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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.
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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.
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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
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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 M. Kretschmann and A. A. Maradudin, Phys. Rev. B 66, 245408 (2002). 10.1103/PhysRevB.66.245408
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