2020
DOI: 10.1103/physreva.102.053503
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Comparative study on epsilon-near-zero transparent conducting oxides: High-order chromatic dispersions and modeling of ultrashort pulse interactions

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Cited by 16 publications
(8 citation statements)
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“…As shown in Figure 2, it is obvious that the real 𝑅𝑒(𝜀) of the permittivity of the ENZ wavelength (𝜆 = 1550 nm) vanishes and the imaginary đŒđ‘š(𝜀) is 0. The parameters of the AZO film are derived from the literature [8], where Δ ∞ = 3.8 is the high-frequency permittivity, Îł = 9.71 × 10 15 rad‱s −1 is the Drude damping rate, ω p = 2.3765 × 10 15 rad‱s −1 is the plasma frequency, ω is the angular frequency of the incident light, n is the carrier concentration, e =1.602 × 10 −19 C is the electron charge, Δ 0 is the permittivity of free space, ” is the electron mobility, m e = 0.38m is the effective electron mass [29] and m is the electron mass. As shown in Figure 2, it is obvious that the real Re(Δ) of the permittivity of the ENZ wavelength (λ ENZ = 1550 nm) vanishes and the imaginary Im(Δ) is 0.3.…”
Section: Methodsmentioning
confidence: 99%
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“…As shown in Figure 2, it is obvious that the real 𝑅𝑒(𝜀) of the permittivity of the ENZ wavelength (𝜆 = 1550 nm) vanishes and the imaginary đŒđ‘š(𝜀) is 0. The parameters of the AZO film are derived from the literature [8], where Δ ∞ = 3.8 is the high-frequency permittivity, Îł = 9.71 × 10 15 rad‱s −1 is the Drude damping rate, ω p = 2.3765 × 10 15 rad‱s −1 is the plasma frequency, ω is the angular frequency of the incident light, n is the carrier concentration, e =1.602 × 10 −19 C is the electron charge, Δ 0 is the permittivity of free space, ” is the electron mobility, m e = 0.38m is the effective electron mass [29] and m is the electron mass. As shown in Figure 2, it is obvious that the real Re(Δ) of the permittivity of the ENZ wavelength (λ ENZ = 1550 nm) vanishes and the imaginary Im(Δ) is 0.3.…”
Section: Methodsmentioning
confidence: 99%
“…ENZ materials exhibit a vanishing real part of permittivity in certain spectral ranges and strong localization of the field, which is a class of zero-refractive-index (NZI) materials [1][2][3][4][5] with a high nonlinear coefficient [6,7] and unprecedented ultrafast nonlinearity in the subwavelength propagation length. Al-doped zinc oxide (AZO) is an ideal ENZ material; it has a lower loss [8] and confines light better than indium tin oxide (ITO). However, the ENZ material only has a large nonlinear response in a relatively narrow spectral range and is sensitive to polarization, which limits its application.…”
Section: Introductionmentioning
confidence: 99%
“…2(b). It can be found that the peak absorption appears at the wavelength that maximizes the ratio of |Im(Δ ITO )|/|Re(Δ ITO )| 2 , near the communication wavelength, and it may be caused by the plasmon resonance of ITO near the ENZ point [42]. With the increase of the number of layers, the thickness of each layer decreases, and the whole multilayer structure shows better absorption effect due to the enhanced light scattering and the enhanced light localization caused by the multimode resonance effect [43], [44].…”
Section: Absorption Mechanisms Of Enz Multilayersmentioning
confidence: 99%
“…In the recent two decades, transparent conductive oxide (TCO) such as indium tin oxide (ITO) 11 , aluminum-doped zinc oxide (AZO) 12 , cadmium oxide (CdO) 13 have attracted considerable interest in epsilon-near-zero (ENZ) spectral region. Such media exhibit a vanishing permittivity at ENZ wavelength, giving rise to a series of new physical phenomena 14 , such as enhanced electric field 15 , large optical nonlinearity 11 , ultrashort pulse interaction 16 , etc., and advanced applications including electro-optical modulator 17 , 18 , all-optical switch 19 , perfect absorber 13 , etc. For all-optical switching, ENZ TCO materials also have several advantages, such as greater refractive index change by pump excitation, ultrafast response time 11 , and intraband optical excitation 13 .…”
Section: Introductionmentioning
confidence: 99%