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Proceeding Paper

SERS Active Periodic 3D Structure for Trapping and High Sensitive Molecular Analysis of Particles or Cells †

1
Institute for Solid State Physics and Optics, Wigner Research Centre for Physics, HAS, Budapest, Hungary
2
Institute of Technical Physics and Materials Science, Centre for Energy Research, HAS, Budapest, Hungary
*
Author to whom correspondence should be addressed.
Presented at the Eurosensors 2017 Conference, Paris, France, 3–6 September 2017.
Proceedings 2017, 1(4), 560; https://doi.org/10.3390/proceedings1040560
Published: 8 August 2017
(This article belongs to the Proceedings of Proceedings of Eurosensors 2017, Paris, France, 3–6 September 2017)

Abstract

:
In this work the highly sensitive molecule recognition performance of a specially designed surface enhanced Raman scattering (SERS) substrate was demonstrated. The general inverse pyramid structures were modified to be able to perform as cavities in perforated membrane applicable for particle and cell filtering, sorting and trapping. In the voids of the gold covered substrate size compatible particles functionalised by different molecules were trapped, their SERS signal was detected and the different molecules were recognised.

1. Introduction

SERS [1] evolves in close vicinity of metallic nanostructures where the interaction between the electromagnetic field of photons and the surface plasmons results in several orders of magnitude enhancement of the Raman signal. This effect extremely improves the sensitivity of Raman spectroscopy achieving the limit of molecule detection in attomolar (10−18 M) concentrations [2]. According to our approach a special size fitted SERS active substrate was prepared to be applicable for particle and cell entrapment and highly sensitive detection of molecules immobilized on their surface.

2. Materials and Methods

Arrays of periodic perforated inverse pyramids were prepared on polished SOI (silicon-on-insulator) wafers. The 3D structure was shaped by alkaline etching from the front side in the 2 μm thick device layer of the wafer by using the appropriate masking pattern. Periodic vertical tapered microchannels (see Figure 1) were formed by etching away the back-side handler silicon and buried oxide and coated with a 50 nm thick evaporated layer of gold. The resulted geometry was used simultaneously as an array of particle traps and a SERS substrate.

3. Results

Raman spectra of benzophenone were recorded (by a Renishaw 1000 micro-Raman spectrometer with Leica DM/LM microscope using 1 micron laser spot size on the sample and 785 nm excitation wavelength) on flat silicon and the structured gold surface. The significant amplification by the SERS substrate is presented in Figure 2.
Polystyrene microparticles labelled with different fluorescent molecules (from Sigma Aldrich and Spherotech) were dissolved in water and dripped onto the periodic structure.
Particles having size (2 μm diameter) similar to the period of the 3D structure were entrapped on the surface after washing. The lateral distribution of the beads was characterized by fluorescent microscopy as presented in Figure 3. The fluorescent molecules were analysed by SERS utilizing the plasmonic enhancement by the structured surface of the traps. The definite and sensitive differentiation of the molecules immobilized on the polystyrene bead surfaces are presented in Figure 4, where a huge increase in the Raman signal can be observed on the SERS surface. Taking into account that the Raman signal recorded from the beads on silicon substrate arises from the total volume of the particles, while SERS occurs only in the few nanometer region close to the SERS substrates, it can be concluded that the observed SERS enhancement of two orders of magnitude is much higher actually.

4. Conclusions

The applicability of special perforated periodic 3D structure was demonstrated for simultaneous particle (or cell) trapping and extremely sensitive Surface-Enhanced Raman Spectroscopy based detection of molecules immobilized on the surfaces of the confined beads.

Acknowledgments

This work was supported by the Hungarian Academy of Sciences. The authors gratefully acknowledge the high-quality technical work of Magda Erős and Margit Payer regarding microfabrication. Miklos Veres is grateful for the support of the János Bolyai Research Scholarship of the Hungarian Academy of Sciences.

Conflicts of Interest

The authors declare no conflict of interest. The founding sponsors had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, and in the decision to publish the results.

References

  1. Ryder, A.G. Surface enhanced Raman scattering for narcotic detection and applications to chemical biology. Curr. Opin. Chem. Biol. 2005, 9, 489–493. [Google Scholar] [CrossRef] [PubMed]
  2. Etchegoin, P.; Maher, R.C.; Cohen, L.F.; Hartigan, H.; Brown, R.J.C.; Milton, M.J.T.; Gallop, J.C. New limits in ultrasensitive trace detection by surface enhanced Raman scattering (SERS). Chem. Phys. Lett. 2003, 375, 84–90. [Google Scholar] [CrossRef]
  3. Acuna, G.P.; Bucher, M.; Stein, I.H.; Steinhauer, C.; Kuzyk, A.; Holzmeister, P.; Schreiber, R.; Moroz, A.; Stefani, F.D.; Liedl, T.; et al. Distance Dependence of Single-Fluorophore Quenching by Gold Nanoparticles Studied on DNA Origami. ACS NANO 2012, 6, 3189–3195. [Google Scholar] [CrossRef]
Figure 1. SEM view of the periodic perforated SERS substrate for particle and cell entrapment.
Figure 1. SEM view of the periodic perforated SERS substrate for particle and cell entrapment.
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Figure 2. Comparison of the Raman signals of benzophenone detected on silicon and the 3D structured surface. The broad band in the 900–1000 cm−1 region is arising from the silicon substrate.
Figure 2. Comparison of the Raman signals of benzophenone detected on silicon and the 3D structured surface. The broad band in the 900–1000 cm−1 region is arising from the silicon substrate.
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Figure 3. Fluorescent beads with appropriate 2 μm diameter (Sigma Aldrich—green and Spherotech—blue) entrapped in the periodic array of perforated pyramidal structures: multichannel fluorescent image (top) and upright optical micrograph (bottom).
Figure 3. Fluorescent beads with appropriate 2 μm diameter (Sigma Aldrich—green and Spherotech—blue) entrapped in the periodic array of perforated pyramidal structures: multichannel fluorescent image (top) and upright optical micrograph (bottom).
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Figure 4. Comparison of the SERS spectra recorded on the clean SERS substrate (black) and different fluorescent beads on silicon (red) and trapped in the periodic array (blue). SA—Sigma Aldrich (a) and ST—Spherotech (b) fluorescent beads, respectively. The broad band in the 900–1000 cm−1 region is arising from the silicon substrate.
Figure 4. Comparison of the SERS spectra recorded on the clean SERS substrate (black) and different fluorescent beads on silicon (red) and trapped in the periodic array (blue). SA—Sigma Aldrich (a) and ST—Spherotech (b) fluorescent beads, respectively. The broad band in the 900–1000 cm−1 region is arising from the silicon substrate.
Proceedings 01 00560 g004
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MDPI and ACS Style

Rigó, I.; Veres, M.; Fürjes, P. SERS Active Periodic 3D Structure for Trapping and High Sensitive Molecular Analysis of Particles or Cells. Proceedings 2017, 1, 560. https://doi.org/10.3390/proceedings1040560

AMA Style

Rigó I, Veres M, Fürjes P. SERS Active Periodic 3D Structure for Trapping and High Sensitive Molecular Analysis of Particles or Cells. Proceedings. 2017; 1(4):560. https://doi.org/10.3390/proceedings1040560

Chicago/Turabian Style

Rigó, István, Miklós Veres, and Péter Fürjes. 2017. "SERS Active Periodic 3D Structure for Trapping and High Sensitive Molecular Analysis of Particles or Cells" Proceedings 1, no. 4: 560. https://doi.org/10.3390/proceedings1040560

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