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1 | P a g e 
COLLEGE NAME 
A 
Technical seminar report 
on 
Ferroelectric liquid crystal display (FLCD) 
In partial fulfillment for the award of the degree 
Of 
BACHELOR OF TECHNOLOGY 
IN 
ELECTRONICS & TELECOMMUNICATION ENGINEERING 
SUBMITTED TO: SUBMITTED BY: 
Assistant Professor
2 | P a g e 
CERTIFICATE 
This is to certify that the technical seminar Report entitled “Ferroelectric 
liquid crystal display” is a bonafied work presented by ROHIT SINGH in a 
partial fulfillment for the award of degree of Bachelor of technology in 
ELECTRONICS & TELECOMMUNICATION ENGINEERING in COLLEGE 
OF ENGINEERING ROORKEE during the year 2011-2015. 
Assistant Professor 
College Of Engineering Roorkee
3 | P a g e 
Content 
1. Introduction on Flcd…………………………………4 
2. Lcd……………………………………………………5 
2.1 Advantages and disadvantages on Lcd………8 
3. Introduction of Amlcd………………………………10 
4. Operation On Flcd………………………………….11 
5. Molecular orientation control……………………..12 
5.1 Key Technologies for the Vmin Mode FLCDs..14 
5.2 Device Structure & Molecular Orientation…….15 
5.3 Gray Scale and Addressing…………………….17 
6. Properties and uses………………………………...19 
7. Challenges…………………………………………..20 
8. Conclusion…………………………………………..21 
9. Refrences……………………………………………22
4 | P a g e 
Ferroelectric Liquid Crystal Display 
Introduction 
Ferro Liquid Display, or Ferro-electric Liquid Display (FLD) or Ferro Fluid Display 
(FFD), is a display technology based on the ferroelectric properties of certain liquids. 
Not all such fluids are crystal but they are generically referred to as Ferro Liquid 
Crystal Displays (FLCD). 
The dot pitch of such displays can be as low as 10 μm giving a very dense 
high resolution display on a small area. These might find applications in 3D displays 
and head mounted displays (HMD) where typical LCDs have failed to provide 
anything better than a 640x480 (RGB pixel) resolution on a sq.cm display area. 
Displays based on these are still experimental or of less commercial value only due 
to the costs. Gradual adoption in consumer electronics is expected to bring the costs 
down. 
A major drawback is that the angle of twist is not easily controlled by intensity of 
magnetic field. To produce color scales, time multiplexing might be used exploiting 
the quick switching time. The materials found so far are sensitive to vibration and 
shock. 
Since Clark and Lagerwall invented the basic 
principle of ferroelectric liquid crystal displays 
(FLCDs), much effort has been devoted to 
the development of FLCDs, aiming 
at practical applications. 
While the conventionally existing LCDs such as 
STN LCDs and TFT-LCDs utilize a nematic liquid 
crystal phase, it is remarked that FLCDs utilize a 
chiral smectic C liquid crystal phase with 
Fig. Principle of FLCD.
spontaneous polarization (Ps). In the chiral smectic C 
phase, liquid crystal molecules have a layer 
structure in which the mean direction of molecular long 
axis is tilted against layers. In thin FLC cells, a bistability 
appears with two bistable states as shown in Fig.1(a)(b) . Ferroelectric 
liquid crystals have a spontaneous polarization (Ps) whose direction is 
perpendicular to the layer. When the electric field is applied, molecules re-align in 
a way that the direction of the spontaneous polarizations is the same as that of the 
electric field. Combining a pair of polarizers (polarizer and analyzer), FLCDs can 
realize dark and bright states. 
Since nematic liquid crystal is paraelectric, the order of response time is usually 
sec. On the contrary, FLC shows sec in its order of response time because of 
the direct interaction between electric field and Ps. In addition, FLCDs have several 
advantages, such as wide viewing angle due to the in-plane switching (IPS) and 
memory effect due to the bistability. The combination of fast response time and 
memory effect allows large-size direct-view simple-multiplexing LCDs with high 
resolution. 
LCD 
LCD (liquid crystal display) (from Whatis) is the technology used for displays in 
notebook and other smaller computers. Like light-emitting diode (LED) and gas-plasma 
technologies, LCDs allow displays to be much thinner than cathode ray tube 
(CRT) technology. LCDs consume much less power than LED and gas-display 
displays because they work on the principle of blocking light rather than emitting it. 
An LCD is made with either a passive matrix or an active matrix display display grid. 
The active matrix LCD is also known as a thin film transistor (TFT) display. The 
passive matrix LCD has a grid of conductors with pixels located at each intersection 
in the grid. A current is sent across two conductors on the grid to control the light for 
any pixel. An active matrix has a transistor located at each pixel intersection, 
requiring less current to control the luminance of a pixel. For this reason, the current 
in an active matrix display can be switched on and off more frequently, improving the 
5 | P a g e
screen refresh time (your mouse will appear to move more smoothly across the 
screen, for example). Active matrix is the superior technology. 
Color LCD 
An LCD that can show colors must have three subpixels with red, green and blue 
color filters to create each color pixel. Through the careful control and variation of the 
voltage applied, the intensity of each subpixel can range over 256 shades. 
