on-current Ion ≥ 1 μ A meets the constraint in inequality (2.20).
The voltage across the pixels has to be free of dc in order to avoid dissociation of the ingredients in the LC material. Therefore, the voltage VLC applied in the next frame time has the alternate sign as indicated in Figure 2.17. As we have observed in Section 2.2.1, the operation of the TN cell is independent of the sign of the electrical field vector. The alteration in sign from frame to frame is mandatory for a sufficient life of the LC cell. The transmitted luminance of an LC cell in Figure 2.13 exhibits a linear dependence on VLC in a range of about 3 V. For 256 grey shades, this results in steps of 11.7 mV/grey shade. Special care will be taken to ensure the accuracy of these steps, as the voltages are altered by parasitic capacitive couplings. Remedies against this damage will be the alternating signs of VLC from row to row, column to column, frame to frame, and combinations of these measures.
TFT-addressed LCDs offer an appealing picture quality, mainly due to the absence of flicker. TFTs are fabricated together with the storage capacitors, ITO electrodes and conductors in thin film technology on glass or plastics as substrates. Glass substrates used to be 1.2 mm thick, and are presently down to 0.7 mm, whereas plastic materials excel in a thickness of only 100 μ to 200 μ. As monocrystalline layers are unfeasible in thin film technology, the semiconductor in the TFTs is either amorphous or polycrystalline. Materials are a-Si, poly-Si and, more seldom, CdSe. Alternative pixel switches are MIMs or thin film diodes.
A more economical method of addressing does not require the above-mentioned pixel switches, and generates the voltages across the pixels by a superposition of voltages at the contact pads. This is called Passive Matrix (PM) addressing which, however, exhibits shortcomings.
A more detailed discussion of all addressing schemes starts with Chapter 10.
References
1 Bahadur, B. (1990) Liquid Crystals, Applications and Uses, vol. 1. World Scientific.
2 Born, M. and Wolf, E. (1980) Principles of Optics, 6th ed., Pergamon Press, Oxford.
3 Demus, D., Goodby, J., Gray, G. W., Spiess, H.-W. and Vill, V. (1998a) Handbook of Liquid Crystals, vol. 2A. Wiley-VCH.
4 Demus, D., Goodby, J., Gray, G. W., Spiess, H.-W. and Vill, V. (1998b) Handbook of Liquid Crystals, vol. 2B. Wiley-VCH.
5 Kaneko, E. (1987) Liquid Crystal TV Displays. KTK Scientific Publishers, Tokyo.
6 Lueder, E. (1998a) Fundamentals of Passive and Active Matrix Liquid Crystal Displays. Short Course S-1, SID, May.
7 Tsvetkov, V. (1942) Acta Physicochim. (USSR) 16, 132.
3
Electro-optic Effects in Untwisted Nematic Liquid Crystals
3.1 The Planar and Harmonic Wave of Light
A planar and harmonic wave of light (Lueder, 1998a; Born and Wolf, 1980; Yeh, 1988) is assumed to propagate through anisotropic liquid crystal layers with refractive indices n|| and n┴. Together with a polarizer and an analyser, they generate grey shades controlled by a voltage. For the derivation of these electro-optic effects, we first need to consider the basic equations for planar harmonic waves. A harmonic electric field E(t) with amplitude E0 is given by the scalar
where t is the time, ω the angular frequency and φ a phase angle. A travelling planar wave is a harmonic oscillation in a plane A in Figure 3.1 in the distance
Maxwell’s equations provide for the speed of light in vacuum
(3.3)
Figure 3.1 The plane A in which a planar wave travels with speed c1 and wave vector
and in materials
where μ0, ε0 are the permeability and permittivity in vacuum, and μr and εr are the pertinent relative constants in materials. Further, for μr = 1 the refractive index is
The wavelength λ in vacuum is given by
where f= ω/2π is the frequency. Equations (3.4), (2.6) and (3.5) provide for μr =1:
which results in the wave vector