1992
DOI: 10.1080/09500349214552341
|View full text |Cite
|
Sign up to set email alerts
|

Enhanced Raman Scattering from Benzene Condensed on a Silver Grating

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

1
7
0

Year Published

1999
1999
2013
2013

Publication Types

Select...
6
2
1

Relationship

2
7

Authors

Journals

citations
Cited by 24 publications
(8 citation statements)
references
References 25 publications
1
7
0
Order By: Relevance
“…Therefore Grewe 24 measured SERS of C 2 H 4 under regulated dynamic C 2 H 4 pressures in the UHV system and regulated temperatures of the Cu substrate above 90 K. During cooling down of the sample from 110 to 80 K, the N‐bands are clearly distinguishable at 90 K. Since the adsorbate is in dynamic equilibrium with the gas phase, it is very unlikely that there is a second layer of C 2 H 4 formed under these conditions. The wavenumber position of the ν 3 Raman band of C 2 H 4 adsorbates on Cu(111) does agree with the position of the N‐band, as could be demonstrated from the Raman signal of an optical grating covered with a Cu film evaporated at 310 K, annealed to 350 K, cooled to 40 K, and exposed to 1–1.5 L of C 2 H 4 (in this case, the enhancement is exclusively due to local plasmon‐polariton field enhancement) 28 . For silver films under similar conditions, the (111) orientation with azimuthal randomness was confirmed by X‐ray scattering, which most likely also holds for the copper films on the grating.…”
Section: The Firm Relation Between the Raman Scattering Backgrousupporting
confidence: 58%
“…Therefore Grewe 24 measured SERS of C 2 H 4 under regulated dynamic C 2 H 4 pressures in the UHV system and regulated temperatures of the Cu substrate above 90 K. During cooling down of the sample from 110 to 80 K, the N‐bands are clearly distinguishable at 90 K. Since the adsorbate is in dynamic equilibrium with the gas phase, it is very unlikely that there is a second layer of C 2 H 4 formed under these conditions. The wavenumber position of the ν 3 Raman band of C 2 H 4 adsorbates on Cu(111) does agree with the position of the N‐band, as could be demonstrated from the Raman signal of an optical grating covered with a Cu film evaporated at 310 K, annealed to 350 K, cooled to 40 K, and exposed to 1–1.5 L of C 2 H 4 (in this case, the enhancement is exclusively due to local plasmon‐polariton field enhancement) 28 . For silver films under similar conditions, the (111) orientation with azimuthal randomness was confirmed by X‐ray scattering, which most likely also holds for the copper films on the grating.…”
Section: The Firm Relation Between the Raman Scattering Backgrousupporting
confidence: 58%
“…The grating period was 500 nm, the amplitude was 20 to 30 nm [24]. The size of the Ag electrode was 2 Â 2 mm 2 .…”
Section: Methodsmentioning
confidence: 99%
“…Propagating surface plasmons excited with the gratings are accompanied by enhanced electric fields near their corrugated surfaces, at which Raman signals from target analytes are amplified. [20][21][22] When 2-D gratings are used in Raman sensing, which is our interest, the use of circular polarization is reasonable, because the optical responses of a spectrometer are usually subject to the polarization of the input signals. In that case, the SPR dips at all orientations would be averaged out, suggesting that using the dip depth or the dip wavelength as a measure of the target molecules would be problematic.…”
Section: Discussionmentioning
confidence: 99%