Combining the subpixels produces a possible palette of 16.8 million colors (256 
shades of red x 256 shades of green x 256 shades of blue), as shown below. These 
color displays take an enormous number of transistors. For example, a typical laptop 
computer supports resolutions up to 1,024x768. If we multiply 1,024 columns by 768 
rows by 3 subpixels, we get 2,359,296 transistors etched onto the glass! If there is a 
problem with any of these transistors, it creates a "bad pixel" on the display. Most 
active matrix displays have a few bad pixels scattered across the screen. 
LCD Features and Attributes 
To evaluate the specifications of LCD monitors, here are a few more things you 
need to know. 
Native Resolution 
Unlike CRT monitors, LCD monitors display information well at only the resolution 
they are designed for, which is known as the native resolution. Digital displays 
address each individual pixel using a fixed matrix of horizontal and vertical dots. If 
you change the resolution settings, the LCD scales the image and the quality 
suffers. Native resolutions are typically: 
17 inch = 1024x768 
19 inch = 1280x1024 
20 inch = 1600x1200 
6 | P a g e
Viewing Angle 
When you look at an LCD monitor from an angle, the image can look dimmer or 
even disappear. Colors can also be misrepresented. To compensate for this 
problem, LCD monitor makers have designed wider viewing angles. (Do not 
confuse this with a widescreen display, which means the display is physically 
wider.) Manufacturers give a measure of viewing angle in degrees (a greater 
number of degrees is better). In general, look for between 120 and 170 degrees. 
Because manufacturers measure viewing angles differently, the best way to 
evaluate it is to test the display yourself. Check the angle from the top and bottom 
as well as the sides, bearing in mind how you will typically use the display. 
Brightness or Luminance 
This is a measurement of the amount of light the LCD monitor produces. It is given 
in nits or one candelas per square meter (cd/m2). One nit is equal to on cd/m2. 
Typical brightness ratings range from 250 to 350 cd/m2 for monitors that perform 
general-purpose tasks. For displaying movies, a brighter luminance rating such as 
500 cd/m2 is desirable. 
Contrast Ratio 
The contrast ratio rates the degree of difference of an LCD monitor's ability to 
produce bright whites and the dark blacks. The figure is usually expressed as a 
ratio, for example, 500:1. Typically, contrast ratios range from 450:1 to 600:1, and 
they can be rated as high as 1000:1. Ratios more than 600:1, however, provide 
little improvement over lower ratios. 
Response Rate 
The response rate indicates how fast the monitor's pixels can change colors. 
Faster is better because it reduces the ghosting effect when an image moves, 
leaving a faint trial in such applications as videos or games. 
Adjustability 
Unlike CRT monitors, LCD monitors have much more flexibility for positioning the 
screen the way you want it. LCD monitors can swivel, tilt up and down, and even 
rotate from landscape (with the horizontal plane longer than the vertical plane) to 
7 | P a g e
portrait mode (with the vertical plane longer than the horizontal plane). In addition, 
because they are lightweight and thin, most LCD monitors have built-in brackets for 
wall or arm mounting. Besides the basic features, some LCD monitors have other 
conveniences such as integrated speakers, built-in Universal Serial Bus (USB) 
ports and anti-theft locks. 
Advantages of Lcd 
 Thin Profile 
LCDs feature very thin profiles, making them the perfect choice for small 
work spaces. 
 Standard Screen Sizes 
Unlike CRTs, there is no variance between the monitor size and the screen 
size. For example, a 17-inch monitor features a 17-inch viewable image. 
 Bright Screens 
LCDs, thanks to the florescent backlight, produce bright, rich images 
 Low Energy Consumption 
In general, LCD monitors consume about half of the energy of standard 
CRTs. 
 Flicker-Free Refresh Rates 
Refresh rate is less of an issue with LCD monitors. LCDs are designed to 
have flicker-free refresh rates at 60Hz. 
 High Contrast Ratios 
LCD monitors tend to feature excellent contrast ratios, which insure bright, 
clear images. Make sure the monitor you purchase has a contrast ratio of at 
least 400:1 or more. 
8 | P a g e
Disadvantages of Lcd 
 Single Resolution 
LCDs are generally designed to work best in a single resolution. They tend 
not to have the flexibility that CRTs have to display multiple resolutions well. 
 Narrow Viewing Angles 
LCDs tend to have a very narrow viewing angle. As you vary from looking at 
a LCD straight-on the image gradually degrades. Look for at least a 160° 
viewing angle. 
 Slow Pixel Response Time 
LCDs tend to have a much slower pixel response time, which can mean 
image artifacts remaining onscreen after movement. For example, when you 
move your mouse quickly across the screen you might see the cursor create 
shadow images of itself briefly. These disappear instantaneously. In order to 
avoid this try to find a monitor that has a response time of 25 milliseconds or 
faster. 
9 | P a g e
Active Matrix Crystal Display 
An active-matrix liquid-crystal display (AMLCD) is a type of flat panel display, the only 
viable technology for high-resolution TVs, computer monitors, notebook 
computers, tablet computers and smartphones with an LCD screen, due to low 
weight, very good image quality, wide color gamut and response time. 
