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Dielectric resonator antenna

About: Dielectric resonator antenna is a research topic. Over the lifetime, 8199 publications have been published within this topic receiving 111090 citations. The topic is also known as: DRA.


Papers
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Journal ArticleDOI
TL;DR: In this article, a frequency-tunable superconducting coplanar waveguide resonator with a tuning range of half a gigahertz and a switching time of 1 ns is presented.
Abstract: We demonstrate a frequency-tunable superconducting coplanar waveguide resonator, with a tuning range of half a gigahertz and a switching time of 1 ns. The resonator is made tunable by inserting a superconducting quantum interference device in the center strip of the resonator. Quantum measurements are made by probing the resonator with a superconducting qubit, allowing us to use microwave photon Fock states to benchmark the resonator performance. Using the resonator, we shuttle energy quanta between the qubit and a microscopic two-level state. The tunable resonator can, therefore, serve as a communication bus or memory element in a prototype quantum processor.

78 citations

Journal ArticleDOI
TL;DR: In this article, a low profile stacked dielectric resonator antenna (DRA) and a microstrip metasurface (MS) antenna are investigated and compared in this communication.
Abstract: A low profile stacked dielectric resonator antenna (DRA) and a microstrip metasurface (MS) antenna are investigated and compared in this communication. It has been found that very similar radiation performance including resonant modes, reflection coefficients, boresight gains, and radiation patterns can be obtained between them, indicating that the dielectric superstrate of stacked DRA plays analogous role with MS in enhancing the antenna bandwidth and realized gain. Based on this observation, a broadband, low profile, and high gain filtering cylindrical stacked DRA is inspired by an MS-based filtering antenna. Four resonant modes including the higher order HEM $_{31\delta }$ mode and HEM $_{13\delta }$ mode are simultaneously excited in the DRA to provide a broad bandwidth of 61.4% and a peak gain of 11.4 dBi within passband, whereas a shorting via and two pairs of transverse stubs are introduced into the feeding microstrip line to generate radiation nulls in stopband and realize filtering function. Second harmonic suppression has been achieved without increasing the footprint of the antenna, and an out-of-band suppression of more than 23 dB is obtained within the wide stopband.

78 citations

Journal ArticleDOI
TL;DR: In this paper, a microwave planar resonator with a very high quality factor is presented for sensing applications, which uses an active feedback loop with a microwave amplifier to generate negative resistance to compensate the resonator's loss and increases the loaded quality factor of the system.
Abstract: A microwave planar resonator with a very high quality factor is presented for sensing applications. The proposed resonator uses an active feedback loop with a microwave amplifier to generate negative resistance to compensate the resonator's loss and increases the loaded quality factor of the system. This high quality resonator is based on a planar microstrip resonator with a primary quality factor of 200. The active loop technique increases the primary quality factor up to 15,480 with no other material in its surrounding environment when measured at 1.55 GHz resonance frequency. The high quality factor of the designed resonator provides very high resolution for detection of permittivity variation in its ambient environment with a theoretical resolution of 0.1 ppb (10−10). It is experimentally demonstrated that the small permittivity variations such as that of foam (with permittivity very close to air) can be detected. The circuit demonstrated a resolution of 26 dB in amplitude for a 1 MHz variation in the frequency domain.

78 citations

Patent
Michael Dydyk1, John R. Welling1
29 Jun 1995
TL;DR: In this article, a temperature compensated resonator (15) was proposed, which has a substrate (110) including a cavity (120, 160) and a resonator layer (150).
Abstract: A temperature compensated resonator (15) and method for making the temperature compensated resonator (15) The temperature compensated resonator (15) has a substrate (110) including a cavity (120, 160) and a resonator layer (150) A bonding medium (159, 160) couples the substrate (110) to the resonator layer (150) The resonator layer (150) is bonded atop the cavity (120, 160) A conductor (215) is included on the resonator layer (150) The conductor (215) heats the resonator layer (150) in response to a current passing through the conductor (215)

78 citations

Patent
12 Oct 1990
TL;DR: In this paper, a CO 2 slab waveguide laser with a pair of spaced apart electrodes having exposed light reflecting surfaces is described, where the electrodes are dimensioned in a manner to guide light in a plane perpendicular to the reflecting surfaces.
Abstract: A CO 2 slab waveguide laser (10) disclosed including a pair of spaced apart electrodes (36,38) having exposed light reflecting surfaces. The electrodes are dimensioned in a manner to guide light in a plane perpendicular to the reflecting surfaces. Light parallel to the reflecting surfaces is not constrained other than by the resonator mirrors (30,32). The resonator structure includes a negative branch unstable resonator in the nonwaveguide dimension. A stable resonator is used in the waveguide dimension but the mirror spacing from the end of the guide is based in part on the configuration of the unstable resonator. A unique support structure is disclosed for maintaining the electrodes in a spaced apart orientation without confining the discharge. Further refinements are disclosed for cooling the laser and for accommodating thermal expansion of the parts. Finally, an improved adjustable mirror assembly (26, 28) is provided which allows the tilt angle of the mirror to be varied from outside of the housing.

78 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
2023101
2022273
2021181
2020224
2019254
2018247