Flat parallel light source

The present invention relates to a flat parallel light source using the principle of the mirror reflection and diffuse reflection, which comprises a light source, a diffuse reflective chamber with high reflectance walls, a light coupler, a small hole array at the top surface of said diffuse reflective chamber, a mirror reflective cone array on the small hole array, and a convex lens array on said cone array. The light generated by the light pass through the light coupler into the diffuse reflective chamber, and then pass through the small hole array, mirror reflective cone array, and lens array to form parallel light. The flat parallel light source can generate a high intensity parallel light with excellent parallelism or a given scattering angle parallel light. It can be used for backlighting for all kinds of LCDs, and other equipment where parallel light is needed. It can also be used in LCDs to increase the brightness of the display image and reduce power consumption.

FIELD OF THE INVENTION 
The present invention relates to a flat parallel light source. More 
specifically, it relates to a device capable of producing high efficiency, 
long lifetime, high brightness parallel light useful as the back light for 
many types of Liquid Crystal Displays ("LCD") to achieve full color, 
multicolor or monochrome displays, and for other equipment which may use 
parallel light as a light source. 
BACKGROUND OF THE INVENTION 
The point light sources such as the metal-halide lamp, the short arc length 
xenon lamp, the reflector and lens systems have been conventionally used 
to generate a parallel light source. These point light sources, although 
capable of producing good parallel light, usually have a short lifetime 
and occupy a large space. In addition, these light sources cannot produce 
any pulse light. Nor can they produce any pulse light comprising three 
colors, namely, red, blue and green. 
It is therefore an object of the present invention to overcome the 
above-mentioned disadvantage of the point light sources by providing a 
flat parallel light source which can produce a long lifetime, high 
efficiency parallel light comprising the white, monochrome or the three 
colors suitably used as the back light source for the scattering LCD, the 
active matrix LCD (AM-LCD) or passive matrix LCD to increase screen 
brightness and to save energy. 
It is a further object of the present invention to provide a flat parallel 
light source suitably used in the stack LCD to produce a multicolor or 
full color display. 
SUMMARY OF THE INVENTION 
The present invention relates to a flat parallel light source capable of 
producing high efficiency, long lifetime, high brightness parallel light. 
Briefly, a flat parallel light source using the principle of the mirror 
reflection and diffuse reflection, and comprising a light source, a 
diffuse reflection chamber, a light coupler and a mirror reflective cone 
array. The light emitted from the light source is guided by the light 
coupler, which is located between the light source and the diffuse 
reflective chamber, into the diffuse reflective chamber. The diffuse 
reflective chamber further comprises a small hole array located at its top 
surface from which the light reflected from the diffuse reflective chamber 
passes through the chamber and enters the mirror reflective cone array. 
The mirror reflective cone array comprises a plurality of mirror 
reflective cones which are located on the top surface of the diffuse 
reflective chamber. Each of the mirror reflective cones has a pointed end 
and a non-pointed end wherein the pointed end is matched connection to and 
in direct alignment with the small hole. The non-pointed ends of the 
mirror reflective cones are connected to the convex lens array which 
consists of a plurality of convex lenses that are so arranged as to share 
the same optical axis with the small holes that the small holes are at or 
near the focal points of the lens. Thus, the light that has passed through 
the small holes into the mirror reflective cones ultimately pass through 
the convex lens to form parallel output light. 
The light source may comprise at least one cold cathode fluorescent lamp or 
at least one hot cathode fluorescent lamp. The lamp may contain a 
reflector or a high reflectance layer such as an Ag, Al or alloy thin film 
on its outside surface to collect the light emitted from the lamp. The 
reflectance layer has at least one slit to permit smooth entry of light to 
the diffuse reflective chamber. The fluorescent lamp may be further 
enclosed within a glass pipe or tube within which a vacuum chamber is 
created between the lamp and the glass pipe or tube for the purposes of 
reducing heat loss from the lamp so as to increase the efficiency of the 
fluorescent lamp and to decrease the effect of the ambient temperature to 
the fluorescent lamp. 