The concept of active-matrix LCDs was invented by Bernard J. Lechner at the RCA 
Laboratories in 1968.The first functional AMLCD display with thin-film transistors was 
made byT Peter Brody and his team at Westinghouse Electric Corporation in 
1973.]However, it took years of additional research by others to launch successful 
products. 
Introduction on Active Matrix Crystal Display 
The most common type of LCD display contains, besides the polarizing sheets and 
cells of liquid crystal, a matrix of thin-film transistors to make a thin-film-transistor 
liquid-crystal display.These devices store the electrical state of each pixel on the 
display while all the other pixels are being updated. This method provides a much 
brighter, sharper display than a passive matrix of the same size. An important 
specification for these displays is their viewing-angle. 
Thin-film transistors are usually used for constructing an active matrix so that the two 
terms are often interchanged, even though a thin-film transistor is just one 
component in an active matrix and some active-matrix designs have used other 
components such as diodes. Whereas a passive matrix display uses a simple 
conductive grid to apply a voltage to the liquid crystals in the target area, an active-matrix 
display uses a grid of transistors and capacitors with the ability to hold a 
charge for a limited period of time. Because of the switching action of transistors, only 
the desired pixel receives a charge, and the pixel acts as a capacitor to hold the 
charge until the next refresh cycle, improving image quality over a passive matrix. 
This is a special version of a sample-and-hold circuit. 
10 | P a g e
FLCD Operating Principle 
An FLCD acts as a classical half-wave plate, one whose optic axis can be reoriented 
by an applied field. 
If the optic axis is parallel or perpendicular to incoming polarized light, the light 
passes through the FLCD unchanged and is blocked by the exit polarizer(oriented at 
90o to the entrance polarizer) 
If the optic axis makes an angle of 45o to the incoming polarized light, the direction of 
polarization changes by 90o and is able to pass through the exit polarizer 
Orientation of FLF molecules is changed by applying a voltage pulse of suitable 
polarity. 
11 | P a g e
• In thin FLC cells, a bistability appears with two bistable states as shown in Fig. 
• Ferroelectric liquid crystals have a spontaneous polarization (Ps) whose 
direction is perpendicular to the layer. 
• When the electric field is applied, molecules re-align in a way that the direction 
of the spontaneous polarizations is the same as that of the electric field. 
• Combining a pair of polarizers (polarizer and analyzer), FLCDs can realize dark 
and bright states. 
Molecular orientation control 
The molecular orientation control is one of the most important key 
technologies for the development of practical FLCDs. The molecular orientations 
of FLCDs are classified as two layer structures: a bookshelf layer and a chevron 
layer. The FLC cells with parallel rubbing, in which the rubbing directions of both 
substrates are the same, have been known to show four orientational states 
with a chevron layer structure: C1-uniform (C1U), C1-twisted (C1T), C2- uniform 
(C2U) and C2-twisted (C2T). Among them, the C1U and C2U orientations are useful 
for practical applications because of their extinction positions between cross nicols. 
12 | P a g e
• So, an unconstrained system, the azimuthal 
direction in which the molecules tilt away from 
the layer normal will differ slightly from one 
layer to the next. 
• Typically, the FLCDs are built with cell gaps 
less than 2 μm for stable molecular alignment. 
• Alignment layer causes perpendicular stacked 
alignment. 
• The cell's polarisation is determined by the 
magnetic field applied. 
That in turn results in opaque or transparent layer 
when used in combination with polarised layers as in 
LCD 
The alignment film with a high pre-tilt angle (over 15 degrees) induced the selective 
formation of the C1U orientation and also that the C1U orientation gave a high 
contrast ratio under simple-multiplexing driving waveforms for FLCDs. Using the 
C1U orientation, Hanyu et al. have developed a 21-inch color FLCD (1024 x 1280 
dots, contrast ratio of 40:1 and 64 colors). 
13 | P a g e 
Fig. Principle of FLCD.
Recently, Mizutani et al. developed a 15" full-color FLCD (768 x 1024 dots, 
36 sec/line, CR=100:1) with a bookshelf layer structure, realizing full-color images 
by a combination of 4-bit spatial dither and dither methods.Futhermore, Koden et al. 
have reported that the C2U orientation can show a high contrast ratio, fast line 
address time and wide memory angle if it is combined with the -Vmin. 
The -Vmin mode utilizes the unique response (t) - voltage (V) characteristics of the 
minimum value, which is observed in FLC materials with large positive dielectric 
biaxiality (negative dielectric anisotropy). The -Vmin mode utilizing the C2U 
orientation is a promising technology for digital gray scale method with temporal 
dither because it can realize faster line address time than the C1U orientation and 
the bookshelf orientation can. 
Compared with the existing LCDs, the FLCD have received an unfavorable 
reputation of poor performance in moving picture with gray scale and also in 
shock stability. In this study, key technologies for the -Vmin mode were 
developed in order to overcome these problems. This paper describes FLC 
materials that show fast response time for the -Vmin mode, the selective 
formation of the C2U orientation, the device structure with high shock stability and 
the digital gray scale driving method, introducing a6-inch color prototype FLCD 
which was fabricated by using these keytechnologies. 
