LEADER 05176nam 2200637Ia 450 001 9910462803403321 005 20200520144314.0 010 $a981-4407-48-8 035 $a(CKB)2670000000361825 035 $a(EBL)1193431 035 $a(OCoLC)844311065 035 $a(SSID)ssj0000872859 035 $a(PQKBManifestationID)12392114 035 $a(PQKBTitleCode)TC0000872859 035 $a(PQKBWorkID)10851198 035 $a(PQKB)10381445 035 $a(MiAaPQ)EBC1193431 035 $a(WSP)00002998 035 $a(Au-PeEL)EBL1193431 035 $a(CaPaEBR)ebr10700623 035 $a(CaONFJC)MIL486882 035 $a(EXLCZ)992670000000361825 100 $a20130419n2013 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aGlassy disordered systems$b[electronic resource] $eglass formation and universal anomalous low-energy properties /$fMichael I. Klinger 210 $aSingapore $cWorld Scientific$d2013 215 $a1 online resource (340 p.) 300 $aDescription based upon print version of record. 311 $a981-4407-47-X 320 $aIncludes bibliographical references and index. 327 $aPreface; 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" 327 $a3.2. 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 frequencies 327 $a6.2. 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 Case 327 $a9.1. 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 excitations 327 $a10.5. 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 model 327 $a12.3. Comparison with the soft-mode model 330 $aThe 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 conside 606 $aOptics 606 $aGlass 608 $aElectronic books. 615 0$aOptics. 615 0$aGlass. 676 $a620.1/44 676 $a620.144 700 $aKlinger$b Michael I$0968222 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910462803403321 996 $aGlassy disordered systems$92199124 997 $aUNINA LEADER 01166nam 2200409 450 001 9910466264503321 005 20200123192848.0 010 $a1-4232-3921-0 035 $a(CKB)4100000007108293 035 $a(MiAaPQ)EBC5558984 035 $a(Au-PeEL)EBL5558984 035 $a(OCoLC)1059415048 035 $a(EXLCZ)994100000007108293 100 $a20200123d2018 uy 0 101 0 $aeng 135 $aurcnu|||||||| 181 $ctxt$2rdacontent 182 $cc$2rdamedia 183 $acr$2rdacarrier 200 10$aPeriodic table basic $ea QuickStudy laminated reference guide /$fMark Jackson 210 1$a[Place of publication not identified] :$cBarCharts,$d[2018] 210 4$dİ2018 215 $a1 online resource 225 0 $aQuickStudy Science 311 $a1-4232-3920-2 606 $aPeriodic table of the elements 608 $aElectronic books. 615 0$aPeriodic table of the elements. 676 $a546.8 700 $aJackson$b Mark$0914205 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910466264503321 996 $aPeriodic table basic$92120765 997 $aUNINA LEADER 02028oam 2200601M 450 001 9910716263303321 005 20200213070503.2 035 $a(CKB)5470000002519491 035 $a(OCoLC)1065769911 035 $a(OCoLC)995470000002519491 035 $a(EXLCZ)995470000002519491 100 $a20071213d1926 ua 0 101 0 $aeng 135 $aurcn||||||||| 181 $ctxt$2rdacontent 182 $cc$2rdamedia 183 $acr$2rdacarrier 200 10$aBuilding permits in the principal cities of the United States in 1925. 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