|
|
Assignee: |
University of Florida Research
Foundation, Inc.
Gainesville
FL
|
Family ID: |
44507525 |
Appl. No.: |
13/963607 |
Filed: |
August 9, 2013 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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13575347 |
Jul 26, 2012 |
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PCT/US11/25667 |
Feb 22, 2011 |
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13963607 |
|
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61307191 |
Feb 23, 2010 |
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Current U.S.
Class: |
257/40 |
Current CPC
Class: |
H01L 51/0059 20130101;
H01L 2251/5361 20130101; H01L 51/5271 20130101; H01L 51/5265
20130101; H01L 51/0085 20130101; H01L 27/3211 20130101; H01L
51/0037 20130101 |
Class at
Publication: |
257/40 |
International
Class: |
H01L 51/52 20060101
H01L051/52 |
Claims
1. A light source, comprising: a plurality of OLEDs disposed on a
glass substrate, wherein each of the plurality of OLEDs is
configured to emit light in substantially orthogonal to the glass
substrate in a predefined spectrum, wherein each of the plurality
of OLEDs comprises: a semi-reflecting layer; and an emitting layer,
wherein the emitting layer in each OLED corresponds to a respective
color of light emitted by the OLED.
2. The light source of claim 1, wherein the semi-reflecting layer
includes a quarter wave stack.
3. The light source of claim 1, wherein the semi-reflecting layer
includes a layer having a low refractive index formed on a layer
having a high refractive index.
4. The light source of claim 1, wherein the semi-reflecting layer
includes a plurality of silicon dioxide layers alternating with a
plurality of titanium dioxide layers.
5. The light source of claim 1, wherein the semi-reflecting layer
includes a silver film.
6. The light source of claim 1, wherein each of the OLEDs further
comprises: a cathode formed on an electron transport layer, wherein
the electron transport layer is formed on the emitting layer; a
hole transport layer formed on an indium tin oxide (ITO) layer,
wherein the emitting layer is formed on the hole transport layer;
and wherein the ITO layer is formed on the semi-reflecting
layer.
7. The light source of claim 6, wherein the electron transport
layer includes a 2,9-dimethly-4,7-diphenyl-1, 10-phenanthroline
(BCP) layer or a tris[3-(3-pyridyl)-mesityl]borane ("3TPYMB")
layer.
8. The light source of claim 6, wherein the cathode includes cesium
carbonate (CsCO.sub.3) and aluminum (Al) or lithium fluoride (LiF)
and Al.
9. The light source of claim 6, wherein the hole transport layer
includes 1,1-bis[(di-4-tolylamino)phenyl]cyclohexane (TAPC).
10. The light source of claim 1, wherein the emitting layer of a
first OLED included in the plurality of OLEDs includes
3,5'-N,N'-dicarbazole-benzene ("mCP") doped with
tris(2-phenylisoquinoline)iridium ("Ir(pig).sub.3").
11. The light source of claim 10, wherein the emitting layer of a
second OLED included in the plurality of OLEDs includes mCP doped
with fac-tris(2-phenylpyridinato)iridium(III)
("Ir(ppy).sub.3").
12. The light source of claim 11, wherein the emitting layer of a
third OLED included in the plurality of OLEDs includes
mCP:Iridium(III)bis[(4,6-di-flourophenyl)-pyridinato-N,C2']
picolinate ("Flrpic").
13. The light source of claim 1, wherein each of the OLEDs includes
a microcavity defined by the semi-reflecting layer and a cathode.
Description
CROSS REFERENCE TO RELATED APPLICATIONS
[0001] This application is a divisional application of U.S.
application Ser. No. 13/575,347, filed Jul. 26, 2012, which is the
35 U.S.C. .sctn.371 national stage of PCT application
PCT/US2011/025667, filed Feb. 22, 2011, which claims priority to
and the benefit of U.S. provisional application entitled
"MICROCAVITY OLEDS FOR LIGHTING" having Ser. No. 61/307,191, filed
Feb. 23, 2010, all of which are hereby incorporated by reference in
their entirety.
BACKGROUND
[0002] A broadband light source can be used to provide good quality
lighting having a lighting spectrum that resembles natural
sunlight. Light sources that do not provide light over the entire
visible light spectrum can make the color of an object appear dull
or even make the object appear to be a different color. For
example, commercial fluorescent lights, which emit a limited amount
of red light, can make an object appear to be dull red or even
brown.
