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Volumn 113, Issue 26, 2014, Pages

Large suppression of quantum fluctuations of light from a single emitter by an optical nanostructure

Author keywords

[No Author keywords available]

Indexed keywords

ELECTROMAGNETIC FIELDS; HYBRID SYSTEMS; NANOSTRUCTURES; QUANTUM ELECTRONICS; SHOT NOISE;

EID: 84937680097     PISSN: 00319007     EISSN: 10797114     Source Type: Journal    
DOI: 10.1103/PhysRevLett.113.263605     Document Type: Article
Times cited : (33)

References (46)
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    • Walls, D.F.1
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    • P. Grünwald and W. Vogel, Phys. Rev. A 88, 023837 (2013). PLRAAN 1050-2947 10.1103/PhysRevA.88.023837
    • (2013) Phys. Rev. A , vol.88 , pp. 023837
    • Grünwald, P.1    Vogel, W.2
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    • See Supplemental Material at, which includes Refs. [20-33], for a detailed derivation, a discussion of the homodyne detection scheme, and a comparison to different systems
    • See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevLett.113.263605, which includes Refs. [20-33], for a detailed derivation, a discussion of the homodyne detection scheme, and a comparison to different systems.
  • 28
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    • L. Mandel, Phys. Rev. Lett. 49, 136 (1982). PRLTAO 0031-9007 10.1103/PhysRevLett.49.136
    • (1982) Phys. Rev. Lett. , vol.49 , pp. 136
    • Mandel, L.1
  • 29
    • 0005338158 scopus 로고
    • W. Vogel, Phys. Rev. Lett. 67, 2450 (1991). PRLTAO 0031-9007 10.1103/PhysRevLett.67.2450
    • (1991) Phys. Rev. Lett. , vol.67 , pp. 2450
    • Vogel, W.1
  • 34
    • 84999589798 scopus 로고    scopus 로고
    • Besides (Equation presented), the cosine in Eq. (2) contains the phase (Equation presented) determined by the driving laser and the coherence operator. Additional phase factors arise in a homodyne scheme for the detection of squeezing and allow for setting the cosine to unity (see Sec. S3 of the Supplemental Material [19]). We impose this condition throughout the numerical evaluations
    • Besides (Equation presented), the cosine in Eq. (2) contains the phase (Equation presented) determined by the driving laser and the coherence operator. Additional phase factors arise in a homodyne scheme for the detection of squeezing and allow for setting the cosine to unity (see Sec. S3 of the Supplemental Material [19]). We impose this condition throughout the numerical evaluations.
  • 39
    • 84999541055 scopus 로고    scopus 로고
    • The condition for squeezing, i.e., (Equation presented) in Eq. (2), sets an upper limit for the driving field intensity, (Equation presented). Notice that this requirement cannot be fulfilled for (Equation presented), which already occurs for pure dephasing larger that half the spontaneous decay rate
    • The condition for squeezing, i.e., (Equation presented) in Eq. (2), sets an upper limit for the driving field intensity, (Equation presented). Notice that this requirement cannot be fulfilled for (Equation presented), which already occurs for pure dephasing larger that half the spontaneous decay rate.


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