Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems

Abstract For relaxor-ferroelectrics and relaxor-ferromagnets, the initial Ehrenfest-classification gives no phase-transition that contradicts the measured order-parameter, while the classification according to order-parameter and its derivatives raises the question about the relationships between th...

Full description

Saved in:
Bibliographic Details
Main Authors: Lai Wei, Li-Li Zhang, Yi-Neng Huang
Format: Article
Language:English
Published: Nature Portfolio 2024-11-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-024-80454-7
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1850162865854480384
author Lai Wei
Li-Li Zhang
Yi-Neng Huang
author_facet Lai Wei
Li-Li Zhang
Yi-Neng Huang
author_sort Lai Wei
collection DOAJ
description Abstract For relaxor-ferroelectrics and relaxor-ferromagnets, the initial Ehrenfest-classification gives no phase-transition that contradicts the measured order-parameter, while the classification according to order-parameter and its derivatives raises the question about the relationships between the phase-transition and the specific-heat peak above and near the transition temperature. Here, based on the free-energy (F) of the thermodynamic limit systems when the external-field (h) tends 0, thermal equilibrium phase-transitions of thermodynamic limit systems with temperature (T) are reclassified into: (1) Discontinuous phase-transition. $$\partial F/\partial h|_{h \to 0}$$ and $$\partial F/\partial T|_{h \to 0}$$ have discontinuities in a T range; (2) Continuous phase-transition. $$\partial F/\partial h|_{h \to 0}$$ and $$\partial F/\partial T|_{h \to 0}$$ are continuous with T, while $$\partial^{2} F/\partial h\partial T|_{h \to 0}$$ and $$\partial^{2} F/\partial T^{2} |_{h \to 0}$$ have discontinuities at a T point; and (3) Diffuse phase-transition. $$\partial^{3} F/\partial h\partial^{2} T|_{h \to 0}$$ and $$\partial^{3} F/\partial T^{3} |_{h \to 0}$$ are continuous with T, while they are respectively equal to 0 at the transition-temperature (T d ) and diffuse-temperature (T s ). The diffuse-region of the phase-transition is $$T_{s} - T_{d}$$ and the diffuse-degree $$\left( {T_{s} - T_{d} } \right)/T_{d} \times {1}00\%$$ , naturally giving the relation of the phase-transition to the specific-heat peak.
format Article
id doaj-art-b2245a3486a94d2aa663ecb171fee037
institution OA Journals
issn 2045-2322
language English
publishDate 2024-11-01
publisher Nature Portfolio
record_format Article
series Scientific Reports
spelling doaj-art-b2245a3486a94d2aa663ecb171fee0372025-08-20T02:22:26ZengNature PortfolioScientific Reports2045-23222024-11-011411710.1038/s41598-024-80454-7Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systemsLai Wei0Li-Li Zhang1Yi-Neng Huang2Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal UniversityXinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal UniversityXinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal UniversityAbstract For relaxor-ferroelectrics and relaxor-ferromagnets, the initial Ehrenfest-classification gives no phase-transition that contradicts the measured order-parameter, while the classification according to order-parameter and its derivatives raises the question about the relationships between the phase-transition and the specific-heat peak above and near the transition temperature. Here, based on the free-energy (F) of the thermodynamic limit systems when the external-field (h) tends 0, thermal equilibrium phase-transitions of thermodynamic limit systems with temperature (T) are reclassified into: (1) Discontinuous phase-transition. $$\partial F/\partial h|_{h \to 0}$$ and $$\partial F/\partial T|_{h \to 0}$$ have discontinuities in a T range; (2) Continuous phase-transition. $$\partial F/\partial h|_{h \to 0}$$ and $$\partial F/\partial T|_{h \to 0}$$ are continuous with T, while $$\partial^{2} F/\partial h\partial T|_{h \to 0}$$ and $$\partial^{2} F/\partial T^{2} |_{h \to 0}$$ have discontinuities at a T point; and (3) Diffuse phase-transition. $$\partial^{3} F/\partial h\partial^{2} T|_{h \to 0}$$ and $$\partial^{3} F/\partial T^{3} |_{h \to 0}$$ are continuous with T, while they are respectively equal to 0 at the transition-temperature (T d ) and diffuse-temperature (T s ). The diffuse-region of the phase-transition is $$T_{s} - T_{d}$$ and the diffuse-degree $$\left( {T_{s} - T_{d} } \right)/T_{d} \times {1}00\%$$ , naturally giving the relation of the phase-transition to the specific-heat peak.https://doi.org/10.1038/s41598-024-80454-7
spellingShingle Lai Wei
Li-Li Zhang
Yi-Neng Huang
Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
Scientific Reports
title Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
title_full Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
title_fullStr Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
title_full_unstemmed Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
title_short Reclassification of thermal equilibrium phase-transitions in thermodynamic limit systems
title_sort reclassification of thermal equilibrium phase transitions in thermodynamic limit systems
url https://doi.org/10.1038/s41598-024-80454-7
work_keys_str_mv AT laiwei reclassificationofthermalequilibriumphasetransitionsinthermodynamiclimitsystems
AT lilizhang reclassificationofthermalequilibriumphasetransitionsinthermodynamiclimitsystems
AT yinenghuang reclassificationofthermalequilibriumphasetransitionsinthermodynamiclimitsystems