Academic literature on the topic 'Lorenz'

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Journal articles on the topic "Lorenz"

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Sihvola, Ari. "Lorenz-Lorentz or Lorentz-Lorenz?" IEEE Antennas and Propagation Magazine 33, no. 4 (August 1991): 56. http://dx.doi.org/10.1109/map.1991.5672658.

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Bladel, J. "Lorenz or Lorentz?" IEEE Antennas and Propagation Magazine 33, no. 2 (April 1991): 69. http://dx.doi.org/10.1109/map.1991.5672647.

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Bladel, J. Van. "Lorenz or Lorentz? [Addendum]." IEEE Antennas and Propagation Magazine 33, no. 4 (August 1991): 56. http://dx.doi.org/10.1109/map.1991.5672657.

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Ghiner, A. V., and G. I. Surdutovich. "Beyond the Lorentz-Lorenz Formula." Optics and Photonics News 5, no. 12 (December 1, 1994): 34. http://dx.doi.org/10.1364/opn.5.12.000034.

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Nevels, R., and Chang-Seok Shin. "Lorenz, Lorentz, and the gauge." IEEE Antennas and Propagation Magazine 43, no. 3 (June 2001): 70–71. http://dx.doi.org/10.1109/74.934904.

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Zlatanovska, Biljana, and Donc̆o Dimovski. "A modified Lorenz system: Definition and solution." Asian-European Journal of Mathematics 13, no. 08 (May 20, 2020): 2050164. http://dx.doi.org/10.1142/s1793557120501648.

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Based on the approximations of the Lorenz system of differential equations from the papers [B. Zlatanovska and D. Dimovski, Systems of difference equations approximating the Lorentz system of differential equations, Contributions Sec. Math. Tech. Sci. Manu. XXXIII 1–2 (2012) 75–96, B. Zlatanovska and D. Dimovski, Systems of difference equations as a model for the Lorentz system, in Proc. 5th Int. Scientific Conf. FMNS, Vol. I (Blagoevgrad, Bulgaria, 2013), pp. 102–107, B. Zlatanovska, Approximation for the solutions of Lorenz system with systems of differential equations, Bull. Math. 41(1) (2017) 51–61], we define a Modified Lorenz system, that is a local approximation of the Lorenz system. It is a system of three differential equations, the first two are the same as the first two of the Lorenz system, and the third one is a homogeneous linear differential equation of fifth order with constant coefficients. The solution of this system is based on the results from [D. Dimitrovski and M. Mijatovic, A New Approach to the Theory of Ordinary Differential Equations (Numerus, Skopje, 1995), pp. 23–33].
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Brown, G. E. "The Ericson-Ericson Lorentz-Lorenz correction." Nuclear Physics A 518, no. 1-2 (November 1990): 99–115. http://dx.doi.org/10.1016/0375-9474(90)90537-v.

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McPhedran, R. C., C. G. Poulton, N. A. Nicorovici, and A. B. Movchan. "Dynamic corrections to the Lorentz-Lorenz formula." Physica A: Statistical Mechanics and its Applications 241, no. 1-2 (July 1997): 179–82. http://dx.doi.org/10.1016/s0378-4371(97)00079-4.

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Vinogradov, A. P. "On the Clausius-Mossotti-Lorenz-Lorentz formula." Physica A: Statistical Mechanics and its Applications 241, no. 1-2 (July 1997): 216–22. http://dx.doi.org/10.1016/s0378-4371(97)00085-x.

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Dwivedi, Sonu, Ashih Kumar Singh, and Arun Kumar Singh. "APPLICATION OF REFRACTIVE INDEX MIXING PRINCIPLES IN BINARY SYSTEMS AT T=298.15, 308.15 AND 318.15K." International Journal of Advanced Research 11, no. 04 (April 30, 2023): 892–97. http://dx.doi.org/10.21474/ijar01/16739.