The light source may be installed from the outside at one side of the 
diffuse reflective chamber, or at the two sides or four sides or at the 
bottom or the top of the diffuse reflective chamber. Alternatively, the 
light source may be installed inside the diffuse reflective chamber and a 
series of reflective strips or dots are placed on the outside of the light 
source to ensure that the light emitted from the light source be 
distributed uniformly in the diffuse reflective chamber. 
The diffuse reflective chamber may be a transparent plate or board made of 
high reflectance walls. The chamber may further comprise a light window 
existing between the interface of the light coupler and the chamber. The 
chamber may be a flat panel or in any other shape, preferably, the side of 
the panel near the light source is thicker, and the other side is thinner, 
to make the output light from the small holes more uniform. The walls of 
the diffuse reflective chamber, in the alternative, may be an efficient 
diffusing wall and made of a rugged surface with high reflectance thin 
films such as Ag, Al or an alloy thin film. In certain circumstances, the 
light coupler can be eliminated so that the light source is directly 
coupled with the diffuse reflective chamber. 
The mirror reflective cones may be made of a transparent medium such as 
plastic, glass, or air consisting of high reflectance walls, and the 
pointed ends of the cones coupled with the small holes of the diffuse 
reflective chamber, and the non-pointed ends of the cones coupled with the 
lens so that the incident light from the small hole can be effectively 
changed into parallel light through the lens. The mirror reflective cone 
may be a circular cone, an elliptical cone, a square cone, a rectangular 
cone, or other shaped cone. In order to eliminate light reflection on the 
interface between the mirror reflective cone and the diffuse reflective 
chamber, an optical adhesive is applied between them to achieve this 
purpose. The reflective cone array and the convex lens array may be made 
as one piece or made as two separate and independent arrays. 
The parallel light source provided by the present invention is also 
amenable to producing light with different scattering angles. For 
instance, the location of the small holes can be adjusted away from the 
focal point of the lens so that the distance between the small hole and 
the focal point can be manipulated to generate output light having 
different scattering angles. In addition, the small hole may be made with 
different sizes ranging from 1% to 90% of the pitch of the small hole in 
order to obtain output light with different scattering angles. 
Furthermore, the angle between the mirror reflective wall and the normal 
line of the diffuse reflective chamber light output surface, may be made 
with different angles from 1.degree. to 60.degree. to obtain output light 
with different scattering angles. 
The parallel light source can be designed and constructed in a variety of 
ways to meet specific needs. For instance, it can be conveniently built as 
one system which comprises at least one diffuse reflective chamber, at 
least one fluorescent lamp, at least one plurality of small holes, at 
least one plurality of mirror reflective cones and at least one plurality 
of convex lenses to generate a very intensive parallel light. 
Alternatively, one or more of these systems can be further combined or 
assembled together to generate very high intensive parallel light. 
The flat parallel light source provided by the present invention can be 
best used as the back light for the conventional LCD including, but 
without limitation to, Active-Matrix LCD or passive LCD to increase the 
brightness of the LCD image or to decrease power consumption. The flat 
multi-color or the R, G and B color parallel light source can also be used 
as the back light for a conventional white/black LCD or a stack LCD to get 
a multi-color or full-color LCD, and can be used for other equipment where 
a parallel light source is needed. 
The foregoing objects and specific construction of the present invention 
will become apparent and understandable from the following detailed 
description thereof, when read in conjunction with the accompanying 
drawings.

DETAILED DESCRIPTION OF THE INVENTION 
Referring to FIG. 1, there is shown a slant view of the prior art device 
capable of generating parallel light. The reference numeral 101 designates 
a point light source such as a metal-halide lamp or a short arc length 
xenon lamp which is located on a first focal point F1 of an ellipse 
reflector 102. The light produced by the point light source 101 will first 
be reflected by the reflector 102 and become focused on a second focus 
point F2, from which the light will pass through a lens 103 to generate 
parallel light 104. As illustrated in FIG. 1, the prior art device would 
require a large space if a large area of parallel light is to be 
generated. 
