2018
DOI: 10.1080/09205071.2018.1435309
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Design of a high gain and high efficiency W-band folded waveguide TWT using phase-velocity taper

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Cited by 11 publications
(2 citation statements)
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“…11(b), because the phase synchronization condition is almost satisfied for the considered frequency band, i.e., β p ≈ β 0 over the shown band (relative band of 2.2% around 88GHz) in this example. Thus, the gain per period resulting from the amplification mode (solid red) is 20 log(e) × 0.027π ≈ 0.74 dB in this frequency range which is close to the small-signal gain 1 dB reported in [20] that was obtained by simulating the serpentine TWT amplifier at 90 GHz.…”
Section: Application To Serpentine-based Twt Amplifiersupporting
confidence: 81%
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“…11(b), because the phase synchronization condition is almost satisfied for the considered frequency band, i.e., β p ≈ β 0 over the shown band (relative band of 2.2% around 88GHz) in this example. Thus, the gain per period resulting from the amplification mode (solid red) is 20 log(e) × 0.027π ≈ 0.74 dB in this frequency range which is close to the small-signal gain 1 dB reported in [20] that was obtained by simulating the serpentine TWT amplifier at 90 GHz.…”
Section: Application To Serpentine-based Twt Amplifiersupporting
confidence: 81%
“…Serpentine SWSs have recently gained a lot of interest due to the growing importance of millimeter wave and terahertz frequencies in modern applications and also due to the advancement of fabrication technologies such as LIGA (LIthographie, Galvanoformung, Abformung). As an illustrative example, we use the same geometry of serpentine SWS discussed in [19], [20], as shown in 10(a). The serpentine waveguide is made of copper and has rectangular cross-section of dimensions a = 1.9 mm and b = 0.325 mm, bending radius of 0.325 mm (radius at half way between inner and outer radii), straight section length of 0.6 mm, beam tunneling radius of 0.175 mm.…”
Section: Application To Serpentine-based Twt Amplifiermentioning
confidence: 99%