Academic literature on the topic 'Electron theory of metals'

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Journal articles on the topic "Electron theory of metals"

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Roshchin, V. E., P. A. Gamov, A. V. Roshchin, and S. P. Salikhov. "ELECTRON THEORY OF METALS REDUCTION: THEORY AND METHODS OF METALS EXTRACTION FROM VARIOUS TYPES OF ORE." Izvestiya. Ferrous Metallurgy 62, no. 5 (June 19, 2019): 407–17. http://dx.doi.org/10.17073/0368-0797-2019-5-407-417.

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The present work analyzes the existing mechanism of solid-phase metals reduction from oxides. It was shown that the existed mechanisms of reduction do not explain the diversity of the practical results leading to a generally accepted opinion that there is no single uniform reduction mechanism. This study presents the results of the solid-phase reduction of metals from lump magnetite, siderite, titanomagnetite and chromite types of ore by carbon from various deposits. The obtained results were compared with the results of reduction of chromium, silicon and aluminum by carbon from pure oxides. Change in the electrical characteristics and analysis of the processes of electron- and mass transfer under reducing conditions were performed to clarify the general theoretical concepts of reduction mechanism. It has been concluded that there is general process of transformation of the crystal lattice of oxide into the crystal lattice of metal for reduction of different metals. The positions of electron theory for solid-phase reduction of metals from crystal lattice of oxides were developed using the basic concepts of chemistry, solid state physics about imperfect crystals, quantum mechanics and character of electron distribution and transfer in metals and ionic semiconductors. The theory embraces all the known results of reduction with formation of metal on the surface of high-grade lump ore, nucleation of metal inside of the complex and low-grade types of ore and formation and sublimation of suboxides. Major ideas of the developing theory of electron reduction have been formulated on the basis of metals reduction as a result of the exchange of electrons between the reducing agent and metal cations in oxides by means of the charged anion vacancies formed on the surface and their scattering in the volume. The transformation of the cations’ ionic bond in oxides into metallic bond of the metal phase on the surface (or inside of the oxide lattice) occurs without the displacement of the cations over significant distances and thermodynamic difficulties for the formation of metallic nucleus when the charged anion vacancies merge (skipping the stage of formation of the atoms of metal). There might be no direct contact between the metal and the reducing agent in case of formation of the metal phase inside of the oxide volume. As a result, harmful impurities from the reducing agent, e.g. carbon and sulphur, do not penetrate into iron during reduction of complex and low-grade types of ore. Therefore, for the reduction of iron from such an ore, it is possible to utilize a low-quality reducing agent, e.g. steam coal. The selective solid-phase reduction of iron from lump complex ore makes it possible to obtain a metal-oxide composite material containing pure DRI and valuable oxides which are difficult for reduction, i.e. oxides of magnesium, titanium and vanadium.
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Sichkar, S. M. "Theory of Phonon–Electron Interaction in Metals." Uspehi Fiziki Metallov 18, no. 1 (March 1, 2017): 27–57. http://dx.doi.org/10.15407/ufm.18.01.027.

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Stachowiak, H., and E. Boroński. "Electron-Positron Interaction in Metals. Theory and Experiment." Acta Physica Polonica A 107, no. 4 (April 2005): 541–53. http://dx.doi.org/10.12693/aphyspola.107.541.

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Giamarchi, T., and H. J. Schulz. "Theory of spin-anisotropic electron-electron interactions in quasi-one-dimensional metals." Journal de Physique 49, no. 5 (1988): 819–35. http://dx.doi.org/10.1051/jphys:01988004905081900.

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CHEN, HUA, and DANIEL C. MATTIS. "TOWARD A RIGOROUS THEORY OF THE SCREENED ELECTRON-ELECTRON INTERACTIONS IN METALS." International Journal of Modern Physics B 05, no. 18 (November 10, 1991): 2951–72. http://dx.doi.org/10.1142/s0217979291001152.