Referring to FIG. 2, there is shown a cross-sectional view of a flat 
parallel light source device capable of generating parallel light in 
accordance with the present invention. The reference numeral 201 is a 
light source which may be a cold cathode fluorescent light ("CCFL") or a 
hot cathode fluorescent lamp ("HCFL"). The numeral 202 designates a light 
reflector whose function is to reflect and focus the light produced by the 
light source 201 into a light coupler 203 through which the focused light 
will enter a diffuse reflective chamber 204. In an alternative design 
(although not shown in FIG. 2), the focused light can enter the diffuse 
reflective chamber 204 directly without the need of a light coupler 203 
connected between the light reflector 202 and the diffuse reflective 
chamber 204. The entire interior surfaces of the diffuse reflective 
chamber 204 are made up of high reflectance surfaces or walls 205 capable 
of performing high efficiency reflection. The upper surface of the diffuse 
reflective chamber 204 has a series of equally spaced small holes 206 
through which the reflected light from the diffuse reflective chamber 204 
pass out of said chamber. The numeral 207 designates a series of mirror 
reflective cones whose pointed ends fixedly connect to and align with the 
small holes 206 of the diffuse reflective chamber 204 to receive the 
reflected light from the diffuse reflective chamber and on the non-pointed 
ends has a series of convex lenses 208, being arranged at the same optical 
axis, and each of the small holes 206 is at or near the focal point of 
each of the convex lenses 208 which enables the light that passes through 
the small holes 206 of the diffuse reflective chamber 204, to pass through 
the convex lenses 208 to form a series of parallel light 209. 
In the case that either a cold cathode fluorescent lamp ("CCFL") or a hot 
cathode fluorescent lamp ("HCFL") is used as the light source 201, it is 
possible to vacuum pack said lamps from the outside with a glass tube or 
alike containers to prevent or to reduce heat loss from said lamps. 
Additionally, the interior or the exterior surfaces of the glass tube or 
alike containers may be coated with a thin film reflector such as silver 
or aluminum to enhance the luminous efficiency of the lamps and reduce any 
adverse impact of ambient temperature on the intensity of the parallel 
light. 
Referring to FIG. 3, the light source 301 with reflector 302 and diffuse 
reflective chamber 303 are further elaborated. As previously discussed, 
the interior surfaces of the diffuse reflective chamber 303 are made up of 
highly reflective surfaces or walls 304 to ensure reflection efficiency. A 
light input window 305 exists between the light coupler 306 and the 
diffuse reflective chamber 303 to permit passage of light from the light 
source to the diffuse reflective chamber 303. Since the combined surface 
of the light input window 305 and the small holes 307 are much smaller 
than the total interior surface of the diffuse reflective chamber 303, the 
light that passed through the light input window may undergo multi-step 
reflections within the diffuse reflective chamber until finding their ways 
to pass through the holes 307. Such a design ensures all the light that 
passed through the small holes 307 possesses the same or substantially the 
same light intensity. 
The diffuse reflective chamber 303 may be made of a transparent board such 
as glass or transparent plastic or, in the alternative, made of several 
pieces of highly reflective walls organized or arranged to form a 
reflective box. The diffuse reflective chamber 303 can be in a variety of 
shapes. For instance, it can be a square and flat board, or a flat yet 
non-square chamber made of boards having different thicknesses. A 
preferred embodiment of the invention is to provide for a diffuse 
reflective chamber whose reflective walls become thicker at one end to 
form a curve-like chamber as it gets closer to the light source to ensure 
the light that passed through the small holes 307 possesses the same or 
substantially the same intensity. The interior surface of the diffuse 
reflective chamber may be made of a high reflectance diffuse reflection 
layer, or rugged surface with Al, Ag or alloy thin film. 
Referring now to FIG. 4, the mirror reflective cones 401 (i.e., 207 shown 
in FIG. 2) are further elaborated. The degree of parallelism of the 
reflected parallel light 402 is determined by the degree of a scattering 
angle a which is the angle between the light beam 402 or 403 that passes 
through the convex lens 404 and the light axis 405, which is perpendicular 
to the reflection top surface b-b of the diffuse reflective chamber 406. 
The scattering angle a can be determined by the following equation 
EQU .alpha.-tan.sup.-1 (a/2D) (1) 
wherein a is the diameter or size of the small hole 407, and D is the 
distance between the small hole 407 and the convex lens 404. Thus, when 
the diameter a is smaller and the distance D is larger, the scattering 
angle is smaller to yield better parallelism for the light 402 and 403 
etc. 
