Journal of the Society for Information Display February 2006 Preview
A preview of the papers appearing in the February 2006issue
of the Journal of the SID. To obtain access to these articles
on-line, please go to www.sid.org
Edited by Aris Silzars
A rollable, organic electrophoretic QVGA display with field-shielded pixel
architecture
G. H. Gelinck, H. E. A. Huitema, M. van Mil, E. van Veenendaal, P. J. G. van Lieshout, F. Touwslager, S. F. Patry, S. Sohn, T. Whitesides, M. D. McCreary
Polymer Vision, Philips Technology Incubator
Abstract — A100-μm thin QVGA
display was made by combining a 25-μm thin organic transistor active-matrix
backplane with an electrophoretic display film. High contrast and low crosstalk
was achieved by the addition of a field shield to the backplane. The display
can be bent repeatedly to a radius of 2 mm without any performance loss. Extended
mechanical tests at a radius of curvature of 7.5 mm show that the display can
be rolled at least 30,000 times without noticeable degradation.
Displays on plastic substrates offer a solution to both the display area and
thickness problems associated with conventional display technologies. A plastic
display can be thin and flexible enough to be rolled up in a tube. Furthermore,
plastic displays are impact resistant and do not need the additional protection
essential for displays on glass. Passive-matrix LCDs using plastic substrates
have been on the market for some time. Their disadvantages include limited size
– a few hundred rows – and relatively low image quality due to high
crosstalk. In contrast, active-matrix displays are characterized by low crosstalk,
resulting in much better image quality. Although they require a thin-film transistor
per pixel, an active matrix offers the important advantage of allowing the displays
to be much larger.
FIGURE 2 — Cross section of the rollable active-matrix
display. Total display thickness is 100 μm. The active-matrix layer stack
is built using six photolithography steps. The third metal layer is used in
order to shield the electric field of the TFT and the electrodes from the electronic-ink
film.
An LTPS active-matrix process with PECVD doped N+
drain/source areas
Holger Baur Sven Jelting Niels Benson Norbert Fruehauf
University of Stuttgart
Abstract — A low-temperature polysilicon active-matrix
process without the need for ion implantation to dope drain and source areas
of TFTs has been developed. A doped silicon layer is deposited by PECVD and
structured prior to the deposition of the intrinsic silicon for the channel.
The dopant is diffused and activated during the excimer-laser crystallization
step. N-channel test TFTs with different geometries were realized. The TFT properties
(mobility, on/off ratio, saturation, etc.) are suitable to realize AMLCDs
and AMOLED displays and to integrate driver electronics on the displays. In
addition to simple TFTs, a full-color 4-in. quarter-VGA AMLCD was realized.
The complete display (including photolithographic masks, active-matrix backplane,
and color-filter/black-matrix frontplane), and an addressing system were developed
and manufactured at the Chair of Display Technology, University of Stuttgart,
Germany. The substitution of ion doping by PECVD deposition overcomes a major
limitation for panel sizes in poly-Si technology and avoids large investment
costs for ion-implantation equipment.
Ion implantation is a major limiting
factor for substrate sizes in polysilicon technology. Additionally, an ion implanter
is among the most costly equipment in display technology. In order to replace
ion doping, a complete active-matrix process using highly doped PECVD layers
as dopant sources for the drain/source areas has been developed. A doped silicon
layer is deposited by PECVD and structured prior to the deposition of the intrinsic
silicon for the channel. The dopant is diffused and activated during the excimer-laser
crystallization step. The idea of using pre-doped silicon layers as dopant sources
for drain and source areas of poly-Si TFTs extends back to the 1980s, but none
of these publications presented an operational display.
FIGURE 16 — Photograph of the poly-Si TFT active
matrix with PECVD-deposited drain/source contacts.
New era for TFT-LCD size and viewing-angle performance
Sang Soo Kim Brian H. Berkeley Jin Hyeok Park Taesung Kim
Samsung Electronics Co., Ltd.
Abstract — Samsung has announced the development of a full-high-definition
(1920 x 1080) 82-in. TFT-LCD panel using Super-PVA (S-PVA) technology, the world's
largest TFT-LCD. In addition to the size breakthrough, this product achieves
600 nits of brightness, a contrast ratio of over 1200:1, an angle of view of
180°, a color gamut of 92%, and an 8-msec response time. Several key enabling
technologies were developed to achieve these specifications, including two-transistor
direct-driven independently controlled S-PVA subpixels, non-even-area-ratio
subpixels for optimal off-axis gamma, gate overlap driving for larger driving
margin, new CCFL technology for higher color gamut, and advanced fabrication
techniques including the use of Samsung's new Gen 7 line. Many of these technologies
will be applied to other products within Samsung's LCD-TV product line. Samsung's
broader development efforts toward the overall LCD-TV market, including production
status of the Gen 7 facility, will be updated.
