Ph.D., Massachusetts Institute of Technology
B.Sc., National Taiwan University
Condensed matter experiments: correlated electronic systems, including high-temperature superconducting cuprates and iron-based compounds and novel magnetic oxides; spintronics; topological materials, including topological insulators and superconductors; physics and devices of low-dimensional systems such as graphene, carbon nanotubes, silicon nano-pillars, and semiconducting quantum dots; development and applications of scanning probe microscopy; nano-science and nano-technology; energy research, including photovoltaic and fuel cells; low-temperature phases of helium; development of superconducting cavity-stabilized oscillators.
From left to right, front row: Slobodan, Prof. Yeh, Jenelyn, Peter; back row: Marcus, Cameron, Andrew, Nils, and Kevin
Please see Nature Communications 6, 6620 (2015) [DOI 10.1038/ncomms7620] and Caltech News (03/18/2015) for more information.
Left image: The LDOS modulations of Y-123 at H = 5T and 6 K over a (22 x 29) nm2 area, showing patterns associated with density-wave modulations and vortices (circled objects) for ω = (a) -9 meV ~ -Δ', (b) -23 meV ~ -ΔSC, (c) -33 meV ~ -VCO and (d) -53 meV. We note that the vortex contrasts are the most apparent at |ω| <~ ΔSC and become nearly invisible for |ω| >>VCO. The vanishing contrast at high energies may be due to the onset of Cu-O optical phonons (~ 50 meV for the cuprates) so that both the collective modes and quasiparticles become scattered inelastically. Right image: FT studies of the conductance maps of Y-123: |F(k,ω)| at H = 5T and ω = -12 meV. We identify three sets of ω- independent wave-vectors in addition to the reciprocal lattice constants and the (π,π) resonance: QPDW and QCDW along (π,0)/(0,π) and QSDW along (π,π), which are circled for clarity. For more information on the measurements in the hole-type cuprate Y-123, please see arxiv:0906.1776 and arxiv:0808.3016 [Europhys. Lett. 87, 37005 (2009)]. For more information on the vortex-state measurements in the infinite-layer electron-type cuprate La0.1Sr0.9CuO2 (La-112), please see arxiv:0809.0541 [Europhys. Lett. 85, 17004 (2009)]. For a recent review on unconventional low-energy excitations in cuprate superconductors, please see Int. J. Mod. Phys. B 23, 4543 - 4577 (2009).
Please see arXiv:1201.5618 [Solid State Comm. 152, 747 (2012)] for more information.
Please see arxiv:1007.5086 [Phys. Rev. Lett. 106, 087004 (2011)] for more information.
Please see arxiv:1009.0081 [Surface Science 605, 1649–1656 (2011)] for more information.
Please see arxiv:1004.1448 [Phys. Rev. B 82, 13441 (2010)] for more information.