1. Key Technologies for the -Vmin Mode FLCDs 
1•1 Ferroelectric Liquid Crystal Materials 
In the -Vmin characteristics of FLC materials, the minimum voltage ismentioned as 
Vmin and the minimum response time as min. Low Vmin and fast min are 
required because the Vmin value determines the drive voltage and the min value 
determines the line address time. Since the Vmin is closely related to a balance of 
the dielectric biaxiality and spontaneous polarization (Ps), FLC materials for the 
-Vmin mode need large positive dielectric biaxiality and small or moderate 
spontaneous polarization, as well as low viscosity in order to obtain fast tmin. 
An INAC phase sequence and long 
helical pitches in nematic and smectic 
14 | P a g e
C phases are required in order to 
yield a high quality of alignment on 
cooling from the isotropic phase.In 
addition, FLC materials require wide 
temperature range of smectic C phase 
because it is related to the operating 
and storage temperature ranges of 
FLCDs. 
15 | P a g e 
Fig. 2 The characteristic of the developed FLC material FDS-2. 
A typical FLC material, FDS-2 was developed for the -Vmin mode. Its 
characteristics are shown in Fig. 2. This material offers fast min value (12 sec) 
and reasonable Vmin value (33V) at 25˚C. 
1•2 Device Structure & Molecular Orientation 
Shown in Fig. 3 is the structure of the developed FLCD. On a color filter substrate 
and a glass substrate with ITO electrodes, there are an insulating film and an 
aligning films coated. The material of the aligning film was polyimide. The rubbing 
direction of both substrates is in the same direction (parallel rubbing). An aligning 
film with a medium pretilt angle (about 3˚) was utilized in order to gain 100% of 
the C2U state without any zigzag defects or any C1 states. The molecular 
orientation model of the C2U state is illustrated in Fig. 4. 
Each pixel is divided into two areas with 1:2 ratio so as to realize spatial dither 
gray scale, as described in the next section. Spacer walls were constructed within 
the panel in order to show high shock stability. The cell spacing was 1.3 m. 
Optimal adhesion between both substrates was obtained, yielding higher shock 
stability more than 20kg/cm2.
16 | P a g e 
Fig. 3 Device structure of 
the developed FLCD. 
Fig. 4 The C2U orientation.
1•3 Gray Scale and Addressing 
Combining 2-bit spatial dither and 3-bit temporal dither, 64 gray levels for each 
color were achieved to realize 262,000 colors. The 2-bit spatial dither ratio was 
one to two (1:2) and 3-bit temporal dither ratio was one to four to sixteen (1:4:16). 
The driving waveforms are shown in Fig.5. The duty ratio was 1/480 and the line 
address time was 23 sec/line. The typical values of voltages were Vs=40V and 
Vd=7V. 
Fig. 5 Drive waveform which is applied in the 6"-prototype FLCD. 
17 | P a g e
2. 6-Inch Color FLCD (Prototype) 
A color 6"-prototype FLCD with 240x320 
dots was fabricated, utilizing key technologies 
described in the above. The main 
specifications are as follows: 
Number of Pixels 240 x 320 dots 
Number of Colors 262,000 colors 
Contrast Ratio 60:1 
Shock Stability 20kg/cm2 
Memory Angle 30 degrees 
More detailed specifications are summarized in 
Table 1 Conclusion 
The development described in this paper has 
solved two fundamental problems of FLCD. 
The one is gray scale and the other is shock 
stability. Further development is required in 
order to realize large size FLCDs with high 
information content and also to solve the 
pseudo edge problem,which is induced by 
digital gray technique as well as PDP. 
18 | P a g e 
Table 1 The specifications of the developed 
6"color FL
Properties and uses 
 Very thin layer (less than 2 μm thick) can help produce a 90° polarisation 
twist. 
19 | P a g e 
1) High density displays with small display areas can be produced. 
2) DisplayTECH claims that a stamp sized FLCD can drive resolutions 
needed for 50 inch screens. 
 Switching time is less than 100 μs 
1) High frame rate video displays are possible. 
 Magnetic polarisation effect is bistable. 
1) Can be used for low frame rate displays that can run on very low 
power 
2) This property can help build display with non-volatile memory with the 
advantage that the memory can be changed easily. 
 Viewing angle is greater than 120° 
1) This makes it suitable for commercial TV applications. 
 Some commercial products do seem to utilize FLCD. 
 High switching allows building optical switches and shutters in printer heads.
20 | P a g e 
Challenges 
• The problems facing ferroelectric researchers are numerous. 
• Alignment defect control (sensitive to shock and vibration) 
• Cell spacing control 
• Temperature range 
• Response time, and Gray Scale 
New fluorinated liquid crystal compounds are being developed to 
help decrease the response time and improve the contrast ratio 
(contrast is limited by defects).
21 | P a g e 
Conclusion 
• Prospects for the future are mixed for this technology. 
• While much research continues, it is unclear what market the 
ferroelectric LCD will serve. 
• Certainly, if the problems can be solved, then the high contrast 
and wide viewing angle achieved with ferroelectric LCDs will 
put them in competition with active matrix LCDs.
22 | P a g e 
References 
 N. A. Clark and S. T. Lagerwall, Appl. Phys. Lett., 36, 899 (1980). 
 Mitsuhiro Koden, Optronics, No.2, 52 (1994). 
