J. Tolédano, V. Janovec, V. Kopský, J. Scott, P. Boček
{"title":"3.1 Structural phase transitions","authors":"J. Tolédano, V. Janovec, V. Kopský, J. Scott, P. Boček","doi":"10.1107/97809553602060000915","DOIUrl":null,"url":null,"abstract":"Aspects of phase transitions in crystals that are of interest to crystallographers are described in this chapter. The chapter starts with a brief introduction aimed at defining the field of structural transitions and the terminology used. The theory of structural phase transitions is then described. This theory relates the symmetry characteristics of the transitions to their physical characteristics. The application of the symmetry principles that derive from this theory is illustrated by the results contained in Tables 3.1.3.1 and 3.1.4.1. The first of these two tables concerns the simple but experimentally widespread situation in which a structural transition is not accompanied by a change in the number of atoms per primitive crystal cell. The second table concerns the general case, in which the number of atoms changes, and which corresponds to the onset of superlattice reflections at the phase transition. This table provides, for a set of hypothetical transformations, the various symmetry-based predictions of the theory. The important topic of soft modes, which is related to the microscopic mechanism of a structural transition, is then discussed. The final section of the chapter is an introduction to the accompanying software package Group Informatics. \n \n \nKeywords: \n \nCurie temperature; \nLandau theory; \nLandau–Devonshire theory; \ndomain states; \nenantiomorphism; \nequitranslational phase transitions; \nequitranslational subgroups; \nferroelastic materials; \nferroelastic phases; \nferroelastic transitions; \nferroelectric materials; \nferroelectric phases; \nferroelectric transitions; \nferroic classes; \nferroic domain states; \nferroic phases; \nferroic single-domain states; \nferroic symmetry; \nferroic transitions; \nfree energy; \nhigh-symmetry phases; \nhigh-temperature superconductors; \nirreducible representations; \nlow-symmetry phases; \nnon-equitranslational phase transitions; \norder parameter; \nparent phases; \nparent symmetry; \nphase transitions; \nphysical property tensors; \nprototype phases; \nsoft modes; \nsuperconductors; \ntensor parameter","PeriodicalId":338076,"journal":{"name":"International Tables for Crystallography","volume":"481 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-12-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Tables for Crystallography","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1107/97809553602060000915","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
Aspects of phase transitions in crystals that are of interest to crystallographers are described in this chapter. The chapter starts with a brief introduction aimed at defining the field of structural transitions and the terminology used. The theory of structural phase transitions is then described. This theory relates the symmetry characteristics of the transitions to their physical characteristics. The application of the symmetry principles that derive from this theory is illustrated by the results contained in Tables 3.1.3.1 and 3.1.4.1. The first of these two tables concerns the simple but experimentally widespread situation in which a structural transition is not accompanied by a change in the number of atoms per primitive crystal cell. The second table concerns the general case, in which the number of atoms changes, and which corresponds to the onset of superlattice reflections at the phase transition. This table provides, for a set of hypothetical transformations, the various symmetry-based predictions of the theory. The important topic of soft modes, which is related to the microscopic mechanism of a structural transition, is then discussed. The final section of the chapter is an introduction to the accompanying software package Group Informatics.
Keywords:
Curie temperature;
Landau theory;
Landau–Devonshire theory;
domain states;
enantiomorphism;
equitranslational phase transitions;
equitranslational subgroups;
ferroelastic materials;
ferroelastic phases;
ferroelastic transitions;
ferroelectric materials;
ferroelectric phases;
ferroelectric transitions;
ferroic classes;
ferroic domain states;
ferroic phases;
ferroic single-domain states;
ferroic symmetry;
ferroic transitions;
free energy;
high-symmetry phases;
high-temperature superconductors;
irreducible representations;
low-symmetry phases;
non-equitranslational phase transitions;
order parameter;
parent phases;
parent symmetry;
phase transitions;
physical property tensors;
prototype phases;
soft modes;
superconductors;
tensor parameter