The light entering through the small holes 407 may, depending on its 
entering angle from the diffuse reflective chamber 406 through the small 
holes 407 to the cones 401, passes through the convex lens 404 directly 
without further reflection to form parallel light or require further 
reflections within the cones 401 to form parallel light. For instance, for 
the purpose of illustration, if the incident angle i is larger than 
.delta., and .delta. can be calculated by the following equation: 
EQU .delta..apprxeq.tan.sup.-1 (P-a)/2D! (2) 
where p is the pitch of the convex lens 404, e.g., the incident light 408 
cannot pass through the convex lens 404 directly to form parallel light. 
Instead it has to be reflected within the cones 401 before passing through 
the lens as parallel light. The angle .phi. of the reflection light may be 
further determined by the following equation: 
EQU .phi.=i-2.theta. (3) 
wherein .phi. is the angle between the normal line of b--b and the light 
409 after it has been reflected within the cone 401, and .theta. is the 
angle formed between the incident light and the reflective wall. Thus, 
when the incident light reflected each time within the cone 401, its 
reflected light angle .phi. will reduce its angle .theta. by two times. 
When the value calculated from equation (3) becomes negative, it indicates 
that the light will be reflected in a direction, which is determined by 
the normal line of b--b, opposite to that before reflection as so 
illustrated as light 410. 
If the incident light has a relatively larger incident angle i, such as 
light 411, it may need to go through two or more reflections. Since each 
reflection angle between the reflected light and the normal line of b--b 
will reduce two times the angle between the light before reflected and the 
reflective walls of the cones 404 by two folds, it is essential that all 
entering light will pass through the convex lens 404 either directly or 
after being reflected within the cones. This ensures the generation of 
parallel light sources with extremely high efficiency. 
The mirror reflective cones 401 and 206 as shown in FIG. 2 may be built 
square, rectangular, round elliptical, or in other shapes. 
As shown in FIG. 4, each of the lenses 404 is built as an integral part of 
each of the mirror reflection cones 401 which may be made of any type of 
transparent materials or medium. Each interior surface of the cones 401 
comprises the high reflectance walls 412 which may be coted with a thin 
film of high reflectance materials such as, but without limitation to, 
silver, aluminum or alloy. The convex lenses 404 may have a non-spherical 
surface to ensure that the light passed through is parallel. In addition, 
the mirror reflective cones 401 and the diffuse reflective chamber 406 may 
be glued together by certain types of optical adhesive or optical glues to 
eliminate light reflection on and between each of the interfaces to 
improve light coupling efficiency if the medium of the cones is not air. 
In the present invention, the walls of the mirror reflective cone are the 
mirror reflective walls, which do not use the principle of the total 
internal reflection, because in the latter case, when the incident angle 
between the light and the normal line of the reflection wall of the 
incident light is less than the critical angle, the light will pass 
through the cone wall, and cannot be changed into the parallel light shown 
as 413, and the efficiency of the parallel light source will be decreased. 
Furthermore, since the walls of the mirror reflective cone are the mirror 
walls, the oblique angle .delta. can be from 1.degree. to 60.degree.. In 
addition, the medium of the mirror reflective cone also has no limit. For 
instance, it may be glass, plastic, or air etc. 
Referring to FIG. 5, there is shown an alternative way to build the convex 
lens 501 in connection with the mirror reflective cones 502. The convex 
lens 501 and the cones 502 may be built as two independent and separate 
layers of plates. Each of the plates may be molded separately before being 
assembly mounted together. The lens 501 may be a plano-convex lens or 
double-convex lens. If the transparent window 503 is located on the focal 
point of the lens 501, the incident light will pass through the lens to 
form a good parallel output light. If one desires to change the scattering 
angle of the output light, the distance d between these two plates can be 
easily adjusted to achieve this purpose. In order to further simplify the 
structure, the mirror reflective cones 502 can be entirely eliminated from 
the device and the light passed through the transparent window 503 can 
pass through the lens 207 directly to form parallel output light. 
FIGS. 6(a) and (b), show still other ways to build the mirror reflective 
cones 601 without the lens. Wherein FIG. 6(a) is the case of an optical 
medium cone i.e., there is an optical medium 602, e.g., transparent 
plastic, in the cones 601. FIG. 6(b) shows the case of an air cone, i.e., 
there is air 603 in the cones. The incident lights 604, 605 can pass 
through the cone plate 606 either directly or after being reflected within 
the cones, to get a wider scattering angle output light. 
