KnE Energy | The 2nd International Symposium "Physics, Engineering and Technologies for Biomedicine" | pages: 69–74

, , and

1. Introduction

Improvement of detection efficiency in biosensing is of great interest due to the potential ability to reveal diseases at the early stages. One of the most widely used sensing methods is the measurement of luminescence signal obtained from the fluorescent markers which could selectively bind to the antigen in the analyte [1]. Detection efficiency could be significantly improved with the use of highly luminescent markers such as semiconductor quantum dots (QDs), or by the use of more sensitive detection set-ups [1]–[3]. Photonic crystals allow one to influence on the luminescent properties of luminophores embedded into their structure and provide the possibility to improve the efficiency of collection of luminescence signal [4]–[6]. On the other hand the activated surface of the photonic crystal should be able to interact with the analyte in order to use it for sensing. Photonic crystals made of porous structures thus could be effectively applied in biosensor field [3], [7], [8].

One of the most interesting materials for fabrication of porous photonic crystals is porous silicon [8] (pSi). Ability to precisely control the fabrication process allows one to obtain highly ordered multi-layer structures and to construct one-dimensional photonic crystals such as distributed Bragg reflectors, Rugate-filters and microcavities [9]–[11]. Due to the oriented cross-cutting pores liquid samples could easily infiltrate the whole porous structure and hence the entire surface could be activated and used for detection. Furthermore, after the embedding of the luminescent particles their luminescence could be enhanced with the Purcell effect at the certain wavelength [12].

In our study we have performed deep investigation of porous silicon as the material for sensor substrates. We have fabricated different types of porous silicon photonic crystals using electro-chemical etching, characterized them and measured their optical characteristics. In order to estimate the influence on the photoluminescence (PL) of the embedded luminophores, QD solutions have been embedded into the structures and spectra and spatial distribution measurements of the luminescence have been made. Finally, we have shown the possibility to improve the detection efficiency of biosensors with the use of porous silicon photonic crystals as the substrates.

2. Materials and methods

Porous silicon photonic crystals have been fabricated using conventional electrochemical etching method in water-alcoholic solutions of hydrofluoric acid [13]. We have used home build PTFE etching cell with etching surface area around 1 cm 2 . Highly doped p-type monocrystalline silicon wafers with (100) orientation have been used as a substrate. Fabricated samples of pSi photonic crystals have been oxidized in order to stabilize their properties and prevent embedded luminophores from quenching.

CdSe/CdS/ZnS QDs have been synthesized using hot injection method described in [14] in details. QD surface have been covered with hexadecylamine. QD photoluminescence has symmetrical Gaussian shaped spectrum with the maximum at 620 nm and a full width at half maximum (FWHM) around 45 nm. QDs have been embedded into the porous structures using drop-casting of small amounts (1-10 µl) of hexane solutions with concentrations around 0,01-0,05 mg/ml.

Scanning electron microscopy (SEM) of the surface and cross-section of porous photonic structures has been made after the fabrication. Results are shown on Figure 1. It could be seen that pSi surface has relatively big pore sizes (10-30 nm), which makes it possible to fill the structure with solutions containing analytes as well as luminescent markers.

Figure 1

Scanning electron microscopy images of (a) the surface and (b) cross-section of the one-dimensional porous silicon photonic crystal.


In order to characterize the optical properties of fabricated photonic crystals reflectance spectra have been measured. Maximum reflection reached 100% in the photonic bandgap region comparing to the aluminum mirror in the visible spectral range. High reflection band was typically around 150-200 nm wide. Microcavities have an eigenmode inside the photonic bandgap with quality factor (Q-factor) in a range of 100-150.

3. Results and discussion

Photoluminescence of the QDs changed significantly after the embedding into the structure of the photonic crystal depending on the distribution of the QDs inside the structure [15]. Morphology of the porous structures determined the embedding depth [16]. In case of the lower porosity of the front porous layer QD solution effectively penetrated into the structure due to the capillary effect. As the result QDs have been uniformly distributed through the whole porous structure with depth around 6 µm. Hereupon PL spectra narrowed and the maximum shifted to the wavelength of the microcavity eigenmode, Figure 2. PL FWHM decreased to 6 nm corresponding to the microcavity Q-factor. In the opposite case of high porosity the front layer QDs mostly formed the film on the surface of photonic crystal leading to the modulation of their photoluminescence by the reflectance of the microcavity. The dip in the photoluminescence spectra appeared at the microcavity eigenmode position.

Figure 2

(a) Microcavity reflection spectrum and (b) photoluminescence spectra of QDs inside the microcavity (black) compared to the luminescence of the QD film on the silicon wafer (red).


Angle resolved measurements were made to control the spatial distribution of the photoluminescence of fabricated structures [17]. Results were compared to the QD PL distribution from the QD film on silicon wafer. Photoluminescence of the QDs embedded inside the pSi microcavity became unidirectional perpendicular to the photonic crystal surface. Such modification makes it very suitable for the improvement of the performance of the biosensors measuring the photoluminescence signals: detector placed just above the substrate surface will collect luminescent signal much more effectively.

Finally we have made time-resolved measurements of the photoluminescence decay rates. QD PL lifetime in hexane solution was around 20 ns. After the embedding it decreased to the 9 ns which is mostly due to the quenching caused by the interaction with the silicon surface. Proper treatment of the silicon surface together with the covering of QDs to stabilize their properties could eliminate the quenching effect and would make it possible to estimate the influence of Purcell enhancement on the change of the PL decay lifetime. Enhancement of the photoluminescence in such structures could significantly improve the sensitivity of biosensing methods based on the measurements of the PL signal values by the lowering of the detection limit.