 M. Koden, Ferroelectrics, 179, 121 (1996). 
 M. Koden, H. Katsuse, A. Tagawa, K. Tamai, N. Itoh, S. Miyoshi and 
T. Wada, Jpn. J. Appl. 
 A. Tsuboyama, Y. Hanyu, S. Yoshihara and J. Kanbe, Proc. Japan 
Display '92, 53 (1992). 
 M. Koden, T. Numao, N. Itoh, M. Shiomi, S. Miyoshi and T. Wada, 
roc. Japan Display '92, 
 Y. Hanyu, K. Namamura, Y. Hotta, S. Yoshihara and J. Kanbe, SID 
93 Digest, 364 (1993). 
 H. Mizutani, A. Tsuboyama, Y. Hanyu, S. Okada, M. Terada and K. 
Katagiri,
23 | P a g e
24 | P a g e

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Seminar file(ferroelectric liquid crystal display)

  • 1. 1 | P a g e COLLEGE NAME A Technical seminar report on Ferroelectric liquid crystal display (FLCD) In partial fulfillment for the award of the degree Of BACHELOR OF TECHNOLOGY IN ELECTRONICS & TELECOMMUNICATION ENGINEERING SUBMITTED TO: SUBMITTED BY: Assistant Professor
  • 2. 2 | P a g e CERTIFICATE This is to certify that the technical seminar Report entitled “Ferroelectric liquid crystal display” is a bonafied work presented by ROHIT SINGH in a partial fulfillment for the award of degree of Bachelor of technology in ELECTRONICS & TELECOMMUNICATION ENGINEERING in COLLEGE OF ENGINEERING ROORKEE during the year 2011-2015. Assistant Professor College Of Engineering Roorkee
  • 3. 3 | P a g e Content 1. Introduction on Flcd…………………………………4 2. Lcd……………………………………………………5 2.1 Advantages and disadvantages on Lcd………8 3. Introduction of Amlcd………………………………10 4. Operation On Flcd………………………………….11 5. Molecular orientation control……………………..12 5.1 Key Technologies for the Vmin Mode FLCDs..14 5.2 Device Structure & Molecular Orientation…….15 5.3 Gray Scale and Addressing…………………….17 6. Properties and uses………………………………...19 7. Challenges…………………………………………..20 8. Conclusion…………………………………………..21 9. Refrences……………………………………………22
  • 4. 4 | P a g e Ferroelectric Liquid Crystal Display Introduction Ferro Liquid Display, or Ferro-electric Liquid Display (FLD) or Ferro Fluid Display (FFD), is a display technology based on the ferroelectric properties of certain liquids. Not all such fluids are crystal but they are generically referred to as Ferro Liquid Crystal Displays (FLCD). The dot pitch of such displays can be as low as 10 μm giving a very dense high resolution display on a small area. These might find applications in 3D displays and head mounted displays (HMD) where typical LCDs have failed to provide anything better than a 640x480 (RGB pixel) resolution on a sq.cm display area. Displays based on these are still experimental or of less commercial value only due to the costs. Gradual adoption in consumer electronics is expected to bring the costs down. A major drawback is that the angle of twist is not easily controlled by intensity of magnetic field. To produce color scales, time multiplexing might be used exploiting the quick switching time. The materials found so far are sensitive to vibration and shock. Since Clark and Lagerwall invented the basic principle of ferroelectric liquid crystal displays (FLCDs), much effort has been devoted to the development of FLCDs, aiming at practical applications. While the conventionally existing LCDs such as STN LCDs and TFT-LCDs utilize a nematic liquid crystal phase, it is remarked that FLCDs utilize a chiral smectic C liquid crystal phase with Fig. Principle of FLCD.
  • 5. spontaneous polarization (Ps). In the chiral smectic C phase, liquid crystal molecules have a layer structure in which the mean direction of molecular long axis is tilted against layers. In thin FLC cells, a bistability appears with two bistable states as shown in Fig.1(a)(b) . Ferroelectric liquid crystals have a spontaneous polarization (Ps) whose direction is perpendicular to the layer. When the electric field is applied, molecules re-align in a way that the direction of the spontaneous polarizations is the same as that of the electric field. Combining a pair of polarizers (polarizer and analyzer), FLCDs can realize dark and bright states. Since nematic liquid crystal is paraelectric, the order of response time is usually sec. On the contrary, FLC shows sec in its order of response time because of the direct interaction between electric field and Ps. In addition, FLCDs have several advantages, such as wide viewing angle due to the in-plane switching (IPS) and memory effect due to the bistability. The combination of fast response time and memory effect allows large-size direct-view simple-multiplexing LCDs with high resolution. LCD LCD (liquid crystal display) (from Whatis) is the technology used for displays in notebook and other smaller computers. Like light-emitting diode (LED) and gas-plasma technologies, LCDs allow displays to be much thinner than cathode ray tube (CRT) technology. LCDs consume much less power than LED and gas-display displays because they work on the principle of blocking light rather than emitting it. An LCD is made with either a passive matrix or an active matrix display display grid. The active matrix LCD is also known as a thin film transistor (TFT) display. The passive matrix LCD has a grid of conductors with pixels located at each intersection in the grid. A current is sent across two conductors on the grid to control the light for any pixel. An active matrix has a transistor located at each pixel intersection, requiring less current to control the luminance of a pixel. For this reason, the current in an active matrix display can be switched on and off more frequently, improving the 5 | P a g e
  • 6. screen refresh time (your mouse will appear to move more smoothly across the screen, for example). Active matrix is the superior technology. Color LCD An LCD that can show colors must have three subpixels with red, green and blue color filters to create each color pixel. Through the careful control and variation of the voltage applied, the intensity of each subpixel can range over 256 shades. Combining the subpixels produces a possible palette of 16.8 million colors (256 shades of red x 256 shades of green x 256 shades of blue), as shown below. These color displays take an enormous number of transistors. For example, a typical laptop computer supports resolutions up to 1,024x768. If we multiply 1,024 columns by 768 rows by 3 subpixels, we get 2,359,296 transistors etched onto the glass! If there is a problem with any of these transistors, it creates a "bad pixel" on the display. Most active matrix displays have a few bad pixels scattered across the screen. LCD Features and Attributes To evaluate the specifications of LCD monitors, here are a few more things you need to know. Native Resolution Unlike CRT monitors, LCD monitors display information well at only the resolution they are designed for, which is known as the native resolution. Digital displays address each individual pixel using a fixed matrix of horizontal and vertical dots. If you change the resolution settings, the LCD scales the image and the quality suffers. Native resolutions are typically: 17 inch = 1024x768 19 inch = 1280x1024 20 inch = 1600x1200 6 | P a g e
