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IEEE International Multitopic Conference (INMIC)

A detector-coupled resonant cavity and instrumentation design for studies in cavity quantum electrodynamics and GHz/THz RF systems

M. H. S. Bukhari

Published Dec 1, 2014• 0 citations
Publisher

Abstract

The design of a hi-Q resonant RF cavity with coupled detection scheme and associated instrumentation is reported for studying quantum vacuum within the framework of Quantum Electrodynamics (QED), the quantum theory of interaction of matter with radiation. Although this system could possibly serve in any general QED, cavity QED and RF applications in the range of a few GHz, the design was specifically devised for an experiment in studying intrinsic noise in quantum vacuum owing to vacuum fluctuations, which we call “Eavesdropping on Vacuum”. The center frequency of the cavity is 2.75GHz (which may be modified slightly to around 2.5GHz band for use in contemporary WiLAN and WiFi RF applications), with a high Q value. Initial design is made using copper but in the next stage it will be replaced with Niobium for use in low-temperature (around 0.1-0.3K) studies, making it an SRF (Superconducting Radio Frequency) cavity. A carefully devised scheme of sensitive RF detectors and ultra-low-noise cryogenic Low-Noise Amplifiers (cLNA) is an integral part of the cavity system. Detection element is an array of cavity-backed Au or Au-NbN spiral antennas in association with GaAs Schottky Barrier Diodes (SBD's), in conjunction with GaAs/InP HEMT's working in the GHz to THz regime. External fields are achieved with the help of time-dependent RF fields delivered to the cavity with the help of an antenna coupled with a GaAs Resonant Tunneling Diode (RTD). In addition to the cavity design, this report presents an overview of the detection scheme as well as necessary instrumentation, including RF detection, amplification, and the DAQ (Data Acquisition) required for digital read-out.

