C. Fink, S. Watkins, T. Aramaki, P. Brink, S. Ganjam, B. Hines, M. Huber, N. Kurinsky, N. Kurinsky, R. Mahapatra, N. Mirabolfathi, W. Page, R. Partridge, M. Platt, M. Pyle, B. Sadoulet, B. Serfass, S. Zuber
{"title":"未来单光声子和红外光子探测器的TES功率噪声表征","authors":"C. Fink, S. Watkins, T. Aramaki, P. Brink, S. Ganjam, B. Hines, M. Huber, N. Kurinsky, N. Kurinsky, R. Mahapatra, N. Mirabolfathi, W. Page, R. Partridge, M. Platt, M. Pyle, B. Sadoulet, B. Serfass, S. Zuber","doi":"10.1063/5.0011130","DOIUrl":null,"url":null,"abstract":"In this letter, we present the performance of a $100~\\mu\\mathrm{m}\\times 400~\\mu\\mathrm{m} \\times 40~\\mathrm{nm}$ tungsten (W) Transition-Edge Sensor (TES) with a critical temperature of 40 mK. This device has a measured noise equivalent power (NEP) of $1.5\\times 10^{-18}\\ \\mathrm{W}/\\sqrt{\\mathrm{Hz}}$, in a bandwidth of $2.6$ kHz, indicating a resolution for Dirac delta energy depositions of $40\\pm 5~\\mathrm{meV}$ (rms). The performance demonstrated by this device is a critical step towards developing a $\\mathcal{O}(100)~\\mathrm{meV}$ threshold athermal phonon detectors for low-mass dark matter searches.","PeriodicalId":8827,"journal":{"name":"arXiv: Instrumentation and Detectors","volume":"6 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-04-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"18","resultStr":"{\"title\":\"Characterizing TES power noise for future single optical-phonon and infrared-photon detectors\",\"authors\":\"C. Fink, S. Watkins, T. Aramaki, P. Brink, S. Ganjam, B. Hines, M. Huber, N. Kurinsky, N. Kurinsky, R. Mahapatra, N. Mirabolfathi, W. Page, R. Partridge, M. Platt, M. Pyle, B. Sadoulet, B. Serfass, S. Zuber\",\"doi\":\"10.1063/5.0011130\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this letter, we present the performance of a $100~\\\\mu\\\\mathrm{m}\\\\times 400~\\\\mu\\\\mathrm{m} \\\\times 40~\\\\mathrm{nm}$ tungsten (W) Transition-Edge Sensor (TES) with a critical temperature of 40 mK. This device has a measured noise equivalent power (NEP) of $1.5\\\\times 10^{-18}\\\\ \\\\mathrm{W}/\\\\sqrt{\\\\mathrm{Hz}}$, in a bandwidth of $2.6$ kHz, indicating a resolution for Dirac delta energy depositions of $40\\\\pm 5~\\\\mathrm{meV}$ (rms). The performance demonstrated by this device is a critical step towards developing a $\\\\mathcal{O}(100)~\\\\mathrm{meV}$ threshold athermal phonon detectors for low-mass dark matter searches.\",\"PeriodicalId\":8827,\"journal\":{\"name\":\"arXiv: Instrumentation and Detectors\",\"volume\":\"6 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-04-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"18\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv: Instrumentation and Detectors\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/5.0011130\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv: Instrumentation and Detectors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/5.0011130","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Characterizing TES power noise for future single optical-phonon and infrared-photon detectors
In this letter, we present the performance of a $100~\mu\mathrm{m}\times 400~\mu\mathrm{m} \times 40~\mathrm{nm}$ tungsten (W) Transition-Edge Sensor (TES) with a critical temperature of 40 mK. This device has a measured noise equivalent power (NEP) of $1.5\times 10^{-18}\ \mathrm{W}/\sqrt{\mathrm{Hz}}$, in a bandwidth of $2.6$ kHz, indicating a resolution for Dirac delta energy depositions of $40\pm 5~\mathrm{meV}$ (rms). The performance demonstrated by this device is a critical step towards developing a $\mathcal{O}(100)~\mathrm{meV}$ threshold athermal phonon detectors for low-mass dark matter searches.