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Liquid glass transition : a unified theory from the two band model /

A glass is disordered material like a viscous liquid and behaves mechanically like a solid. A glass is normally formed by supercooling the viscous liquid fast enough to avoid crystallization, and the liquid-glass transition occurs in diverse manners depending on the materials, their history, and the...

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Detalles Bibliográficos
Clasificación:Libro Electrónico
Autor principal: Kitamura, Toyoyuki (Autor)
Formato: Electrónico eBook
Idioma:Inglés
Publicado: Amsterdam : Elsevier, 2013.
Colección:Elsevier insights.
Temas:
Acceso en línea:Texto completo

MARC

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082 0 4 |a 530.4/24  |2 23 
100 1 |a Kitamura, Toyoyuki,  |e author. 
245 1 0 |a Liquid glass transition :  |b a unified theory from the two band model /  |c Toyoyuki Kitamura, Nagasaki Institute of Applied Science, Nagasaki, Japan. 
264 1 |a Amsterdam :  |b Elsevier,  |c 2013. 
300 |a 1 online resource (xv, 384 pages) :  |b illustrations. 
336 |a text  |b txt  |2 rdacontent 
337 |a computer  |b c  |2 rdamedia 
338 |a online resource  |b cr  |2 rdacarrier 
490 1 |a Elsevier insights 
504 |a Includes bibliographical references. 
520 |a A glass is disordered material like a viscous liquid and behaves mechanically like a solid. A glass is normally formed by supercooling the viscous liquid fast enough to avoid crystallization, and the liquid-glass transition occurs in diverse manners depending on the materials, their history, and the supercooling processes, among other factors. The glass transition in colloids, molecular systems, and polymers is studied worldwide. This book presents a unified theory of the liquid-glass transition on the basis of the two band model from statistical quantum field theory associated with the temperature Green's function method. It is firmly original in its approach and will be of interest to researchers and students specializing in the glass transition across the physical sciences. Examines key theoretical problems of the liquid-glass transition and related phenomena. Clarifies the mechanism and the framework of the liquid-glass transition. 
588 0 |a Print version record. 
505 0 |a Half Title; Liquid Glass Transition; Contents; Introduction; 1.1 The Structure of the Condensed States and the Quantum Regime; 1.1.1 The Structure of Condensed States, the Pair Distribution Function, and Hopping of Particles; 1.1.2 The Nambu-Goldstone Bosons, Phonons, and Sound; 1.1.3 The Liquid-Glass Transition Occurs in the Quantum Regime; 1.2 The Two Band Model for the Liquid-Glass Transition; 1.2.1 The Two Band Model; 1.2.2 Sound; 1.2.3 Phonons and Boson Peak; 1.2.4 The Dissipative and Relaxation Processes; 1.2.5 The Kauzmann Entropy and the Kauzmann Entropy Crisis 
505 8 |a 1.2.6 The Gap of the Specific Heat at the Glass Transition Temperature Tg1.2.7 The Hopping Amplitude and the VTF Law; 1.2.8 Phonon Fluctuation Entropy and the Liquid-Glass Transition; 1.2.9 Panic; Supercooling Process Associated with the Kauzmann Entropy Crisis and the VTF Law; 1.2.10 Mode Coupling Theory and the Adam-Gibbs Formula; 1.3 Perspective of This Book; 1.3.1 Introductary Part; 1.3.2 Preliminary Part; 1.3.3 Core Part; 1.3.4 Extensional Part; References; Sound and Elastic Waves in the Classical Theory; 2.1 Sound in the Classical Fluid Mechanics 
505 8 |a 2.1.1 Sound in the Isothermal and Adiabatic Processes2.1.2 Free Energy of Sound in the Classical Fluid Mechanics; 2.1.3 Energy of Sound in the Classical Fluid Mechanics; 2.1.4 The Relation Between the Isothermal and Adiabatic Sounds; 2.2 Elastic Waves in the Classical Elastic Theory; 2.2.1 Strain Tensor and Stress Tensor; 2.2.2 Thermodynamics in Deformation; 2.2.3 The Fick's Law in the Isothermal Process; 2.2.4 The Fick's Law in the Adiabatic Process; 2.2.5 Elastic Waves; 2.3 Sound and Phonons in the Classical Microscopic Theory 
505 8 |a 2.3.1 The Hamiltonians and the Equations of Motion for Sound and Phonons2.3.1.1 Sound and diffusivity; 2.3.2 The Equations of Motion for Density Fluctuations; 2.3.3 The Canonical Equations of Motion for Sound; 2.3.4 Dissipative and Relaxation Processes; 2.3.4.1 Phonons, boson peak, and viscosity; 2.4 The Kauzmann Entropy, the Vogel'226Tamman'226Fulcher Law and Specific Heat; 2.4.1 The Limitations of the Microscopic Classical Theory and the Roles of Quantum Statistics; References; Fundamentals of Quantum Field Theory; 3.1 The Number Representation and the Fock Space 
505 8 |a 3.1.1 The Number Representation3.1.2 The Fock Space; 3.1.3 Creation and Annihilation Operators; the Commutation Relations; 3.1.3.1 Bosons; 3.1.3.2 Fermions; 3.1.4 Creation and Annihilation Operators for Wave Packets of Particles; 3.2 An Example of Unitarily Inequivalent Representations; The Bogoliubov Transformation of Boson Operators; 3.2.1 The Bogoliubov Transformation of Boson Operators; 3.3 The Physical Particle Representation and the Dynamical Map; 3.3.1 The Physical Particles and the Heisenberg Fields in the Heisenberg Equation 
650 0 |a Liquids  |x Thermal properties. 
650 0 |a Glass transition temperature. 
650 0 |a Crystallization  |x Mathematical models. 
650 0 |a Quantum field theory. 
650 6 |a Liquides  |x Propri�et�es thermiques.  |0 (CaQQLa)201-0036327 
650 6 |a Temp�erature de transition vitreuse.  |0 (CaQQLa)201-0279609 
650 6 |a Cristallisation  |0 (CaQQLa)201-0018431  |x Mod�eles math�ematiques.  |0 (CaQQLa)201-0379082 
650 6 |a Th�eorie quantique des champs.  |0 (CaQQLa)201-0022048 
650 7 |a Crystallization  |x Mathematical models  |2 fast  |0 (OCoLC)fst00884647 
650 7 |a Glass transition temperature  |2 fast  |0 (OCoLC)fst00943273 
650 7 |a Liquids  |x Thermal properties  |2 fast  |0 (OCoLC)fst00999713 
650 7 |a Quantum field theory  |2 fast  |0 (OCoLC)fst01085105 
650 7 |a Glasumwandlung  |2 gnd  |0 (DE-588)4215431-5 
650 7 |a B�andermodell  |2 gnd  |0 (DE-588)4143892-9 
776 0 8 |i Print version:  |a Kitamura, Toyoyuki.  |t Liquid glass transition.  |d Chennai ; Oxford : Elsevier, 2013  |z 9780124071773  |w (OCoLC)813855589 
830 0 |a Elsevier insights. 
856 4 0 |u https://sciencedirect.uam.elogim.com/science/book/9780124071773  |z Texto completo