DOI
10.1109/inmic.2014.7096900

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The design of a hi-Q resonant RF cavity with coupled detection scheme and associated instrumentation is reported for studying quantum vacuum within the framework of Quantum Electrodynamics (QED), the quantum theory of interaction of matter with radiation. Although this system could possibly serve in any general QED, cavity QED and RF applications in the range of a few GHz, the design was specifically devised for an experiment in studying intrinsic noise in quantum vacuum owing to vacuum fluctuations, which we call “Eavesdropping on Vacuum”. The center frequency of the cavity is 2.75GHz (which may be modified slightly to around 2.5GHz band for use in contemporary WiLAN and WiFi RF applications), with a high Q value. Initial design is made using copper but in the next stage it will be replaced with Niobium for use in low-temperature (around 0.1-0.3K) studies, making it an SRF (Superconducting Radio Frequency) cavity. A carefully devised scheme of sensitive RF detectors and ultra-low-noise cryogenic Low-Noise Amplifiers (cLNA) is an integral part of the cavity system. Detection element is an array of cavity-backed Au or Au-NbN spiral antennas in association with GaAs Schottky Barrier Diodes (SBD's), in conjunction with GaAs/InP HEMT's working in the GHz to THz regime. External fields are achieved with the help of time-dependent RF fields delivered to the cavity with the help of an antenna coupled with a GaAs Resonant Tunneling Diode (RTD). In addition to the cavity design, this report presents an overview of the detection scheme as well as necessary instrumentation, including RF detection, amplification, and the DAQ (Data Acquisition) required for digital read-out.
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Three-dimensional radio frequency cavities demonstrate excellent frequency selectivity and, as such, are known for their use in RF filters. These cavities have potential applications in quantum information science, precision displacement metrology, and quantum electrodynamics. Additionally, coupled cavities that form a spectral doublet allow for parametric gain when incorporating mechanical elements. Here, we investigate normal-mode splitting in a pair of quarter-wave stub microwave cavities at room temperature and cryogenic environments in order to identify coupling mechanics for normal and superconducting systems. Superconducting quarter-wave stub cavities with a resonant frequency of 10 GHz are made from reactor-grade niobium and exhibit Q ranging from 105 to 109. We varied cavity-to-cavity coupling to observe several normal-mode splittings of increasing peak separation until we observed a mode crossing. The minimum observed peak separation was 7 MHz for room temperature tests and 200 kHz for cryogenic tests. We also report on values of an intrinsic quality factor for the tuning cavity as a dielectric rod is translated along its symmetry axis. The realization of coupled superconducting radio frequency (SRF) cavities of this type is a necessary step toward implementation of parametric SRF-mechanical gain.
Radio frequency (RF) signals are frequently used in emerging quantum applications due to their spin state manipulation capability. Efficient coupling of RF signals into a particular quantum system requires the utilization of carefully designed and fabricated antennas. Nitrogen vacancy (NV) defects in diamond are commonly utilized platforms in quantum sensing experiments with the optically detected magnetic resonance (ODMR) method, where an RF antenna is an essential element. We report on the design and fabrication of high efficiency coplanar RF antennas for quantum sensing applications. Single and double ring coplanar RF antennas were designed with -37 dB experimental return loss at 2.87 GHz, the zero-field splitting frequency of the negatively charged NV defect in diamond. The efficiency of both antennas was demonstrated in magnetic field sensing experiments with NV color centers in diamond. An RF amplifier was not needed, and the 0 dB output of a standard RF signal generator was adequate to run the ODMR experiments due to the high efficiency of the RF antennas.
Abstract Here we consider a tunable superconducting cavity that can be used either as a tunable coupler to a qubit inside the cavity or as a tunable low noise, low temperature, RF filter. Our design consists of an array of radio-frequency superconducting quantum interference devices (rf SQUIDs) inside a superconducting cavity. This forms a tunable metamaterial structure which couples to the cavity through its magnetic plasma frequency. By tuning the resonant frequency of the metamaterial through an applied magnetic flux, one can tune the cavity mode profile. This allows us to detune the cavity initially centered at 5.593 GHz by over 200 MHz. The maximum quality factor approaches that of the empty cavity, which is 4.5 × 106. The metamaterial electromagnetic response is controlled via a low-frequency or dc magnetic flux bias, and we present a control line architecture that is capable of applying sufficient magnetic flux bias with minimal parasitic coupling. Together this design allows for an in-situ tunable cavity which enables low-temperature quantum control applications.
We propose a new detection technique based on radio-frequency (RF) bias and readout of an antenna-coupled superconducting nanobolometer. This approach is suitable for Frequency-Division-Multiplexing (FDM) readout of large arrays using broadband low-noise RF amplifier. We call this new detector RFTES. This feasibility study was made on demonstrator devices which are made in all-Nb technology and operate at 4.2 K. The studied RFTES devices consist of an antenna-coupled superconducting nanobolometer made of ultrathin niobium films with transition temperature Tc = 5.2 K. The 0.65-THz antenna and nanobolometer are embedded as a load into a GHz-range coplanar niobium resonator (Tc = 8.9 K, Q = 4000). To heat the superconducting Nb nanobolometer close to the Tc, the RF power at resonator frequency f = 5.8 GHz is applied via a transmission line which is weakly coupled (-11 dB) to the loaded resonator. The THz-antenna of RFTES was placed in the focus of a sapphire immersion lens inside a He4-cryostat equipped with an optical window and a semiconductor RF amplifier. We have demonstrated optical response of the RFTES to THz radiation. The demonstrator receiver system employing the RFTES device showed an optical Noise-Equivalent Power (NEP) 1e-14 W/sqrt(Hz) at 4.2 K.
The combination of an ion trap with a high finesse optical cavity is an ideal system for the investigation of strong coupling cavity quantum electrodynamics, and allows the observation of a number of interesting quantum phenomena. To achieve the small mode volumes required without impairing the ion trapping small traps with a short ion electrode distance are needed. Two microscopic linear rf ion traps have been developed and built to accommodate experimental cavities of lengths of several 100 microns. The first trap design, the 'sandwich' trap, was successfully used to trap 40Ca+ - ions for several hours. It was characterised extensively including a measurement of the heating rates of the ions in the trap. Spectroscopy measurements of the cooling transition, as well as the two repumping transitions were carried out. The second trap design, the 'alumina' trap, also successfully trapped 40Ca+ - ions, and a full characterisation of this trap was made. The experimental cavity was installed at a preliminary cavity length distance of 3.7 mm. The cavity characteristics were examined. Finally the trapped ions were overlapped with the cavity mode by adjusting the trap minimum position along the trap axis via dc voltages and the vertical position of the cavity. To progress further a locking scheme for the cavity length as well as a single - photon detection setup are necessary. To achieve strong coupling a reduction of the cavity length will have to be made.