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A microscopic formula for the effective two-body interaction between electrons or holes in an ideal metal is derived within the linear response theory. Both the zero-range Hubbard interaction U0 and the long-range Coulomb interaction, denoted by ΔV(q), are included. The effective interaction, which is necessarily spin-dependent, is expressed in terms of the exact charge and spin density-density correlation functions and of their higher order mixtures. These correlation functions are analyzed diagrammatically. Attention is paid to clarifying the different roles played by U0 and ΔV(q). We also display the corresponding new formula for the free energy. Comparison is made with previous theories.
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Kostrobiy, P. P., Bogdan M. Markovych, and Yuri Suchorski. "Revisiting Local Electric Fields on Close-Packed Metal Surfaces: Theory Versus Experiments." Solid State Phenomena 128 (October 2007): 219–24. http://dx.doi.org/10.4028/www.scientific.net/ssp.128.219.

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An external electrostatic field of the order of a few tens of a volt per nanometer causes significant changes in the electron density distribution near a metal surface. Because of differing electronic distributions and varying responses of electrons to the applied field for various metals, the resulting local field distribution in the close vicinity of the surface should depend on the electronic properties of the particular metal, even for flat surfaces. Field-free and field-modified electron density distributions for different metal surfaces were calculated using the functional integration method. This approach enables the exchange-correlation effects to be correctly considered and makes it possible to account for the proper field-effect for broad field ranges without using the perturbation theory. The results of calculations are compared with the field-ion microscopic observations.
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Roshchin, V. E., and A. V. Roshchin. "General electron theory of reduction and oxidation of metals." Izvestiya. Ferrous Metallurgy 63, no. 3-4 (May 26, 2020): 271–85. http://dx.doi.org/10.17073/0368-0797-2020-3-4-271-285.

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OSMAN, S. M., and S. M. MUJIBUR RAHMAN. "STRUCTURAL AND THERMODYNAMIC PROPERTIES OF 3d TRANSITION METALS: PSEUDOPOTENTIAL THEORY REVISITED." Modern Physics Letters B 09, no. 09 (April 20, 1995): 553–64. http://dx.doi.org/10.1142/s0217984995000504.

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Structural and thermodynamic properties of 3d transition metals are calculated in terms of the pseudopotential theory. The s − p and d electrons are treated in a pseudoadiabatic approximation in such a way that the s − p and d electrons are treated separately under the same footing. The s − p electrons are treated in terms of the conventional second order pseudopotential theory, while the tightly bound d electrons are treated in terms of the Wills–Harrison prescription that makes use of the Friedel rectangular electron density of states (DOS) model. The predictions of the structural phase stability and other relevant thermodynamic properties are found to be consistent with experiments for almost all of the metals.
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Olszewski, Stanislaw, and Marek Gluzinski. "Calculating the Magnetoresistance Effect in Metals." Zeitschrift für Naturforschung A 66, no. 5 (May 1, 2011): 311–20. http://dx.doi.org/10.1515/zna-2011-0507.

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Transversal magnetoresistance is calculated for numerous metal cases on the basis of simple electron theory. Any metal can be represented by a single band of states having a closed Fermi surface which is assumed to be similar in shape to a sphere. In an external electromagnetic field the electron transport seems to be regulated by two kinds of relaxation times. The first one is due to the electric field, and its size is not appreciably influenced by that field. On the other hand, electron motion in the magnetic field is associated with a relaxation time that is strongly dependent on the strength of that field. Both time parameters combine to an effective relaxation time according to Matthiessen’s rule. A good agreement between experiment and theory is obtained for Li, Cu, Ag, Au and Pd, Pt metals.
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Li, D. H., R. A. Moore, and S. Wang. "Variational thermodynamic calculations for some liquid sd metals." Canadian Journal of Physics 64, no. 1 (January 1, 1986): 75–83. http://dx.doi.org/10.1139/p86-011.

