A. Takamizawa, S. Yanagimachi, T. Tanabe, K. Hagimoto, I. Hirano, K. Watabe, T. Ikegami, J. Hartnett
{"title":"Development of the cesium fountain frequency standard, NMIJ-F2","authors":"A. Takamizawa, S. Yanagimachi, T. Tanabe, K. Hagimoto, I. Hirano, K. Watabe, T. Ikegami, J. Hartnett","doi":"10.1109/EFTF.2014.7331518","DOIUrl":null,"url":null,"abstract":"We have made much progress on NMIJ-F2, which is our second cesium fountain frequency standard aiming an uncertainty of <; 1×10<sup>-15</sup> as an immediate goal. The frequency stability is improved to 8.3×10<sup>-14</sup>τ<sup>-1/2</sup> (τ: averaging time) by applying a cryogenic sapphire oscillator using a pulse-tube cryocooler as a local oscillator and optically pumping the atoms to the Zeeman sublevel mF = 0. Then, the homogeneous magnetic field in the interrogation region is obtained with magnetic shielding, a long solenoid coil, and two additional coils. The fractional frequency correction for the 2nd-order Zeeman shift is evaluated to be -165.5×10<sup>-15</sup>. Moreover, the fractional frequency correction for the collisional shift (the frequency shift due to collisions between cold atoms) is measured to be (+3.3±0.5)×10<sup>-15</sup> by an extrapolation method.","PeriodicalId":129873,"journal":{"name":"2014 European Frequency and Time Forum (EFTF)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2014-06-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2014 European Frequency and Time Forum (EFTF)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/EFTF.2014.7331518","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
We have made much progress on NMIJ-F2, which is our second cesium fountain frequency standard aiming an uncertainty of <; 1×10-15 as an immediate goal. The frequency stability is improved to 8.3×10-14τ-1/2 (τ: averaging time) by applying a cryogenic sapphire oscillator using a pulse-tube cryocooler as a local oscillator and optically pumping the atoms to the Zeeman sublevel mF = 0. Then, the homogeneous magnetic field in the interrogation region is obtained with magnetic shielding, a long solenoid coil, and two additional coils. The fractional frequency correction for the 2nd-order Zeeman shift is evaluated to be -165.5×10-15. Moreover, the fractional frequency correction for the collisional shift (the frequency shift due to collisions between cold atoms) is measured to be (+3.3±0.5)×10-15 by an extrapolation method.