02230 am 2200469 n 450 9910495901403321202001292-7574-2686-910.4000/books.septentrion.81373(CKB)5590000000431745(FrMaCLE)OB-septentrion-81373(oapen)https://directory.doabooks.org/handle/20.500.12854/87067(PPN)253362911(EXLCZ)99559000000043174520210111j|||||||| ||| 0freuu||||||m||||txtrdacontentcrdamediacrrdacarrierL’écrivain-reporter au coeur des années trente /Myriam BoucharencVilleneuve d'Ascq Presses universitaires du Septentrion20201 online resource (246 p.) Objet2-85939-842-2 La tentation du reportage destiné à la grande presse n’a épargné presque aucun des écrivains des années trente : Carco, Cocteau, Cendrars, Soupault, Simenon, Kessel, Malraux et combien d’autres encore, se sont lancés, sous le patronage de la figure mythique d’Albert Londres, dans le genre incertain de l’enquête, pour le plus grand plaisir des lecteurs du Matin, de Paris-Soir ou de Voilà. Phénomène aussi remarquable que méconnu de la vie culturelle de l’Entre-deux-guerres, la vogue de l’écrivain-reporter soulève quelquesunes des questions essentielles que se pose alors la littérature, à mi-chemin du livre et du journal, de l’écriture et de l’action.French literature20th centuryHistory and criticismJournalismFranceHistory20th centuryJournalism and literatureFranceHistory20th centurylittératureécrivainreportervoyageurFrench literatureHistory and criticism.JournalismHistoryJournalism and literatureHistoryBoucharenc Myriam734693FR-FrMaCLEBOOK9910495901403321L’écrivain-reporter au coeur des années trente3019485UNINA05044oam 2200541 450 991078696830332120190911112728.0981-4407-48-8(OCoLC)897557540(MiFhGG)GVRL8QYI(EXLCZ)99267000000036182520130408h20132013 uy 0engurun|---uuuuatxtccrGlassy disordered systems glass formation and universal anomalous low-energy properties /Michael I. Klinger, Bar-Ilan University, IsraelSingapore World Scientific2013New Jersey :World Scientific,[2013]�20131 online resource (xii, 326 pages) illustrationsGale eBooksDescription based upon print version of record.981-4407-47-X Includes bibliographical references and index.Preface; CONTENTS; I. Fundamental Properties of Glasses; 1. General Description of Glasses and Glass Transition; 1.1. Metastability and disorder. Types of glasses; 1.2. Qualitative description of glass (liquid-to-glass) transition; 1.3. Kinetic and thermodynamic properties; 1.4. Slow relaxation processes; 2. Models of Glassy (Topologically Disordered) Structures; 2.1. Characteristics of glassy structures; 2.2. Homogeneous (ideal) models; 2.3. Inhomogeneous (cluster) models; 3. Some Theoretical Models of Glass Transition; 3.1. Vogel-Fulcher relation and "entropy crisis"3.2. Role of configurational entropy, free-volume effects and "defects" diffusion3.3. Mode-coupling model: Dynamic liquid-glass transition; 4. Kohlrausch-William-Watt (KWW) Relaxation; 4.1. General features of slow relaxation processes; 4.2. Parallel-diffusion relaxation models; 4.3. Correlated, hierarchically constrained, relaxation models; 4.4. Concluding remarks; II. Anomalous Low-Energy Dynamics of Glasses; 5. Origin of Anomalous Low-Energy Properties of Glasses; 6. Experimental Background for Anomalous Low-Energy Atomic Dynamics; 6.1. Very low temperatures and frequencies6.2. Moderately low temperatures and frequencies7. Soft-Mode Model of Low-Energy Atomic Dynamics; 7.1. Atomic soft modes and related potentials; 7.2. Probability distribution densities; 7.3. Low-energy excitations: Density of states and concentration; 7.4. Interaction of soft-mode excitations with acoustic phonons; 8. Soft-Mode Excitations of Very Low and "Intermediate" Energies; 8.1. Soft-mode tunneling states (independent two-level systems); 8.2. Soft-mode excitations of "intermediate" energies; 9. Tunneling States as Very Low Energy Limit Case9.1. Standard tunneling model: Independent two-level systems9.2. Advanced tunneling model: Interacting two-level systems; 9.2.1. Mean-field approximation: "Spectral diffusion"; 9.2.2. Many-body effects: Collective excitations; 10. Soft-Mode Excitations of Moderately-Low Energies (Boson Peak); 10.1. Ioffe-Regel crossover for acoustic phonons as origin of boson peak; 10.2. Independent soft-mode vibrational excitations; 10.3. Total vibrational density of independent soft-mode states; 10.4. Generalization for interacting harmonic excitations10.5. Total vibrational density of states: dynamic properties10.6. Width (attenuation) of acoustic phonons; 10.7. Thermal vibrational properties of glasses; 11. On Universal and Non-Universal Dynamic Properties of Glasses; 11.1. Very low temperatures and frequencies; 11.1.1. On universality of basic distributions in ATM; 11.1.2. On universality of soft-mode distribution inSMM; 11.2. Moderately low temperatures and frequencies; 12. Other Models for Glasses with High Frequency Sound; 12.1. Theoretical mode-coupling model; 12.2. Theoretical random-matrix model12.3. Comparison with the soft-mode modelThe present book describes the fundamental features of glassy disordered systems at high temperatures (close to the liquid-to-glass transition) and for the first time in a book, the universal anomalous properties of glasses at low energies (i.e. temperatures/frequencies lower than the Debye values) are depicted. Several important theoretical models for both the glass formation and the universal anomalous properties of glasses are described and analyzed. The origin and main features of soft atomic-motion modes and their excitations, as well as their role in the anomalous properties, are consideGlassEffect of high temperatures onGlassThermomechanical propertiesAtomic structureGlassEffect of high temperatures on.GlassThermomechanical properties.Atomic structure.620.1/44620.144Klinger Michael I1529552MiFhGGMiFhGGBOOK9910786968303321Glassy disordered systems3773881UNINA