  • 7. Viewing Angle When you look at an LCD monitor from an angle, the image can look dimmer or even disappear. Colors can also be misrepresented. To compensate for this problem, LCD monitor makers have designed wider viewing angles. (Do not confuse this with a widescreen display, which means the display is physically wider.) Manufacturers give a measure of viewing angle in degrees (a greater number of degrees is better). In general, look for between 120 and 170 degrees. Because manufacturers measure viewing angles differently, the best way to evaluate it is to test the display yourself. Check the angle from the top and bottom as well as the sides, bearing in mind how you will typically use the display. Brightness or Luminance This is a measurement of the amount of light the LCD monitor produces. It is given in nits or one candelas per square meter (cd/m2). One nit is equal to on cd/m2. Typical brightness ratings range from 250 to 350 cd/m2 for monitors that perform general-purpose tasks. For displaying movies, a brighter luminance rating such as 500 cd/m2 is desirable. Contrast Ratio The contrast ratio rates the degree of difference of an LCD monitor's ability to produce bright whites and the dark blacks. The figure is usually expressed as a ratio, for example, 500:1. Typically, contrast ratios range from 450:1 to 600:1, and they can be rated as high as 1000:1. Ratios more than 600:1, however, provide little improvement over lower ratios. Response Rate The response rate indicates how fast the monitor's pixels can change colors. Faster is better because it reduces the ghosting effect when an image moves, leaving a faint trial in such applications as videos or games. Adjustability Unlike CRT monitors, LCD monitors have much more flexibility for positioning the screen the way you want it. LCD monitors can swivel, tilt up and down, and even rotate from landscape (with the horizontal plane longer than the vertical plane) to 7 | P a g e
  • 8. portrait mode (with the vertical plane longer than the horizontal plane). In addition, because they are lightweight and thin, most LCD monitors have built-in brackets for wall or arm mounting. Besides the basic features, some LCD monitors have other conveniences such as integrated speakers, built-in Universal Serial Bus (USB) ports and anti-theft locks. Advantages of Lcd  Thin Profile LCDs feature very thin profiles, making them the perfect choice for small work spaces.  Standard Screen Sizes Unlike CRTs, there is no variance between the monitor size and the screen size. For example, a 17-inch monitor features a 17-inch viewable image.  Bright Screens LCDs, thanks to the florescent backlight, produce bright, rich images  Low Energy Consumption In general, LCD monitors consume about half of the energy of standard CRTs.  Flicker-Free Refresh Rates Refresh rate is less of an issue with LCD monitors. LCDs are designed to have flicker-free refresh rates at 60Hz.  High Contrast Ratios LCD monitors tend to feature excellent contrast ratios, which insure bright, clear images. Make sure the monitor you purchase has a contrast ratio of at least 400:1 or more. 8 | P a g e
  • 9. Disadvantages of Lcd  Single Resolution LCDs are generally designed to work best in a single resolution. They tend not to have the flexibility that CRTs have to display multiple resolutions well.  Narrow Viewing Angles LCDs tend to have a very narrow viewing angle. As you vary from looking at a LCD straight-on the image gradually degrades. Look for at least a 160° viewing angle.  Slow Pixel Response Time LCDs tend to have a much slower pixel response time, which can mean image artifacts remaining onscreen after movement. For example, when you move your mouse quickly across the screen you might see the cursor create shadow images of itself briefly. These disappear instantaneously. In order to avoid this try to find a monitor that has a response time of 25 milliseconds or faster. 9 | P a g e
  • 10. Active Matrix Crystal Display An active-matrix liquid-crystal display (AMLCD) is a type of flat panel display, the only viable technology for high-resolution TVs, computer monitors, notebook computers, tablet computers and smartphones with an LCD screen, due to low weight, very good image quality, wide color gamut and response time. The concept of active-matrix LCDs was invented by Bernard J. Lechner at the RCA Laboratories in 1968.The first functional AMLCD display with thin-film transistors was made byT Peter Brody and his team at Westinghouse Electric Corporation in 1973.]However, it took years of additional research by others to launch successful products. Introduction on Active Matrix Crystal Display The most common type of LCD display contains, besides the polarizing sheets and cells of liquid crystal, a matrix of thin-film transistors to make a thin-film-transistor liquid-crystal display.These devices store the electrical state of each pixel on the display while all the other pixels are being updated. This method provides a much brighter, sharper display than a passive matrix of the same size. An important specification for these displays is their viewing-angle. Thin-film transistors are usually used for constructing an active matrix so that the two terms are often interchanged, even though a thin-film transistor is just one component in an active matrix and some active-matrix designs have used other components such as diodes. Whereas a passive matrix display uses a simple conductive grid to apply a voltage to the liquid crystals in the target area, an active-matrix display uses a grid of transistors and capacitors with the ability to hold a charge for a limited period of time. Because of the switching action of transistors, only the desired pixel receives a charge, and the pixel acts as a capacitor to hold the charge until the next refresh cycle, improving image quality over a passive matrix. This is a special version of a sample-and-hold circuit. 10 | P a g e