4. Conclusions

In our study we have fabricated hybrid systems based on the porous silicon photonic crystals with embedded QDs and performed the investigation of their properties. Also we have analyzed the perspectives of the use for the improvement of biosensors sensitivity. We have shown spectral narrowing of the QD photoluminescence after embedding into the pSi microcavities as well as the unidirectional distribution of the PL in the perpendicular direction to the photonic crystal surface. Porous silicon photonic crystals have shown to be the promising material for improving of the biosensors efficiency.


This study was supported by the Federal Target Program for Research and Development of the Ministry of Education and Science of the Russian Federation, grant no. 14.616.21.0042 (ID RFMEFI61615X0042).



U. Resch-Genger M. Grabolle S. Cavaliere-Jaricot R. Nitschke T. Nann Quantum dots versus organic dyes as fluorescent labels Nature Methods 2008597637752-s2.0-5084910452910.1038/nmeth.1248


D. Dovzhenko V. Terekhin K. Vokhmincev A. Sukhanova I. Nabiev Improvement of antigen detection efficiency with the use of two-dimensional photonic crystal as a substrate Journal of Physics: Conference Series 201778412-s2.0-8501305473110.1088/1742-6596/784/1/012018012018


G. Gaur1 ntegrating Colloidal Quantum Dots with Porous Silicon for High Sensitivity Biosensing Mater. Res. Soc. Symp. Proc 2011131416


Z.-B. Wang Y.-H. Ye J.-Y. Zhang Modified spontaneous emission from dye molecules inside a photonic crystal microcavity Chinese Physics Letters 2007248, article no. 027225222542-s2.0-3454759514110.1088/0256-307X/24/8/027


X. W. Yuan L. Shi Q. Wang Spontaneous emission modulation of colloidal quantum dots via efficient coupling with hybrid plasmonic photonic crystal Optics Express 2014221923473234792-s2.0-8490754271710.1364/OE.22.023473


D. Dovzhenko E. Osipov I. Martynov P. Linkov A. Chistyakov Enhancement of Spontaneous Emission from CdSe/CdS/ZnS Quantum Dots at the Edge of the Photonic Band Gap in a Porous Silicon Bragg MirrorProceedings of the 4th International Conference of Photonics and Information Optics, PhIO 2015Russia1261302-s2.0-8496088208610.1016/j.phpro.2015.09.132


V. S.-Y. Lin K. Motesharei K.-P. S. Dancil M. J. Sailor M. R. Ghadiri A porous silicon-based optical interferometric biosensor Science 199727853398408432-s2.0-184237684010.1126/science.278.5339.840


G. E. Kotkovskiy Y. A. Kuzishchin I. L. Martynov A. A. Chistyakov I. Nabiev The photophysics of porous silicon: Technological and biomedical implications Physical Chemistry Chemical Physics 2012144013890139022-s2.0-8486702582510.1039/c2cp42019h


P. J. Reece G. Lérondel W. H. Zheng M. Gal Optical microcavities with subnanometer linewidths based on porous silicon Applied Physics Letters 20028126489548972-s2.0-003716492910.1063/1.1531226


P. A. Snow E. K. Squire P. S. J. Russell L. T. Canham Vapor sensing using the optical properties of porous silicon Bragg mirrors Journal of Applied Physics 1999864178117842-s2.0-003261371610.1063/1.370968


R. A. Rakhimov E. V. Osipov D. S. Dovzhenko I. L. Martynov A. A. Chistyakov Influence of electro-chemical etching parameters on the reflectance spectra of porous silicon rugate filters Journal of Physics: Conference Series 201673712-s2.0-8498988415810.1088/1742-6596/737/1/012026012026


E. M. Purcell R. V. Pound N. Bloembergen Nuclear Magnetic Resonance Absorption in Hydrogen Gas Physical Review A: Atomic, Molecular and Optical Physics 19467011-1298698710.1103/PhysRev.70.986


R. L. Smith S. D. Collins Porous silicon formation mechanisms Journal of Applied Physics 1992718R1R222-s2.0-3364491010610.1063/1.350839


P. Samokhvalov P. Linkov J. Michel M. Molinari I. Nabiev Photoluminescence quantum yield of CdSe-ZnS/CdS/ZnS core-multishell quantum dots approaches 100% due to enhancement of charge carrier confinementProceedings of the Colloidal Nanoparticles for Biomedical Applications IXFebruary 2014USA2-s2.0-8490162884010.1117/12.2040196


D. S. Dovzhenko I. L. Martynov P. S. Samokhvalov K. E. Mochalov A. A. Chistyakov I. Nabiev Modulation of quantum dot photoluminescence in porous silicon photonic crystals as a function of the depth of their penetrationProceedings of the Photonic Crystal Materials and Devices XIIApril 2016Belgium2-s2.0-8498226733110.1117/12.2228990


N. A. Tokranova S. W. Novak J. Castracane I. A. Levitsky Deep infiltration of emissive polymers into mesoporous silicon microcavities: Nanoscale confinement and advanced vapor sensing The Journal of Physical Chemistry C 20131174422667226762-s2.0-8488985402410.1021/jp405071n


V. E. Borisenko S. V. Gaponenko V. S. Gurin C. H. Kam Spatial and spectral properties of CdSe/CdS/ZnS quantum dots luminescence in one-dimensional photonic structures based on porous silicon Phys. Chem. Appl. nanostructures 2015144147



  • Downloads 7
  • Views 69



ISSN: 2413-5453