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A tractable and reliable expression for the one valence-electron eigenenergies, required in calculating the total energy of a disordered sd-type metal, is formulated in the context of the model-potential theory. With the aid of this expression, the variational calculation of the Helmholtz free energy using the hard-sphere model as a reference system, as employed in ab initio calculations of the thermodynamic properties for the nearly-free-electron-like (NFE) liquid metals, can now be extended with reasonable accuracy to those liquid sd metals in which the d-like valence-electron states below the Fermi level are not very localized. Also, the ab initio-type pseudopotential calculation of the interionic pair potentials, as carried out for the NFE-like metals in the literature, is made practical for these sd metals in their disordered states.
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Dissertations / Theses on the topic "Electron theory of metals"

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Yang, Xiaodong. "Effects of Electron-Phonon Interaction in Metals." Diss., Temple University Libraries, 2010. http://cdm16002.contentdm.oclc.org/cdm/ref/collection/p245801coll10/id/83903.

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Physics
Ph.D.
Phonons and electrons are two types of excitations which are responsible for many properties of condensed matter materials. The interaction between them plays an important role in condensed matter physics. In this thesis we present some theoretical investigations of the effects due to the interactions between phonons and electrons interactions. We show evidence that a structural martensitic transition is related to significant changes in the electronic structure, as revealed in thermodynamic measurements made in high magnetic fields. The effect of the magnetic field is considered unusual, as many influential investigations of martensitic transitions have emphasized that the structural transitions are primarily lattice dynamical and are driven by the entropy due to the phonons. We provide a theoretical frame-work which can be used to describe the effect of a magnetic field on the lattice dynamics in which the field dependence originates from the dielectric constant. The temperature-dependence of the phonon spectrum of alpha-uranium has recently been measured by Manley et al. using inelastic neutron scattering and x-ray scattering techniques. Although there is scant evidence of anharmonic interactions, the phonons were reported to show some softening of the optic modes at the zone boundary. The same group of authors later reported that an extra vibrational mode was observed to form at a temperature above 450 K. The existence of the proposed new mode is inconsistent with the usual theory of harmonic phonons, as applied to a structure composed of a monoclinic Bravais lattice with a two-atom basis. We investigate the effect that the f electron-phonon interaction has on the phonon spectrum and its role on the possible formation of a breathing mode of mixed electronic and phonon character. We examine the model by using Green’s function techniques to obtain the phonon spectral density. Some materials undergo phase transitions from a high temperature state with periodic translational invariance to a state in which the electronic charge density is modulated periodically. The wave vector of the modulation may be either commensurate or incommensurate with the reciprocal lattice vectors of the high temperature structure. In the case of an incommensurate charge density wave, the system supports phason excitation. For an incommensurate state, the new ground state has a lower symmetry than the high temperature state since the charge density does not have long-ranged periodic translational order. If the metal is ideal (with no impurities), a charge density wave should be able to slide throughout the crystal without resistance, resulting in current flow similar to that of a superconductor. The phason is an excitation of the charge density wave which is related to the collective motion of electrons. We estimate the phason density of states, and the phason contribution to the specific heat. Angle-resolved photoemission experiments have been performed on USb2, and very narrow quasiparticle peaks have been observed in a band which local spin-density approximation (LSDA) predicts to osculate the Fermi energy. The observed band is found to be depressed by 17 meV below the Fermi energy. The experimentally observed quasiparticle dispersion relation for this band exhibits a kink at an energy of about 23 meV below the Fermi energy. The kink is not found in LSDA calculations and, therefore, is attributable to a change in the quasiparticle mass renormalization by a factor of approximately 2. The existence of a kink in the quasiparticle dispersion relation of a band which does not cross the Fermi energy is unprecedented. The kink in the quasiparticle dispersion relation is attributed to the effect of the interband self-energy involving transitions from the osculating band into a band that does cross the Fermi energy.
Temple University--Theses
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Hara, Takayuki. "A calculation of fermi energy in selected materials using doppler broadened positron annihilation spectroscopy." Thesis, Georgia Institute of Technology, 1986. http://hdl.handle.net/1853/20238.

