![]() Inguscio, Optical double-resonance spectroscopy of trapped Cs atoms: hyperfine structure of the 8s and 6d excited states. Kimble, Two-photon spectroscopy of the 6S 1/2-6D 5/2 transition of trapped atomic cesium. Yang, Investigation of the two-color polarization spectroscopy between the excited states based on cesium atoms. Wang, Narrow linewidth two-color polarization spectroscopy due to atomic coherence effect in a ladder-type atomic system. Weatherill, Polarization spectroscopy of an excited state transition. Wang, Double resonance optical pumping-polarization spectroscopy of an excited state transition. Adams, Coherent optical detection of highly excited Rydberg states using electromagnetically induced transparency. Wang, Electromagnetically induced transparency without a Doppler background in a multilevel ladder-type cesium atomic system. Wang, Measuring the hyperfine splitting and deriving the hyperfine interaction constants of the cesium 5p 67d 2D 5/2 excited state. Jia, Determination of hyperfine structure constants of 5D 5/2 and 7S 1/2 states of rubidium in cascade atomic system. Lindley, Hyperfine structure in the 6 2D 3/2 and 6 2D 5/2 states of 87Rb and 85Rb. Wang, Determination of the hyperfine structure constants of the 87Rb and 85Rb 4D 5/2 state and the isotope hyperfine anomaly. Suh, Hyperfine-structure-constant determination and absolute-frequency measurement of the Rb 4D 3/2 state. Kim, Double resonance optical pumping spectrum and its application for frequency stabilization of a laser diode. Minoshima, Doppler-free dual-comb spectroscopy of Rb using optical-optical double resonance technique, Opt. Tanner, Femtosecond frequency comb measurement of absolute frequencies and hyperfine coupling constants in cesium vapor. Bragdon, Measurement of the 6d 2D J hyperfine structure of cesium using resonant two-photon sub-Doppler spectroscopy. Williams, Absolute frequency measurement of the 6D 5/2 level of neutral 133Cs using two-photon spectroscopy. Suryanarayana, Hyperfine structure of the 7d 2D 3/2 level in cesium measured by Doppler-free two-photon spectroscopy, Phys. Suzuki, Doppler-free two-photon spectroscopy of 6S 1/2-6D 3/2,5/2 transition in cesium. Cheng, Absolute frequency of cesium 6S 1/2-6D 3/2 hyperfine transition with a precision to nuclear magnetic octupole interaction. Chui, Hyperfine coupling constants of cesium 7D states using two-photon spectroscopy. Wang, Measurement of the magnetic dipole hyperfine constant A hfs of cesium 7S 1/2 state. Yoon, Absolute frequency measurement of the 6s6p 1P 1-6s7s 1S 0 transition of 174Yb in a Yb hollow-cathode lamp. Dareau, Lifetime measurement of the cesium 5 2 D 5 / 2 state. Kanhaiya, Hyperfine measurement of the 6P 1/2 state in 87Rb using double resonance on blue and IR Transition. ![]() Ray, Exploring hyperfine levels of non-Rydberg excited states in a Ξ system using Autler-Townes splitting. Suryanarayana, Precision measurement of the hyperfine structure of 8d 2D 3/2 state of 133Cs by the radio-frequency phase modulation technique, Opt. Budker, Measurement of hyperfine structure and isotope shifts in the Dy 421 nm transition. Gupta, Hyperfine structure and lifetime measurements of the second-excited D states of rubidium and cesium by cascade fluorescence spectroscopy. A simple and self-calibration method of measuring the unknown hyperfine structure of an excited state using its own known hyperfine splitting of another state is demonstrated without the aid of any extra frequency calibration tools.Ĭ. With the measured values of hyperfine splitting, the hyperfine coupling constants of the 6D 5/2 state are determined as magnetic dipole A hfs = − 4.60 (5) MHz and electric quadrupole B hfs = 0.23 (47) MHz, which are consistent with previous results. The SAS as a frequency scale is used to measure the frequency intervals of hyperfine splitting of the 6D 5/2 excited state via the OODR spectra. Based on cesium 6S 1/2-6P 3/2-6D 5/2 (852 nm + 917 nm) ladder-type system, we simultaneously obtain the Doppler-free saturated absorption spectroscopy (SAS) between the 6S 1/2 → 6P 3/2 transition and optical–optical double resonance (OODR) spectroscopy between the 6P 3/2 → 6D 5/2 transition, when the frequency of 852 nm laser is scanned over the lower transition while keeping the 917 nm laser resonant on the upper transition.
0 Comments
Leave a Reply. |
AuthorWrite something about yourself. No need to be fancy, just an overview. ArchivesCategories |