PhD Thesis

Artificial Piezoelectricity in Silicon Phononic Crystals
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Brief overview:

We develop a new class of metamaterials designed to achieve artificial piezoelectricity in centrosymmetric materials.  Our focus is on silicon, a centrosymmetric material that lacks natural piezoelectric properties, which is crucial for various silicon-based on-chip applications.  We demonstrate how heterogeneous metal-on-silicon phononic crystals can induce artificial piezoelectricity in silicon.  Our structure(s) introduce a comprehensive analytical framework for one- and two-dimensional meta-atom structures that replicate piezoelectric behaviors.  We derive constitutive relations for the direct and converse piezoelectric effects and the electromechanical coupling factor.  We designate the 1D structure as a piezorope and the quasi-2D structure as a piezosheet.  By applying a DC bias to create dipoles in sub-units of simple geometric silicon structures, we configure these sub-units back-to-back to form a phononic crystal.  One application of this artificial piezoelectricity is an electrically tunable mechanical filter in silicon.  


We found that near unity electromechanical coupling factor can in principle be achieved by driving the system near resonance, with the added advantage of low voltage operation.  Moreover, our structure permits scalable frequency operation up to tens of giga hertz (GHz).  We have also designed and simulated realistic 2D metal-on-silicon phononic crystal structures on the Silicon-on-Insulator (SOI) platform and demonstrated artificial piezoelectricity by numerical experiment.  By tailoring both the electromagnetic and phononic band structures of these periodic structures, efficient excitation of coherent phononic modes can be achieved, which can potentially have novel applications in acousto-optics, acousto-electromagnetics, transducers, and quantum phononics.


Scientific papers


Brief Overview:

Traditional microscopic techniques, such as confocal microscopy, use ballistic photons and can image only tens of micrometers in depth, smaller than 1 transport mean free path (TMFP) which is typically < 1 mm.  Diffuse optical tomography can be used to image deeper than microscopy, typically > 1 cm, depths larger than 10 TMFP, but the resolution is poor (currently mm-cm resolutions for diffuse optical tomography).  Photo-acoustic imaging is playing a role to bridge this gap.  In optical-resolution photo-acoustics microscopy (PAM), optical focusing of light inside tissue determines the lateral resolution, whereas in acoustic-resolution PAM, the ultrasonic focusing dictates the lateral resolution.  In both cases, the axial resolution is determined by bandwidth of the transducer.  However, the photo-acoustic sensitivity is typically at micro-molar to milli-molar range. This is several orders of magnitude weaker than fluorescence methods, which is typically in the nano-molar range.  The higher the fluorescence quantum yield the less the photo-acoustic effect, in fact, it is (1 - fluorescence quantum yield). We illustrate the potential of unprecedented resolution fluorescence molecular tomography in the transport regime using reflection-mode illumination and detection.