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Breitkreiz, Maxim. "Transport Theory for Metals with Excitonic Instabilities." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2015. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-190697.

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Metals with excitonic instabilities are multiband systems with significant electron-electron interaction. The electronic transport in such systems is affected by collective fluctuations of the electrons, leading to anomalous features in the measured transport coefficients. Many of these anomalies have not been well understood because the transport mechanisms in these systems tend to be rather complex. The complexity arises, on the one hand, from the multiband nature and, on the other, from the anisotropic scattering of electrons accompanied by emitting or absorbing collective fluctuations. Previous works considering scattering due to collective fluctuations have mainly focused on single-band systems, for example in the context of the normal-state transport in cuprates. The recent discovery of high-temperature superconductivity in iron pnictides has renewed the interest in multiband systems. Exploring the transport mechanisms in multiband systems, I find some interesting new aspects, which do not occur in single-band systems. In particular, anisotropic scattering in a model with electronlike and holelike Fermi surfaces can lead to a negative conductivity contribution of the minority carriers, i.e., in an electric field, the minority carriers drift in the direction opposite of what one would expect based on their charge. I show that this effect can explain a reduced magnetoresistance in connection with an enhanced Hall coefficient, which has been measured in pnictides. Of particular interest are multiband models with hot spots on the Fermi surface, in part because of their relevance for the iron pnictides. Hot spots are states with enhanced scattering and therefore reduced excitation lifetimes. In single-band systems, the hot spots are found to have a much lower contribution to the total conductivity than other parts of the Fermi surface, which leads to the so-called hot-spot structure. I show that in the multiband case, the conductivity contributions are much more isotropic around the Fermi surface so that hot spots contribute to transport with a similar strength as other parts of the Fermi surface. I discuss this effect on the basis of an approximate analytical solution of the transport problem and numerically calculate the temperature dependence of several transport coefficients. It turns out that in the nematic phase of iron pnictides, the unexpectedly strong conductivity contribution of hot spots can explain the puzzling behavior of the resistive anisotropy. I show that the experimental observations can be explained within a scenario in which the anisotropy is mainly due to the broken symmetry of the spin-fluctuation spectrum in the nematic phase. In the spin-density-wave state, strongly anisotropic scattering can arise due to the propagating magnons. Using a two-band model relevant for iron pnictides, I find that this scattering can lead to an unusual interruption of the orbital motion of electrons in the magnetic field. As a consequence, the low-field magnetoresistance is linear with an alternating sign of the slope as a function of the direction of the current. In strong magnetic fields, the interrupted orbital motion makes the system unstable, which is characterized by a drop of the resistivity to zero.
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Awad, Mohamed Khaled Hassan. "Small molecule chemisorption on metals and carbon-hydrogen and hydroxy 1 bond activation by electron hold centers: Molecular orbital theory." Case Western Reserve University School of Graduate Studies / OhioLINK, 1990. http://rave.ohiolink.edu/etdc/view?acc_num=case1054910441.

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Östlin, Andreas. "Electronic structure studies and method development for complex materials." Licentiate thesis, KTH, Tillämpad materialfysik, 2013. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-118467.

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Over the years electronic structure theory has proven to be a powerful method with which one can probe the behaviour of materials, making it possible to predict properties that are difficult to measure experimentally. The numerical tools needed for these methods are always in need of development, since the desire to calculate more complex materials pushes this field forward. This thesis contains work on both this implementational and developmental aspects. In the first part we investigate the structural properties of the 6d transition metals using the exact muffin-tin orbitals method. It is found that these elements behave similarly to their lighter counterparts, except for a few deviations. In these cases we argue that it is relativistic effects that cause this anomalous behaviour. In the second part we assess the Padé approximant, which is used in several methods where one wants to include many-body effects into the electronic structure. We point out difficulties that can occur when using this approximant, and propose and evaluate methods for their solution.