BRIEF DESCRIPTION OF THE DRAWINGS
[0003] Many aspects of the present disclosure can be better
understood with reference to the following drawings. The components
in the drawings are not necessarily to scale, emphasis instead
being placed upon clearly illustrating the principles of the
present disclosure. Moreover, in the drawings, like reference
numerals designate corresponding parts throughout the several
views.
[0004] FIG. 1 is a graphical representation illustrating a
non-limiting example of the transmission of emitted light through a
plurality of layers of a white-emitting OLED in accordance with
various embodiments of the present disclosure.
[0005] FIG. 2 is a graphical representation illustrating of the
various modes of the plurality of layers of the white-emitting OLED
of FIG. 1 in accordance with various embodiments of the present
disclosure.
[0006] FIGS. 3 and 4 are graphical representations of examples of
microcavity organic light emitting diodes (OLEDs) in accordance
with various embodiments of the present disclosure.
[0007] FIGS. 5 and 6 are graphical representations of examples of
semi-reflecting mirrors of the microcavity OLEDs of FIGS. 3 and 4
in accordance with various embodiments of the present
disclosure.
[0008] FIGS. 7 and 8 are graphical representations illustrating
non-limiting examples of the light intensity of a microcavity OLED
of FIGS. 3 and 4 and an OLED that lacks a microcavity in accordance
with various embodiments of the present disclosure.
[0009] FIG. 9 is a graphical representation of an example of a
white-light emitting light source including a plurality of
microcavity OLEDs of FIGS. 3 and 4 in accordance with various
embodiments of the present disclosure.
[0010] FIG. 10 is a graphical representation illustrating a
non-limiting example of the light intensity of the white-light
emitting light source of FIG. 9 in accordance with various
embodiments of the present disclosure.
[0011] FIG. 11 is a flow chart illustrating the fabrication of
microcavity OLEDs of FIGS. 3 and 4 in accordance with various
embodiments of the present disclosure.
DETAILED DESCRIPTION
[0012] Disclosed herein are various embodiments of a light source
including one or more organic light emitting diodes (OLEDs) having
a microcavity and methods of fabricating the same. Reference will
now be made in detail to the description of the embodiments as
illustrated in the drawings, wherein like reference numbers
indicate like parts throughout the several views.
[0013] A microcavity OLED emits light substantially orthogonal to
the OLED substrate. The microcavity of the OLED allows the OLED to
be highly efficient and produce intense light because light emitted
by the OLED is directed out of the OLED instead of allowing the
emitted light to be retained within the OLED. Additionally, the
present application describes a white light source including a
plurality of microcavity OLEDs. In some embodiments, the white
light source includes a microcavity OLED that emits intense red
light in a narrow spectrum, microcavity OLED that emits intense
green light in a narrow spectrum, and a microcavity OLED that emits
intense blue light in a narrow spectrum. Since each microcavity
OLED intensely emits the specific colors in a narrow spectrum, when
the white light source illuminates an object, the visible colors
reflected by the object may be vibrant and warm due to the
intensity and the selection of bands of light emitted by the white
light source.
[0014] A variety of light sources are available including
luminaires using incandescent and/or fluorescent light bulbs.
Luminaires are sometimes used in commercial, industrial, or office
settings, and are often in the form of a light panel. Luminaires
may lose 40-50% of the light they emit due to poor light
extraction. Also, even if a light source such as a state of the art
LED has a luminous efficacy of 100 lm/W (lumens per Watt), the
efficacy of a luminaire may be as low as 40 lm/W.
[0015] The broader the band of light that a light source emits, the
more the light emitted by the light source resembles sunlight. A
figure of merit used in lighting is color rendering index (CRI).
CRI is a quantitative measure of the ability of a light source to
reproduce the colors of various objects in comparison with a
natural light source, such as the sun. A broadband light source
covering the entire visible spectrum has a CRI larger than 90. In
contrast, a commercial fluorescent light tube, which emits a small
amount of red light, has a CRI as low as 50. Because of this lack
of red light, a red object appears to be dull red or even brown
when illuminated by a commercial fluorescent light tube.
White-emitting OLEDs are useful for lighting because organic
materials have wide emission spectra. Combining red, green and blue
emitters in a single OLED panel yields an OLED that has a CRI
higher than 80 depending on the emission spectrum.
