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The energy levels of isolated atoms have definite values and electrons fill these levels according to the laws of quantum mechanics However, when atoms approach one another, their electron shells interact and the positions of the individual energy levels change When the set of atoms finally forms a crystal lattice, the original energy levels combine to form energy bands; each of these bands corresponds to an energy level in the isolated atom Each energy level in a given band can contain a maximum of two electrons When some of the energy bands at a given temperature are completely occupied by electrons and bands with higher energy are empty, and a large amount of energy is required to transfer an electron from the highest occupied energy band to the lowest unoccupied band, the substance is an insulator Metals are examples of the opposite type of solid substance.



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Figure 8.17 RTR-A keeps a database of links and how those links form a path to each network. RTR-A will be able to determine from the updates it receives that it can reach network 2.2.2.0/24 via interface 1/1/1 through RTR-C and then on to RTR-B, but it will know that it can also reach the network through interface 1/1/2 to RTR-B directly, and this will likely be the lower cost and preferred path.

The conductivity band, corresponding to the highest, partially occupied energy levels of the metal atom in the ground state, contains a sufficient number of.

1/1/1 1/1/2 RTR-A RTR-B Network 2.2.2.0 / 24





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Fig 22 Band structure of a semiconductor eg denotes the energy gap (width of the forbidden band) electrons even at absolute zero of temperature to produce the typical high conductivity of metals These loosely bound electrons form an 'electron gas' Under the influence of an external electric field, their originally random motion becomes oriented It should be pointed out that the increase in the electron velocity in the direction of the electric field is much smaller than the average velocity of their random motion Semiconductors form a special group of electronic conductors These are substances with chemically bonded valence electrons (forming a 'valence' band); however, when energy is supplied externally (eg by irradiation), these electrons can be excited to an energetically higher conduction band (see Fig 22) A 'forbidden' band lies between the valence and conductivity bands.

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Adjacency Database RTR-B on 1/1/2 RTR-C on 1/1/1

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The energy difference between the lowest energy level of the conductivity band and the highest level of the valence band is termed the band gap sg (the width of the forbidden band) Electric current is conducted either by these excited electrons in the conduction band or by 'holes' remaining in place of excited electrons in the original valence energy band These holes have a positive effective charge If an electron from a neighbouring atom jumps over into a free site (hole), then this process is equivalent to movement of the hole in the opposite direction In the valence band, the electric current is thus conducted by these positive charge carriers Semiconductors are divided into intrinsic semiconductors, where electrons are thermally excited to the conduction band, and semiconductors with intentionally introduced impurities, called doped semiconductors, where the traces of impurities account for most of the conductivity.

Link State Database RTR-A to RTR-C, cost =1000 RTR-A to RTR-B, cost =1000 RTR-C to RTR-B, cost =1000 RTR-B to 2.2.2.0 / 24, cost =1000 Routing Table 2.2.2.0/24 via 1/1/2

If the impurity is an electron donor (for germanium and silicon, group V elements, eg arsenic or antimony), then a new energy level is formed below the conduction band (see Fig 23A) The energy difference between the lowest level of the conductivity band and this new level is denoted as sd This quantity is much smaller than the energy gap ed Thus electrons from this donor band pass readily into the conductivity band and represent the main contribution to the semiconductor conductivity As the charge carriers are electrons, ie negatively charged species, these materials are termed n-type semiconductors..

To achieve information convergence, each router performs a series of procedures to build its routing table. First, it keeps track of all of its neighboring routers. Second, it builds an LSP that lists neighbor router names and link metrics (cost). This includes new neighbors, changed metrics, and links to neighbors that are down. These steps are illustrated in Figure 8.18.

Fig. 2.3 Schematic structure of a silicon semiconductor of (A) n type and (B) / type together with the energy level array. (According to C. Kittel)

Figure 8.18 When link state protocols are used, each router keeps a database of each of its links and the associated cost for each link. The cost is usually based on a default value that is a function of the speed of the interface.

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