QC 20130219

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Thulasi, Sunita. "Theory of the two-dimensional airy electron gas Hartee-Fock and density-functional studies /." Diss., Columbia, Mo. : University of Missouri-Columbia, 2006. http://hdl.handle.net/10355/4111.

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Thesis (Ph. D.)--University of Missouri-Columbia, 2006.
The entire dissertation/thesis text is included in the research.pdf file; the official abstract appears in the short.pdf file (which also appears in the research.pdf); a non-technical general description, or public abstract, appears in the public.pdf file. Title from title screen of research.pdf file viewed on (May 17, 2007) Vita. n following parenthesis in formula (LaTiO₃) should be subscript. Includes bibliographical references.
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Horne, Masae. "A theory of resonant x-ray scattering and electronic structure for light rare earth metals." Thesis, Keele University, 2004. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.401120.

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Mizielinski, Matthew. "A theory of electron-hole pair excitation in the adsorption of simple atoms on metal surfaces." Thesis, University of Bath, 2007. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.436869.

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Recent experiments have provided direct evidence for the excitation of electronhole pairs during the adsorption of atoms on metal surfaces. The excitation of electron-hole pairs is an inherently non-adiabatic process which is often ignored in standard theoretical treatments of surface phenomena, using tools such as density functional theory (DFT), as the Born-Oppenheimer approximation cannot be used. To obtain a theoretical model for the electronic excitation process it is therefore necessary to go beyond conventional methods. Previous theoretical descriptions have used a nearly-adiabatic approximation to describe electronic excitations. However, these methods have been found to fail in situations where an adsorbing atom undergoes a transition between a spin-polarised and unpolarised state. In this thesis we develop a fully non-adiabatic theory using a simple description of the adsorbate-metal interaction; the time-dependent, mean-field Newns- Anderson model. This model describes a simple electronic system in which a band of metal states interacts with a single atomic orbital, which can undergo a ‘spin-transition’. We derive expressions describing the time-dependent transfer of charge and energy between the adsorbate and surface, as well as the spectrum of electronic excitations generated. Each of these results describe the evolution of the electronic system in terms of a simple set of parameters. These results are demonstrated using a set of example parameter variations to explore the impact of variables such as adsorbate speed and the temperature of the system. A set of parameter variations describing the interaction of hydrogen isotopes with copper and silver surfaces are obtained from DFT calculations. These parameters are used to drive our model through a single approach of the adsorbate to the surface. We find the results of these calculations to be in good agreement with reported experimental results. Our conclusions, and some possible directions for further work, are summarised in the final chapter.
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Jenkins, Anne Ceri. "Applications of spin-polarised relativistic scattering theory to the calculation of the electronic properties of heavy metals and alloys." Thesis, Keele University, 1997. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.321408.

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Li, Peng. "Novel quantum magnetic states in low dimensions." Click to view the E-thesis via HKUTO, 2006. http://sunzi.lib.hku.hk/hkuto/record/B36883062.

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Books on the topic "Electron theory of metals"

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Lifshits, I. M., M. Ya Azbel’, and M. I. Kaganov. Electron Theory of Metals. Boston, MA: Springer US, 1995. http://dx.doi.org/10.1007/978-1-4615-8558-9.

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Yamada, K. Electron correlation in metals. Cambridge: Cambridge Univ Press, 2010.

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An introduction to the electron theory of metals. London: Institute of Metals, 1988.

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Paul, Ziesche, ed. Electronic properties of metals. Amsterdam: Elsevier, 1990.

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Kübler, Jürgen K. Theory of itinerant electron magnetism. Oxford: Oxford University Press, 2009.

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Kübler, Jürgen K. Theory of itinerant electron magnetism. Oxford: Oxford University Press, 2009.

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1927-, March Norman H., ed. Electrons in metals and alloys. London: Academic Press, 1989.

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Abrikosov, A. A. Fundamentals of the theory of metals. Amsterdam: North-Holland, 1988.

