Hom damped high-frequency resonator
View Patent ↗A HOM attenuated high frequency resonator provided with a cylindrical resonator cavity on the outer surface of which are arranged three circular tapered waveguides with two symmetrically arranged ridges each, the cut-off frequency of the waveguide base mode being kept constant over the length of the waveguides by varying the height of the ridges, and the ridge waveguides being provided at their end of the smaller diameter with an impedance transformer each for the broadband adjustment of the coaxial line is to be cost-efficiently manufacturable as a compact structure and is to be of improved attenuation properties while at the same time having, relative to prior art arrangements, a high shunt impedance for the fundamental modes.
1. A HOM attenuated high frequency resonator, comprising:
a cylindrical resonator cavity on the outer surface of which are arranged three circular tapered waveguides with two symmetrically arranged ridges each, a cut-off frequency of a waveguide base mode being kept constant over the length of the waveguides by varying the height of the ridges, and the waveguides being provided at an end of the waveguides having a smaller diameter with an impedance transformer each for a broadband adjustment of a coaxial line, wherein
the waveguides with two symmetrically arranged ridges for adjusting an asymmetry relative to a center plane of the cylindrical resonator cavity are arranged offset on the outer surface of the resonator cavity, and
the waveguides with the two symmetrically arranged ridges are structured for adjusting an angularity of the waveguides relative to an axis of the cylindrical resonator cavity and the ridges of the waveguides protrude into the cylindrical resonator cavity such that modes of higher order are optimally coupled.
2. The HOM attenuated resonator of claim 1 , wherein
the ridges of the waveguides are arranged parallel relative to the axis of the cylindrical resonator cavity.
3. The HOM attenuated resonator of claim 1 , wherein
the waveguides have a ridge height defined over the length of the waveguide by a second order polynomial
y= 3.6328+0.0347513 x+ 0.000183869 x 2 ,
wherein x is the length (in mm) of the tapered waveguide and y is half the spacing of the ridges (in mm) between each other.
4. The HOM attenuated resonator of claim 1 , wherein
each impedance transformer is provided with a section structured as the coaxial line.
5. The HOM attenuated resonator of claim 1 , wherein
the resonator cavity is provided with a beam hole of nose-shaped expansion for a concentration of an accelerating field on the axis of the cylindrical resonator cavity.