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Binary liquid mixes of 1-butanol, 1-pentanol, 1-hexanol, and 1-heptanol with hexadecane and heptadecane have had their densities and refractive indices experimentally determined at 298.15, 308.15, and 318.15 K. To determine whether the Lorentz-Lorenz (L-L), Weiner-Heller (W-H), and Gladstone-Dale (G-D) relations for predicting the refractive index of a liquid are valid for the eight binaries over the entire mole fraction range of hexadecane and heptadecane at the three temperatures, a comparative study of these relationships has been conducted. The average percentage deviation has been used to compare different mixing rules. Comparatively speaking, the Weiner and Gladstone-Dale relations perform better than the Lorentz-Lorenz and Heller relations.
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Dissertations / Theses on the topic "Lorenz"

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Ekola, Tommy. "A Numerical Study of the Lorenz and Lorenz-Stenflo Systems." Doctoral thesis, Stockholm, 2005. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-172.

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Winckler, Björn. "Renormalization of Lorenz Maps." Doctoral thesis, KTH, Matematik (Avd.), 2011. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-34314.

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This thesis is a study of the renormalization operator on Lorenz αmaps with a critical point. Lorenz maps arise naturally as first-return maps for three-dimensional geometric Lorenz flows. Renormalization is a tool for analyzing the microscopic geometry of dynamical systems undergoing a phase transition. In the first part we develop new tools to study the limit set of renormalization for Lorenz maps whose combinatorics satisfy a long return condition. This combinatorial condition leads to the construction of a relatively compact subset of Lorenz maps which is essentially invariant under renormalization. From here we can deduce topological properties of the limit set (e.g. existence of periodic points of renormalization) as well as measure theoretic properties of infinitely renormalizable maps (e.g. existence of uniquely ergodic Cantor attractors). After this, we show how Martens’ decompositions can be used to study the differentiable structure of the limit set of renormalization. We prove that each point in the limit set has a global two-dimensional unstable manifold which is a graph and that the intersection of an unstable manifold with the domain of renormalization is a Cantor set. All results in this part are stated for arbitrary real critical exponents  α> 1. In the second part we give a computer assisted proof of the existence of a hyperbolic fixed point for the renormalization operator on Lorenz maps of the simplest possible nonunimodal combinatorial type. We then show how this can be used to deduce both universality and rigidity for maps with the same combinatorial type as the fixed point. The results in this part are only stated for critical exponenta α= 2.
QC 20110627
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Vidarte, José Humberto Bravo. "Smooth pertubations of Lorenz-like flows." Universidade de São Paulo, 2014. http://www.teses.usp.br/teses/disponiveis/55/55135/tde-15072014-155326/.

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Given a Geometric Lorenz Flow X on \'R POT. n+2\' of class \'C POT. k+1\'; by definition there exists a Poincaré map \'P IND. X\' of class \'C POT. k+1\'; often so-called Lorenz-type map [ABS83]. The main purpose in this dissertation is to show that under certain conditions the Lorenz-type map \'P IND.X\' can be associate to it a one-dimensional transformation \'f IND. X\' of class \'C POT. k\' (defined on an interval). This association is so-called the reduction transformation R; so we have \'RP IND. X\' = \'f IND. X\'. This association would allow us to study the dynamical properties for the original flow using techniques of one-dimensional dynamics of class \'C POT. k\'
Dado um Fluxo Geométrico de Lorenz X em \'R POT. n+2\' de classe \'C POT. k+1\'; por definição, existe uma aplicação de Poincaré \'P IND. X\'\' de classe \'C POT. k+1\'; frequentemente chamado aplicação do tipo Lorenz [ABS83]. O objetivo principal desta tese é mostrar que, sob certas condições a aplicação do tipo Lorenz \'P IND. X\' pode ser associado a ele uma transformação unidimensional \'f IND. X\' de classe \'C POT. k\' (definida em um intervalo). Esta associação é chamada de transformação de redução R; assim temos que , \'RP IND. X\' = \'f IND. X\'. Esta associação nos permitiria estudar as propriedades dinâmicas do fluxo original utilizando técnicas da dinâmica unidimensional de classe \'C POT. k\'
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Wendler, André [Verfasser], Lorenz [Akademischer Betreuer] [Gutachter] Engell, and Peter [Gutachter] Geimer. "Anachronismen: Historiografie und Kino / André Wendler ; Gutachter: Lorenz Engell, Peter Geimer ; Betreuer: Lorenz Engell." Weimar : Professur Medienphilosophie, 2012. http://d-nb.info/1115807145/34.