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Theory of itinerant electron magnetism. Oxford: Clarendon Press, 2000.

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Howard, Cottrell Alan. Introduction to the modern theory of metals. London: Institute of Metals, 1988.

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Book chapters on the topic "Electron theory of metals"

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Quinn, John J., and Kyung-Soo Yi. "Free Electron Theory of Metals." In Solid State Physics, 79–107. Berlin, Heidelberg: Springer Berlin Heidelberg, 2009. http://dx.doi.org/10.1007/978-3-540-92231-5_3.

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Quinn, John J., and Kyung-Soo Yi. "Free Electron Theory of Metals." In UNITEXT for Physics, 83–112. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-73999-1_3.

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Amusia, Miron Ya, Konstantin G. Popov, Vasily R. Shaginyan, and Vladimir A. Stephanovich. "Metals with a Strongly Correlated Electron Liquid." In Theory of Heavy-Fermion Compounds, 139–54. Cham: Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-10825-4_8.

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Ballentine, L. E. "Theory of Electron States in Liquid Metals." In Advances in Chemical Physics, 263–327. Hoboken, NJ, USA: John Wiley & Sons, Inc., 2007. http://dx.doi.org/10.1002/9780470143834.ch5.

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Kosevich, A. M. "Topology in the Electron Theory of Metals." In Springer Series in Solid-State Sciences, 3–29. Berlin, Heidelberg: Springer Berlin Heidelberg, 2006. http://dx.doi.org/10.1007/3-540-31264-1_2.

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Forwood, C. T., and L. M. Clarebrough. "Dislocation Theory of Interfaces." In Electron Microscopy of Interfaces in Metals and Alloys, 1–23. Boca Raton: Routledge, 2021. http://dx.doi.org/10.1201/9780203758656-1.

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Rosier, M., and W. Brauer. "Theory of electron emission from nearly-free-electron metals by proton and electron bombardment." In Springer Tracts in Modern Physics, 1–65. Berlin, Heidelberg: Springer Berlin Heidelberg, 1991. http://dx.doi.org/10.1007/bfb0041377.

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Bishop, Marilyn F., and A. W. Overhauser. "Theory of Electron-Phason Scattering and the Low-Temperature Resistivity of Potassium." In Anomalous Effects in Simple Metals, 302–26. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA, 2010. http://dx.doi.org/10.1002/9783527631469.ch40.

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Overhauser, Albert W. "Insights in Many-Electron Theory From the Charge Density Wave Structure of Potassium." In Anomalous Effects in Simple Metals, 383–93. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA, 2010. http://dx.doi.org/10.1002/9783527631469.ch47.

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Guet, C., and L. Plagne. "Electron Dynamics in Metal Clusters." In Theory of Atomic and Molecular Clusters, 209–27. Berlin, Heidelberg: Springer Berlin Heidelberg, 1999. http://dx.doi.org/10.1007/978-3-642-58389-6_9.

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Conference papers on the topic "Electron theory of metals"

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Feng, Bo, Zhixin Li, and Xing Zhang. "Thermal and Electrical Conductivities of Polycrystalline Metallic Nanofilms Based on the Kinetic Theory." In ASME 2008 First International Conference on Micro/Nanoscale Heat Transfer. ASMEDC, 2008. http://dx.doi.org/10.1115/mnht2008-52009.

