Integrated optical sensor based on a FBG in parallel with a LPG

LIANG Ju-fa, JING Shi-mei, MENG Ai-hua, CHEN Chao, LIU Yun, YU Yong-sen*

( 1.State Key Laboratory on Integrated Optoelectronics,College of ElectronicScience and Engineering,Jilin University, Changchun 130012,China;2.State Key Laboratory of Luminescence and Application,Changchun Institute of Optics,Fine Mechanics and Physics,Chinese Academy of Sciences,Changchun 130033,China)*Corresponding author, Email:yuys@jlu.edu.cn

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Integrated optical sensor based on a FBG in parallel with a LPG

LIANG Ju-fa1, JING Shi-mei1, MENG Ai-hua1, CHEN Chao2, LIU Yun2, YU Yong-sen1*

( 1.State Key Laboratory on Integrated Optoelectronics,College of ElectronicScienceandEngineering,JilinUniversity,Changchun130012,China;2.StateKeyLaboratoryofLuminescenceandApplication,ChangchunInstituteofOptics,FineMechanicsandPhysics,ChineseAcademyofSciences,Changchun130033,China)*Correspondingauthor,Email:yuys@jlu.edu.cn

In order to improve the performance of the fiber optic sensors and further reduce the size of them, a new integrated optical sensor based on a fiber Bragg grating(FBG) in parallel with a long-period grating(LPG) in a single mode fiber is reported in this paper. The FBG and the LPG are fabricated by femtosecond laser using direct inscription process. The variations of temperature and refractive index will cause the variations of resonant wavelengths of FBG and LPG. The experimental results show that the refractive index sensitivities of the FBG and the LPG respectively are 0 nm/RIU and 196.46 nm/RIU, and the temperature sensitivities of them are 12.98 pm/℃ and 10.93 pm/℃ respectively. Therefore, this sensor can be used for measuring temperature and refractive index simultaneously according to the dual parameters sensing matrix.

integrated optical sensor;fiber Bragg grating(FBG);long-period grating(LPG);femtosecond laser

1　Introduction

Since the first fiber grating was fabricated by the standing wave method in 1978[1], the fiber grating has attracted considerable attention for applications in telecommunications and fiber sensor systems[2-8]. In-fiber gratings, including fiber Bragg gratings(FBGs) and long-period gratings(LPGs), have been used to measure various physical parameters. In the FBGs the forward-propagating core mode is coupled to the backward-propagating core mode, while in the LPGs the core mode is coupled to the cladding mode with its evanescent fields extending to the surrounding environment. As a result, FBGs are sensitive to the temperature and strain, while LPGs are sensitive to the surrounding refractive-index(SRI) besides temperature and strain[6-8]. Because FBGs and LPGs have different optical properties, there is a great interest in combination of the FBG and the LPG as a novel sensor. Recently, Ming Hanetal. have demonstrated an optical fiber refractometer based on a cladding-mode Bragg grating, which consists of a LPG followed by a FBG[9]. Similarly, Ming Yue-Fu has suggested that one may achieve measurement of SRI using a concatenation of a FBG and a LPG[10]. To our knowledge, most previous publication have used concatenation of the FBG and the LPG to measure physical parameters. However, the size of these sensors based on concatenation of the FBG and the LPG(2-gratings-length) are larger than the single LPG or FBG, thus, it is not convenient to utilize them in the integrated optical system. Femtosecond laser direct inscription technology can be used to inscribe vavious sizes of gratings in any position of the optical fiber, and the RI modulation intensity of gratings can be controled through the regulation of the laser power. Thus, the difficulty of the optical integration in fiber is greatly reduced with this technology.

In this article, we propose a simple and novel integrated optical sensor based on a FBG in parallel with a LPG by femtosecond direct inscription technology. The sensor consists of a FBG and a LPG, in which the FBG is inscribed in the center position of the fiber core, while LPG is in the off-center position. Thus, this integration of the FBG and the LPG is much smaller(1-grating-length). The FBG and the LPG in this sensor have maintained their respective optical properties: the FBG is sensitive to temperature, but not to SRI, while the LPG is sensitive to temperature and SRI. Therefore, the working principle of the sensor is that the changes of temperature and SRI result in the different wavelength changes of the FBG's resonant peak and the LPG′s. According to the dual parameters matrix, we can use these different wavelength changes to measure temperature and refractive index simultaneously.

2　Experiments

The FBG and the LPG in this integrated optical sensor were inscribed in the SMF-28e by femtosecond direct inscription process. The schematic diagram of the sensor is shown in Fig.1. In our experiments, a Ti:sapphire regenerative amplifier laser system(Spectra Physics) operating at 800 nm was adopted. The laser beam was focused into the fiber core via an oil-immersed 60 Olympus objective(N.A.,1.42). We mounted the fiber on a computer-controlled three-axis translation stage with a motion spatial resolution of 20 nm. The transmission spectra of the sensor were monitored by a broadband light source(Superk Compact, NKT Photonics) and an optical spectrum analyzer(OSA, AQ6370D, Yokogawa) with a resolution of 0.02 nm.

