摘要We propose an experimental scheme of vacuum ultraviolet (VUV) and extreme ultraviolet (XUV) optical frequency standards with noble gas atoms. Considering metastable state 3P2 noble atoms pumped by a conventional discharging method, the atomic beam is collimated with transverse laser cooling at the metastable state and enters into the laser cavity in the proposed setup. Due to stimulated emission from the metasable state to the ground state inside the laser cavity consisting of VUV reflection coating mirrors, our calculations show that with enough population inversion to compensate for the cavity loss, an active optical frequency standard at VUV and XUV is feasible.
Abstract:We propose an experimental scheme of vacuum ultraviolet (VUV) and extreme ultraviolet (XUV) optical frequency standards with noble gas atoms. Considering metastable state 3P2 noble atoms pumped by a conventional discharging method, the atomic beam is collimated with transverse laser cooling at the metastable state and enters into the laser cavity in the proposed setup. Due to stimulated emission from the metasable state to the ground state inside the laser cavity consisting of VUV reflection coating mirrors, our calculations show that with enough population inversion to compensate for the cavity loss, an active optical frequency standard at VUV and XUV is feasible.
[1] Jiang Y Y, Ludlow A D, Lemke N D, Fox R W, Sherman J A, Ma L S and Oates C W 2011 Nature Photon. 5 158
[2] Katori H 2011 Nature Photon. 5 203
[3] Swallows M D, Bishof M, Lin Y, blatt S, Martin M J, Rey A M and Ye J 2011 Science 331 1043
[4] Chou C W, Hume D B, Koelemeij J C J, Wineland D J and Rosenband T 2010 Phys. Rev. Lett. 104 070802
[5] Liu Q, Huang Y, Cao J, Ou B Q, Guo B, Guan H, Huang X R and Gao K L 2011 Chin. Phys. Lett. 28 013201
[6] Kandula D Z, Gohle C, Pinkert T J, Ubachs W and Eikema K S E 2010 Phys. Rev. Lett. 105 063001
[7] Yost D C, Schibli T R, Ye J, Tate J L, Hostetter J, Gaarde M B and Schafer K J 2009 Nature Phys. 5 815
[8] Gohle C, Udem T, Herrmann M, Rauschenberger J, Holzwarth R, Schuessler H A, Krausz F and Hänsch T W 2005 Nature 436 14
[9] Jones R J, Moll K D, Thorpe M J and Ye J 2005 Phys. Rev. Lett. 94 193201
[10] Herrmann M, Haas M, Jentschura U D, Kottmann F, Leibfried D , Saathoff G, Gohle C, Ozawa A, Batteiger V, Knuenz S, Kolachevsky N, Schuessler H A, Hänsch T W and Udem Th 2009 Phys. Rev. A 79 052505
[11] An K, Childs J J, Dasari R R and Feld M S 1994 Phys. Rev. Lett. 73 25
[12] Chen J and Chen X 2005 Proceedings of the IEEE International Frequency Control Symposium and Exposition (Vancouver, Canada 29–31 August 2005) p 608
[13] Chen J 2009 Chin. Sci. Bull. 54 348
[14] Yu D and Chen J 2008 Phys. Rev. A 78 013846
[15] Meiser D, Ye J, Carlson D R and Holland M J 2009 Phys. Rev. Lett. 102 163601
[16] Zhuang W and Chen J 2010 Proceedings of the IEEE International Frequency Control Symposium (Newport Beach, California, USA 2–4 June 2010) p 222
[17] Meiser D and Holland M J 2010 Phys. Rev. A 81 033847
[18] An K and Feld M S 1997 Phys. Rev. A 56 1662
[19] Zinner M and Spoden P, Kraemer T, Gerhard B and Ertmer W 2003 Phys. Rev. A 67 010501(R)
[20] Lefers J, Miller N, Rupke D, Tong D and Walhout M 2002 Phys. Rev. A 66 012507
[21] Kuppens S J M, Tempelaars J G C, Mogendorff V P , Claessens B J, Beijerinck H C W and Vredenbregt E J D 2002 Phys. Rev. A 65 023410
[22] Kuppens S J M et al 1994 Phys. Rev. Lett. 73 3815