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Scanning circuitry

As an example, linear arrays of silicon photodiodes (photodiode arrays) are available as a package complete with the necessary circuitry to read out the array following exposure. Arrays are available with up to 2048 elements, and they are read out on an element by element basis. The scanning circuitry can access an element in 10 - 25 /rs, which suggests that the entire array can be read out in approximately 20 - 50 ms. Thus modulation frequencies can not exceed 50 Hz. However, as was discussed earlier, PEMs are driven at a resonant frequency which usually varies between 50 and 100 kHz, and this exceeds the readout rate of the photodiode array by three orders-of-magnitude. [Pg.27]

Figure 54. Thin film transistor matrix display with peripheral scanning circuitry (after reference [115]). Figure 54. Thin film transistor matrix display with peripheral scanning circuitry (after reference [115]).
Electron Beam Techniques. One of the most powerful tools in VLSI technology is the scanning electron microscope (sem) (see Microscopy). A sem is typically used in three modes secondary electron detection, back-scattered electron detection, and x-ray fluorescence (xrf). AH three techniques can be used for nondestmctive analysis of a VLSI wafer, where the sample does not have to be destroyed for sample preparation or by analysis, if the sem is equipped to accept large wafer-sized samples and the electron beam is used at low (ca 1 keV) energy to preserve the functional integrity of the circuitry. Samples that do not diffuse the charge produced by the electron beam, such as insulators, require special sample preparation. [Pg.356]

Another important field where inorganic nanotubes can be useful is as tips in scanning probe microscopy (16). Here, applications in the inspection of microelectronics circuitry have been demonstrated and potential applications in nanolithography are being contemplated. A comparison between a WS2 nanotube tip and a microfabricated Si tip indicates that while the microfabricated conical-shaped Si tip is unable to probe the bottom of deep and narrow grooves, the slender and inert... [Pg.308]

The precision resistors R5, R16, and R36 provide 10-fold changes in time constant (and therefore scan rate) via SW2. Figure 6.15 shows the control and current conversion circuitry that when combined with Figure 6.14 give a complete cyclic voltammetry instrument. [Pg.182]

The time range of the electrochemical measurements has been decreased considerably by using more powerful -> potentiostats, circuitry, -> microelectrodes, etc. by pulse techniques, fast -> cyclic voltammetry, -> scanning electrochemical microscopy the 10-6-10-1° s range has become available [iv,v]. The electrochemical techniques have been combined with spectroscopic ones (see -> spectroelectrochemistry) which have successfully been applied for relaxation studies [vi]. For the study of the rate of heterogeneous -> electron transfer processes the ILIT (Indirect Laser Induced Temperature) method has been developed [vi]. It applies a small temperature perturbation, e.g., of 5 K, and the change of the open-circuit potential is followed during the relaxation period. By this method a response function of the order of 1-10 ns has been achieved. [Pg.580]

Very large chemical shifts are possible, which require long times to scan (hours to days), and may require retuning circuitry or changing radio-frequency coils. [Pg.6231]

Complete MCP s can be stacked to provide even higher gains. For response in the vacuum ultra-violet spectral region (50-200 nm) a SSANACON, self-scanned anode array with microchannel plate electron multiplier, has been used (36). This involves photoelectron multiplication through two MOP S, collection of the electrons directly on aluminum anodes and readout with standard diode array circuitry. In cases where analyte concentrations are well above conventional detection limits, multi-element analysis with multi-channel detectors by atomic emission has been demonstrated to be quite feasible (37). Spectral source profiling has also been done with photodiode arrays (27.29.31). In molecular spectrometry, imaging type detectors have been used in spectrophotometry, spectrofluometry and chemiluminescence (23.24.26.33). These detectors are often employed to monitor the output from an HPLC or GC (13.38.39.40). [Pg.61]

Hardware. To employ the IDA, the user must supply a clock signal, a begin scan signal, and data acquisition hardware. The hardware to accomplish this has been based on a PDP 11/20 minicomputer or a KIM microcomputer plus additional external hardware (13-15). The clock signal determines the rate at which the diodes are interrogated during readout and was 33 kHz with the minicomputer and 125 kHz with the microcomputer. This means the time to read out all 512 diodes and hence the minimum integration time varies from 15 ms to 3.7 ms, respectively. For the microcomputer, direct memory access (DMA) circuitry was used to increase the data acquisition rate. [Pg.157]

We believe that 2.5-D DFT techniques should be developed to resolve the above problems. The test data compression technique would be essential to test a partial netlist with a large number of inter-chip contacts based I/O. Extra testing circuitry should be inserted so that compressed test results can be accessed through conventional testing pads (e.g., on the boundary) of a chip. Meanwhile, scan chains... [Pg.172]

Constant height mode of operation is reserved for small scan areas and atomically smooth surfaces. The use of little or no feedback during scanning in constant height mode makes it possible to scan at much higher rates than in constant current mode, which is limited by the feedback circuitry. [Pg.135]

Figure 6-5. Film thickness by capacitance with a scanning deposited chromium transducer. (a) Chromium electrode and electrical circuitry, (b) Oscilloscope trace of potential across resistance R. Figure 6-5. Film thickness by capacitance with a scanning deposited chromium transducer. (a) Chromium electrode and electrical circuitry, (b) Oscilloscope trace of potential across resistance R.
By now it should be clear that fully characterizing an electrochemical process by impedance methods can be a tedious operation, because one requires information at a set of frequencies ranging over 2 to 3 decades and at a set of potentials ranging over E 100 mV. For example, the data in Figure 10.5.4 alone required eight ac polarograms, each scanned with the tuned circuitry set to a different frequency and each having the in-phase... [Pg.407]


See other pages where Scanning circuitry is mentioned: [Pg.65]    [Pg.287]    [Pg.300]    [Pg.117]    [Pg.119]    [Pg.148]    [Pg.65]    [Pg.287]    [Pg.300]    [Pg.117]    [Pg.119]    [Pg.148]    [Pg.1018]    [Pg.431]    [Pg.94]    [Pg.180]    [Pg.140]    [Pg.16]    [Pg.941]    [Pg.199]    [Pg.238]    [Pg.356]    [Pg.128]    [Pg.60]    [Pg.425]    [Pg.20]    [Pg.227]    [Pg.581]    [Pg.891]    [Pg.455]    [Pg.724]    [Pg.23]    [Pg.69]    [Pg.242]    [Pg.140]    [Pg.38]    [Pg.47]    [Pg.251]    [Pg.116]    [Pg.746]    [Pg.506]   
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