Surface acoustic waves and nanoscale imaging
Background on SAW devices, their nanofabrication, and imaging GHz acoustic waves with microwave impedance microscopy.
Background · Fabrication · TMIM
This page gives the background for my work on nanoscale surface acoustic wave devices: what these waves are, how they are generated and fabricated on chip, and how we image them.
What is a surface acoustic wave?
Mechanical vibrations in a solid travel as elastic waves: strain and stress coupled through the material’s elasticity. In the bulk, these waves fill the whole volume. At a free surface, the boundary conditions allow a different class of solutions: surface acoustic waves (SAWs), whose energy is confined within roughly one wavelength of the surface.
Depending on the stack and polarization, several surface-guided modes exist:
- Rayleigh waves, with elliptical particle motion in the sagittal plane.
- Love waves, which are shear-horizontal waves guided by a slower surface layer.
- Lamb waves, which are plate modes in thin membranes.
In a piezoelectric material, each of these mechanical waves carries an electric potential with it. This coupling is what lets us launch, detect, and image them electrically.
SAW in MEMS: interdigital transducers
The standard way to generate a SAW on chip is an interdigital transducer (IDT): interleaved metal fingers patterned on a piezoelectric film. An RF voltage across the fingers creates a periodic strain through the piezoelectric effect. When the drive frequency matches the finger period (λ = 2d in the schematic), the strain adds up coherently into a propagating surface wave.
Because SAW velocities are only a few kilometers per second, a micrometer-scale wavelength corresponds to gigahertz frequencies. This makes SAW devices compact RF components: they are the filters in every mobile phone. They are also a platform for sensing, acoustofluidics, and quantum acoustics.
Fabrication of nano-SAW devices
Building a device is a loop: simulation → CAD → fabrication → characterization, with each measurement feeding back into the next design. On the fabrication side, I patterned features using:
- Electron-beam lithography: spin-coat resist, expose, and develop.
- Metal deposition and lift-off to form electrodes.
- Etching to transfer patterns into the piezoelectric layer. Physical sputtering, plasma etching, and reactive-ion etching differ in anisotropy and selectivity.
Conventional characterization
The workhorse measurement is a vector network analyzer (VNA). It records S-parameters, the reflection and transmission between ports, as a function of frequency. This is precise and fast, but it only sees the device from its electrical ports and does not reveal where the energy goes.
Optical and X-ray methods, such as laser interferometry and stroboscopic X-ray imaging, can map the wave field. However, they are limited in spatial resolution, frequency range, or accessibility for nanoscale gigahertz devices.
Transmission-mode microwave impedance microscopy
Transmission-mode microwave impedance microscopy (TMIM) puts the detector on a scanning tip:
- The IDT launches the acoustic wave.
- A shielded cantilever probe picks up the oscillating piezoelectric potential at its position.
- The signal is demodulated against the source reference, giving two channels proportional to cos(kx + φ) and sin(kx + φ). Together they give the local amplitude and phase of the wave.
TMIM works up to about 10 GHz, with roughly 100 nm spatial resolution and a displacement sensitivity of about 1 fm/√Hz. That is enough to image wavefronts, standing waves, and leakage directly inside a working device.
In my work, I built a microwave impedance microscopy setup and developed Python tools to align and stitch scans, which made it possible to map large device areas.