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Volumn 80, Issue 11, 2009, Pages

Integrated plasmonic waveguides: A mode solver based on density of states formulation

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EID: 70350578356     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.115419     Document Type: Article
Times cited : (45)

References (27)
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    • Ph.D. thesis, Facultes Universitaires Notre Dame de la Paix, Namur
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    • A slightly different definition is also possible. Writing δ (ky ′2 - ky2) =1/2 | ky | [δ (ky′ - ky) +δ (ky′ + ky)], we obtain ρ (ky2) =1/2 ky [ρ (ky) +ρ (- ky)] (ky >0). Moreover, ρ (- ky) =ρ (ky) since ± ky simply defines forward and backward propagations. This lead to Δρ (ky; ω) =g/2πΔ ky /2/ (ky - ky0) 2 + (Δ ky /2) 2 instead of Eq. 8 and a degeneracy g/2, excluding forward/backward propagation degeneracy.
    • A slightly different definition is also possible. Writing δ (ky ′2 - ky2) =1/2 | ky | [δ (ky′ - ky) +δ (ky′ + ky)], we obtain ρ (ky2) =1/2 ky [ρ (ky) +ρ (- ky)] (ky >0). Moreover, ρ (- ky) =ρ (ky) since ± ky simply defines forward and backward propagations. This lead to Δρ (ky; ω) =g/2πΔ ky /2/ (ky - ky0) 2 + (Δ ky /2) 2 instead of Eq. 8 and a degeneracy g/2, excluding forward/backward propagation degeneracy.
  • 16
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    • DOS can also be expressed in the frequency space for fixed momentum ky. Noticing that θ is a function of both ω and v= ky2, we use the identity | θ ω | v | ω v | θ | v θ | ω =-1 that leads to | θ ω | ky =- | v ω | v | θ v | ω =-2 ky / vg πΔ ρ (ky2; ω) =-π/ vg Δρ (ky; ω). A Taylor expansion near the resonance frequency ω0 gives then Δρ (ky; ω) g vg /πΔω/2/ (ω- ω0) 2 + (Δω/2) 2, with Δω=-2ImD (ω0; ky) / [ReD (ω; ky) /ω] (ω= ω0) =1/τ= vg / LSPP, and τ is the mode lifetime. See also 10.1103/PhysRevB.66.245408
    • DOS can also be expressed in the frequency space for fixed momentum ky. Noticing that θ is a function of both ω and v= ky2, we use the identity | θ ω | v | ω v | θ | v θ | ω =-1 that leads to | θ ω | ky =- | v ω | v | θ v | ω =-2 ky / vg πΔ ρ (ky2; ω) =-π/ vg Δρ (ky; ω). A Taylor expansion near the resonance frequency ω0 gives then Δρ (ky; ω) g vg /πΔω/2/ (ω- ω0) 2 + (Δω/2) 2, with Δω=-2ImD (ω0; ky) / [ReD (ω; ky) /ω] (ω= ω0) =1/τ= vg / LSPP, and τ is the mode lifetime. See also M. Kretschmann and A. A. Maradudin, Phys. Rev. B 66, 245408 (2002). 10.1103/PhysRevB.66.245408
    • (2002) Phys. Rev. B , vol.66 , pp. 245408
    • Kretschmann, M.1    Maradudin, A.A.2
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    • M. Paulus and O. J. F. Martin, Phys. Rev. E 63, 066615 (2001). 10.1103/PhysRevE.63.066615
    • (2001) Phys. Rev. e , vol.63 , pp. 066615
    • Paulus, M.1    Martin, O.J.F.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.