[0016] Some efficient white-emitting OLEDs have efficacies up to
100 lm/W. However, that requires exotic light extraction methods
which are not practical for manufacturing. FIG. 1 is a diagram of a
non-limiting example of the transmission of emitted light 102
through a plurality of layers of a white-emitting OLED 100. As can
be seen in FIG. 1, because light emitted from the white-emitting
OLED 100 is trapped due to refraction and reflection in an organic
layer 104, an Indium Tin Oxide (ITO) layer 106, and/or a glass
substrate 108, only a small fraction of the emitted light 102 is
extracted into air 110. Examples of the indices of refraction (n)
for the organic layers 104, the ITO layer 106, and the glass
substrate 108 are also illustrated.
[0017] FIG. 2 is a diagram of the various modes of the plurality of
layers of the white-emitting OLED 100. As can be seen in FIG. 2,
thin film guided modes 202 (i.e., modes of the organic layer 104
and/or the ITO layer 106 of FIG. 1) trap about 40-50% of the
emitted light 102, substrate modes 204 (i.e., modes of the glass
substrate 108 of FIG. 1) trap about 20-30% of the emitted light
102, and only about 20-30% of the emitted light 102 reach the air
modes 206. While a glass substrate mode 204 may be eliminated using
lens arrays or photonic crystals, a thin-film guided mode 202 is
very difficult to eliminate because the organic/ITO layers 104/106
are inside the OLED 100 and are not accessible to the outside.
[0018] FIG. 3 is a diagram of a non-limiting embodiment of a
microcavity OLED 300. The microcavity OLED 300 includes a glass
substrate 302 and a semi-reflecting mirror 304 formed on the glass
substrate 302. In some embodiments, the semi-reflecting mirror 304
is a thin silver layer (e.g., about 10-20 nm thick), and in other
embodiments the semi-reflecting mirror 304 is a quarter wave stack
including stacks of silicon dioxide (SiO.sub.2) and titanium
dioxide (TiO.sub.2), which will be discussed in further detail
below. Further, an ITO layer 306 is formed on the semi-reflecting
mirror 304. In some embodiments, the ITO layer 306 is about 100 nm
thick.
[0019] A hole transport layer 308 is formed on the ITO layer 306.
In some embodiments, the hole transport layer 308 includes a
1,1-bis[(di-4-tolylamino)phenyl]cyclohexane (TAPC) layer, which may
be about 50 nm thick. An emitting layer 310 is formed on the hole
transport layer 308. The material included in the emitting layer
310 determines the color (or the spectral frequencies) of the light
emitted by the microcavity OLED 300. For example, for a microcavity
OLED 300 that emits red light in the range of, e.g., about 585 nm
to about 675 nm, the emitting layer 310 may include
3,5'-N,N'-dicarbazole-benzene ("mCP") doped with
tris(2-phenylisoquinoline)iridium ("Ir(pig).sub.3"). Similarly, for
a microcavity OLED 300 that emits green light in the range of,
e.g., about 525 nm to about 655 nm, the emitting layer 310 may
include mCP doped with fac-tris(2-phenylpyridinato)iridium(III)
("Ir(ppy).sub.3"). Likewise, for a microcavity OLED 300 that emits
blue light in the range of, e.g., about 435 nm to about 540 nm, the
emitting layer 310 may include 3,5'-N,N'-dicarbazole-benzene
(mCP):Iridium(III)bis[(4,6-di-flourophenyl)-pyridinato-N,C2']
picolinate ("Flrpic").
[0020] An electron transport layer 312 is formed on the emitting
layer 310. The electron transport layer 312 may include
2,9-dimethly-4,7-diphenyl-1, 10-phenanthroline (BCP) layer and/or a
tris[3-(3-pyridyl)-mesityl]borane ("3TPYMB") layer. Further, a
cathode 314 is formed on the electron transport layer 312. The
cathode 314 includes a metal layer. For example, the cathode 314
may include cesium carbonate (CsCO.sub.3) (about 1 nm thick) and
aluminum (Al) (about 100 nm thick) or lithium fluoride (LiF) (about
1 nm thick) and Al (about 100 nm thick).
[0021] FIG. 4 is a diagram of another non-limiting embodiment of a
microcavity OLED 300 that emits blue light. In the embodiment
illustrated in FIG. 4, the cathode 314 includes an aluminum (Al)
layer 414a, which is about 100 nm thick, and a LiF layer 414b that
is about 1 nm thick. The LiF layer 414b is deposited on an electron
transport layer 312 including a BCP layer 412 that is about 40 nm
thick. The BCP layer 412 is deposited on an emitting layer 310
including an mCP: Firpic layer 410 that is about 20 nm thick.
