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Camp 1 - Quynh Nguyen Official Website
Camp 1 - Quynh Nguyen Official Website

Schrodinger Equation and Quantum Chemistry
Schrodinger Equation and Quantum Chemistry

... even better than those obtained from experiments. In this connection, the well-known sentence reported in the introduction of the textbook by Eyring, Walter, Kimball on quantum chemistry: “..In so far as quantum mechanics is correct, chemical questions are problems in applied mathematics…” springs t ...
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... Solution: The magnitude of the force is given by F=BqvSin(θ), so for cases (a) and (b) the force will be F=(1.5 T)( 6.25 µC)( 29,979 m/s)= 0.28N. The force in case (c) is zero because the magnetic field and the velocity are collinear. We find the direction of the force in cases (a) and (b) using the ...
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... for studies of the polar magneto-optical Kerr effect (Wijngaard et a1 1988) and the anomalous Hall effect (Parkin and Friend 1980b). Mnl13TaS2is also ferromagnetic, but its easy axis of magnetisation is perpendicular to the c axis. All 3d transition-metal intercalates of TaSz show metallic conductiv ...
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... refrigerators, etc., when they are not “magnetic”? The materials are all “soft” ferromagnets. The external field temporarily aligns the domains so there is a net dipole, which is then attracted to the bar magnet. - The effect vanishes with no applied B field - It does not matter which pole is used. ...
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... frequency, and energy of electromagnetic radiation. b. Demonstrating an ability to understand electronic transitions by working problems involving the Rydberg equation for hydrogen-like species. [OPTIONAL] c. Comparing and contrasting the particle and wave description of light. d. Relating important ...
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... the so-called phason degree of freedom. ) For H greater than the critical value, the ground state is commensurate and is locked: Varying the phase of the helix requires a definite nonzero energy. For our purposes the main conclusion is that associated with each commensurate state of wavelength pa, w ...
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Condensed matter physics



Condensed matter physics is a branch of physics that deals with the physical properties of condensed phases of matter. Condensed matter physicists seek to understand the behavior of these phases by using physical laws. In particular, these include the laws of quantum mechanics, electromagnetism and statistical mechanics.The most familiar condensed phases are solids and liquids, while more exotic condensed phases include the superconducting phase exhibited by certain materials at low temperature, the ferromagnetic and antiferromagnetic phases of spins on atomic lattices, and the Bose–Einstein condensate found in cold atomic systems. The study of condensed matter physics involves measuring various material properties via experimental probes along with using techniques of theoretical physics to develop mathematical models that help in understanding physical behavior.The diversity of systems and phenomena available for study makes condensed matter physics the most active field of contemporary physics: one third of all American physicists identify themselves as condensed matter physicists, and the Division of Condensed Matter Physics is the largest division at the American Physical Society. The field overlaps with chemistry, materials science, and nanotechnology, and relates closely to atomic physics and biophysics. Theoretical condensed matter physics shares important concepts and techniques with theoretical particle and nuclear physics.A variety of topics in physics such as crystallography, metallurgy, elasticity, magnetism, etc., were treated as distinct areas, until the 1940s when they were grouped together as solid state physics. Around the 1960s, the study of physical properties of liquids was added to this list, forming the basis for the new, related specialty of condensed matter physics. According to physicist Phil Anderson, the term was coined by him and Volker Heine when they changed the name of their group at the Cavendish Laboratories, Cambridge from ""Solid state theory"" to ""Theory of Condensed Matter"" in 1967, as they felt it did not exclude their interests in the study of liquids, nuclear matter and so on. Although Anderson and Heine helped popularize the name ""condensed matter"", it had been present in Europe for some years, most prominently in the form of a journal published in English, French, and German by Springer-Verlag titled Physics of Condensed Matter, which was launched in 1963. The funding environment and Cold War politics of the 1960s and 1970s were also factors that lead some physicists to prefer the name ""condensed matter physics"", which emphasized the commonality of scientific problems encountered by physicists working on solids, liquids, plasmas, and other complex matter, over ""solid state physics"", which was often associated with the industrial applications of metals and semiconductors. The Bell Telephone Laboratories was one of the first institutes to conduct a research program in condensed matter physics.References to ""condensed"" state can be traced to earlier sources. For example, in the introduction to his 1947 ""Kinetic theory of liquids"" book, Yakov Frenkel proposed that ""The kinetic theory of liquids must accordingly be developed as a generalization and extension of the kinetic theory of solid bodies"". As a matter of fact, it would be more correct to unify them under the title of ""condensed bodies"".
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