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A model is developed for in-plane thermal conductivity of nanostructured metallic films based on the kinetic theory, which attributes the reduced thermal conductivity to the reduced mean free path of electrons. The partially inelastic electron-surface scattering and grain-boundary impedance by quantum mechanical treatment are elaborately included. Meanwhile, the mean free path of electrons is also used to study in-plane electrical conductivity of nanofilms. Both electrical conductivity and thermal conductivity, varying with film thickness and temperature, are observed to be lower than corresponding bulk values, agreeing well with the experimental data. The grain-boundary scattering is theoretically found to dominate over surface scattering to enhance the size effect on electrical and thermal conductivities. In addition, the size effect in low temperature appears more dramatic due to larger electron Knudsen number. We further examine the Lorenz number of nanofilms and find the Wiedemann-Franz law is seriously violated. The Coulomb blockade and the neutral excitation of electron-hole pair are used to offer a more detailed picture. Excessive thermal conductivity is also evaluated resorting to concepts in granular metals to show the validity of this account.
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Voloshina, Elena, Beate Paulus, Theodore E. Simos, and George Maroulis. "Electron-Correlation Effects in Metals from First Principles: a Multi-Reference Incremental Scheme." In COMPUTATIONAL METHODS IN SCIENCE AND ENGINEERING: Theory and Computation: Old Problems and New Challenges. Lectures Presented at the International Conference on Computational Methods in Science and Engineering 2007 (ICCMSE 2007): VOLUME 1. AIP, 2007. http://dx.doi.org/10.1063/1.2836060.

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Efros, A. L. "Density of states and the metal - non-metal transition in the 2-D electron gas." In Frontiers in condensed matter theory. AIP, 1990. http://dx.doi.org/10.1063/1.39725.

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Rovira, C., J. Veciana, J. Tarres, N. SantaIo, E. Molins, M. Mas, D. O. Cowan, S. Yang, and E. Canadell. "Towards tridimensional organic metals. synthesis and study of mlrlti sulfur /spl pi/-electron donors and their charge transfer complexes and salts." In International Conference on Science and Technology of Synthetic Metals. IEEE, 1994. http://dx.doi.org/10.1109/stsm.1994.835659.

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Shiraishi, K., P. Ahmet, K. Ohmori, H. Watanabe, T. Chikyow, M. L. Green, Y. Nara, et al. "Universal theory of workfunctions at metal/Hf-based high-k dielectrics interfaces - guiding principles for gate metal selection." In International Electron Devices Meeting 2005. IEEE, 2005. http://dx.doi.org/10.1109/iedm.2005.1609260.

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Zhang, Peng, and Y. Y. Lau. "An exact theory of ultrafast electron emission on a biased metal surface." In 2016 IEEE International Conference on Plasma Science (ICOPS). IEEE, 2016. http://dx.doi.org/10.1109/plasma.2016.7534258.

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Dragobetskii, Volodymyr, Viktoriia Nevliudova, Dmytro Moloshtan, Denis Mospan, Vladyslav Mospan, and Viktor Kotsyuba. "Possibilities of the Electric Drive in the Implementation of the Intensifying Factors in the Plastic Deformation of Metals." In 2020 IEEE Problems of Automated Electrodrive. Theory and Practice (PAEP). IEEE, 2020. http://dx.doi.org/10.1109/paep49887.2020.9240873.

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Stoyanova, A., C. de Graaf, R. Broer, Theodore E. Simos, and George Maroulis. "Many-Electron Bands in Transition Metal Compounds." In COMPUTATIONAL METHODS IN SCIENCE AND ENGINEERING: Theory and Computation: Old Problems and New Challenges. Lectures Presented at the International Conference on Computational Methods in Science and Engineering 2007 (ICCMSE 2007): VOLUME 1. AIP, 2007. http://dx.doi.org/10.1063/1.2836029.

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Eldabbagh, Fadi, Appadurai Ramesh, Karl K. Rink, and Janusz A. Kozinski. "Biomass Combustion With Emphasis on Interactions Between Metals and Inorganic Particulate." In 18th International Conference on Fluidized Bed Combustion. ASMEDC, 2005. http://dx.doi.org/10.1115/fbc2005-78090.

