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In this way an energy barrier is produced, as shown at Figure 318b, that the electrons are unable to climb over and the holes (for which increased energy is downward) are unable to crawl under The height of this potential barrier is the device s open-circuit contact potential Note that there is almost no place along the length of the device where there are simultaneously many electrons in the conduction band of energy and at the same place many holes in the valence band However, if one now applies a forward current, as at Figure 318c, wherein the electrons ow from the right, the large potential barrier that we had for the open-circuited condition Figure 3.

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1 The individual s wishes will harm me or others unnecessarily 2 The individual is reasoning erroneously he may be thinking illogically he may be deriving false conclusions, or he may have false beliefs (but, if so, then an attempt must be made to move him as soon as possible to the point where the autonomy ip can occur) Note: At this point in the Autonomy Test it is very important to bear in mind the distinction between physical autonomy the freedom that a person has to live without physical obstruction and mental autonomy the freedom that a person has to make decisions and act on them.

18b is reduced, which reduces the coulomb repulsion that was holding the electrons on one side and holes on the other, and the depletion layer is no longer depleted there are electrons in the conduction band and holes in the valence band at the same place along the device, namely near the interface between the n-side and the p-side The result is shown at Figure 318d, where holes and electrons at the same place combine to produce radiation of the frequency Eg/h As we saw with the P I curve of Figure 314, as the current is increased, the potential barrier is reduced still further, more photons are produced, and if there are mirror facets at the ends of the active region (vertically in the diagram), stimulated emission rapidly predominates over spontaneous emission, and lasing starts taking place.

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If there are no mirrors, spontaneous emission continues to grow in intensity with injected current, thus forming not a laser but an LED The converse processes for a so-called PN photodiode are shown in Figure 319 Going back to Figures 318a and 318b, we see the open-circuit condition, as before Now, as Figure 319 shows, sending current through the device in the opposite direction, as shown at Figure 319a, the depletion region of Figure 319b, instead of getting narrower becomes even wider than in the unbiased case of Figures 318a and 318b The potential barrier becomes even taller, that is, the voltage difference across the depletion region becomes even stronger, and every time an electron-hole pair is created by an incident photon of f Eg/h arriving.

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