2015
DOI: 10.1016/j.optmat.2015.01.001
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Photoexcited broadband blueshift tunable perfect terahertz metamaterial absorber

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Cited by 20 publications
(14 citation statements)
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“…3(b) and 3(d) that the electric field is distributed not only on both inner ends of the square ring but also on the adjacent area between the unit cell; the y component of the magnetic field gathers in the middle and both sides of the STO dielectric layer, which indicates that there exists two kinds of different magnetic dipole resonance. Referring to the similar report [28,29] , we deduce that the resonance absorption at high frequency f m2 is caused by a new coupled mode, which combines the fundamental electromagnetic dipole mode with the electromagnetic mode caused by the neighboring square ring. We will discuss this in detail later when analyzing the influence of the geometric parameter.…”
supporting
confidence: 58%
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“…3(b) and 3(d) that the electric field is distributed not only on both inner ends of the square ring but also on the adjacent area between the unit cell; the y component of the magnetic field gathers in the middle and both sides of the STO dielectric layer, which indicates that there exists two kinds of different magnetic dipole resonance. Referring to the similar report [28,29] , we deduce that the resonance absorption at high frequency f m2 is caused by a new coupled mode, which combines the fundamental electromagnetic dipole mode with the electromagnetic mode caused by the neighboring square ring. We will discuss this in detail later when analyzing the influence of the geometric parameter.…”
supporting
confidence: 58%
“…3(c). The resonant phenomenon at low frequency f m1 is the fundamental electromagnetic dipole resonance that appeared in some literature [15,21,[27][28][29] . As for the frequency f m2 , it can be seen from Figs.…”
mentioning
confidence: 99%
“…Recent progress in the passive tuning by the incorporation of naturally occurring materials within or as part of the metamaterial elements has recently been reported. For example, metamaterials have been tuned by loading dielectrics onto their surface and also by integrating semiconductors or carbon nanotubes within the structure to provide electronic or optical control of the resonance frequency [16][17][18][19][20]. Some designers used the methods of using the thermal control to realize the tunability, some were based on a variation of temperature altering the intrinsic carrier density in a semiconductor (InSb) [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Some designers used the methods of using the thermal control to realize the tunability, some were based on a variation of temperature altering the intrinsic carrier density in a semiconductor (InSb) [21,22]. Others used the photoexcited carrier by integrating semiconductors into metamaterial designs [19,20,23] and also someone used the property of ferrimagnetic/paramagnetic transition of the M A N U S C R I P T A C C E P T E D ACCEPTED MANUSCRIPT ferrites [24]. In addition to the magnetically tunable metamaterial is also a more effective way, some of them used the ferromagnetic precession of ferrite [25] , and others used the ferromagnetic resonance (FMR) frequency which can be influenced by the dimension of the ferrites [26].…”
Section: Introductionmentioning
confidence: 99%
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