{"title":"声子冷却热电子热计量混频器:最新研究成果综述","authors":"Gregory N. Gol’tsman, Eugene M. Gershenzon","doi":"10.1016/S0964-1807(99)00024-1","DOIUrl":null,"url":null,"abstract":"<div><p><span><span>The paper presents an overview of recent results for NbN phonon-cooled hot electron<span> bolometric (HEB) mixers. The noise temperature of the receivers based on both quasioptical and </span></span>waveguide versions of HEB mixer has crossed the level of 1</span> <!-->K·GHz<sup>−1</sup> at 430 GHz (410<!--> <!-->K) and 600–650 GHz (480<!--> <!-->K) and is close to this level at 820 GHz (1100<!--> <!-->K) and 900 GHz (980<!--> <span><span>K). The gain bandwidth measured for quasioptical HEB mixer at 620 GHz reached 4 GHz and the noise temperature bandwidth was almost 8 GHz. </span>Local oscillator power requirements are about 1 </span><em>μ</em><span>W for mixers made by photolithography and are about 100 nW for mixers made by </span><em>e</em><span>-beam lithography. The studies in terahertz receivers based on HEB superconducting mixers now present a dynamic, rapidly developing field.</span></p></div>","PeriodicalId":100110,"journal":{"name":"Applied Superconductivity","volume":"6 10","pages":"Pages 649-655"},"PeriodicalIF":0.0000,"publicationDate":"1999-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0964-1807(99)00024-1","citationCount":"4","resultStr":"{\"title\":\"Phonon-cooled hot-electron bolometric mixer: overview of recent results\",\"authors\":\"Gregory N. Gol’tsman, Eugene M. Gershenzon\",\"doi\":\"10.1016/S0964-1807(99)00024-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p><span><span>The paper presents an overview of recent results for NbN phonon-cooled hot electron<span> bolometric (HEB) mixers. The noise temperature of the receivers based on both quasioptical and </span></span>waveguide versions of HEB mixer has crossed the level of 1</span> <!-->K·GHz<sup>−1</sup> at 430 GHz (410<!--> <!-->K) and 600–650 GHz (480<!--> <!-->K) and is close to this level at 820 GHz (1100<!--> <!-->K) and 900 GHz (980<!--> <span><span>K). The gain bandwidth measured for quasioptical HEB mixer at 620 GHz reached 4 GHz and the noise temperature bandwidth was almost 8 GHz. </span>Local oscillator power requirements are about 1 </span><em>μ</em><span>W for mixers made by photolithography and are about 100 nW for mixers made by </span><em>e</em><span>-beam lithography. The studies in terahertz receivers based on HEB superconducting mixers now present a dynamic, rapidly developing field.</span></p></div>\",\"PeriodicalId\":100110,\"journal\":{\"name\":\"Applied Superconductivity\",\"volume\":\"6 10\",\"pages\":\"Pages 649-655\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1999-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/S0964-1807(99)00024-1\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Superconductivity\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0964180799000241\",\"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/S0964180799000241","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Phonon-cooled hot-electron bolometric mixer: overview of recent results
The paper presents an overview of recent results for NbN phonon-cooled hot electron bolometric (HEB) mixers. The noise temperature of the receivers based on both quasioptical and waveguide versions of HEB mixer has crossed the level of 1 K·GHz−1 at 430 GHz (410 K) and 600–650 GHz (480 K) and is close to this level at 820 GHz (1100 K) and 900 GHz (980 K). The gain bandwidth measured for quasioptical HEB mixer at 620 GHz reached 4 GHz and the noise temperature bandwidth was almost 8 GHz. Local oscillator power requirements are about 1 μW for mixers made by photolithography and are about 100 nW for mixers made by e-beam lithography. The studies in terahertz receivers based on HEB superconducting mixers now present a dynamic, rapidly developing field.