Francesco Chiavaioli - Università degli Studi di Siena
Transcription
Francesco Chiavaioli - Università degli Studi di Siena
Flow cell for strain- and temperature-compensated refractometric measurements by means of cascaded optical fiber long period and Bragg gratings as promising label-free biosensing system Francesco Chiavaioli Università degli Studi di Siena, Via Roma 56, 53100 Siena, Italy e-mail: chiavaioli@dii.unisi.it Tutor: Prof. Valerio Vignoli; Tutor at IFAC-CNR: Prof. Massimo Brenci [joint work with “Nello Carrara” Institute of Applied Physics – National Research Council] Introduction Refractometric measurements in biological fluids have been used for many years in the quantitative measurements of analytes, by employing chemical/biochemical recognition layers deposited on suitable substrates. Chemical/biochemical interactions with these layers lead to changes in the refractive index of the layer which can be detected by means of optical methods, and which depends on the concentration of the interacting analyte. This approach is known as the label-free approach [1, 2], in contrast with the methodology that makes use of luminescent markers chemically bound to recognition elements. Within the optical approach, optical fiber long period gratings (LPG) have been recently proposed for chemical /biochemical sensing [3]. These sensors show a high sensitivity to the refractive index of the medium surrounding the fiber and thus a number of refractometric measurement systems have been proposed in the past [4-7]. However, LPGs have great sensitivity not only to the external refractive index, but also to temperature, strain and fiber bending. A number of techniques have been proposed in order to get rid of the influence of these cross-sensitivities [8, 9], which can be critical when an accurate refractometric measurement is carried out with the investigated sample flowing within a flow cell, as generally occurs in the chemical /biochemical sensing. In this scenario our goal is to describe the design and characterization of a thermo-stabilized flow cell of low volume (tens of µL) for accurate refractometric measurements using LPG and a methodology for measuring and correcting all the LPG cross-sensitivity, by means of a fiber Bragg grating (FBG) written on the same fiber and an accurate temperature measurement system [10-13]. Measurements Strain characterization Theory and methodology Definition: an optical fiber grating is a permanent periodic modulation of the fiber core refractive index. Classification (according to the grating period Λ, which sets out a specific coupling of light): Short period or fiber Bragg gratings (FBGs): Grating period in the range of hundreds of nanometers; Coupling between the fundamental core mode and its respective counter-propagating mode; Characteristic equation [14]: 2Λ , Long period gratings (LPGs): Grating period in the range of hundreds of micrometers; Coupling between the fundamental core mode and a discrete set of forward-propagating cladding modes; Characteristic equation [15]: , Λ , , The specific coupling between the modes verifying the phasematching condition generates in the LPG transmission spectrum a series of attenuation bands centered at discrete wavelengths. Methodology: Theoretical expressions: Δ (1) Δ ⁄ (2) Once the four coefficients in the foregoing equations are determined experimentally, and by measuring the ⁄ can be wavelength shift of the two gratings and the temperature, the value of the nonlinear function attained. Experimental setup 1. Flow cell: the sketch of the flow cell, its picture, and the block diagram of the experimental setup are shown in the three figures below. 2. Fabrication of the gratings Temperature characterization Refractive index measurements FBG: by irradiating a photosensitive B-Ge co-doped optical fiber (Fibercore PS1250/1500) through a rectangular phase mask (1059.9 nm period) with an Excimer KrF laser [14]; LPG: by irradiating the same fiber through an appropriately shaped and focused laser spot; the ad hoc developed fabrication setup is made up of a motorized translation stage and a control/management program for choosing both the grating period and the number of shots for each step (point-to-point technique). The maximum sensitivity and resolution (3120 nm/RIU and 2*10-5 RIU) are observed when the refractive index of the solution is close to that of the fiber cladding. To summarize, the proposed system makes it possible to accurately measure the refractive index and to control the following parameters: strain: by means of the FBG, with a resolution of 15 pm corresponding to ±3.8 pm of ∆ ; temperature: by means of the thermocouple, with a resolution of 0.01 °C corresponding to ±3.6 pm of ∆ ; temperature stabilization: by means of the TEC system (tenth of degree). 