Fig.1　Schematic diagram of the integrated optical sensor

Fig.2　Side-view microscope image of RI modulation region of the FBG and the LPG in the fiber core(the inset is the enlarged view of the grating structure)

Fig.3　Transmission spectra of the FBG and the FBG in parallel with the LPG in the oil(the inset is the details of the Bragg resonant peak)

Fig.4　Transmission spectrum of the integrated optical sensor in the air and the high order cladding modes corresponding to the loss peaks of the LPG

First of all, the laser frequency and the laser power were respectively set at 100 Hz and 70 nJ/pulse, and the translation speed of the fiber was set at 0.107 1 mm/s. Using point-by-point(PbP) direct inscription process[11], a 2.4-mm-long FBG was written in the center of the fiber core, and the period of which was 1.07 μm. Thus it is the second order FBG with a Bragg wavelength around 1 550 nm. Then we set the laser frequency at 1 000 Hz and the translation speed at 0.01 mm/s, and the laser power was maintained at 70 nJ/pulse to write the LPG. The 2.4-mm-long LPG was written at the position deviated from the center of the core of about 1.8 μm, which was in parallel with the FBG as shown in Fig.2. The period of the LPG is 60 μm. We can observe that the fabrication process of LPG did not damage the RI modulation region of the FBG. In Fig.3, we can note that in the fabrication process, the inscription of the LPG did not vary the wavelength of the FBG resonant peak, however, just reduced the overall power of the transmission. Fig.4 shows the experimental transmission spectrum of the sensor in the air. We can observe that there are seven loss peaks of the LPG and one Bragg resonant peak from 1 100 nm to 1 700 nm. The reason why we inscribe this short period compact LPG is that it has a high surrounding refractive-index(SRI) sensitivity[12]. According to the previous report[12], we can infer that the seven loss peaks of the LPG correspond to seven different cladding modes(HE1, 20 and HE1, 23 correspond to the first order diffraction, and HE1, 29-HE1, 33 correspond to the second-order diffraction). Because of the high localization of the PbP FBG, there are some cladding mode resonances in the shortwave direction of Bragg resonant peak, but it does not affect the performance of the sensor. In the FBG the forward-propagating core mode is coupled to the backward-propagating core mode, while in the LPG the core mode is coupled to the cladding mode. In this integrated optical sensor, the FBG and the LPG maintain their respective properties.

3　Sensing characteristics

After the fabrication process, we studied the sensing characteristics of the integrated optical sensor. The loss peak around 1 555 nm corresponding to the HE1, 29 mode at the second-order diffraction and the Bragg resonant peak at 1 550 nm were chosen for sensing applications. We first measured the SRI sensitivity of the sensor. The fiber sensor was placed into a glass slot and kept it straight. After the sensor was fixed, we injected RI solutions into the glass slot so that the sensor was totally immersed. After the spectrum was recorded, the sensor were then cleaned using ethanol and deionized water. The procedure was repeated to measure the other RI solutions(different volume ratio of glycerin and water mixed solutions). The RI of the solution was measured by the Abbe refractometer at room temperature. As shown in Fig.5, in the RI range from 1.33 to 1.44, the wavelength of the resonant peak of the FBG almost has no change, while the loss peak of the LPG exhibits an obvious redshift. From the function of the loss peak wavelength shift and the SRI, we can achieve the RI sensitivity of 196.46 nm/RIU and the linearity of 0.994 8, as shown in Fig.6(a).

Fig.5　Shifts of the loss peak wavelength of the sensor with different RI solutions

Fig.6　(a)Wavelengths of the Bragg resonant peak and the LPG loss peak change with the SRI, (b)wavelengths of the Bragg resonant peak and the LPG loss peak change with temperature

The temperature sensitivity of the sensor was also measured. The sensor was placed in a digitally controlled furnace. Later, the furnace was heated up from 30 ℃ to 90 ℃ with the increment of 10 ℃ for one step. After one-step increment, we kept the sensor at that temperature for 20 minutes and recorded the transmission spectrum at each step. We can observe that the wavelengths of the chosen loss peak and the Bragg resonant peak have redshift with the increasement of temperature(as shown in Fig.6(b) ). In this temperature range, we analysis the function of the FBG′s and the LPG′s resonant wavelengths and the temperature, and we obtain that the temperature sensitivities of the FBG and the LPG are 12.98 pm/℃ and 10.93 pm/℃, respectively, and their linearities are 0.999 6 and 0.999 3. We can observe that the temperature sensitivity of the LPG is very small, even smaller than the FBG′s. The reason is that the LPG in this sensor was writen in the off-center position and the period of the LPG is just 60 μm, which is much smaller than the general LPGs(hundreds of micrometers). When the temperature changes, the changes of effective indice and the period of the LPG are smaller than the other LPGs. Therefore, this LPG has such small temperature sensitivity.

