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@ARTICLE{Kerfoot:634412,
author = {Kerfoot, James and Legge, Elizabeth J. and Collins, Amy and
Chauhan, Jasbinder and Rossnagel, Kai and Beton, Peter H.
and Mellor, Christopher J. and Pollard, Andrew J. and Rance,
Graham A. and George, Michael W.},
title = {{B}enchmarking {TERS} and {TEPL} probes: towards a
reference sample for quantification of near-field
enhancement factors in gap and non-gap modes},
journal = {The analyst},
volume = {150},
number = {14},
issn = {0003-2654},
address = {Cambridge},
publisher = {Soc.},
reportid = {PUBDB-2025-02495},
pages = {3077 - 3088},
year = {2025},
note = {JK, GAR and MWG acknowledge funding from the Engineeringand
Physical Science Research Council (EPSRC) (Project:
EP/V053884/1) and support from the Nanoscale and
MicroscaleResearch Centre (nmRC). EJL and AJP would like to
acknowl-edge the National Measurement System (NMS) of
theDepartment for Science, Innovation and Technology
(DSIT),UK ( projects #128826) for funding. The authors
thankDongkuk Kim and Sebastian Wood at the National
PhysicalLaboratory, U.K., for discussion associated with
themanuscript.},
abstract = {Benchmarking the near-field signal enhancement attained
using plasmonic metal-coated atomic force microscopy (AFM)
probes for tip-enhanced Raman spectroscopy (TERS) and
tip-enhanced photoluminescence (TEPL) measurements is
challenging given the absence of a suitable reference sample
that is simple to prepare, easy to use and compatible with
different instrument configurations. To this end, in this
study, we have fabricated a flake of monolayer tungsten
diselenide (1L-WSe$_2$) stamped across the interface of gold
and silver thin films on silicon dioxide and glass. We have
demonstrated these samples to be effective for the facile
determination of near-field Raman and photoluminescence
contrast factors in both gap and non-gap mode, respectively.
We show that the near-degenerate E$^1$$_{2g}$ + A$_{1g}$ and
2LA(M) peaks in the Raman spectra of WSe$_2$2 enable
quantification of Raman contrast factors, with a ∼1.6-fold
increase in TERS signal enhancement in gap mode, relative to
non-gap mode, observed for a typical probe. Similar
differences in the photoluminescence contrast factors were
observed comparing in-contact and out-of-contact signal
intensity ratios from gap and non-gap mode TEPL
measurements. Moreover, in developing a reference
methodology we found that the line shape of the TEPL profile
was dependent upon the magnitude of the signal enhancement,
with a disproportionate increase in the longer wavelength
shoulder of the emission observed in gap mode. As this
contribution to the asymmetric line shape is tentatively
assigned to a dark exciton, which possesses an out-of-plane
transition dipole moment, our TEPL measurements indicate
that the directionality of the near-field enhancement
provides a further handle enabling quantification of probe
performance. Using samples prepared on glass, and comparing
results obtained from two different instruments, each with a
different excitation laser wavelength and optical access, we
demonstrate the universal applicability of our reference
material for sensitivity benchmarking of metallised AFM
probes in both gap and non-gap mode, suitable for both
reflection and transmission geometries, and across the range
of laser wavelengths typically used for TERS and TEPL.},
cin = {FS-SXQM},
ddc = {540},
cid = {I:(DE-H253)FS-SXQM-20190201},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632)},
pid = {G:(DE-HGF)POF4-632},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:40525753},
doi = {10.1039/D5AN00456J},
url = {https://bib-pubdb1.desy.de/record/634412},
}