<p>This dissertation focuses primarily on the development of
next generation acoustic and magnetic resonators for radio frequency
communication. Through novel design and fabrication techniques, acoustic and
magnetic devices with improved performance are demonstrated. </p>
<p> </p>
<p>Chapter 1 begins with an introduction to the current
wireless communication industry and the roles of resonators in RF front-end
architecture, as well as the requirements for next generation resonators to meet
the needs of 5G technology. </p>
<p> </p>
<p>Chapter 2 describes our work on lithium niobate acoustic
MEMS resonators. The theory section introduces the general working principles
of acoustic resonators utilizing piezoelectricity, and is followed by an
overview of various types of commonly used acoustic resonators. Subsequently, the
design, modeling, fabrication, and measurement of Al-IDT driven laterally
vibrating LN resonator on LN-on-LN platform are presented. With novel
fabrication techniques, resonators with competitive quality factor and superior
thermal stability have been achieved. Specifically, we demonstrate S0 and SH0
mode LN thin-film resonators with a quality factor (Q) ranging from more than
500 up to 2600 and
from 2% to
11.6% with a constant temperature coefficient of frequency in various power
ranges (-12dBm to -1dBm) with device dimensions of only
. </p>
<p> </p>
<p>Chapter 3 presents
the design, fabrication, and characterization of octave-tunable magnetostatic
wave YIG resonators on a chip, starting with an introduction to spin wave
theory. At 4.77GHz, the 0.68mm<sup>2</sup> resonator has achieved a Q >5000
with a bias field of 987Oe. We also demonstrate YIG resonator tuning by more
than one octave from 3.63GHz to 7.63GHz by applying an in-plane external
magnetic field. The measured quality factor of the resonator is consistently greater
than 3000 above 4GHz. We achieved this technological breakthrough by developing
a YIG film etching process and fabricating a thick aluminum coplanar waveguide inductor
loop around each resonator to individually address and excite magnetostatic
waves. The micromachining technology enables the fabrication of multiple single-port
and two-port YIG resonators on the same chip, with all resonators demonstrating
octave tunability and high Q, thus allowing for potential monolithic high order
MSW filters and multiplexers as a chip-scale SHF multiplexing solution. </p>
<p> </p>
<p>Chapter 4 presents the first MSW YIG resonator on YIG-on-insulator,
taking advantage of the YIG film layer transfer technique that we developed by using
surface activated bonding and ion slicing for heterostructure integration.
Surface and crystalline structure characterization is presented to demonstrate
applicability to device fabrication. The YIG resonator is measured with a
magnetic bias changing from 560Oe to 3610Oe, thus resulting in a resonance ranging
from 2.6GHz to 13.2GHz. With the removal of substrate constraints, this
technology enables a chip-scale multiplexing solution as well as new
possibilities for low damping magnetic quantum computing components. </p>
<p> </p>
<p>Chapter 5 presents our preliminary results in three active
research areas. First, the design of a strain-tunable free standing MSW YIG
resonator is presented, together with batches of fabrication process
optimization. Second, the thermal strain induced anisotropy frequency tuning
from the thermal mismatch between YIG film and Si substrate is measured with in-plane
ferromagnetic resonance at different in-plane orientations. Third, a YIG
circulator on a silicon chip is proposed with high isolation, low insertion
loss, and a size 1000 times smaller than that of the state-of-the-art
commercial product.</p><p></p>