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Abstract:
Biomass is clean, stored solar energy. Not only is it a plentiful fuel, but its use also reestablishes the natural carbon cycle helping mitigate greenhouse gas emissions. This renewable energy source is nearly CO2 neutral. Overall, it is possible to achieve a 93% reduction in net CO2 emissions per unit heating value by switching from coal to biomass and a 84% reduction by switching from natural gas-fired cogeneration to biomass. Due to inherent advantages of the biomass in substituting fossil fuels, and increasing legislative pressures against CO2 emissions (Kyoto Protocol), biomass-based power is genuinely considered. It seems practically impossible to meet Kyoto requirements by replacing fossil fuels combustion with nuclear energy, hydropower or fuel cells. Simply, there is not enough time. In this context, there exists a niche for the biomass-based power generation. This paper compares interactions between metals and solid particles evolving from biomass during the classical Fluidized Bed Combustion (FBC) and a new Low-High-Low temperature (LHL) combustion. Experiments, conducted at a pilot-scale, reveal a clear pattern of surface predominance of light metals (Ca, K) and core predominance of heavy metals (Cd, Cr) within the LHL-generated particles. No such behavior was induced by the classical FBC approach. Metals migration is linked to the evolution of inorganic particles. A composite picture of the metals rearrangements in the particles was obtained by the combination of independent analytical techniques including electron probe microanalysis, field emission scanning electron microscopy, inductively-coupled plasma spectrometry and X-ray diffractometry. It is suggested that the combination of (i) the high-temperature region in the LHL and (ii) changes in the surface free energy of the particles is the driving force for the metal-particle behavior. Important practical implications of the observed phenomena are proposed including removal of hazardous submicron particulate and reduction in fouling/slagging during biomass combustion. These findings may contribute to redesigning currently operating FBC units in order to generate non-hazardous, non-leachable, re-usable particles where heavy metals are immobilized while environmental and technological problems reduced.
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Bogomolova, A. A., A. V. Solodkiy, and A. A. Zaharov. "Features of phenomenological theory giant magnetoresistance in granular media ferromagnet — Nonmagnetic metal." In 2010 International Conference on Actual Problems of Electron Devices Engineering (APEDE 2010). IEEE, 2010. http://dx.doi.org/10.1109/apede.2010.5624074.

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Reports on the topic "Electron theory of metals"

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Akella, J., S. T. Weir, G. S. Smith, and C. Ruddle. Phase changes in f-electron metals: discrepancies between experiment and theory. Office of Scientific and Technical Information (OSTI), October 1996. http://dx.doi.org/10.2172/481815.

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Colson, W. B. Free Electron Laser Theory. Fort Belvoir, VA: Defense Technical Information Center, July 1986. http://dx.doi.org/10.21236/ada172996.

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Griffin, Donald C. Theory of Electron-Ion Collisions. Office of Scientific and Technical Information (OSTI), October 2009. http://dx.doi.org/10.2172/965260.

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Bohdan Andraka. Synthesis and Study of Unconventional f-Electron Metals. Office of Scientific and Technical Information (OSTI), July 2002. http://dx.doi.org/10.2172/797610.

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Lindsey, T. F. Theory of ordering transformations in metals and minerals. Office of Scientific and Technical Information (OSTI), July 1991. http://dx.doi.org/10.2172/5173755.

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Reu, Phillip L. Development of the doppler electron velocimeter: theory. Office of Scientific and Technical Information (OSTI), March 2007. http://dx.doi.org/10.2172/902221.

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Freund, Henry P. Theory and Simulation of Free-Electron Lasers. Office of Scientific and Technical Information (OSTI), September 2013. http://dx.doi.org/10.2172/1093356.

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Onley, D. S., and L. E. Wright. Theory of photon and electron induced reactions. Office of Scientific and Technical Information (OSTI), January 1992. http://dx.doi.org/10.2172/5692108.

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Tang, C. M. Recent Advanced in Free Electron Laser Theory. Fort Belvoir, VA: Defense Technical Information Center, June 1991. http://dx.doi.org/10.21236/ada236826.

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Chandler, David. Theory of Electron Transfer in Complex Systems. Office of Scientific and Technical Information (OSTI), October 2004. http://dx.doi.org/10.2172/833679.

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