Qifeng Li

Dr. Qifeng Li


Research Focus & Metrics

Academic Career Length

24Years (2003-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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20 April 2009 in The Journal of Physical Chemistry C
Verified
Journal Article
Closed access
ZYZheng Yang
Zheng Yang
QLQifeng Li
Qifeng Li
KCKeng C. Chou
Keng C. Chou

1 December 2009 in Biophysical Journal
Verified
Journal Article
Closed access
QLQifeng Li
Qifeng Li
SWSherry S.H. Wu
Sherry S.H. Wu
KCKeng C. Chou
Keng C. Chou

29 December 2007 in The Journal of Physical Chemistry B
Verified
Journal Article
Closed access
QLQifeng Li
Qifeng Li
RHRui Hua
Rui Hua
ICIgnatius J. Cheah
Ignatius J. Cheah
KCKeng C. Chou
Keng C. Chou

1 February 2008 in The Journal of Physical Chemistry B
Verified
Journal Article
Closed access
QLQifeng Li
Qifeng Li
RHRui Hua
Rui Hua
KCKeng C. Chou
Keng C. Chou

25 February 2009 in Physical Chemistry Chemical Physics
Verified
Journal Article
Closed access
PDF file
QLQifeng Li
Qifeng Li
CKChiung Wen Kuo
Chiung Wen Kuo
ZYZheng Yang
Zheng Yang
PCPeilin Chen
Peilin Chen
KCKeng C. Chou
Keng C. Chou
Surface-enhanced IR–visible sum frequency generation (SFG) was studied using Ag and Au films over nanospheres (AgFON and AuFON), which provided large area of reproducible nanoscale structures with well-defined morphology. SFG vibrational spectra for a self-assembled monolayer of octadecanethiol were investigated on spheres with diameters ranging from 300 nm to 620 nm. With an input wavelength of 532 nm, a sphere diameter near 360 nm produced the maximum enhancement, which was consistent with the localized surface-plasmon resonant wavelength identified by minimum reflectivity. The measured second-order susceptibility for the asymmetric CH3 stretch mode of octadecanethiol was enhanced by up to 27 times on AgFON, which corresponded to an SFG enhancement factor of ∼730. The SFG enhancement factor for AuFON was a quarter of that from AgFON. The SFG enhancement factor for the symmetric CH3 mode was about 10 times smaller than that for the asymmetric CH3 mode. This difference can be explained by the highly directional electrical-field parallel to the surface, created at the junction between nanospheres. Polarization-dependent studies also indicated that excitations with the electrical field parallel to the surface was the main contribution to the observed surface enhancements, and the electrical field perpendicular to the surface offered little enhancement.

18 June 2008 in Advanced Materials
Verified
Journal Article
Closed access
PDF file
APAgostino Pietrangelo
Agostino Pietrangelo
BSBryan C. Sih
Bryan C. Sih
BBBritta N. Boden
Britta N. Boden
ZWZhenwei Wang
Zhenwei Wang
QLQifeng Li
Qifeng Li
MWMichael O. Wolf
Michael O. Wolf