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Lucena, Rafael Nóbrega de Oliveira. "Propriedades ergódicas do modelo geométrico do atrator de Lorenz." Universidade Federal de Alagoas, 2011. http://repositorio.ufal.br/handle/riufal/1054.

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This work has its motivation in the study of the ergodic properties of the Lorenz geometric model, constructed to approximate the behavior of solutions of the Lorenz equations. Simultaneously, Afraimovich in [17] and Guckenheimer and Williams [18], constructed a geometric model that mimics the dynamics of the original Lorenz equations. Here, we build ergodic physical measures for two types of applications that arise from the Lorenz geometric model. The first one is a piecewise expanding one-dimensional map and the second is a two-dimensional application wich contracts the leaves of an invariant foliation. To construct the ergodic physical measure for the one dimensional Lorenz map, we make use of an operator (transfer operator) acting in the space of bounded variation functions, while the second uses the Riesz representation theorem and some other topological properties.
Fundação de Amparo a Pesquisa do Estado de Alagoas
Este trabalho tem sua motivação no modelo geométrico construído para aproximar o comportamento das soluções das equações de Lorenz. Simultaneamente Afraimovich em [17] e Guckenheimer e Williams [18] construíram um modelo geométrico. Essencialmente ele consiste na construção de medidas físicas e ergódicas para dois tipos de aplicações, uma unidimensional que é seccionalmente expansora (piecewise expanding) e outra bidimensional que contrai as folhas de uma folheação invariante. A primeira faz uso de um operador (operador de transferência) agindo no espaço das funções de variação limitada, enquanto que a segunda utiliza o teorema de representação Riesz bem como algumas outras propriedades topológicas.
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El-Rifai, E. A. "Positive braids and Lorenz links." Thesis, University of Liverpool, 1988. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.384365.

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In this work a new foundation for the study of positive braids in Artin's braid groups is given. The basic braids considered are the set SBn of positive permutation braids, defined as those positive braids where each pair of arcs cross at most once. These are shown to be in 1-1 correspondence with the permutations in S . A canonical n form for positive braids as products of braids in SB is given, ton gether with an explicit algorithm for writing every positive braid in canonical form and a practical test for use in the algorithm. This is a useful approach to braid theory because permutations can be particularly easily handled. Applications of this canonical form are: (1) An easily handled approach to Garside's solution of the word problem in B . n (2) An algorithm to decide whether (/1 ) k is a factor of a positive n braid; this happens if and only if at most k canonical factors have equal to /1 n (where /1 n is the positive braid with each pair of arcs cross exactly once). (3) A proof that a positive braid is a factor of (/1 ) k if and only if n its canonical form has at most k factors. (4) An improvement of Garside's solution of the conjugacy problem, this is by reducing the summit set to a much smaller invariant class under conjugation (super summit set). This includes a necessary and sufficient condition for positive braid to contain /1 n up to conjugation. The linear generators of the Hecke algebras used by Morton. and/ Short are in 1-1 correspondence with the elements of SB. The n canonical forms above give a quick proof that the number of strands in a twist positive braid (one of the form (/1 )2mp for positive braid n P and for positive integer m) is the braid index of the closure of that braid, which was first proved by Franks and Williams. It is also shown that if the 2-variable link invariant P L (v, z) for an oriented link L has width k in the variable v, then it is the same as the polynomial of a closed k-braid, for k = 1, 2. A complete list of 3-braids of width 2, which close to knots, is given. It is also shown that twist positive 3-braids do not admit exchange moves (in the sense of Birman). Consequently the conjugacy class of a twist positive 3-braid representative is a complete link invariant, provided that Birman's conjecture about Markov's moves and exchange moves holds. Lorenz knots and links are studied as an example of positive links. It is proved that a positive permutation braid 1T is a Lorenz braid if and only if all braid words which equal 1T have the same single starting letter. A semicanonical form for a minimal braid representative of a Lorenz link is given. It is proved that every algebraic link of c components is a Lorenz link, for c = 1, 2. (The case for knots was first proved by Birman and Williams). Consequently a necessary and sufficient condition for a knot to be algebraic is given, together with a canonical form for a minimal braid representative for every algebraic knot. To some extent the relation between Lorenz knots and their companions is studied. It is shown that Lorenz knots and links of braid index 3 are determined by conjugacy classes in B 3. A complete list of 3 -braids which close to Lorenz knots and links is given and a complete list of pure 4-braids which close to Lorenz links is also given. It is shown that Lorenz knots and links of braid index 3 are determined by their Alexander polynomials. As a further analogy with the properties of algebraic links it is shown that the linking pattern of a Lorenz link L with pure braid representative and braid index t ~4, determines a unique braid representative for L and so determines L.
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Herrgård, Max. "Synchronization in the Lorenz system." Thesis, Uppsala universitet, Tillämpad matematik och statistik, 2016. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-312814.

