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Volumn 77, Issue 3, 2008, Pages

Optomechanical trapping and cooling of partially reflective mirrors

Author keywords

[No Author keywords available]

Indexed keywords

COOLING; MIRRORS; PRESSURE EFFECTS; RADIATION;

EID: 40849114649     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.77.033819     Document Type: Article
Times cited : (209)

References (34)
  • 2
    • 33750595448 scopus 로고    scopus 로고
    • NATUAS 0028-0836 10.1038/nature05231
    • D. Kleckner and D. Bouwmeester, Nature (London) NATUAS 0028-0836 10.1038/nature05231 444, 75 (2006).
    • (2006) Nature (London) , vol.444 , pp. 75
    • Kleckner, D.1    Bouwmeester, D.2
  • 6
    • 34547927801 scopus 로고    scopus 로고
    • PRLTAO 0031-9007 10.1103/PhysRevLett.99.073601
    • M. Bhattacharya and P. Meystre, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.99.073601 99, 073601 (2007).
    • (2007) Phys. Rev. Lett. , vol.99 , pp. 073601
    • Bhattacharya, M.1    Meystre, P.2
  • 8
    • 11144232978 scopus 로고    scopus 로고
    • NATUAS 0028-0836 10.1038/nature03118
    • C. H. Metzger and K. Karrai, Nature (London) NATUAS 0028-0836 10.1038/nature03118 432, 1002 (2004).
    • (2004) Nature (London) , vol.432 , pp. 1002
    • Metzger, C.H.1    Karrai, K.2
  • 11
    • 40849084395 scopus 로고    scopus 로고
    • Stabilization is usually implemented using electronic feedback, but all-optical stabilization has also been achieved. From this perspective our proposal for the 3MC offers an interesting way to control instabilities purely optically.
    • Stabilization is usually implemented using electronic feedback, but all-optical stabilization has also been achieved. From this perspective our proposal for the 3MC offers an interesting way to control instabilities purely optically.
  • 12
    • 40849087042 scopus 로고    scopus 로고
    • We clarify that in passive cooling experiments-as opposed to cold damping experiments-the low-frequency part of the "error" signal is fed back to lock the cavity while the high frequency part is used to acquire the noise spectrum of the mirror. The force due to electronic feedback thus degrades quickly outside the low-frequency bandwidth ωb which is much smaller than the effective response frequency of the mirror ωeff. At ωeff the radiation effects thus dominate the feedback force, leading to the mentioned asymmetric optical potential.
    • We clarify that in passive cooling experiments-as opposed to cold damping experiments-the low-frequency part of the "error" signal is fed back to lock the cavity while the high frequency part is used to acquire the noise spectrum of the mirror. The force due to electronic feedback thus degrades quickly outside the low-frequency bandwidth ωb which is much smaller than the effective response frequency of the mirror ωeff. At ωeff the radiation effects thus dominate the feedback force, leading to the mentioned asymmetric optical potential.
  • 15
    • 0035477942 scopus 로고    scopus 로고
    • PYLAAG 0375-9601 10.1016/S0375-9601(01)00550-3
    • F. Ya. Khalili, Phys. Lett. A PYLAAG 0375-9601 10.1016/S0375-9601(01) 00550-3 288, 251 (2001).
    • (2001) Phys. Lett. A , vol.288 , pp. 251
    • Ya. Khalili, F.1
  • 19
    • 0000294788 scopus 로고
    • SCIEAS 0036-8075 10.1126/science.209.4456.547
    • V. B. Braginsky, Y. I. Vorontsov, and K. S. Thorne, Science SCIEAS 0036-8075 10.1126/science.209.4456.547 209, 547 (1980).
    • (1980) Science , vol.209 , pp. 547
    • Braginsky, V.B.1    Vorontsov, Y.I.2    Thorne, K.S.3
  • 21
    • 0022152057 scopus 로고
    • IEJQA7 0018-9197 10.1109/JQE.1985.1072577
    • W. J. Fader, IEEE J. Quantum Electron. IEJQA7 0018-9197 10.1109/JQE.1985.1072577 21, 1838 (1985).
    • (1985) IEEE J. Quantum Electron. , vol.21 , pp. 1838
    • Fader, W.J.1
  • 22
    • 40849098335 scopus 로고
    • IEJQA7 0018-9197 10.1109/JQE.1986.1073104
    • W. Weng Chow, IEEE J. Quantum Electron. IEJQA7 0018-9197 10.1109/JQE.1986.1073104 22, 1174 (1986).
    • (1986) IEEE J. Quantum Electron. , vol.22 , pp. 1174
    • Weng Chow, W.1
  • 23
    • 2542479058 scopus 로고    scopus 로고
    • PLRAAN 1050-2947 10.1103/PhysRevA.69.033811
    • S. Wieczorek and W. W. Chow, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.69.033811 69, 033811 (2004).
    • (2004) Phys. Rev. A , vol.69 , pp. 033811
    • Wieczorek, S.1    Chow, W.W.2
  • 24
    • 40849093395 scopus 로고    scopus 로고
    • We also note that the experimental arrangement corresponding to this model is that of the 3MC irradiated from both sides, unlike Fig. 1. In this case both end mirrors have a small transmissivity Tend (Table 1).
    • We also note that the experimental arrangement corresponding to this model is that of the 3MC irradiated from both sides, unlike Fig. 1. In this case both end mirrors have a small transmissivity Tend (Table 1).
  • 30
    • 33745333599 scopus 로고
    • PLRAAN 1050-2947 10.1103/PhysRevA.35.5288
    • E. X. DeJesus and C. Kaufman, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.35.5288 35, 5288 (1987).
    • (1987) Phys. Rev. A , vol.35 , pp. 5288
    • Dejesus, E.X.1    Kaufman, C.2
  • 31
    • 0001493516 scopus 로고    scopus 로고
    • PRLTAO 0031-9007 10.1103/PhysRevLett.83.3174
    • P. F. Cohadon, A. Heidmann, and M. Pinard, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.83.3174 83, 3174 (1999).
    • (1999) Phys. Rev. Lett. , vol.83 , pp. 3174
    • Cohadon, P.F.1    Heidmann, A.2    Pinard, M.3
  • 33
    • 1542349755 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.68.155311
    • E. K. Irish and K. Schwab, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.68.155311 68, 155311 (2003).
    • (2003) Phys. Rev. B , vol.68 , pp. 155311
    • Irish, E.K.1    Schwab, K.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.