Microwave passive filters, which are widely used in many wireless communication systems, may be formed from a newtork or configuration of one or more resonators. A significant parameter for describing such a resonator is its Quality (Q) factor, which is defined as the ratio of the stored energy with the resonator divided by the amount of energy lost per cycle. A high Q factor indicates a relatively low level of damping.
Usually, the use of resonators with finite values of Q factor produces two major kinds of undesired features: the lack of flatness in the passband of the transmission parameter, and the increment of the insertion loss level. The insertion loss can be compensated with a subsequent amplification, but the main challenge lies in keeping a certain degree of flatness of the transmission coefficient along the passband.
Filter design is usually a tradeoff between the insertion loss, loss and group delay variation in the passband, isolation, physical dimensions and mass. In the case when additional offset in the insertion loss is tolerated, lossy or predistortion techniques can help to obtain a close to ideal frequency response (high selectivity, isolation and flat amplitude response in the passband) of the filter.
Predistortion and lossy filter techniques are commonly applied to improve the in-band flatness impacting (strongly in the predistortion case) the absolute insertion losses.
The present invention has been developed as a new methodolody to overcome the drawbacks mentioned above.
This is valid in applications where the in-band absolute insertion loss is not a critical parameter, such as in the channelizer or frequency converters, where -as long as the IL (Insertion Loss) is not excessive- it can be recovered by the gain of the LNA (Low Noise Amplifier) / PA (Programmable Amplilfier) without having impact on the system performance.
Moreover these approaches not only improve the filter performance but may also significantly reduce the size and mass of the physical filter, which in satellite applications are very critical considerations.
The present radio frequency passband filter consists of an array of different types of open-loop resonators in a non-transverse topology. The middle resonators are centrally loaded with resistors and with proper loading resistances, the passband flatness can be improved very effectively. The classical lossy technicque are based on either the resistive coupling between resonators or the non-uniform Q distribution in a transverse topology.