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Lorenz, Björn [Verfasser]. "Serialität der Romanhefte / Björn Lorenz." Göttingen : Niedersächsische Staats- und Universitätsbibliothek Göttingen, 2020. http://d-nb.info/121590617X/34.

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Adametz, Julian [Verfasser], Lorenz-Peter [Akademischer Betreuer] Schmidt, and Lorenz-Peter [Gutachter] Schmidt. "Polarimetrische Dekompositionsverfahren für bildgebende Nahbereichsradarsysteme / Julian Adametz ; Gutachter: Lorenz-Peter Schmidt ; Betreuer: Lorenz-Peter Schmidt." Erlangen : Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), 2018. http://d-nb.info/1159377413/34.

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Chen, Kanglin [Verfasser], Dirk [Akademischer Betreuer] Lorenz, and Peter [Akademischer Betreuer] Maaß. "Optimal Control based Image Sequence Interpolation / Kanglin Chen. Gutachter: Dirk Lorenz ; Peter Maaß. Betreuer: Dirk Lorenz." Bremen : Staats- und Universitätsbibliothek Bremen, 2011. http://d-nb.info/1071898078/34.

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Books on the topic "Lorenz"

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Spring, Lorenz. Lorenz Spring. Basel: Galerie Carzaniga und Ueker, 1996.

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Max, Lorenz. Max Lorenz. Wien: Amt der Niederösterreichischen Landesregierung, Abt. III/2, Kulturabteilung, 1996.

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1928-, Dittmann Lorenz, Bothmer Hans-Caspar Graf von, Güthlein Klaus 1942-, and Kuhn Rudolf 1939-, eds. Festschrift Lorenz Dittmann. Frankfurt am Main: P. Lang, 1994.

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Sicklinger, Andreas, and Giulia Decorti. Reactions: Peter Lorenz. Melfi (Potenza): Librı̀a, 2006.

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Carzaniga, Galerie, ed. Lorenz Spring: Zeitfluss. Basel: Galerie Carzaniga, 2018.

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Gerhardt, Johannes. Eduard Lorenz Lorenz-Meyer. Ein Hamburger Kaufmann und Künstler. Hamburg: Hamburg University Press, 2007.

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Gouesbet, Gérard, and Gérard Gréhan. Generalized Lorenz-Mie Theories. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-46873-0.

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Gouesbet, Gérard, and Gérard Gréhan. Generalized Lorenz-Mie Theories. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-17194-9.

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Breidbach, Olaf, Hans-Joachim Fliedner, and Klaus Ries, eds. Lorenz Oken (1779–1851). Stuttgart: J.B. Metzler, 2001. http://dx.doi.org/10.1007/978-3-476-02768-9.

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Evang.-Luth. Kirchengemeinde St. Lorenz (Nuremberg, Germany), ed. St. Lorenz in Nürnberg. Lindenberg: J. Fink, 2011.