Additionally, the emitting layer 310 is deposited on a hole
transport layer 308 including a TAPC layer 408a, which is about 50
nm thick. Furthermore, the emitting layer 310 includes a PEDOT:PSS
layer 408b that is about 25 nm thick and which is formed on an ITO
layer 306 that is about 50 nm thick.
[0022] FIG. 5 is a diagram of a non-limiting example of a
semi-reflecting mirror 304 of the embodiment of a microcavity OLED
300 illustrated in FIGS. 3 and 4. The illustrated example of the
semi-reflecting mirror 304 is a quarter wave stack that includes a
silicon dioxide (SiO.sub.2) layer 504a, which is formed on a
titanium dioxide (TiO.sub.2) layer 504b. The thicknesses of the
SiO.sub.2 layer 504a and the TiO.sub.2 layer 504b each correspond
to a quarter wavelength of light. Accordingly, the thickness of the
layers 504a and 504b of the semi-reflecting mirror 304 depend upon
the wavelength of light emitted by the microcavity OLED 300. In one
implementation, the silicon dioxide layer 504a is about 79 nm thick
and the titanium dioxide layer 504b is about 48 nm thick. The
semi-reflecting mirror 304 is formed on the glass substrate 302,
which may be about 1 mm thick. In some embodiments, the
semi-reflecting mirror 304 has a width of about one inch. In some
embodiments, the area of the semi-reflecting mirror 304 is about
one inch by about one inch. Also, in some embodiments, the
semi-reflecting mirror 304 has a reflectance (R) that is
substantially equal to 0.39 at 475 nm. The reflectivity of the
semi-reflecting mirror 304 may vary between about 40% and about
70%, and the reflection spectrum is broad.
[0023] FIG. 6 is a diagram of another non-limiting example of a
semi-reflecting mirror 304 of the embodiment of a microcavity OLED
300 illustrated in FIGS. 3 and 4. The example of the
semi-reflecting mirror 304 illustrated in FIG. 6 is similar to the
example of the semi-reflecting mirror 304 illustrated in FIG. 5
except that the semi-reflecting mirror 304 illustrated in FIG. 6
includes two sets of silicon dioxide and titanium dioxide layers
(504a/504b and 604a/604b) instead of one set (504a/504b) as
illustrated in FIG. 5. In one implementation, the silicon dioxide
layers 504a and 604a are about 79 nm thick and the titanium dioxide
layer 504b and 604b are about 48 nm thick. In other
implementations, the silicon dioxide layers 504a and 604a and/or
the titanium dioxide layer 504b and 604b may have different
thicknesses. Further, in other embodiments, the semi-reflecting
mirror 304 may include three or more sets of silicon dioxide and
titanium dioxide layers. In some embodiments, such as the one
illustrated in FIG. 6, the semi-reflecting mirror 304 has an R that
is substantially equal to 0.70 at 475 nm. Each of the
semi-reflecting mirrors 304 illustrated in FIGS. 5 and 6 include
alternating layers of a material having a low refractive index
(e.g., SiO.sub.2) with a material having a high refractive index
(e.g., TiO.sub.2).
[0024] Referring back to FIG. 3, the operation of the microcavity
OLED 300 will now be described. The cathode 314 of the microcavity
OLED 300 acts as a reflecting mirror and the semi-reflecting mirror
304 acts as a half mirror, thus forming a microcavity 320 between
the cathode 314 and the semi-reflecting mirror 304. The microcavity
320 has the properties of both low transmissivity and high
reflectivity. In other words, the semi-reflecting mirror 304 is a
partially transmissive and partially transparent layer. As photons
are generated inside the microcavity 320, they are reflected by the
mirrors from both sides of the microcavity 320 and transmitted out
of the half mirror provided by the semi-reflecting mirror 304.
Consequentially, the light 316 that is transmitted from the
semi-reflecting mirror 304 through the glass substrate 302 is
transmitted in a direction that is substantially orthogonal to the
glass substrate 302 instead of in all directions. Because the
microcavity 320 orients the emitted light in a particular
direction, a considerable amount of the light that is emitted by
the microcavity OLED 300 is also transmitted out of the microcavity
OLED 300 and not retained within the microcavity OLED 300.