As a vertically aligned LC technology, PVA is normally
black. PVA is a multi-domain (four-domain) VA mode. In its on-state, fringe
fields are formed by patterned ITO. These fields cause the LC molecules to tilt
according to the ITO patterns, forming the multi-domain LC cell. Other VA technologies
rely on protrusions in order to form the multi-domain LC cell. Unlike IPS, no
rubbing process is required for VA technologies. As a conventional VA mode,
PVA has a viewing-angle dependence which causes off-axis performance limitations.
This problem can be solved by introducing more domains, as we have done with
S-PVA.
FIGURE 2 — Motion of LC molecules in eight-domain
S-PVA cell.
True 3-D scanned voxel displays using single or multiple light sources
Brian T. Schowengerdt Eric J. Seibel
University of Washington
Abstract — Conventional stereoscopic
displays require viewers to unnaturally keep eye accommodation fixed at one focal
distance while they dynamically change vergence to view objects at different distances.
This forced decoupling of reflexively linked processes fatigues eyes, causes discomfort,
compromises image quality, and may lead to pathologies in developing visual systems.
Volumetric displays can overcome this conflict, but only for small objects placed
within a limited range of viewing distances and accommodation levels and cannot
render occlusion cues correctly. Our multi-planar true 3-D displays generate accommodation
cues that match vergence and stereoscopic retinal disparity demands and can display
images and objects at viewing distances throughout the full range of human accommodation
(from 6.25 cm to infinity), better mimicking natural vision and minimizing eye fatigue.
The most common displays used for the presentation of
three-dimensional (3-D) data are stereoscopic displays. Unfortunately, although
stereoscopic displays can create a compelling perception of depth, they do not
completely recreate the conditions of viewing real 3-D objects. This imperfect
mimicry of true 3-D conditions creates oculomotor and sensory conflicts in the
visual system, leading to eye fatigue and discomfort. This problem is similar
to the better-known phenomenon of motion sickness (or "seasickness"), experienced
below decks on a rocking boat. In that case, the sense of balance accurately
reports that a person is moving but, because the person cannot see him/herself
rocking relative to the horizon, the sense of vision asserts that the person
is not moving — a sensory conflict that can cause extreme discomfort,
headaches, and nausea. The conflicts within the visual system that are generated
by stereoscopic displays can cause similar discomfort.
FIGURE 1 — Matching ocular accommodation and
vergence when viewing real objects.
Electrically controlled light scattering in FLC cells
Alexander L. Andreev Yury P. Bobylev Tatiyana B. Fedosenkova Nshan A. Gubasaryan Igor N. Kompanets Eugene P. Pozhidaev Vadim M. Shoshin, Yuliya P. Shumkina
P. N. Lebedev Physical Institute
Abstract — Three types of light-scattering
effects distinguished by physical mechanisms were studied in detail in monomeric
ferroelectric liquid-crystal (FLC) compositions at different boundary conditions
and electrical pulse regimes. The total time of the scattering switching on and
switching off is less than 150, 250, and 500 μsec at ±50 V for different
scattering types in helix and non-helix FLCs. They are quite fast, and FLC cells
are quite transparent and were used in a stack of 30–100 light-scattering
shutters for a volumetric screen of a 3-D display.
The 3-D objects are visualized in volumetric displays most effectively by the
light scattering at section planes of a volumetric medium. To compose a 3-D
object, one can use a stack of LC shutters and send corresponding light signals
into every addressed (i.e., scattering) plane while other (non-addressed)
planes are transparent (Fig. 1). The more sections, the faster the pattern must
be visualized in every section, or the faster the light scattering must be switched
on/off at a section plane (and viceversa) for real-time displaying.
Because the time of the scattering switching on/off must be minimal with respect
to the direct scattering time, the scattering must be strong and diffusive,
and no scattering must be in the transparent state of a volumetric medium.
FIGURE 1 — A schematic of a volumetric screen
based on a stack of electrically controlled light-scattering shutters. A section
pattern is visualized only at plane C where a shutter scatters light.
Spatio-temporal scanning backlight mode for field-sequential-color optically-compensated-bend
liquid-crystal display
Abstract — A spatially and temporally scanning backlight consisting of ten isolated
micro-structured light guides has been developed to be combined with a fast-response
optically-compensated-bend-mode field-sequential-color LCD in which the liquid-crystal
cell does not contain color filters. The sequential fields of three primary colors
are generated by illumination of the red-, green-, and blue-light-emitting diodes,
each illuminating for one-half of the field, resulting in a luminance of 200 cd/m2
for the LCD. The effect of light leakage between the blocks in the scanning backlight
in field-sequential-color applications was measured and will be described.