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Book chapters on the topic "Lorenz"

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Kämpke, Thomas, and Franz Josef Radermacher. "Lorenz Densities and Lorenz Curves." In Lecture Notes in Economics and Mathematical Systems, 29–54. Cham: Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-13224-2_3.

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Laubichler, Manfred D. "Lorenz, Konrad." In Kindlers Literatur Lexikon (KLL), 1. Stuttgart: J.B. Metzler, 2020. http://dx.doi.org/10.1007/978-3-476-05728-0_15425-1.

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Hamel, Jürgen. "Eichstad, Lorenz." In Biographical Encyclopedia of Astronomers, 644. New York, NY: Springer New York, 2014. http://dx.doi.org/10.1007/978-1-4419-9917-7_401.

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Blaauw, Adriaan, Robert A. Garfinkle, James Dye, Matthew Stanley, Virginia Trimble, Roy H. Garstang, Jürgen Hamel, et al. "Eichstad, Lorenz." In The Biographical Encyclopedia of Astronomers, 327–28. New York, NY: Springer New York, 2007. http://dx.doi.org/10.1007/978-0-387-30400-7_401.

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Kotrschal, Kurt. "Konrad Lorenz." In Encyclopedia of Animal Cognition and Behavior, 3800–3812. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-319-55065-7_941.

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Kakwani, Nanak. "Lorenz Curve." In The New Palgrave Dictionary of Economics, 1–3. London: Palgrave Macmillan UK, 1987. http://dx.doi.org/10.1057/978-1-349-95121-5_1117-1.

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Kakwani, Nanak. "Lorenz Curve." In The New Palgrave Dictionary of Economics, 1–3. London: Palgrave Macmillan UK, 2008. http://dx.doi.org/10.1057/978-1-349-95121-5_1117-2.

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Fellman, Johan. "Lorenz Curve." In International Encyclopedia of Statistical Science, 760–62. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-04898-2_345.

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Kotrschal, Kurt. "Konrad Lorenz." In Encyclopedia of Animal Cognition and Behavior, 1–13. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-47829-6_941-1.

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Kakwani, Nanak. "Lorenz Curve." In The New Palgrave Dictionary of Economics, 8025–27. London: Palgrave Macmillan UK, 2018. http://dx.doi.org/10.1057/978-1-349-95189-5_1117.

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Conference papers on the topic "Lorenz"

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Nagy, Réka, Mihai Alexandru Suciu, and D. Dumitrescu. "Lorenz equilibrium." In the fourteenth international conference. New York, New York, USA: ACM Press, 2012. http://dx.doi.org/10.1145/2330163.2330233.

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Ghiner, A. V., and G. I. Surdutovich. "What replaces the Lorentz-Lorenz formula for a cooled resonance gas?" In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1993. http://dx.doi.org/10.1364/oam.1993.mqq.6.

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A rarefied gas of neutral atoms cooled and trapped by means of the resonance light pressure forces’ is an example of a system when n λ3 ≤ 1, but Nα ≥1. Here N denotes the density of atoms, λ is the light wavelength, a is the microscopic polarizability. It means that local field effects are essential, whereas Lorentz–Lorenz relation between α and refractive index n already, generally speaking, is not applicable. For rarefied gas even the question of the method integral equation2 applicability in itself is not evident, but in any case its application implies that the Lorentz’s sphere radius must be much larger than wavelength, which is incompatible with the traditional approach. With the choice of a large Lorentz sphere the variables substitution method3 allowed to calculate simultaneously linear and nonlinear medium characteristics and to obtain a connection between local and macroscopic fields when the spatial dispersion is taken into account. These characteristics essentially depend on the interaction law between the particles. In the no-interaction condition (ideal gas) Lorentz-Lorenz formula is valid for arbitrary densities, including the case Nλ3<< 1. It has been revealed that for repulsive forces between the atoms in a case Nα ≥ 1 an effect of the optical transparency (n2− 1 << 1) takes place.
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Aljumaily, G. A., G. E. Carver, J. B. Barton, S. A. Locknar, S. K. Chanda, and R. L. Johnson. "Optical and Physical Properties of Annealed Amorphous Nb2O5 Thin Films." In Optical Interference Coatings. Washington, D.C.: Optica Publishing Group, 2022. http://dx.doi.org/10.1364/oic.2022.tha.4.

