{"title":"YBCO中塞贝克系数的量子理论","authors":"S. Fujita, A. Suzuki","doi":"10.5772/INTECHOPEN.86378","DOIUrl":null,"url":null,"abstract":"The measured in-plane thermoelectric power (Seebeck coefficient) S ab in YBCO below the superconducting temperature T c ( (cid:1) 94 K) S ab is negative and T -independent. This is shown to arise from the fact that the “ electrons ” (minority carriers) having heavier mass contribute more to the thermoelectric power. The measured out-of-plane thermoelectric power S c rises linearly with the temperature T . This arises from moving bosonic pairons (Cooper pairs), the Bose-Einstein condensation (BEC) of which generates a supercurrent below T c . The center of mass of pairons moves as bosons. The resistivity ρ ab above T c has T -linear and T -quadratic components, the latter arising from the Cooper pairs being scattered by phonons.","PeriodicalId":124160,"journal":{"name":"Advanced Thermoelectric Materials for Energy Harvesting Applications","volume":"25 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Quantum Theory of the Seebeck Coefficient in YBCO\",\"authors\":\"S. Fujita, A. Suzuki\",\"doi\":\"10.5772/INTECHOPEN.86378\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The measured in-plane thermoelectric power (Seebeck coefficient) S ab in YBCO below the superconducting temperature T c ( (cid:1) 94 K) S ab is negative and T -independent. This is shown to arise from the fact that the “ electrons ” (minority carriers) having heavier mass contribute more to the thermoelectric power. The measured out-of-plane thermoelectric power S c rises linearly with the temperature T . This arises from moving bosonic pairons (Cooper pairs), the Bose-Einstein condensation (BEC) of which generates a supercurrent below T c . The center of mass of pairons moves as bosons. The resistivity ρ ab above T c has T -linear and T -quadratic components, the latter arising from the Cooper pairs being scattered by phonons.\",\"PeriodicalId\":124160,\"journal\":{\"name\":\"Advanced Thermoelectric Materials for Energy Harvesting Applications\",\"volume\":\"25 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-05-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advanced Thermoelectric Materials for Energy Harvesting Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.5772/INTECHOPEN.86378\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Thermoelectric Materials for Energy Harvesting Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5772/INTECHOPEN.86378","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
在YBCO中,在超导温度T c ((cid:1) 94 K)以下测得的面内热电功率(塞贝克系数)S ab为负且与T无关。这是由于具有更大质量的“电子”(少数载流子)对热电功率的贡献更大。测得的面外热电功率sc随温度T线性上升。这是由运动的玻色子对(库珀对)引起的,玻色子-爱因斯坦凝聚(BEC)产生低于T c的超电流。对子的质心像玻色子一样运动。T c以上的电阻率ρ ab具有T线性分量和T二次分量,后者是由库珀对被声子散射引起的。
The measured in-plane thermoelectric power (Seebeck coefficient) S ab in YBCO below the superconducting temperature T c ( (cid:1) 94 K) S ab is negative and T -independent. This is shown to arise from the fact that the “ electrons ” (minority carriers) having heavier mass contribute more to the thermoelectric power. The measured out-of-plane thermoelectric power S c rises linearly with the temperature T . This arises from moving bosonic pairons (Cooper pairs), the Bose-Einstein condensation (BEC) of which generates a supercurrent below T c . The center of mass of pairons moves as bosons. The resistivity ρ ab above T c has T -linear and T -quadratic components, the latter arising from the Cooper pairs being scattered by phonons.