[0025] Because of the microcavity effects discussed above, a
microcavity OLED 320 has very different emission characteristics
from OLEDs that lack a microcavity 320. An OLED that lacks a
microcavity 320 is a Lambertian light source that emits light in
all directions. A Lambertian light source is undesirable for
lighting because a large amount of the emitted light is wasted
(e.g., not directly illuminating the object or area to be
illuminated). On the other hand, a microcavity OLED 300 is a
directional emitter depending on the reflecting properties of the
microcavity 320. As a result, a microcavity OLED 300 can have
efficiencies about three to four times the efficiencies of OLEDs
that lack a microcavity 320.
[0026] FIG. 7 is a graph of the emission spectra of an embodiment
of the microcativity OLED 300 illustrated in FIG. 3 and an
embodiment of an OLED that lacks a microcavity 320. Specifically,
FIG. 7 is a graph of EL intensity versus wavelength for a
microcavity OLED 320 versus a green-emitting OLED that lacks a
microcavity 320. The luminance of the microcavity OLED 320 is about
385 nits versus the luminance of the green-emitting OLED, which is
about 108 nits, as can be seen in FIG. 7.
[0027] FIG. 8 is a polar plot of the intensity of light versus the
angle of the light for the embodiment of the microcativity OLED 300
of FIG. 7 versus an OLED that lacks a microcavity 320. As can be
seen in FIG. 8, the OLED that lacks a microcavity 320 (marked
"noncavity" 810) has a lower intensity than the microcavity OLED
300 (marked "cavity" 820), and the light is emitted from the light
source at an angle primarily between -30 degrees and +30 degrees.
Considering FIGS. 7 and 8 together, it can be seen that for a
microcavity OLED 300 both the spectrum of light emitted and the
angle of emission are narrow.
[0028] FIG. 9 is a diagram of a non-limiting embodiment of a
white-light emitting light source 900 including a plurality of
microcavity OLEDs 300a, 300b, 300c. The microcavity OLEDs 300a,
300b, 300c are phosphorescent OLEDs, which can be very efficient.
For example, the luminous efficiency of a green light emitting,
microcavity OLED 300b can be as high as 300 lm/W whereas a green
light emitting OLED without a microcavity may have a luminous
efficiency of only 100 lm/W. Further, the efficiency of a blue
light emitting, microcavity OLED 300a and red light emitting,
microcavity OLED 300c may each be over 60 lm/W. Accordingly, the
white-emitting light source 900 including the plurality of
microcavity OLEDs 300a, 300b, 300c may achieve an overall
efficiency of about 150-200 lm/W. This efficiency may be three to
four times greater than the efficiency of LEDs used in
luminaries.
[0029] White light generated from the red, green, and blue
microcavity OLEDs 300a, 300b, 300c has an emission spectrum similar
to the spectrum shown in FIG. 10. As can be seen in FIG. 10, the
blue light 316a (FIG. 9) may include an intensity 1010
corresponding to a wavelength substantially within a range of about
435 nm to about 540 nm, the green light 316b (FIG. 9) may include
an intensity 1020 corresponding to a wavelength substantially
within a range of about 525 nm to about 655 nm, and the red light
316c (FIG. 9) may include an intensity 1030 corresponding to a
wavelength substantially within a range of about 585 nm to about
675 nm. Similarly, as can also be seen in FIG. 10, the blue light
may include a peak intensity corresponding to a wavelength
substantially within a range of about 450 nm to about 480 nm, the
green light may include a peak intensity corresponding to a
wavelength substantially within a range of about 530 nm to about
575 nm, and the red light may include a peak intensity
corresponding to a wavelength substantially within a range of about
620 nm to about 650 nm. Accordingly, white light emitted by the
white-light emitting light source 900 does not include the same
intensity for all wavelengths, but rather the emission spectrum
includes a narrow spectrum including a peak intensity for certain
colors. When the light source 900 illuminates objects, the color
that reflects off the objects appears to be saturated because the
three narrow emission bands of the light emitted by microcavity
OLEDs 300a, 300b, 300c peak at saturated RGB colors. When an
embodiment of the white-light emitting light source 900 illuminates
an object, the colors of the object appear warmer, more vibrant,
and less dull as a result of the predefined bands of light emitted
by the white-light emitting light source 900 and reflected off the
object. For example, an object that is red appears to have more of
a fire engine red color when illuminated by a white-light emitting
light source 900 than a brick red or claret color that appears when
the object is illuminated by an incandescent light source.
Additionally, no external luminaries are needed since the light
emitted by a white-light emitting light source 900 is highly
directional.
[0030] Referring next to FIG. 11, shown is a flow chart 1100
illustrating an example of a method of fabricating a microcavity
OLED 300 (FIG. 3). Beginning with block 1102, a glass substrate 302
(FIG. 3) is provided. In block 1104, a semi-reflecting mirror 304
(FIG. 3) is deposited on the glass substrate 302. In the case of a
semi-reflecting mirror 304 including a stack of SiO.sub.2 and
TiO.sub.2 layers (FIGS. 5 and 6), each layer of SiO.sub.2 and
TiO.sub.2 may be deposited by sputtering. In the case of the
semi-reflecting mirror 304 including a thin layer of silver, the
silver can be deposited by vacuum evaporation. In some embodiments,
the layer of silver is about 10-20 nm thick.
[0031] Next, in block 1106, an ITO layer 306 (FIG. 3) is deposited
by sputtering. In some embodiments, the ITO layer 306 is about 100
nm thick. A hole transport layer 308 (FIG. 3) is then deposited in
block 1108. Vacuum evaporation may be used to deposit the hole
transport layer 308 on the ITO layer 306. Subsequently, an emitting
layer 310 (FIG. 3) is then deposited in block 1110 on the hole
transport layer 308. Vacuum evaporation may be used to deposit the
emitting layer 310. Further, an electron transport layer 312 (FIG.
3) is deposited on the emitting layer 310 in block 1112. Vacuum
evaporation may be used to deposit the electron transport layer
312. After the emitting layer 310 is deposited, a cathode 314 (FIG.
3) is formed in block 1114. In some implementations, the cathode
314 may be formed by depositing a layer of cesium carbonate
(CsCO.sub.3) (about 1 nm thick), aluminum (about 100 nm thick),
and/or lithium fluoride (LiF) (about 1 nm thick) on the electron
transport layer 312.
[0032] Referring to FIG. 9, a method of fabricating a white-light
emitting light source 900 includes fabricating a plurality of
microcavity OLEDs 300a, 300b, 300c. The plurality of microcavity
OLEDs 300a, 300b, 300c may be fabricated on a common substrate 302
as illustrated in FIG. 9. Additionally, the method includes the
steps described above with respect to fabricating microcavity OLED
300, except that three different emitting layers 310a, 310b, and
310c corresponding to blue, green, and red light are deposited for
each microcavity OLEDs 300a, 300b, 300c. For example, the common
substrate 302 may be provided in block 1102. Each of the plurality
of microcavity OLEDs 300a, 300b, 300c may then be fabricated as
described with respect to blocks 1104 through 1114. The plurality
of microcavity OLEDs 300a, 300b, 300c may be concurrently or
consecutively fabricated on the common substrate 302. While FIG. 9
depicts three microcavity OLEDs 300a, 300b, 300c, other embodiments
of white-light emitting light sources 900 can include other
multipes, combinations and/or configurations of microcavity
OLEDs.
[0033] It should be emphasized that the above-described embodiments
of the present disclosure are merely possible examples of
implementations set forth for a clear understanding of the
principles of the disclosure. Many variations and modifications may
be made to the above-described embodiment(s) without departing
substantially from the spirit and principles of the disclosure. All
such modifications and variations are intended to be included
herein within the scope of this disclosure and protected by the
following claims.
[0034] It should be noted that ratios, concentrations, amounts, and
other numerical data may be expressed herein in a range format. It
is to be understood that such a range format is used for
convenience and brevity, and thus, should be interpreted in a
flexible manner to include not only the numerical values explicitly
recited as the limits of the range, but also to include all the
individual numerical values or sub-ranges encompassed within that
range as if each numerical value and sub-range is explicitly
recited. To illustrate, a concentration range of "about 0.1% to
about 5%" should be interpreted to include not only the explicitly
recited concentration of about 0.1 wt % to about 5 wt %, but also
include individual concentrations (e.g., 1%, 2%, 3%, and 4%) and
the sub-ranges (e.g., 0.5%, 1.1%, 2.2%, 3.3%, and 4.4%) within the
indicated range. The term "about" can include traditional rounding
according to significant figures of numerical values. In addition,
the phrase "about `x` to `y`" includes "about `x` to about
`y`".
* * * * *