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studied in condensed-matter physics The macroscopic quantum phenomena observed in quantum liquids, such as super uidity, is also seen in certain metallic and ceramic materials as superconductivity [22] Metals8 do not hold on to their electrons very tightly An important e ect of the electropositive nature of metals is that the orbitals in metals are highly di use and cover a large volume of space around the atoms, which allows the orbitals to interact directly with many other atoms at once to create molecular orbitals which are delocalized, or spread out over a large distance The net e ect is a continuous band of available locations and energies for the electrons within the substance Finally, metals tend to have more orbitals available than electrons to ll them.

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ascertain its deviation from atness. Let us consider a spherical surface of large radius of curvature R in contact with the optical at. Then the sag of the surface is given by x2 =2R, where x is the distance measured from the center of symmetry. Hence the OPD is given by x2 =R l=2, and the positions of the dark fringes are expressed by x2 nl: R Hence the distance of the nth dark fringe from the center is given by xn p nRl: 1:5 1:4

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Combining this fact with the banded nature of the available energies and the delocalization of the orbitals results in material that easily transports excess charge from location to location within the bulk substance a conductor in other words The electrons in nonmetals are held more tightly to the atomic nuclei Those electrons used for bonding are not di use and interact strongly only with a few neighbors Instead the molecular orbitals and the electrons in them are constrained to exist only in small areas between individual atoms This results in consequences for the band structure of nonmetals Bulk nonmetals also contain many atoms and therefore many molecular orbitals that form continuous bands Unlike metals, however, the nonmetals are characterized by multiple nonoverlapping band sets.

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Editing within a floating box is the same as editing directly on the page. To edit text within a floating box, type, select, copy, paste, or delete it just as you do with any other text. To move text, drag over it to select it, and then point to it and drag. Selected text counts as an object so when you point to it, your cursor shows the object selection cursor with the rectangle at its tail. To move a graphic, place your cursor over the graphic so the arrow becomes the object selection cursor, and then drag the graphic into its new position. Remember that items in a floating box are inline with the I-beam. The only exception is when a grid is in the box and the items are on the grid. But then, the grid is inline with the I-beam.

of the 20th century that could be interpreted by classical mechanics only if it was assumed that light was composed of a stream of particles. Speci cally, certain metals emit electrons when they are exposed to a source of light; this is called the photoelectric e ect. One nds that [59, 60]: 1. The number of electrons released from the surface increases as the intensity of the light is increased, but the energies of the emitted electrons are independent of the intensity of the light. This implies that light cannot be a wave motion in the classical sense because when light waves strike a substance only the number of emitted electrons increases as the intensity is increased; the energy of the most energetic electrons remains constant. This can be explained only if it is assumed that the energy in a beam of light is not transmitted in the manner characteristic of a wave, but rather that the energy comes in discrete bundles or packets (a packet of light energy is called a photon) and that the size of the packet is determined by the frequency of the light. 2. No electrons are emitted from the surface of the metal unless the frequency of the light is greater than a certain minimum value. When electrons are ejected from the surface, they exhibit a range of velocities, from zero up to some maximum value. The energy of the electrons with the maximum velocity is found to increase linearly with an increase in the frequency of the incident light, namely,

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