The recent development of fast-response LCDs, such as optically-compensated-bend
(OCB) mode, and highly efficient light-emitting diodes (LEDs) for three primary
colors have enabled the reintroduction of the field-sequential-color (FSC) displaying
method, which was one method used at the very beginning of the introduction
of color display systems in the mid 20th century. The FSC display is now expected
to be a future color LCD with low power consumption.
FIGURE 15 — The developed OCB-mode LCD with the
scanning backlight.
LED-backlight feedback control system with integrated amorphous-silicon color
sensor on an LCD panel
Ki-Chan Lee Seung-Hwan Moon Brian Berkeley Sang-Soo Kim
Samsung Electronics Co., Ltd.
Abstract — TFT-LCDs have the largest
market share of all digital flat-panel displays. An LCD backlighting system
employing a three-color red-green-blue light-emitting-diode (RGB-LED) array
is very attractive, considering its wide color gamut, tunable white point, high
dimming ratio, long lifetime, and environmental compatibility. But the high-intensity
LED has problems with thermal stability and degradation of brightness over time.
Color and white luminance levels are not stable over a wide range of temperature
due to inherent long-term aging characteristics. In order to minimize color
point and brightness differences over time, optical feedback control is the
key technology for any LED-backlight system. In this paper, the feasibility
of an optical color-sensing feedback system for an LED backlight by integrating
the amorphous-silicon (a-Si) color sensor onto the LCD panel will be presented.
To minimize the photoconductivity degradation of a-Si, a new laser exposure
treatment has been applied. The integrated color-sensor optical-feedback-controlled
LED-backlight system minimized the color variation to less than 0.008 Δu¢v¢
(CIE1976) compared to 0.025 for an open-loop system over the temperature range
of 42–76°C.
In order to minimize color-point and brightness
differences over temperature and time, optical feedback control is the key technique
for any LED-backlight system. There are many practical issues in implementation
such as placement of the photosensor, sampling of light signals for feedback, effect
of the LED drive current waveform on sensor signal integrity (crosstalk), and control
system design. A three-color RGB LED-backlight system with an integrated color sensor
on the LCD panel is depicted in Fig. 3.
FIGURE 3 — LED-backlight system with optical
feedback control.
Architectural choices in the Aptura™ scanning
backlight for large LCD TVs
A. A. S. Sluyterman H. J. G. Gielen
Philips Lighting
Abstract — A production-ready scanning LCD backlight system for TV sets of 32 in. and
larger has been designed. It improves the representation of moving objects and allows
fast and deep dimming for higher contrast. The architectural choices made for these
designs will be described.
Imagine an object that moves over the
screen from left to right in 2 sec, which is not uncommon at all. Assume, furthermore,
a frame rate of 60 Hz and an LCD panel with 1440 pixels per line. Then the image
smear due to the hold effect would be 12 pixels! This is unacceptable even for standard-definition
television, let alone for HDTV. Interestingly enough, the absence of an image does
not contribute to image smearing, while an image at the wrong place does. This phenomenon
is exploited in the CRT to the extreme, where each part of the image is only present
for less than a millisecond. By adopting a dynamic scanning backlight, which illuminates
each part of the panel for only a short moment, this principle can also be applied
to LCDs.
FIGURE 13 — A see-through view of the Aptura™
backlight system shows eight fluorescent lamps, each with a diameter of 16 mm.
High-quality images on electrophoretic displays
Mark T. Johnson Guofu Zhou Robert Zehner Karl Amundson Alex Henzen Jan van de Kamer
Philips Research Laboratories
Abstract
— High-resolution micro-encapsulated active-matrix electrophoretic displays
showing 2-bit gray-tone images and text with high contrast and high reflectance
are commercially available. Methods of realizing high-quality images on these displays
will be covered in this paper.
As illustrated in Fig. 2 for a dual-particle system,
MEP displays operate by the motion of charged pigment particles between two
planar electrodes, in response to an electric field. By applying a positive
voltage on a pixel, the positively charged white particles are forced to move
towards the top transparent electrode, creating a white state when the display
is viewed from this side. In contrast, by applying a negative voltage on a pixel,
the negatively charged black particles are forced to move towards the top electrode,
creating a black state. Between these two end states exists an analog range
of intermediate-reflectivity gray tones. In addition to gray-tone capability,
MEP displays can exhibit high-resolution images. The resolution of a MEP display
is not limited by the size of the microcapsule because the particles in the
same capsule, crossing two neighboring pixels, can be partially switched to
white state on one pixel and black state on the other pixel, as can be seen
in Fig. 2.
