{"title":"单电子晶体管的噪声特性","authors":"A.N. Tavkhelidze, J. Mygind","doi":"10.1016/S0964-1807(98)00085-4","DOIUrl":null,"url":null,"abstract":"<div><p>We have measured the low frequency (5<!--> <!-->mHz<<em>f</em><30<!--> <!-->Hz) noise in current biased aluminium single electron tunneling (SET) transistors. A refined high frequency (HF) shielding allows us to maintain and study a given background charge configuration for many hours at <em>T</em><100 mK. At frequencies below 10<!--> <!-->Hz the noise is mainly due to charge traps, and the noise pattern superimposed on the <em>V</em>(<em>V</em><sub>g</sub><span><span>)-curve strongly depends on the particular background charge configuration resulting from the cooling sequence and the applied RF irradiation, including </span>thermal radiation from the 4.2</span> <!-->K environment. The noise spectra, which show both 1/<em>f</em> and 1/<em>f</em><sup>1/</sup><sup>2</sup> dependencies and saturate at <em>f</em><100<!--> <!-->mHz can be fitted by two-level fluctuators (TLF) with Debye–Lorentz spectra and relaxation times on the order of seconds.</p></div>","PeriodicalId":100110,"journal":{"name":"Applied Superconductivity","volume":"6 7","pages":"Pages 399-403"},"PeriodicalIF":0.0000,"publicationDate":"1998-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0964-1807(98)00085-4","citationCount":"0","resultStr":"{\"title\":\"Noise Properties of Single Electron Transistors\",\"authors\":\"A.N. Tavkhelidze, J. Mygind\",\"doi\":\"10.1016/S0964-1807(98)00085-4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We have measured the low frequency (5<!--> <!-->mHz<<em>f</em><30<!--> <!-->Hz) noise in current biased aluminium single electron tunneling (SET) transistors. A refined high frequency (HF) shielding allows us to maintain and study a given background charge configuration for many hours at <em>T</em><100 mK. At frequencies below 10<!--> <!-->Hz the noise is mainly due to charge traps, and the noise pattern superimposed on the <em>V</em>(<em>V</em><sub>g</sub><span><span>)-curve strongly depends on the particular background charge configuration resulting from the cooling sequence and the applied RF irradiation, including </span>thermal radiation from the 4.2</span> <!-->K environment. The noise spectra, which show both 1/<em>f</em> and 1/<em>f</em><sup>1/</sup><sup>2</sup> dependencies and saturate at <em>f</em><100<!--> <!-->mHz can be fitted by two-level fluctuators (TLF) with Debye–Lorentz spectra and relaxation times on the order of seconds.</p></div>\",\"PeriodicalId\":100110,\"journal\":{\"name\":\"Applied Superconductivity\",\"volume\":\"6 7\",\"pages\":\"Pages 399-403\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/S0964-1807(98)00085-4\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Superconductivity\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0964180798000854\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0964180798000854","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
We have measured the low frequency (5 mHz<f<30 Hz) noise in current biased aluminium single electron tunneling (SET) transistors. A refined high frequency (HF) shielding allows us to maintain and study a given background charge configuration for many hours at T<100 mK. At frequencies below 10 Hz the noise is mainly due to charge traps, and the noise pattern superimposed on the V(Vg)-curve strongly depends on the particular background charge configuration resulting from the cooling sequence and the applied RF irradiation, including thermal radiation from the 4.2 K environment. The noise spectra, which show both 1/f and 1/f1/2 dependencies and saturate at f<100 mHz can be fitted by two-level fluctuators (TLF) with Debye–Lorentz spectra and relaxation times on the order of seconds.