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solid-state physics


n.

The branch of physics that deals with the physical properties of solid materials, especially the electromagnetic, thermodynamic, and structural properties of crystalline solids. Also called condensed matter physics.


 
 
Sci-Tech Encyclopedia: Solid-state physics

The study of the physical properties of solids, such as electrical, dielectric, elastic, and thermal properties, and their understanding in terms of fundamental physical laws. Most problems in solid-state physics would be called solid-state chemistry if studied by scientists with chemical training, and vice versa. Solid-state physics emphasizes the properties common to large classes of compounds rather than the dependence of properties upon compositions, the latter receiving greater emphasis in solid-state chemistry. In addition, solid-state chemistry tends to be more descriptive, while solid-state physics focuses upon quantitative relationships between properties and the underlying electronic structure. See also Solid-state chemistry.

Many of the scientists who study the physics of liquids identify with solid-state physics, and the term “condensed-matter physics” has been used by some researchers to replace “solid-state physics” as a division of physics. It includes noncrystalline solids such as glass as well as crystalline solids. See also Amorphous solid; Glass.

In solid-state physics it is generally assumed that the electronic states can be described as wavelike. The individual electronic states, called Bloch states, have energies which depend upon the wave number (a vector equal to the momentum divided by , which is Planck's constant divided by 2π), and the wave number is restricted to a domain called the Brillouin zone. This energy given as a function of the wave number is called the band structure. There are several curves, called bands, for each line in the Brillouin zone. See also Brillouin zone.

The total energy of a solid includes a sum of the energies of the occupied electronic states. Since the energy bands depend upon the positions of the atoms, so does the total energy, and the stable crystal structure is that which minimizes this energy. The theory has not proved adequate to really predict the crystal structure of various solids, but it is possible to predict the changes in energy under various distortions of the lattice. There are in fact three times as many independent distortions, called normal modes, as there are atoms in the solid. Each has a wave number, and the frequencies of the normal vibrational modes, as a function of wave number in the Brillouin zone, form vibrational bands in direct analogy with the electronic energy bands. These can be directly calculated from quantum theory or measured by using neutron or x-ray diffraction. See also Crystal; Lattice vibrations; Neutron diffraction; X-ray diffraction.


 
Britannica Concise Encyclopedia: solid-state physics

Branch of physics concerned with the physical properties of solid materials. It deals with the properties of crystal-lattice arrangements of atoms, and dislocations and defects in the arrangements. These structures are especially important in the study of the conductance of heat and electricity through solid materials.

For more information on solid-state physics, visit Britannica.com.

 
Columbia Encyclopedia: solid-state physics,
study of the properties of bulk matter rather than those of the individual particles that compose it. Solid-state physics is concerned with the properties exhibited by atoms and molecules because of their association and regular, periodic arrangement in crystals. The descriptive side of the study of solids is crystallography. From a practical point of view, searches are made for new characteristics and behavior of various materials. The most spectacular discovery resulting from these searches has been the transistor. From a theoretical point of view, attempts are made to predict and explain the nature of aggregates of atoms in terms of the basic laws of the quantum theory and the well-understood properties of individual atoms. An important concern of solid-state physics is the mechanical and thermal behavior of solids; specific areas of study include the allowed vibration modes of crystals (see phonon), the transmission of vibrational energy (thermal conductivity), the amount of energy that must be absorbed to produce a given change in temperature (specific heat), and phase transitions such as the melting points of crystals. Although the crystalline, mechanical, thermal, and optical properties of solids are of great interest, it is the electrical properties that most clearly demarcate the various types of materials and which exhibit the greatest diversity of behavior. The single most important electrical characteristic of a solid is its electrical conductivity (the ease with which electric currents flow through it). See conduction. Metals are highly conductive solids that offer little resistance to electric currents. Most solid nonmetals, on the other hand, are insulators (solids whose conductivity is nearly zero); they offer virtually infinite resistance to electric currents. A third class of solids possesses electrical conductivity that is neither very high nor very low; these solids are called semiconductors. A principal triumph of quantum mechanics in solid-state physics is the explanation of these extreme variations of electrical conductivity in terms of the atomic structure of the three types of solids.


 
Wikipedia: solid-state physics

Solid-state physics, the largest branch of condensed matter physics, is the study of rigid matter, or solids. The bulk of solid-state physics theory and research is focused on crystals, largely because the periodicity of atoms in a crystal — its defining characteristic —facilitates mathematical modeling, and also because crystalline materials often have electrical, magnetic, optical, or mechanical properties that can be exploited for engineering purposes.

The framework of most solid-state physics theory is the Schrödinger (wave) formulation of non-relativistic quantum mechanics. Bloch's Theorem, which characterizes the wavefunctions of electrons in a periodic potential, is an important starting point for much analysis. Since Bloch's Theorem applies only to periodic potentials, and since unceasing random movements of atoms in a crystal disrupt periodicity, this use of Bloch's Theorem is only an approximation, but it has proven to be a tremendously valuable approximation, without which most solid-state physics analysis would be intractable. Deviations from periodicity are treated by quantum mechanical perturbation theory.

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Dictionary. The American Heritage® Dictionary of the English Language, Fourth Edition Copyright © 2007, 2000 by Houghton Mifflin Company. Updated in 2007. Published by Houghton Mifflin Company. All rights reserved.  Read more
Sci-Tech Encyclopedia. McGraw-Hill Encyclopedia of Science and Technology. Copyright © 2005 by The McGraw-Hill Companies, Inc. All rights reserved.  Read more
Britannica Concise Encyclopedia. Britannica Concise Encyclopedia. © 2006 Encyclopædia Britannica, Inc. All rights reserved.  Read more
Columbia Encyclopedia. The Columbia Electronic Encyclopedia, Sixth Edition Copyright © 2003, Columbia University Press. Licensed from Columbia University Press. All rights reserved. www.cc.columbia.edu/cu/cup/  Read more
Wikipedia. This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Solid-state physics" Read more

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