FIGURE 2 — Schematic of a microcapsulated electrophoretic
(MEP) display with positively charged white particles and negatively charged
black particles, showing the switching between the black and white states.
Single-substrate encapsulated cholesteric LCDs: Coatable, drapable, and foldable
Irina Shiyanovskaya Asad Khan Seth Green Greg Magyar Oleg Pishnyak Duane Marhefka J. William Doane
Kent Displays, Inc.
Abstract — The first ever, reflective
cholesteric liquid-crystal displays (ChLCDs) on single textile substrates made with
simple coating processes have been developed. A novel approach for fabrication of
ultra-thin encapsulated ChLCDs with transparent conducting polymers as bottom and
top electrodes will be reported. These displays are fabricated from the bottom-up
by sequential coating of various functional layers on fabric materials. Encapsulation
of the cholesteric liquid-crystal droplets in a polymer matrix and the mechanical
flexibility of the conducting polymers allow for the creation of durable and highly
conformable textile displays. The development and status of this next-generation
display technology for both monochrome and multicolor cholesteric displays will
be discussed.
Cholesteric liquid-crystal materials naturally provide
high brightness and require low power due to the inherent bistability of the
cholesteric textures. The pure reflective nature of the cholesteric materials
does not require the use of filters, polarizers, and backlighting. All these
features enable the fabrication of light-weight low-power ChLCDs on flexible
substrates if special care is taken to prevent liquid-crystal flow under the
pressure caused by display deformation which is unavoidable for flexible applications.
The elegant solution is to confine small liquid-crystal droplets in a polymer
matrix. In addition to the elimination of the material flow under pressure,
encapsulation of the LC provides good film-forming properties and high durability
of the encapsulated LC layer.
FIGURE 7 — Fully functional deformed ChLCDs coated
on the textile substrates, segmented and 16 x 13 passive matrix.
A single-panel LCoS engine based on light guides
Jeffrey A. Shimizu Peter J. Janssen Khalid Shahzad
Philips Research USA
Abstract —
By using light-guide components, a new scrolling-color engine for single-panel LCoS
projection has been developed. Light guides allow for loss-less delivery of light
leading to a simpler and more-compact system. Engine design and construction based
on a single 0.88-in.-diagonal LCoS panel is described. Separate results with a multilayer
optical film Cartesian PBS show that a significant improvement in system efficiency
is possible.
A layout of the light-guide engine is shown in Fig.
2. The figure shows the path without the lamp. Light from the lamp is focused
at the input to the light-guide assembly. The input is rectangular in shape
and one-half the length of the illumination stripe. A small polarization conversion
system (PCS) is used to create a full-length stripe of one polarization. The
light-guide assembly splits the light into three primary colors and directs
the light towards the three scanning prisms. Color splitting filters are placed
on the hypotenuse of right-angle prisms in the light-guide assembly. Each colored
stripe passes through a scanning prism. The colors are then recombined in the
x-cross filter assembly.
FIGURE 2 — Layout of the optical path without
a lamp. Distance from input plane to LCOS plane is 239 mm.
Abstract — An advanced screen for use
with LCD/LCoS/DMD rear-projection TV has been developed. A lenticular lens having
a pitch of 64 μm has been developed without loss in any other optical property.
A 70% black-stripe ratio was obtained by optimizing the patterning process, which
maintains high contrast. As described in this paper, the FC-Screen manufacturing
technology has been further developed.
The optimum lens pitch is determined by moiré
simulation (as shown in Fig. 3). A 98-μm lenticular-lens pitch can be used
for 1080p screen diagonals larger than 40 in. A 64-μm lens pitch
leads to less moiré on every pixel size. A lenticular lens pitch of 64
μm is suitable for use with QSXGA as well as 1080p. The super-fine-pitch
FC Screen, which is also able to achieve a 70% black-stripe ratio, is optically
identical to a conventional screen and to fine-pitch FC Screens.
Abstract — A new projection optical
system with an exceptionally wide field angle of 160° and a short projection
distance of 125 mm for a 62-in. screen has been developed. It is constructed
based on the Direct Projection Method which does not require a back mirror.
This paper presents a new optical design concept and the characteristics of
a prototype optical system.
FIGURE 9 — Outline layout of projection system.
FIGURE 15 — First prototype optical engine in
a front-projection configuration.