3. 4. Note: interference problem of the attenuation bands. Interrogation system: for each measurement step, the software routine centers at the resonance wavelength, fixes the λ-span (LPG: 20 nm; FBG: 2 nm), acquires the spectrum and extrapolates the minimum wavelength by means of a Lorentzian data fitting (first for the LPG and then for the FBG). Fluidics system and chemicals Solutions at a different refractive index (1.334 – 1.467) were prepared by mixing glycerol and water in different ratios, and the refractive index was measured by means of a hand-held refractometer. Measurement protocol: flow rate of about 0.5 mL/min for 4 minutes, afterwards halting of the pump and acquisition of FBG and LPG minima for 10 minutes. References [1] M. Cooper, Label-free screening of bio-molecular interactions, Anal. Bioanal. Chem., vol. 377, pp. 834-842, 2003. [2] X. Fan, I. M. White, S. I. Shopova, H. Zhu, J. D. Suter, and Y. Sun, Sensitive optical biosensors for unlabeled targets: a review, Anal. Chim. Acta, vol. 620, pp. 8-26, 2008. [3] P. Pilla, P. Foglia Manzillo, V. Malachovska, A. Busciolo, S. Campopiano, A. Cutolo, L. Ambrosio, M. Giordano, and A. Cusano, Long period grating working in transition mode as promising technological platform for label-free biosensing, Opt. Express, vol. 17, pp. 20039-20050, 2009. [4] H. J. Patrick, A. D. Kersey, and F. Bucholtz, Analysis of the response of long period fibre gratings to external index of refraction, J. Lightwave Technol., vol. 16, pp. 1606-1612, 1998. [5] S. W. James, and R. P. Tatam, Optical fibre long-period grating sensors: characteristics and application, Meas. Sci. Technol., vol. 14, pp. R49-R61, 2003. [6] B. H. Lee, Y. Liu, S. B. Lee, S. S. Choi, and J. N. Jang, Displacements of the resonant peaks of a long-period fiber grating induced by a change of ambient refractive index, Opt. Lett., vol. 22, pp. 1769-1771, 1997. [7] Y. Zhu, J. H. Chong, P. Shum, H. Haryono, A. Yohana, M. K. Rao, and C. Lu, Measurements of refractive index sensitivity using long-period grating refractometer, Opt. Comm., vol. 229, pp. 65-69, 2004. [8] V. Bhatia, Applications of long-period gratings to single and multi-parameter sensing, Opt. Express, vol. 4, pp. 457-466, 1999. [9] V. Bhatia, D. Campbell, R. O. Claus, and A. Vengsarkar, Simultaneous strain and temperature measurement with long-period gratings, Opt. Lett., vol. 22, pp. 648-650, 1997. [10] F. Baldini, M. Brenci, R. Falciai, A. Giannetti, C. Trono, F. Chiavaioli, and M. Mugnaini, Long period and fiber Bragg gratings written within the same fiber for sensing purposes, Proceedings of SPIE Photonics West, vol. 7941, paper [7941-40], San Francisco California, USA, 2011. [11] C. Trono, F. Baldini, M. Brenci, F. Chiavaioli, and R. Falciai, Flow cell with hybrid LPF and FBG optical fiber sensor for refractometric measurements, Submitted to 21st International Conference on Optical Fiber Sensors, OFS-21, 15-19 May, Ottawa, Canada, 2011. [12] C. Trono, F. Baldini, M. Brenci, F. Chiavaioli, R. Falciai, and A. Giannetti, Cascaded optical fibre long period and Bragg gratings for strain and temperature cross-sensitivities compensation in refractive index measurements, Submitted to SPIE Optics + Optoelectronics Conference, 18-21 April, Prague, Czech Republic, 2011. [13] C. Trono, F. Baldini, M. Brenci, F. Chiavaioli, and M. Mugnaini, Flow cell for strain- and temperature-compensated refractive index measurements by means of cascaded optical fibre long period and Bragg gratings, Submitted to Meas. Sci. Technol.. [14] K. O. Hill, and G. Meltz, Fibre Bragg grating technology fundamentals and overview, J. Lightwave Technol., vol. 15, pp. 1263-1276, 1997. [15] T. Erdogan, Cladding-mode resonances in short- and long-period fibre grating filters, J. Opt. Soc. Am. A, vol. 14, pp. 1760-1773, 1997.