As mentioned above, the sensitivities of the Bragg resonant peak to temperature and SRI are different with the sensitivities of the loss peak of LPG, so this integrated optical sensor can be used to measure temperature and SRI simultaneously. The relationship between these variables can be expressed in the form of matrix:

(1)

whereA1 andA2 are the SRI sensitivity and temperature sensitivity for the Bragg resonant peak respectively, whileB1 andB2 are the sensitivities for the loss peak of LPG. Substituting the values obtained from experiments into the matrix, the final expression can be written as:

(2)

4　Conclusion

In conclusion, we have fabricated a small size and novel integrated optical sensor based on a FBG in parallel with a LPG in a common SMF using fs-laser direct inscription process. The length of this integrated optical sensor is 2.4 mm. The RI modulation of the gratings can be controlled through changing laser pulses power, laser frequency and the translation speed of the fiber. In addition, we have demonstrated the measurement for temperature and the SRI by this sensor and obtained the sensing matrix to achieve dual parameters sensing.

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Authors′ biographies：

2016-03-03；

2016-03-23

吉林省科技發(fā)展計(jì)劃資助項(xiàng)目(No.20150520089JH)；長(zhǎng)春市科技局重大科技攻關(guān)專項(xiàng)資助項(xiàng)目 (No.13KG22)

2095-1531(2016)03-0329-06

基于光纖布拉格光柵與長(zhǎng)周期光柵并聯(lián)的集成光學(xué)傳感器

梁居發(fā)1，敬世美1，孟愛(ài)華1，陳超2，劉云2，于永森1*

(1.吉林大學(xué) 電子科學(xué)與工程學(xué)院 集成光電子國(guó)家重點(diǎn)實(shí)驗(yàn)室，吉林 長(zhǎng)春 130012；2. 中國(guó)科學(xué)院 長(zhǎng)春光學(xué)精密機(jī)械與物理研究所 發(fā)光學(xué)及應(yīng)用國(guó)家重點(diǎn)實(shí)驗(yàn)室，吉林 長(zhǎng)春 130033)

為了提高光纖傳感器的性能和進(jìn)一步縮小傳感器的尺寸，通過(guò)實(shí)驗(yàn)制備出一種基于光纖布拉格光柵(FBG)與長(zhǎng)周期光柵(LPG)并聯(lián)的新型集成光學(xué)傳感器。該傳感器中的FBG和LPG是利用飛秒激光直寫技術(shù)直接在普通單模光纖中刻寫的。FBG和LPG是并聯(lián)關(guān)系，因此很大程度地縮小了傳感器的長(zhǎng)度。外界的溫度和折射率的變化會(huì)引起FBG和LPG的諧振峰波長(zhǎng)位置發(fā)生變化，據(jù)此對(duì)該集成傳感器進(jìn)行溫度和折射率測(cè)量。實(shí)驗(yàn)結(jié)果表明：FBG諧振峰對(duì)折射率和溫度的靈敏度分別為0 nm/RIU和12.98 pm/℃，而LPG在1 555 nm附近諧振峰對(duì)折射率和溫度的靈敏度為196.46 nm/RIU和10.93 pm/℃。因此，根據(jù)雙參數(shù)傳感矩陣，該傳感器可以對(duì)溫度和外界折射率進(jìn)行同時(shí)傳感。

集成光學(xué)傳感器；光學(xué)布拉格光柵(FBG)；長(zhǎng)周期光柵(LPG)；飛秒激光

TN253

A

LIANG Ju-fa(1990—), male, born in Yunfu, Guangdong Province. He received his bachelor's degree in College of Electronic Science and Engineering, Jilin University in 2013. Now he is a master student in College of Electronic Science and Engineering, Jilin University. His research interest is optical fiber sensors. E-mail:souldean@163.com

YU Yong-sen(1974—), male, born in Changchun, Jilin Province. He received his doctor's degree in College of Electronic Science and Engineering, Jilin University in 2005. And now he is a professor in College of Electronic Science and Engineering, Jilin University. His research interest is optical fiber gratings and optical fiber sensors. E-mail:yuys@jlu.edu.cn

10.3788/CO.20160903.0329

Supported by Jilin Provincial Science and Technology Development Plan Project(No.20150520089JH)， Changchun City Science and Technology Bureau Major Scientific Research Project(No.13KG22)