scholarly journals Electric‐field‐induced Raman spectroscopy

1988 ◽  
Vol 88 (10) ◽  
pp. 6039-6048 ◽  
Author(s):  
David L. Andrews ◽  
Nick P. Blake
2007 ◽  
Vol 91 (7) ◽  
pp. 071910 ◽  
Author(s):  
M. Cazayous ◽  
D. Malka ◽  
D. Lebeugle ◽  
D. Colson

2015 ◽  
Vol 17 (11) ◽  
pp. 7095-7099 ◽  
Author(s):  
Sumeet Walia ◽  
Aditya K. Shah ◽  
Paul R. Stoddart ◽  
Madhu Bhaskaran ◽  
Sharath Sriram

This work demonstrates the ability to detect and isolate an analyte from a multianalyte mixture by SERS sensing.


2000 ◽  
Vol 85 (19) ◽  
pp. 4180-4183 ◽  
Author(s):  
E. J. Ayars ◽  
H. D. Hallen ◽  
C. L. Jahncke

2006 ◽  
Vol 527-529 ◽  
pp. 431-434 ◽  
Author(s):  
Michael A. Capano ◽  
A.R. Smith ◽  
Byeung C. Kim ◽  
E.P. Kvam ◽  
S. Tsoi ◽  
...  

3C-SiC p-type epilayers were grown to thicknesses of 1.5, 3, 6 and 10 μm on 2.5° off-axis Si(001) substrates by chemical vapor deposition (CVD). Silane and propane were used as precursors. Structural analysis of epilayers was performed using transmission electron microscopy (TEM), high-resolution x-ray diffractometry (HRXRD), and Raman spectroscopy. TEM showed defect densities (stacking faults, twins and dislocations) decreasing with increasing distance from the SiC/Si interface as the lattice mismatch stress is relaxed. This observation was corroborated by a monotonic decrease in HRXRD peak width (FWHM) from 780 arcsecs (1.5 μm thick epilayer) to 350 arcsecs (10 μm thick epilayer). Significant further reduction in x-ray FWHM is possible because the minimum FWHM detected is greater than the theoretical FWHM for SiC (about 12 arcsecs). Raman spectroscopy also indicates that the residual biaxial in-plane strain decreases with increasing epilayer thickness initially, but becomes essentially constant between 6 and 10 μm. Structural defect density shows the most significant reduction in the first 2 μm of growth. Phosphorus implantation was used to generate n+/p junctions for the measurement of the critical electric field in 3C-SiC. Based on current-voltage analyses, the critical electric field in p-type 3C-SiC with a doping of 2x1017 cm-3 is 1.3x106 V/cm.


Nanoscale ◽  
2019 ◽  
Vol 11 (28) ◽  
pp. 13484-13493 ◽  
Author(s):  
Huan Yang ◽  
Ben Q. Li ◽  
Xinbing Jiang ◽  
Jinyou Shao

Hybrid resonance enhanced local electric field for Raman sensing.


2016 ◽  
Vol 2016 ◽  
pp. 1-8
Author(s):  
Wei Qi ◽  
Weigen Chen ◽  
Fu Wan ◽  
Jingxin Zou ◽  
Zhaoliang Gu

Furfural is an important chemical solvent and intermediate. Sensitive detection of this compound has attracted great interest in various fields. Surface-enhanced Raman spectroscopy (SERS) is a highly sensitive method for material detection because of its optical enhancement effect of plasmonic nanostructures. This study presents a simple and versatile method to synthesize a SERS substrate, where polyaminothiophenol (PATP) was used to realize the stable combination of Au nanoparticles (AuNPs) and Au film via self-assembly. The near-field electric field distribution was calculated using the finite difference time domain (FDTD) simulation to determine the parameters responsible for electric field enhancement. The simulation results show that SERS enhanced factors are sensitive to interparticle spacing and materials for solid support but insensitive to particle size. Moreover, the experimental results show that the optimized substrates with the highest Raman activity were formed by six layers of 60 nm AuNPs decorated on a 30 nm thick Au film, thereby validating the simulation results. The SERS factor of the optimal substrates is approximately 5.57 × 103, and thein situdetection limit is 4.8 ppm. The 3D Raman spectra, relative standard deviation values for major peaks, and changes in signal intensity with time show the good reproducibility and stability of the substrates.


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