2016
DOI: 10.1088/0022-3727/49/42/425102
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Low frequency absorption properties of a thin metamaterial absorber with cross-array on the surface of a magnetic substrate

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Cited by 34 publications
(18 citation statements)
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“…At lower resonance frequencies at 4.2 GHz and 5.6 GHz, the top surface current is strong coupled along the edges of DSA. Thus, the strong induced electric field is created and it reverses to the incident electric field, which confirms the excited electric field is stronger than the incident electric field 27 . Therefore, the electric resonance is excited at 4.2 GHz and 5.6 GHz.…”
Section: Resultsmentioning
confidence: 61%
“…At lower resonance frequencies at 4.2 GHz and 5.6 GHz, the top surface current is strong coupled along the edges of DSA. Thus, the strong induced electric field is created and it reverses to the incident electric field, which confirms the excited electric field is stronger than the incident electric field 27 . Therefore, the electric resonance is excited at 4.2 GHz and 5.6 GHz.…”
Section: Resultsmentioning
confidence: 61%
“…The electric field distribution pattern reveals that as the electric field strength increases with frequency, so does the absorption. This effective induced electric field reverts to the electric field incident, which in turn energizes the electric field than the electric field incident 43 ensuring electrical resonance. The z-component of the E-field vector by using Maxwell’s Eqs.…”
Section: Surface Current E Field and H Field Distribution Of Maa Unit Cellmentioning
confidence: 99%
“…The electric field distribution pattern reveals that as the electric field strength increases with frequency, so does the absorption. This effective induced electric field reverts to the electric field incident, which in turn energizes the electric field than the electric field incident [37] ensuring electrical resonance. The z-component of the E-field vector by using Maxwell's Eqs.…”
Section: Surface Current E Field and H Field Of Maa Unit Cellmentioning
confidence: 99%