Shanta, N. Li, Ghulam Hussain, X. Zhao and X. F. Sun
{"title":"反铁磁化合物MBaYb(BO3)2 (M = K, Na)的结构、磁性和各向异性磁热学性质","authors":"Shanta, N. Li, Ghulam Hussain, X. Zhao and X. F. Sun","doi":"10.1039/D5TC00518C","DOIUrl":null,"url":null,"abstract":"<p >In this study, high-quality single crystals of MBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> (where M = K, Na) were successfully grown using the self-flux technique. The structural, anisotropic magnetic, and magnetocaloric properties of KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> and NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> were comprehensively studied through X-ray diffraction (XRD), isothermal magnetization, anisotropy susceptibility response, and specific heat tests. The powder X-ray diffraction scan of the crushed as-grown crystal confirms that both compounds crystallize in a trigonal symmetry, classified under the <em>R</em><img><em>m</em> (no. 166) space group, but they exhibit distinct structural arrangements. The temperature-dependent anisotropic susceptibility and specific heat data for KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> and NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> show no evidence of long-range magnetic ordering down to 2 K, suggesting paramagnetic behavior in the low-temperature regime. Furthermore, using Maxwell's equations, the calculated magnetic entropy change (−Δ<em>S</em><small><sub>m</sub></small>) attains a highest value of 7.7 J mol<small><sup>−1</sup></small> K<small><sup>−1</sup></small> for KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> with a change in applied field from 0 to 7 T at 2 K, while for NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> it is 7.0 J mol<small><sup>−1</sup></small> K<small><sup>−1</sup></small>. Additionally, KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> exhibits an adiabatic temperature change (−Δ<em>T</em><small><sub>ad</sub></small>) of 3.4 K, compared to 1.6 K for NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small>, under a field change from 0 to 7 T. The MBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> (where M = K, Na) could be strong candidates for magnetic coolant in the cryogenic temperature range, as indicated by a notable magnetic entropy change in the magnetocaloric effect (MCE) parameters, which is comparable to or even exceeds that of well-known magnetic refrigerants.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" 24","pages":" 12317-12328"},"PeriodicalIF":5.1000,"publicationDate":"2025-05-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Structural, magnetic, and anisotropic magnetocaloric properties in antiferromagnetic compounds MBaYb(BO3)2 (M = K, Na)\",\"authors\":\"Shanta, N. Li, Ghulam Hussain, X. Zhao and X. F. Sun\",\"doi\":\"10.1039/D5TC00518C\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >In this study, high-quality single crystals of MBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> (where M = K, Na) were successfully grown using the self-flux technique. The structural, anisotropic magnetic, and magnetocaloric properties of KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> and NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> were comprehensively studied through X-ray diffraction (XRD), isothermal magnetization, anisotropy susceptibility response, and specific heat tests. The powder X-ray diffraction scan of the crushed as-grown crystal confirms that both compounds crystallize in a trigonal symmetry, classified under the <em>R</em><img><em>m</em> (no. 166) space group, but they exhibit distinct structural arrangements. The temperature-dependent anisotropic susceptibility and specific heat data for KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> and NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> show no evidence of long-range magnetic ordering down to 2 K, suggesting paramagnetic behavior in the low-temperature regime. Furthermore, using Maxwell's equations, the calculated magnetic entropy change (−Δ<em>S</em><small><sub>m</sub></small>) attains a highest value of 7.7 J mol<small><sup>−1</sup></small> K<small><sup>−1</sup></small> for KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> with a change in applied field from 0 to 7 T at 2 K, while for NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> it is 7.0 J mol<small><sup>−1</sup></small> K<small><sup>−1</sup></small>. Additionally, KBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> exhibits an adiabatic temperature change (−Δ<em>T</em><small><sub>ad</sub></small>) of 3.4 K, compared to 1.6 K for NaBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small>, under a field change from 0 to 7 T. The MBaYb(BO<small><sub>3</sub></small>)<small><sub>2</sub></small> (where M = K, Na) could be strong candidates for magnetic coolant in the cryogenic temperature range, as indicated by a notable magnetic entropy change in the magnetocaloric effect (MCE) parameters, which is comparable to or even exceeds that of well-known magnetic refrigerants.</p>\",\"PeriodicalId\":84,\"journal\":{\"name\":\"Journal of Materials Chemistry C\",\"volume\":\" 24\",\"pages\":\" 12317-12328\"},\"PeriodicalIF\":5.1000,\"publicationDate\":\"2025-05-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Materials Chemistry C\",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2025/tc/d5tc00518c\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Materials Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/tc/d5tc00518c","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
Structural, magnetic, and anisotropic magnetocaloric properties in antiferromagnetic compounds MBaYb(BO3)2 (M = K, Na)
In this study, high-quality single crystals of MBaYb(BO3)2 (where M = K, Na) were successfully grown using the self-flux technique. The structural, anisotropic magnetic, and magnetocaloric properties of KBaYb(BO3)2 and NaBaYb(BO3)2 were comprehensively studied through X-ray diffraction (XRD), isothermal magnetization, anisotropy susceptibility response, and specific heat tests. The powder X-ray diffraction scan of the crushed as-grown crystal confirms that both compounds crystallize in a trigonal symmetry, classified under the Rm (no. 166) space group, but they exhibit distinct structural arrangements. The temperature-dependent anisotropic susceptibility and specific heat data for KBaYb(BO3)2 and NaBaYb(BO3)2 show no evidence of long-range magnetic ordering down to 2 K, suggesting paramagnetic behavior in the low-temperature regime. Furthermore, using Maxwell's equations, the calculated magnetic entropy change (−ΔSm) attains a highest value of 7.7 J mol−1 K−1 for KBaYb(BO3)2 with a change in applied field from 0 to 7 T at 2 K, while for NaBaYb(BO3)2 it is 7.0 J mol−1 K−1. Additionally, KBaYb(BO3)2 exhibits an adiabatic temperature change (−ΔTad) of 3.4 K, compared to 1.6 K for NaBaYb(BO3)2, under a field change from 0 to 7 T. The MBaYb(BO3)2 (where M = K, Na) could be strong candidates for magnetic coolant in the cryogenic temperature range, as indicated by a notable magnetic entropy change in the magnetocaloric effect (MCE) parameters, which is comparable to or even exceeds that of well-known magnetic refrigerants.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors