{"title":"The heat capacity of high-purity dysprosium from 0.5 to 20 K","authors":"R. W. Hill, K. Gschneidner","doi":"10.1088/0305-4608/18/12/006","DOIUrl":null,"url":null,"abstract":"Measurements have been made on a two single-crystal specimens of high purity dysprosium. After heat treatment to remove hydrogen, the specimens give identical results. Analysis shows that there may still be small (1%) effects due to hydrogen, and this is the main cause of uncertainty in the deduced values of the electronic specific heat coefficient gamma =4.9+or-0.1 mJ K-2 mol-1 and the Debye temperature in the low temperature limit theta 0=192+or-2 K. At the higher temperatures the magnetic contribution accounts for about half the total specific heat, and its temperature dependence can be represented by an expression of the form AT\" exp(-Eg/kT). For n=1.5 it is found that Eg=26 K, but other pairs of n and Eg fit equally well.","PeriodicalId":16828,"journal":{"name":"Journal of Physics F: Metal Physics","volume":"22 1","pages":"2545-2557"},"PeriodicalIF":0.0000,"publicationDate":"1988-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics F: Metal Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0305-4608/18/12/006","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
Measurements have been made on a two single-crystal specimens of high purity dysprosium. After heat treatment to remove hydrogen, the specimens give identical results. Analysis shows that there may still be small (1%) effects due to hydrogen, and this is the main cause of uncertainty in the deduced values of the electronic specific heat coefficient gamma =4.9+or-0.1 mJ K-2 mol-1 and the Debye temperature in the low temperature limit theta 0=192+or-2 K. At the higher temperatures the magnetic contribution accounts for about half the total specific heat, and its temperature dependence can be represented by an expression of the form AT" exp(-Eg/kT). For n=1.5 it is found that Eg=26 K, but other pairs of n and Eg fit equally well.