  • 11. FLCD Operating Principle An FLCD acts as a classical half-wave plate, one whose optic axis can be reoriented by an applied field. If the optic axis is parallel or perpendicular to incoming polarized light, the light passes through the FLCD unchanged and is blocked by the exit polarizer(oriented at 90o to the entrance polarizer) If the optic axis makes an angle of 45o to the incoming polarized light, the direction of polarization changes by 90o and is able to pass through the exit polarizer Orientation of FLF molecules is changed by applying a voltage pulse of suitable polarity. 11 | P a g e
  • 12. • In thin FLC cells, a bistability appears with two bistable states as shown in Fig. • Ferroelectric liquid crystals have a spontaneous polarization (Ps) whose direction is perpendicular to the layer. • When the electric field is applied, molecules re-align in a way that the direction of the spontaneous polarizations is the same as that of the electric field. • Combining a pair of polarizers (polarizer and analyzer), FLCDs can realize dark and bright states. Molecular orientation control The molecular orientation control is one of the most important key technologies for the development of practical FLCDs. The molecular orientations of FLCDs are classified as two layer structures: a bookshelf layer and a chevron layer. The FLC cells with parallel rubbing, in which the rubbing directions of both substrates are the same, have been known to show four orientational states with a chevron layer structure: C1-uniform (C1U), C1-twisted (C1T), C2- uniform (C2U) and C2-twisted (C2T). Among them, the C1U and C2U orientations are useful for practical applications because of their extinction positions between cross nicols. 12 | P a g e
  • 13. • So, an unconstrained system, the azimuthal direction in which the molecules tilt away from the layer normal will differ slightly from one layer to the next. • Typically, the FLCDs are built with cell gaps less than 2 μm for stable molecular alignment. • Alignment layer causes perpendicular stacked alignment. • The cell's polarisation is determined by the magnetic field applied. That in turn results in opaque or transparent layer when used in combination with polarised layers as in LCD The alignment film with a high pre-tilt angle (over 15 degrees) induced the selective formation of the C1U orientation and also that the C1U orientation gave a high contrast ratio under simple-multiplexing driving waveforms for FLCDs. Using the C1U orientation, Hanyu et al. have developed a 21-inch color FLCD (1024 x 1280 dots, contrast ratio of 40:1 and 64 colors). 13 | P a g e Fig. Principle of FLCD.
  • 14. Recently, Mizutani et al. developed a 15" full-color FLCD (768 x 1024 dots, 36 sec/line, CR=100:1) with a bookshelf layer structure, realizing full-color images by a combination of 4-bit spatial dither and dither methods.Futhermore, Koden et al. have reported that the C2U orientation can show a high contrast ratio, fast line address time and wide memory angle if it is combined with the -Vmin. The -Vmin mode utilizes the unique response (t) - voltage (V) characteristics of the minimum value, which is observed in FLC materials with large positive dielectric biaxiality (negative dielectric anisotropy). The -Vmin mode utilizing the C2U orientation is a promising technology for digital gray scale method with temporal dither because it can realize faster line address time than the C1U orientation and the bookshelf orientation can. Compared with the existing LCDs, the FLCD have received an unfavorable reputation of poor performance in moving picture with gray scale and also in shock stability. In this study, key technologies for the -Vmin mode were developed in order to overcome these problems. This paper describes FLC materials that show fast response time for the -Vmin mode, the selective formation of the C2U orientation, the device structure with high shock stability and the digital gray scale driving method, introducing a6-inch color prototype FLCD which was fabricated by using these keytechnologies. 1. Key Technologies for the -Vmin Mode FLCDs 1•1 Ferroelectric Liquid Crystal Materials In the -Vmin characteristics of FLC materials, the minimum voltage ismentioned as Vmin and the minimum response time as min. Low Vmin and fast min are required because the Vmin value determines the drive voltage and the min value determines the line address time. Since the Vmin is closely related to a balance of the dielectric biaxiality and spontaneous polarization (Ps), FLC materials for the -Vmin mode need large positive dielectric biaxiality and small or moderate spontaneous polarization, as well as low viscosity in order to obtain fast tmin. An INAC phase sequence and long helical pitches in nematic and smectic 14 | P a g e
  • 15. C phases are required in order to yield a high quality of alignment on cooling from the isotropic phase.In addition, FLC materials require wide temperature range of smectic C phase because it is related to the operating and storage temperature ranges of FLCDs. 15 | P a g e Fig. 2 The characteristic of the developed FLC material FDS-2. A typical FLC material, FDS-2 was developed for the -Vmin mode. Its characteristics are shown in Fig. 2. This material offers fast min value (12 sec) and reasonable Vmin value (33V) at 25˚C. 1•2 Device Structure & Molecular Orientation Shown in Fig. 3 is the structure of the developed FLCD. On a color filter substrate and a glass substrate with ITO electrodes, there are an insulating film and an aligning films coated. The material of the aligning film was polyimide. The rubbing direction of both substrates is in the same direction (parallel rubbing). An aligning film with a medium pretilt angle (about 3˚) was utilized in order to gain 100% of the C2U state without any zigzag defects or any C1 states. The molecular orientation model of the C2U state is illustrated in Fig. 4. Each pixel is divided into two areas with 1:2 ratio so as to realize spatial dither gray scale, as described in the next section. Spacer walls were constructed within the panel in order to show high shock stability. The cell spacing was 1.3 m. Optimal adhesion between both substrates was obtained, yielding higher shock stability more than 20kg/cm2.
  • 16. 16 | P a g e Fig. 3 Device structure of the developed FLCD. Fig. 4 The C2U orientation.
  • 17. 1•3 Gray Scale and Addressing Combining 2-bit spatial dither and 3-bit temporal dither, 64 gray levels for each color were achieved to realize 262,000 colors. The 2-bit spatial dither ratio was one to two (1:2) and 3-bit temporal dither ratio was one to four to sixteen (1:4:16). The driving waveforms are shown in Fig.5. The duty ratio was 1/480 and the line address time was 23 sec/line. The typical values of voltages were Vs=40V and Vd=7V. Fig. 5 Drive waveform which is applied in the 6"-prototype FLCD. 17 | P a g e
  • 18. 2. 6-Inch Color FLCD (Prototype) A color 6"-prototype FLCD with 240x320 dots was fabricated, utilizing key technologies described in the above. The main specifications are as follows: Number of Pixels 240 x 320 dots Number of Colors 262,000 colors Contrast Ratio 60:1 Shock Stability 20kg/cm2 Memory Angle 30 degrees More detailed specifications are summarized in Table 1 Conclusion The development described in this paper has solved two fundamental problems of FLCD. The one is gray scale and the other is shock stability. Further development is required in order to realize large size FLCDs with high information content and also to solve the pseudo edge problem,which is induced by digital gray technique as well as PDP. 18 | P a g e Table 1 The specifications of the developed 6"color FL
  • 19. Properties and uses  Very thin layer (less than 2 μm thick) can help produce a 90° polarisation twist. 19 | P a g e 1) High density displays with small display areas can be produced. 2) DisplayTECH claims that a stamp sized FLCD can drive resolutions needed for 50 inch screens.  Switching time is less than 100 μs 1) High frame rate video displays are possible.  Magnetic polarisation effect is bistable. 1) Can be used for low frame rate displays that can run on very low power 2) This property can help build display with non-volatile memory with the advantage that the memory can be changed easily.  Viewing angle is greater than 120° 1) This makes it suitable for commercial TV applications.  Some commercial products do seem to utilize FLCD.  High switching allows building optical switches and shutters in printer heads.
  • 20. 20 | P a g e Challenges • The problems facing ferroelectric researchers are numerous. • Alignment defect control (sensitive to shock and vibration) • Cell spacing control • Temperature range • Response time, and Gray Scale New fluorinated liquid crystal compounds are being developed to help decrease the response time and improve the contrast ratio (contrast is limited by defects).
  • 21. 21 | P a g e Conclusion • Prospects for the future are mixed for this technology. • While much research continues, it is unclear what market the ferroelectric LCD will serve. • Certainly, if the problems can be solved, then the high contrast and wide viewing angle achieved with ferroelectric LCDs will put them in competition with active matrix LCDs.
  • 22. 22 | P a g e References  N. A. Clark and S. T. Lagerwall, Appl. Phys. Lett., 36, 899 (1980).  Mitsuhiro Koden, Optronics, No.2, 52 (1994).  M. Koden, Ferroelectrics, 179, 121 (1996).  M. Koden, H. Katsuse, A. Tagawa, K. Tamai, N. Itoh, S. Miyoshi and T. Wada, Jpn. J. Appl.  A. Tsuboyama, Y. Hanyu, S. Yoshihara and J. Kanbe, Proc. Japan Display '92, 53 (1992).  M. Koden, T. Numao, N. Itoh, M. Shiomi, S. Miyoshi and T. Wada, roc. Japan Display '92,  Y. Hanyu, K. Namamura, Y. Hotta, S. Yoshihara and J. Kanbe, SID 93 Digest, 364 (1993).  H. Mizutani, A. Tsuboyama, Y. Hanyu, S. Okada, M. Terada and K. Katagiri,
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