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Optical fiber gratings have developed into a mature technology with a wide range of applications in various areas, including physical sensing for temperature, strain, acoustic waves and pressure. All of these applications rely on the perturbation of the period or refractive index of a grating inscribed in the fiber core as a transducing mechanism between a quantity to be measured and the optical spectral response of the fiber grating. This paper presents a relatively recent variant of the fiber grating concept, whereby a small tilt of the grating fringes causes coupling of the optical power from the core mode into a multitude of cladding modes, each with its own wavevector and mode field shape. The main consequence of doing so is that the differential response of the modes can then be used to multiply the sensing modalities available for a single fiber grating and also to increase the sensor resolution by taking advantage of the large amount of data available. In particular, the temperature cross-sensitivity and power source fluctuation noise inherent in all fiber grating designs can be completely eliminated by referencing all the spectral measurements to the wavelength and power level of the core mode back-reflection. The mode resonances have a quality factor of 10 5 , and they can be observed in reflection or transmission. A thorough review of experimental and theoretical results will show that tilted fiber Bragg gratings can be used for high resolution refractometry, surface plasmon resonance applications, and multiparameter physical sensing (strain, vibration, curvature, and temperature).
Optical fiber gratings have developed into a mature technology with a wide range of applications in various areas, including physical sensing for temperature, strain, acoustic waves and pressure. All of these applications rely on the perturbation of the period or refractive index of a grating inscribed in the fiber core as a transducing mechanism between a quantity to be measured and the optical spectral response of the fiber grating. This paper presents a relatively recent variant of the fiber grating concept, whereby a small tilt of the grating fringes causes coupling of the optical power from the core mode into a multitude of cladding modes, each with its own wavevector and mode field shape. The main consequence of doing so is that the differential response of the modes can then be used to multiply the sensing modalities available for a single fiber grating and also to increase the sensor resolution by taking advantage of the large amount of data available. In particular, the temperature cross-sensitivity and power source fluctuation noise inherent in all fiber grating designs can be completely eliminated by referencing all the spectral measurements to the wavelength and power level of the core mode back-reflection. The mode resonances have a quality factor of 10 5 , and they can be observed in reflection or transmission. A thorough review of experimental and theoretical results will show that tilted fiber Bragg gratings can be used for high resolution refractometry, surface plasmon resonance applications, and multiparameter physical sensing (strain, vibration, curvature, and temperature).
High sensitivity biological sample measurement has been achieved by using a 10° tilted fiber Bragg grating sensing probe. Human acute leukemia cells with different intracellular densities were clearly discriminated by identifying their slight refraction index (RI) perturbations in the range from 1.3342 to 1.3344, combining with a temperature self-calibration property. We studied the relationship between the intracellular density of cells (S50 and S60) and their RIs, the experimental results provide a potential way to verify the hypothesis for "density alteration in non-physiological cells (DANCE)". The tilted fiber Bragg gratings (TFBGs) [1,2], due to the induction of a tilted angle between the UV laser beam and the fiber axis (otherwise similar to the normal straight fiber grating), provides an effective way which couples the input light from the forward-propagating core mode to backwardpropagating cladding modes [3][4][5][6]. Because of these cladding excitations, TFBG shows good sensitivity to surrounding refraction index (SRI) change [7][8][9][10][11]. With the increase of tilt angle, the envelope of the cladding-mode resonance shifts towards shorter wavelength, which shows a much improved RI sensitivity as these cladding modes propagate close to the interface between the cladding mode and the outside media. The dominant cladding modes of TFBG cover the very important region near 1.3 which can be used to measure the water and water-like solutions. Therefore, TFBGs provide a good choice for biochemical sensing. At the same time, all the wavelength resonances of a TFBG have the same temperature dependence (they shift by ~10 pm/°C), so we could only consider the relative wavelength shifts and the temperature cross sensitivity over RI measurement can be definitely eliminated [12]. In this paper, the discrimination of a group of biological samples, named S50 and S60 (corresponding to cells with different intracellular densities), which were separated from human acute leukemia cell line (K562) [13][14][15][16][17][18] by using discontinuous sucrose gradient centrifugation (DSGC) [19,20], has been achieved through a high sensitivity RI measurement by using a 10° TFBG sensing probe. By comparing the slight RI difference between S50 and S60 (ranging from 1.3343 to1.3344), we studied the relationship between the intracellular density of cells and their RI, which provide a potential way to verify the hypothesis for "density alteration in non-physiological cells (DANCE)" [21,22].
In this paper, the mode coupling mechanism of tilted fiber Bragg gratings (TFBGs) is briefly introduced at first. And a general review on the fabrication, theoretical and experimental research development of TFBGs is presented from a worldwide perspective, followed by an introduction of our current research work on TFBGs at the Institute of Modern Optics, Nankai University (IMONK), including TFBG sensors for single-parameter measurements, temperature cross sensitivity of TFBG sensors, and TFBG-based interrogation technique. Finally, we would make a summary of the related key techniques and a remark on prospects of the research and applications of TFBGs.
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