Referring to FIG. 7, there is shown another way to build the diffuse 
reflective chamber, reflective cone and the lens that generates parallel 
light with good parallelism. The reference number 701 is a diffuse 
reflective chamber. The numeral 702 designates a reflective cone, which is 
in the diffuse reflective chamber, and the direction is opposite with the 
mirror reflective cone 206 as shown in FIG. 2, the non-pointed ends of the 
cone 702 are positioned opposite to the bottom of the diffuse reflective 
chamber. The numeral 703 designates the pointed ends of the cone, and is 
also the small hole of the diffuse reflective chamber. The numeral 704 is 
the lens. The small hole 703 is positioned at or near the focal point of 
the lens 704, which is arranged at the same optical axis. All the incident 
light in the solid angle .psi. can go through the small hole 703 and lens 
704 to become to the parallel light 705. The effect of reflective cone 702 
is to reflect the incident light beyond the solid angle .psi., e.g., 705 
and 706, to the bottom of the diffuse reflective chamber 701, and then 
reflect and go through the small hole and lens to become parallel light. 
The numeral 707 designates the high reflectance walls of diffuse 
reflective chamber 701 and 708 designates the high reflectance diffuse or 
mirror reflective walls of the reflective cone 702. The numeral 709 
designates a black spacer between lens plate 704 and the diffuse 
reflective chamber 701, which is used for assembly and absorbing the stray 
light. 
Referring jointly to FIGS. 8 and 9, there are shown the various 
arrangements of the light source with respect to the diffuse reflective 
chamber. The light source may be placed on one end outside of the diffuse 
reflective chamber as shown in FIG. 2, 201. Alternatively, FIG. 8 shows 
that light source 802 may be placed on both the top and bottom sides or 
both the left and right ends, or even the entire outside area surrounding 
the diffuse reflective chamber 801 or placed on the bottom outside of the 
diffuse reflective chamber 801. FIG. 9 shows the light source 901 placed 
inside the diffuse reflective chamber 902 in which the light source may be 
enclosed within a light tube or alike structures on which a plurality of 
reflective strips or reflective points are evenly or unevenly placed on 
the surface of the tube to make the light illuminated from the inside 
placed light source to distribute uniformly within the diffuse reflective 
chamber. 
The parallel light source provided by the present invention may be used in 
backlighting for a liquid crystal display such as a polymer dispersed LCD 
(PDLCD) as so described in a pending application, U.S. patent application 
Ser. No. 08/283,616 now U.S. Pat. No. 5,510,995 filed by the present 
inventors. In addition, the parallel light source can also be used as the 
backlighting for an active-matrix LCD (AM-LCD) or a passive-matrix LCD 
(PM-LCD) as illustrated below. 
Referring to FIG. 10, there is shown the use of a parallel light source in 
AM-LCD or PM-LCD 1002. The parallel light source 1001 may be designed to 
emit light forming certain scattering angles .beta. in that the output 
light will focus on and within a certain range of viewing angles to 
increase the brightness of the backlight and reduce power consumption. 
This design is particularly desirable in battery-driven LCD equipment, 
such as a lap-top computer and a pocket LCD TV etc. due to its ability to 
save battery power consumption. For example, the prior art backlight used 
in the lap-top computer contains a diffuser whose function is to disperse 
the output light uniformly to the surrounding environment at an angle 
equal to 2.pi. solid angle. However, if the parallel light source of the 
present invention is used as the backlight, the light can be outputted at 
a desirable diffusing angle .OMEGA. within which the intensity of the 
output light will be enhanced by 2.pi./.OMEGA. folds; wherein .OMEGA. is 
the solid angle of the output light which is expressed as 
.OMEGA.=2.pi.(1-cos .beta.). Thus, assuming the scattering angle in the 
lap-top computer is .+-.20.degree. and the viewing distance (i.e., the 
distance between the viewer's eye to the lap-top screen) is 30 cm, and the 
viewing width is 21 cm, the brightness can be enhanced by 
2.pi.K/2.pi.(1-cos .beta.)=11 folds, where K is the efficiency ratio of 
the parallel backlight to the conventional backlight, e.g., K=0.7. In 
other words, the light source of the present invention is capable of 
maintaining the same brightness of LCD image as the prior art backlight 
while consuming only 1/10 of the energy required for the prior art device. 
