Analysis and Design of Ultra Thin Electromagnetic Absorbers Comprising Resistively Loaded High Impedance Surfaces
By Filippo Costa, Agostino Monorchio, Giuliano Manara. IEEE Transactions on Antennas and Propagation, 2010
738 citations recorded by the source corpus.
High-impedance surfaces (HIS) comprising lossy frequency selective surfaces (FSS) are employed to design thin electromagnetic absorbers. The structure, despite its typical resonant behavior, is able to perform a very wideband absorption in a reduced thickness. Losses in the frequency selective surface are introduced by printing the periodic pattern through resistive inks and hence avoiding the typical soldering of a large number of lumped resistors. The effect of the surface resistance of the FSS and dielectric substrate characteristics on the input impedance of the absorber is discussed by means of a circuital model. It is shown that the optimum value of surface resistance is affected both by substrate parameters (thickness and permittivity) and by FSS element shape. The equivalent circuit model is then used to introduce the working principles of the narrowband and the wideband absorbing structure and to derive the best-suited element for wideband absorption.
Subfields: Aerospace Engineering, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/9aa24a8db2c797a8186676f2f8bdcb8bc04ee2b1
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Citations in the corpus
- Optical absorbers based on strong interference in ultra‐thin films (2016, background): “isbury screens [5], in which a resistive sheet is placed a quarter wavelength above a ground plane, and related structures such as Jaumann absorbers [6] and resistively loaded high impedance surfaces [7] [8], have been used for minimizing the radar cross-section of objects for stealth technology [9]”
- A Circuit-Based Model for the Interpretation of Perfect Metamaterial Absorbers (2012, background): “through zero of the imaginary part [3].”
- A Chipless RFID Based on Multiresonant High-Impedance Surfaces (2013, methodology): “When the resonance condition of the HIS structure is fulfilled [25], the real part of simplifies as follows [21]:”
- An Overview of Equivalent Circuit Modeling Techniques of Frequency Selective Surfaces and Metasurfaces (2014, background): “Nowadays, FSSs [19], [20] are employed at microwave frequencies for designing frequency selective radomes [21], leaky wave/Fabry-Perot, low-profile and low-RCS antennas [22]-[24], reflectarays, trasmittarrays and lenses [25], [26], polarization converting surfaces [27], waveguide filters [28], elect”
- Design of a Tunable Low-Frequency and Broadband Radar Absorber Based on Active Frequency Selective Surface (2016, background): “and absorbers based on resistive FSS [7], [8] are quite ef-”
- A Frequency Selective Radome With Wideband Absorbing Properties (2012, methodology): “Such lumped value leads to different distributed surface resistances depending on the filling factor of the FSS element [16].”
- 3-D Frequency Selective Rasorber: Concept, Analysis, and Design (2016, methodology): “In the past, an FSR was realized by cascading a lossy array of Jaumann or circuit analog absorber [8] and a lossless FSS [9], where the transmission characteristic was provided by the conventional FSSs, while the absorption is achieved by the lossy array, such as resistive cross dipoles [10], [11], ”
- Polarization-Independent and Ultrawideband Metamaterial Absorber Using a Hexagonal Artificial Impedance Surface and a Resistor-Capacitor Layer (2014, background): “Another approach for a broadband absorber is a lossy pattern, which is created from a resistive ink [16], [18]–[20].”
- On the Design of Single-Layer Circuit Analog Absorber Using Double-Square-Loop Array (2013, methodology): “A resistive square loop was used in [10] as the unit cell of a wide-band absorber and the theoretically realized bandwidth is 112%with a thickness of .”
- Frequency-Selective Rasorber With Interabsorption Band Transparent Window and Interdigital Resonator (2018, background): “The traditional resistive sheet in CAA designs [24]–[26] can only be equivalent to a series RLC circuit, which cannot”