Superconducting Parametric Amplifier Impedance Matching With CPW Stubs
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Solution Overview
Problem
Existing superconducting impedance matched Josephson parametric amplifiers have low yield, high manufacturing cost, and insufficient performance due to complex structure, sensitivity to parameters, and large dielectric capacitance insertion loss.
Innovation Solution
A method to determine superconducting impedance matched parametric amplifiers by calculating structural parameters based on environmental parameters, including center wavelength, gain, and bandwidth, to optimize impedance matching and reduce capacitance, using coplanar waveguides and stub dimensions for improved manufacturing yield and reduced loss.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If a superconducting impedance matched Josephson parametric amplifier is designed with traditional impedance matching structure, then impedance matching is achieved, but the structure becomes complex and manufacturing yield decreases
Solution Approach 1:
The patent extracts the traditional complex impedance matching network and replaces it with a simplified coplanar waveguide structure with optimized characteristic impedance. By removing unnecessary matching components and using direct coplanar waveguide connections with specific impedance values (e.g., 50Ω, 70.7Ω), the design achieves impedance matching without the complexity of traditional multi-component matching networks, thereby improving manufacturing yield while maintaining performance.
Solution Approach 2:
The patent changes the key parameter from structural complexity to electrical parameter optimization. Instead of using complex physical structures for impedance matching, the invention optimizes the characteristic impedance parameter of the coplanar waveguide (adjusting conductor width, spacing, and substrate properties) to achieve proper impedance matching. This parameter-based approach simplifies the structure and makes manufacturing more reliable.
2Reliability
If traditional dielectric capacitance is used in the parametric amplifier, then capacitance function is provided, but insertion loss increases and performance deteriorates
Solution Approach 1:
The patent substitutes traditional dielectric capacitance (which suffers from loss) with kinetic inductance-based capacitance simulation using superconducting coplanar waveguide structures. By using the kinetic inductance of superconducting materials to simulate capacitive behavior, the design eliminates dielectric losses while maintaining the required capacitance function, thereby reducing insertion loss and improving amplifier performance.
Solution Approach 2:
The patent employs composite superconducting structures (combining conductors, substrates, and oxidation layers) to create lossless capacitance simulation. The composite coplanar waveguide structure uses superconducting materials with specific properties to achieve both the capacitance function and minimal loss, replacing traditional lossy dielectric capacitors with a superconducting-based equivalent.
3Adaptability or versatility
If the parametric amplifier is designed for high bandwidth, then frequency range is expanded, but manufacturing precision requirements increase
Solution Approach 1:
The patent changes the design approach from precision-critical structural dimensions to parameter-optimized electrical characteristics. By focusing on optimizing the characteristic impedance parameter and kinetic inductance parameter rather than requiring precise mechanical dimensions, the design achieves high bandwidth with relaxed manufacturing tolerances. The coplanar waveguide geometry allows for parameter tuning that is less sensitive to fabrication variations.
4Reliability
If complex impedance matching structure is used, then impedance matching is improved, but manufacturing cost increases
Solution Approach 1:
The patent removes complex impedance matching components and networks from the design, replacing them with simplified coplanar waveguide structures. This extraction of unnecessary complexity directly reduces manufacturing cost by eliminating multiple fabrication steps, materials, and assembly operations while maintaining impedance matching performance through optimized waveguide impedance.
Solution Approach 2:
The patent merges the impedance matching function directly into the coplanar waveguide transmission line structure itself, rather than using separate matching networks. By combining the transmission and impedance matching functions into a single integrated structure, the design reduces component count and simplifies manufacturing, thereby lowering cost while maintaining performance.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
Enhances amplifier performance, increases yield, and lowers manufacturing costs by optimizing structural parameters for impedance matching, achieving high bandwidth and low insertion loss.
Implementation Method 1
calculates, based on the impedance value of the impedance matching line, a line width dimension of a coplanar waveguide of the superconducting impedance matched parametric amplifier
Implementation Method 2
calculates, based on the impedance value of the impedance matching line and the capacitance value of the amplifier, a stub dimension of the superconducting impedance matched parametric amplifier
Data Source
Figure 1~3
Figure 4~5A
Figure 5B~7C
AI summary
Provided in the present application are a determination method and apparatus for a superconducting impedance transformation parametric amplifier, a superconducting impedance transformation parametric amplifier, an electronic device, a computer program product and a computer-readable storage medium. The method comprises: based on a wavelength parameter, a gain parameter and a bandwidth parameter, calculating an impedance value of an impedance transformation line of a superconducting impedance transformation parametric amplifier and a capacitance value of the amplifier; based on the impedance value of the impedance transformation line, calculating a linewidth dimension of a coplanar waveguide of the superconducting impedance transformation parametric amplifier; based on the impedance value of the impedance transformation line and the capacitance value of the amplifier, calculating a stub dimension of the superconducting impedance transformation parametric amplifier; and based on the linewidth dimension and the stub dimension, determining structural parameters of the superconducting impedance transformation parametric amplifier.