2019
DOI: 10.1109/tap.2019.2922778
|View full text |Cite
|
Sign up to set email alerts
|

Exceptional Points of Degeneracy in Periodic Coupled Waveguides and the Interplay of Gain and Radiation Loss: Theoretical and Experimental Demonstration

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
35
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
6
2

Relationship

6
2

Authors

Journals

citations
Cited by 48 publications
(35 citation statements)
references
References 46 publications
0
35
0
Order By: Relevance
“…One issue that must be considered when implementing this design in the gigahertz frequency range and above, is the decrease of inductor quality factor with increasing frequency, especially in the integrated circuit technology where inductor Q is only 20–30. An obvious workaround the inductor low Q e limitation is the elimination of all lumped elements by means of implementation of the unit cell with degeneracy condition in another technology, such as microstrip or waveguide where there is no need for lumped elements [14, 16, 43, 44]. As previously mentioned, the simple lumped element structure of this paper already mimics the RF/microwave distributed TL model and, with minor alteration, can easily be translated to a different technology such as TLs, and more specifically microstrip waveguides.…”
Section: Conclusion and Remarksmentioning
confidence: 99%
“…One issue that must be considered when implementing this design in the gigahertz frequency range and above, is the decrease of inductor quality factor with increasing frequency, especially in the integrated circuit technology where inductor Q is only 20–30. An obvious workaround the inductor low Q e limitation is the elimination of all lumped elements by means of implementation of the unit cell with degeneracy condition in another technology, such as microstrip or waveguide where there is no need for lumped elements [14, 16, 43, 44]. As previously mentioned, the simple lumped element structure of this paper already mimics the RF/microwave distributed TL model and, with minor alteration, can easily be translated to a different technology such as TLs, and more specifically microstrip waveguides.…”
Section: Conclusion and Remarksmentioning
confidence: 99%
“…In this paper, we present an example of a DBE oscillator based on two periodic, coupled transmission lines (CTLs) as in one of the configurations proposed in [20] and shown in Fig. 1(a).…”
Section: Introductionmentioning
confidence: 99%
“…In order to quantify the coalescence of the eigenvectors we use the concept of "coalescence parameter" introduced in [22] for the DBE and in [4] for the SIP. Here, we use a coalescence parameter σ defined similarly to that in [4].…”
Section: A Analytic Dispersion Relation For An Sipmentioning
confidence: 99%
“…Here, θ mn is the angle between two 6-dimensional complex vectors ψ m , ψ n , which is defined as stated in equation ( 16) using the inner product < ψ i |ψ j >= ψ † i ψ j with the dagger symbol † representing the complex conjugate transpose operation and ψ m denotes the norm of ψ m [4]. In this paper, we calculate the coalescence parameter using the norm based on the euclidean distance between the parameters θ mn , ∀m, n, and zero, [23], instead of using the arithmetic average used in [4,22]. The reason for this change is that the optimization algorithm converges faster using the euclidean distance than the arithmetic average, as long as the algorithm does not generate a lot of points far from the optimization goal (known as outliers) [24].…”
Section: A Analytic Dispersion Relation For An Sipmentioning
confidence: 99%