1. Technical Field
The present disclosure relates to electromagnetic bandgap (EBG) structures, and particularly to a stacked EBG structure with more and wider stopbands.
2. Description of Related Art
The EBG structure 1 of related art, such as that shown in
The via 40 has a self-inductance. The ground plane 10 and the EBG layer 20 have a predetermined capacitance. A stopband center frequency of the EBG structure 1 changes depending on the self-inductance and the capacitance. However, the EBG structure 1 of related art can supply only stopbands in a limited number and with limited operating frequencies.
Therefore, it is desirable to provide a stacked EBG structure with more and wider stopbands.
Many aspects of the present disclosure can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure.
Embodiments of the present disclosure will be described with reference to the drawings.
The first ground plane 100, the first power plane 200, the second power plane 300, and the via 400 form a first EBG structure 101. The first ground plane 100, the second ground plane 500, the third power plane 600 and the ground vias 700 form a second EBG structure 102. The first EBG structure 101 and the second EBG structure 102 have different stopband bandwidths. Furthermore, the ground vias 700 have guard ring characteristics, thus achieving an increase in stopband bandwidth in the stacked EBG structure 1′.
A vertical axis represents a power noise coupling coefficient S21 and a horizontal axis represents a frequency. A dotted line S1 represents results when a power noise coupling coefficient S21 is measured in frequency domain when the first EBG structure 101 is employed. A dotted line S2 represents results when a power noise coupling coefficient S21 is measured in frequency domain when the second EBG structure 102 is employed. A full line S3 represents results when a power noise coupling coefficient S21 is measured in frequency domain when the stacked EBG structure 1′ is employed.
The full line S3 shows that the stacked EBG structure 1′ provides stopbands having a wider frequency band compared with the first structure 101 and the second structure 102.
It will be understood that the above particular embodiments are shown and described by way of illustration only. The principles and the features of the present disclosure may be employed in various and numerous embodiments thereof without departing from the scope of the disclosure. The above-described embodiments illustrate the possible scope of the disclosure but do not restrict the scope of the disclosure.
Number | Date | Country | Kind |
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102111336 A | Mar 2013 | TW | national |
Number | Name | Date | Kind |
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8595924 | McKinzie, III | Dec 2013 | B2 |
20130003333 | Toyao et al. | Jan 2013 | A1 |
Number | Date | Country | |
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20140291007 A1 | Oct 2014 | US |