TY - JOUR
T1 - Near-unity Raman β-factor of surface-enhanced Raman scattering in a waveguide
AU - Fu, Ming
AU - Mota, Mónica P.d.S.P.
AU - Xiao, Xiaofei
AU - Jacassi, Andrea
AU - Güsken, Nicholas A.
AU - Chen, Yuxin
AU - Xiao, Huaifeng
AU - Li, Yi
AU - Riaz, Ahad
AU - Maier, Stefan A.
AU - Oulton, Rupert F.
N1 - Funding Information:
This work was supported by the EPSRC Reactive Plasmonics Programme (EP/M013812/1, R.F.O. and S.A.M.), the EPSRC Catalysis Plasmonics Programme (EP/W017075/1, R.F.O. and S.A.M.) and the Leverhulme Trust (RPG-2016-064, R.F.O. and S.A.M.). In addition, S.A.M. acknowledges the Lee-Lucas Chair in Physics. This project has received funding from the European Union’s Horizon 2020 research and innovation programme under a Marie Skłodowska-Curie Fellowship (grant agreement no. 844591, M.F.). M.F. thanks R. Hoggarth for his support on laser maintenance and alignment. N.A.G. thanks the German National Academy of Sciences Leopoldina for their support via the Leopoldina Postdoc Fellowship (LPDS2020-12).
Publisher Copyright:
© 2022, The Author(s), under exclusive licence to Springer Nature Limited.
PY - 2022/12
Y1 - 2022/12
N2 - The Raman scattering of light by molecular vibrations is a powerful technique to fingerprint molecules through their internal bonds and symmetries. Since Raman scattering is weak1, methods to enhance, direct and harness it are highly desirable, and this has been achieved using optical cavities2, waveguides3–6 and surface-enhanced Raman scattering (SERS)7–9. Although SERS offers dramatic enhancements2,6,10,11 by localizing light within vanishingly small hot-spots in metallic nanostructures, these tiny interaction volumes are only sensitive to a few molecules, yielding weak signals12. Here we show that SERS from 4-aminothiophenol molecules bonded to a plasmonic gap waveguide is directed into a single mode with >99% efficiency. Although sacrificing a confinement dimension, we find a SERS enhancement of ~103 times across a broad spectral range enabled by the waveguide’s larger sensing volume and non-resonant waveguide mode. Remarkably, this waveguide SERS is bright enough to image Raman transport across the waveguides, highlighting the role of nanofocusing13–15 and the Purcell effect16. By analogy to the β-factor from laser physics10,17–20, the near-unity Raman β-factor we observe exposes the SERS technique to alternative routes for controlling Raman scattering. The ability of waveguide SERS to direct Raman scattering is relevant to Raman sensors based on integrated photonics7–9 with applications in gas sensing and biosensing.
AB - The Raman scattering of light by molecular vibrations is a powerful technique to fingerprint molecules through their internal bonds and symmetries. Since Raman scattering is weak1, methods to enhance, direct and harness it are highly desirable, and this has been achieved using optical cavities2, waveguides3–6 and surface-enhanced Raman scattering (SERS)7–9. Although SERS offers dramatic enhancements2,6,10,11 by localizing light within vanishingly small hot-spots in metallic nanostructures, these tiny interaction volumes are only sensitive to a few molecules, yielding weak signals12. Here we show that SERS from 4-aminothiophenol molecules bonded to a plasmonic gap waveguide is directed into a single mode with >99% efficiency. Although sacrificing a confinement dimension, we find a SERS enhancement of ~103 times across a broad spectral range enabled by the waveguide’s larger sensing volume and non-resonant waveguide mode. Remarkably, this waveguide SERS is bright enough to image Raman transport across the waveguides, highlighting the role of nanofocusing13–15 and the Purcell effect16. By analogy to the β-factor from laser physics10,17–20, the near-unity Raman β-factor we observe exposes the SERS technique to alternative routes for controlling Raman scattering. The ability of waveguide SERS to direct Raman scattering is relevant to Raman sensors based on integrated photonics7–9 with applications in gas sensing and biosensing.
UR - http://www.scopus.com/inward/record.url?scp=85140822576&partnerID=8YFLogxK
U2 - 10.1038/s41565-022-01232-y
DO - 10.1038/s41565-022-01232-y
M3 - Article
C2 - 36302960
AN - SCOPUS:85140822576
SN - 1748-3387
VL - 17
SP - 1251
EP - 1257
JO - Nature Nanotechnology
JF - Nature Nanotechnology
IS - 12
ER -