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The impact of post-deposition annealing on the optical and physical properties of sputtered and evaporated metal-oxide coatings was examined. Models based on the Lorentz-Lorenz equation and potential energy considerations are used to explain the data.
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Nosov, Victor V. "Refractive index of any gaseous mixtures in Lorentz-Lorenz spectroscopy." In 13th Symposium and School on High-Resolution Molecular Spectroscopy, edited by Leonid N. Sinitsa. SPIE, 2000. http://dx.doi.org/10.1117/12.375407.

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Nagy, Reka, Mihai Suciu, and D. Dumitrescu. "Exploring Lorenz Dominance." In 2012 14th International Symposium on Symbolic and Numeric Algorithms for Scientific Computing (SYNASC). IEEE, 2012. http://dx.doi.org/10.1109/synasc.2012.48.

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Vladimirov, Andrei G., Vladislav Y. Toronov, and Vladimir L. Derbov. "Complex Lorenz equations." In Nonlinear Dynamics of Laser and Optical Systems, edited by Valery V. Tuchin. SPIE, 1997. http://dx.doi.org/10.1117/12.276193.

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Sparrow, C. "The Lorenz Model." In Instabilities and Dynamics of Lasers and Nonlinear Optical Systems. Washington, D.C.: Optica Publishing Group, 1985. http://dx.doi.org/10.1364/idlnos.1985.tub2.

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The three-dimensional set of ordinary differential equations, known as the Lorenz equations were first introduced by Ed Lorenz [2] in 1963 as a model of convection in a two-dimensional cell. Since then other authors, e.g. Haken [1] have shown that the same equations can be derived from the Maxwell-Bloch equations for single-mode lasers with damping. The equations are of mathematical interest because of the wide variety of behaviours that they display -- including chaotic behaviour and the existence of strange attractors -- for different values of the three parameters r, σ and b. It seems that the relevant range of parameters for laser applications is σ < b + 1 which, it must be confessed, is not the parameter range of greatest interest from a mathematical point of view. However, providing 3σ - 1 > 2b attracting chaotic behaviour will still occur [3,4] though it will occur at parameter values for which the equations also have stable stationary points and these may determine most of the observed behaviour of the system.
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Laguarta, F., J. Pujol, R. Vilaseca, and R. Corbalán. "Instabilities in Doppler Broadened Optically Pumped Far-Infrared Lasers." In Optical Bistability. Washington, D.C.: Optica Publishing Group, 1988. http://dx.doi.org/10.1364/obi.1988.we.11.

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Recently Weiss and Brock observed Lorenz-type chaos in the 81.5μm emission from an optically-pumped 14NH3 laser1. The theoretical interpretation of the experimental results is an open question, however. In fact, the Lorenz-Haken model refers to incoherently pumped lasers with homogeneously-broadened two-level active media2. Models based on (at least) a three-level system are needed to describe optically-pumped lasers, whose dynamics is known to reduce to that of the Lorez-Haken model under certain limiting conditions3. But these conditions are not met in the 14NH3 laser, and indeed theoretical predictions of a model for this laser, which considered a homogeneously-broadened three-level active medium4, revealed striking differences with the experimental observations1.
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Maki, Jeffery J., Robert W. Boyd, Michelle S. Malcuit, and John E. Sipe. "Lorentz red shift and self-broadening of atomic potassium vapor." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1990. http://dx.doi.org/10.1364/oam.1990.fff3.

