Related Experiment Video
Updated: Nov 1, 2025

10:31
Plasma-assisted Molecular Beam Epitaxy of N-polar InAlN-barrier High-electron-mobility Transistors
Published on: November 24, 2016
8.8K
Passive High Power RF Comb Filters Using Epitaxial GaN/NbN/SiC HBARs
Summary
Researchers developed novel radio frequency (RF) comb filters using epitaxial Gallium Nitride/Niobium Nitride/Silicon Carbide (GaN/NbN/SiC) high overtone bulk acoustic resonators (epi-HBARs). These compact filters offer high performance for advanced RF applications.
Area of Science:
- Materials Science
- Electrical Engineering
- Acoustics
Background:
- Traditional RF comb filters can be bulky and limited in power handling.
- Gallium Nitride (GaN) and Niobium Nitride (NbN) are promising materials for high-frequency electronics.
- Silicon Carbide (SiC) substrates offer excellent thermal and mechanical properties.
Purpose of the Study:
- To demonstrate the first passive RF comb filters utilizing GaN/NbN/SiC epi-HBARs.
- To characterize the performance of these novel comb filters in terms of passband distribution, bandwidth, and figure of merit.
- To assess the high-power handling capabilities and potential applications of the developed filters.
Main Methods:
- Fabrication of two-port devices using epitaxial GaN/NbN/SiC layers.
- Electrical transduction and acoustic coupling for device operation.
- Characterization of filter response, including passband count, free spectral range (FSR), bandwidth (BW), and f x Q values.
Main Results:
- Demonstrated a multi-mode epi-HBAR comb filter with 158 passbands from 1 to 4 GHz.
- Achieved individual passbands with BWs up to 800 kHz and f x Q values up to 7x10^14 Hz.
- Observed linear, distortion-free performance up to 1 W CW and 10 W pulsed RF power.
Conclusions:
- Epi-HBARs offer a compact and high-performance solution for RF comb filters.
- These filters exhibit excellent high-power handling, suitable for demanding RF applications.
- Potential for co-fabrication with GaN electronics, enabling integrated RF systems for spectrum sensing and radar.
Related Concept Videos
Active Filters
1.1K
Active filters are electronic circuits that use operational amplifiers (op-amps), resistors, and capacitors to filter out unwanted frequency components from a signal. A first-order low-pass active filter is designed to pass signals with a frequency lower than a certain cutoff frequency and attenuate frequencies higher than that cutoff frequency. The transfer function for a first-order low-pass active filter is:
1.1K
Passive Filters
755
Passive filters are utilized to shape the frequency spectrum of signals across a diverse array of applications. These filters, using only passive elements like resistors (R), inductors (L), and capacitors (C), are capable of selectively allowing or blocking certain frequency ranges without the need for external power sources.
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
755
Biasing of FET
417
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
417
Biasing of P-N Junction
1.2K
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
1.2K
MOSFET Amplifiers
266
The MOSFET, when operating in its active region, functions as a voltage-controlled current source. In this region, the gate-to-source voltage controls the drain current. This principle underlies the operation of the transconductance MOSFET amplifier. The output current is directed through a load resistor to convert this amplifier into a voltage amplifier. The output voltage is then obtained by subtracting the voltage drop across the load resistance from the supply voltage. This process results...
266
Biasing of Metal-Semiconductor Junctions
403
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
403

