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Matrix array

The ultrasonic tomograph A1230 was developed to visualize in case of one side access the internal reinforced concrete structure at the depth of 1 m. This device uses 36-elements matrix array. [Pg.911]

The fifth of the color methods places the three emitting structures in a stack one on top of the other, rather than side by side ]20l ]. Clearly there is a requirement here that the two electrodes in the middle of the structure must be transparent. The advantages are that the display can be made much brighter with up to three times the luminance from each pixel, and the requirements for high resolution patterning are relaxed by a factor of three. The disadvantages are that three times as many layers must be coated (without defects) over the area of the display and electrical driving circuitry must make contact with four sets of elec- trades. It will be extremely difficult to incorporate a stacked OLED into a active matrix array. [Pg.553]

Examples for Selecting Elements from a Matrix, Array, or Data Frame... [Pg.324]

This work introduced the concept of a vibronic R-matrix, defined on a hypersurface in the joint coordinate space of electrons and intemuclear coordinates. In considering the vibronic problem, it is assumed that a matrix representation of the Schrodinger equation for N+1 electrons has been partitioned to produce an equivalent set of multichannel one-electron equations coupled by a matrix array of nonlocal optical potential operators [270], In the body-fixed reference frame, partial wave functions in the separate channels have the form p(q xN)YL(0, radial channel orbital function i/(q r) and antisymmetrized in the electronic coordinates. Here 0 is a fixed-nuclei A-electron target state or pseudostate and Y] is a spherical harmonic function. Both and i r are parametric functions of the intemuclear coordinate q. It is assumed that the target states 0 for each value of q diagonalize the A-electron Hamiltonian matrix and are orthonormal. [Pg.169]

Fig. 11.14. Schematic diagram of a typical pixel circuit for an active-matrix array. Fig. 11.14. Schematic diagram of a typical pixel circuit for an active-matrix array.
Variations of the ON and OFF current of an active matrix array of 100 OTFTs on a PET substrate. (Reprinted with permission from Ref. [72]). [Pg.317]

Fig. 3. Design of a-Si H FET. (a) Section through device, (b) FET in part of matrix array. ITO, indium-tin oxide squares A, contact hole etched through SiN film. [From Snell et al. (1981a).]... Fig. 3. Design of a-Si H FET. (a) Section through device, (b) FET in part of matrix array. ITO, indium-tin oxide squares A, contact hole etched through SiN film. [From Snell et al. (1981a).]...
On the Si MOS-switching-FET matrix array, a-Si H is deposited by rf reactive sputtering in Ar and H2 atmosphere. This sputtered a-Si H is also used in vidicons (Imamura et al., 1980). Then the ITO common electrode is... [Pg.154]

Finally the four matrix arrays ss, gs, SS, and SG of direct and total exchange areas must satisfy matrix conservation relations, i.e.,... [Pg.25]

The metastability phenomena influence the performance of the active matrix arrays. Defect creation in the channel causes a threshold voltage shift when a TFT is held on for an extended time and results in a slow drift of the on-current. Fortunately the rate of defect creation is low at room temperature and represents a minor problem. There is a larger effect on the characteristics of the high voltage TFTs. Resistors fabricated from n a-Si H change their resistance slowly because of defect equilibration and can affect the gain of amplifier circuits. [Pg.395]

Matrix array hybridization on silicon wafers ( genosensors on chips )... [Pg.303]

Discussion The program reads and prints the ALTERA data cards, and checks for illegal compartments or species names. Then it puts the matrix entry on the data card into the array AIJ in place of whatever entry was there. A matrix entry may be changed to zero, or changed from zero, if desired. Since new (non-zero) entries may be put in where zero entries were previously, this will affect the total number of entries NAIJ as well as the matrix arrays. This program ignores the c—value field of the data... [Pg.100]

DELETE affects the matrix arrays AIJ, IROW and JCOL, and the number of entries NAIJ. The array C of free—energy values is affected. The rows data in storage is not changed in any way but the number of rows to be used in the problem, M, is adjusted. Thus a row which has been removed from the problem is still available and can be restored. [Pg.111]


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See also in sourсe #XX -- [ Pg.262 ]




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