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The Lorentz-Lorenz equation predicts that the dispersion feature of an isolated optical resonance should have a density-dependent frequency shift toward the red end of the spectrum. We have investigated the dispersion feature experimentally by observing the frequency dependence of the Fresnel reflection (selective reflection) from the boundary between a dense atomic potassium vapor and the window of the vessel containing the vapor. We find that the selective-reflection features of both the S1/2-P1/2 (770.1 nm) and S1/2-P3/2 (766.7 nm) lines of potassium shift increasingly toward the red and broaden as the number density of the vapor is increased to 2 × 1017 atoms/cm3. We compare the results of the experiment to theoretical predictions for the selective reflection. The broadening is well described by conventional binary collision theory; however, the observed red shift of both of the lines is somewhat larger than that predicted by the Lorentz-Lorenz equation. It is possible that other mechanisms that lead to frequency shifts are occurring.
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Ghiner, A. V., and G. I. Surdutovich. "Nonlocal Field Effects and Macroscopic Optical Properties of Self-Assembled Films." In Organic Thin Films for Photonic Applications. Washington, D.C.: Optica Publishing Group, 1993. http://dx.doi.org/10.1364/otfa.1993.wd.23.

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Controlable thickness, surface uniformity and a high degree of orientational order of self-assembled organic films raise the problem of direct calculation of their macroscopic optical characteristics in terms of isolated molecule parameters. The two-dimensional character of the problem requires rethinking of the standard approach to the local field effects which in a three-dimensional case are given by the Lorentz-Lorenz formula.
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Reports on the topic "Lorenz"

1

Long, J. Lorenz APIs and REST Services. Office of Scientific and Technical Information (OSTI), April 2013. http://dx.doi.org/10.2172/1078546.

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Long, J. Lorenz: Using the Web to Make HPC Easier. Office of Scientific and Technical Information (OSTI), July 2013. http://dx.doi.org/10.2172/1090027.

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Long, J., and J. Martinez. Level-2 Milestone 4468: Lorenz Simulation Interface Beta Release. Office of Scientific and Technical Information (OSTI), January 2012. http://dx.doi.org/10.2172/1093932.

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Rasiah, Rajah. Fostering Clusters in the Malaysian Electronics Industry. Inter-American Development Bank, November 2005. http://dx.doi.org/10.18235/0006838.

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The meaning of clusters has evolved considerably over several decades. This presentation seeks to use a synthesis of the concept from the time of Mill and Marshall (industrial districts), and Smith and Young on differentiation and division of labour to encompass the work of Brusco, Becatini, Sabel, Sengenberger, Zeitlin, Pyke, Richardson, North, Lorenz, Wilkinson and Piore to extract the influence of socio-economic relationships (a blend of markets and trust-loyalty), and subsequently the contributions of Porter (traditional and high tech clusters) and Best (organizational change, techno-diversity, open-system flows and speciation). This presentation examines clustering in the electronics industry in Malaysia with a policy focus on the embedding environment within which this process has evolved in the two main regions of Penang and Kelang Valley. This presentation was presented at the Latin America/Caribbean and Asia/Pacific Economics and Business Association (LAEBA)'s 2nd Annual Meeting held in Buenos Aires, Argentina on November 28th-29th, 2005.
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Breuer, Kenneth. Lorentz Force Control of Turbulence. Fort Belvoir, VA: Defense Technical Information Center, January 2005. http://dx.doi.org/10.21236/ada432664.

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Amandolia, Kenneth, and Charles Lane. Untangling Coefficients for Lorentz Violation. Journal of Young Investigators, May 2018. http://dx.doi.org/10.22186/jyi.34.5.26-30.

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İlarslan, Kazim, Ali Uçum, and Ivaïlo M. Mladenov. Sturmian Spirals in Lorentz-Minkowski Plane. Jgsp, 2015. http://dx.doi.org/10.7546/jgsp-37-2015-25-42.

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Ungar, Abraham A. The Proper-Time Lorentz Group Demystified. Journal of Geometry and Symmetry in Physics, 2012. http://dx.doi.org/10.7546/jgsp-4-2005-69-95.

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Abe, K. Tau Lorentz Structure with Polarization at SLD. Office of Scientific and Technical Information (OSTI), January 2004. http://dx.doi.org/10.2172/826624.

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Kabel, A. MAXWELL-LORENTZ EQUATIONS IN GENERAL FRENET-SERRET COORDINATES. Office of Scientific and Technical Information (OSTI), September 2004. http://dx.doi.org/10.2172/833082.

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