For instance, a conventional 10.4" color TFT-LCD may use 3.8 W for its 
backlight illumination while the same brightness can be achieved by the 
light source provided by the present invention at only 0.4 W. 
Referring to FIG. 11, the use of the parallel light source in stack 
multi-color or full color LCD is described. The numeral 1101 designates 
the parallel light source. The numeral 1102 designates a stack LCD which 
comprises two or three different color LCDs stacked together to achieve 
multicolor or full color LCD. The numeral 1103 designates a diffuser. 
Since this type of LCD usually maintains a distance between each of its 
LCD plates, the light 1104 of backlighting must maintain good parallelism 
to achieve good overlapping of the images produced by each of the plates 
to obtain multicolor or full color display. The prior art technology uses 
M-H light or other point light sources to produce parallel lights which 
require a larger space to accommodate the light source, needs more energy 
and has a short lifetime. To the contrary, the light source provided by 
the present invention has the advantages of high efficiency, energy-saving 
and long lifetime. 
Referring to FIG. 12, the parallel light source can also be used to 
generate red, blue and green parallel light. The numeral 1201 designates 
three colors, red, blue and green light sources R, G, B. The numeral 1202 
designates the diffuse reflective chamber. The light produced by the light 
sources 1201 will be reflected by a series of reflectors 1203, which are 
placed onto the outside surface of the tube enclosing the light source, to 
enter the diffuse reflective chamber. The light passed through the small 
hole into plates 1204 containing the mirror reflective cones and convex 
lens to form parallel light 1205. In order to accommodate LCD scanning, 
the diffuse reflective chamber can be subdivided into several sections and 
each of which may have one or more sets of red, blue and green light 
sources. This design allows sequential production of red, blue and green 
parallel light to coordinate and accomplish the scanning requirement 
necessitated by the LCD scanning as so described in pending application, 
08/283,616 now U.S. Pat. No. 5,510,915, filed by the same inventors. 
Referring to FIG. 13, there is shown a variant of the present invention in 
which the diffuse reflective chamber is subdivided into a plurality of 
smaller chambers, each of which has a light source to generate high 
intensity parallel light. The numeral 1301 designates a fluorescent lamp. 
The numeral 1302 designates a reflector layer coated on the outside 
surface of the lamp 1301. The numeral 1303 designates a light coupling 
window located between a diffuse reflective chamber 1305 and the 
fluorescent lamp 1301. The numeral 1304 designates the high reflectance 
diffuse reflective walls. The numeral 1306 designates a light entering 
window. The light entering window 1306 is tightly matched and mounted 
together, by a certain optical adhesive, with the light coupling window 
1303 to permit entry of the light from the lamp 1301 to the diffuse 
reflective chamber 1305. The diffuse reflective chamber may be in a cone 
or other shape and the interior of which is made of highly reflective 
walls. Each diffuse reflective chamber has a plurality of small holes 1307 
between the interface of the chamber 1305 and a cone reflector 1308 to 
permit entry of light from the diffuse reflective chamber to the cone 
reflector from where the light can be effectively reflected out of the 
cone reflector 1308 through a convex lens 1309 to form highly intensive 
parallel light 1310. 
Referring to FIG. 14, there is shown yet another variant of the present 
invention whose structure is essentially identical with the device shown 
in FIG. 13 except that the light source 1401 comprising a set of red, 
green and blue fluorescent lights R, G, and B for each of the diffuse 
reflective chambers 1405. As described above in FIG. 13, this design can 
be adjusted to produce high intensity, color parallel light. 
FIG. 15 is a cross-sectional view of a parallel light source to illustrate 
another embodiment of the invention. As shown in FIG. 15, the side of the 
diffuse reflective chamber 1504 closer to the light source 1501 is thicker 
and the other side away from the light source is thinner, to make the 
output light 1509 from lenses 1508 and the cones 1507 more uniform. As 
before, the light source 1501 is enclosed within a glass pipe or tube 1502 
and the light from the source is coupled to the chamber 1504 through a 
light coupler 1503.