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The sound is applied to the transition.
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Figure 5.6. (a) The structure of a fabricated solution-processed LTPS TFT. (b) The transfer characteristics of LTPS TFTs, whose silicon lm was formed by CVD (dotted line), spin coating (dashed line), and inkjet printing (solid line), respectively. The drain current of the inkjetted TFT is normalized to have the same channel width and length as the CVD-formed and spin-coated TFTs, for comparison. [Reproduced with permission from Ref. 10. Copyright 2006 Nature Publishing Group.]
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FigurE 3-14: The Pictures hub is, perhaps, the most obvious example of why this UI type is such a good idea.
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The reason for this different behavior is as follows. By taking away a mass E from the central part of a distribution F and moving one-half of it to the extreme left, and the other half to the extreme right, we get a distribution that is within Prohorov , distance E , but within LCvy distance ~ / 2 of the original F .
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1: 2 fo = 7.128 GHz w o = 2pfo = 2p *7.128 GHz CS1 = 0.632 pF LS2 = LS3 = 0.789 nH
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As an introduction to the rather involved subject of multipath propagation and fading, we consider the simplest possible case time-invariant propagation along two paths. We transmit a sinusoidal waveform and determine the (complex) transfer function at the location of the RX. First, consider a single wave. Let the transmit signal be a sinusoidal wave: ETX (t) cos(2 fc t) (5.1)
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