I. Introduction
With the growing popularity of wireless communication, radio frequency (RF) devices are covering more and more frequencies to cater for either additional bandwidth requirements or new applications [1]–[10]. Although there are national standards for maximum electromagnetic interference (EMI) and radio power ratings for each device, the large numbers of RF devices working in close proximity suffer from radio interference. Besides, there are increasing concerns about the effects of extensive electromagnetic exposure to humans. This is particularly true for vulnerable patients and newborn babies in hospital environments. Therefore, there is considerable interest in selective RF shielding and researchers are striving to develop new materials and designs to shield the electromagnetic waves. For example, high-performance shielding materials, capable of absorbing the EM wave, have been widely studied in the past few decades [11]–[14]. However, the absorption of these materials is frequency insensitive, which means that both wanted and unwanted frequencies of EM waves are shielded. Moreover, the absorbed EM waves are converted into heat, which is not conducive to many applications. Frequency-selective surface (FSS) reflector, on the contrary, provides selective shielding where unwanted frequency bands are reflected and other bands are allowed to pass through. FSS has been widely used in a radar radome design, special filtering, electromagnetic shielding, and many other fields [15]–[17]. Novel fabrication techniques, such as screen printing with conductive ink, are also providing FSS with flexibility and transparency for new applications [18]–[22]. With flexibility and transparency, FSS can provide EM shielding for unconventional mediums and applications. For example, a newborn incubator in a hospital or a glass window in a car or home can reflect the unwanted EM waves without losing the glass transparency.