Micro-Structured Fiber Interferometer as Sensitive Temperature Sensor

: We report on a fast and sensitive temperature sensor using a micro-structured or photonic crystal fiber interferometer with a high germanium doped fiber core. The wavelength sensitivity for temperature variation was as high as ∆λ/∆Τ= 78 pm/ ℃ up to 500 ℃ , which was 6 times more sensitive than the fiber Bragg grating temperature sensitivity of ∆λ/∆Τ= 13 pm/ ℃ at 1550 nm. The sensor device was investigated concerning the sensitivity characteristics and response time.


Introduction
Many different kinds of temperature fiber sensors have been demonstrated by different research groups. A simple structure like a temperature fiber sensor was manufactured using a Fabry-Perot interferometer made between two cleaved sapphire fiber end faces [1]. Nguyen et al. [2] reported a temperature sensor using a combination of multi-single-multimode fibers between single mode fibers with a high temperature sensitivity of 88 pm/℃. Villatoro et al. [3] reported a new kind of Mach-Zehnder fiber interferometer where a photonic crystal fiber (PCF) stub was spliced between single mode fibers, and in the splice region, the PCF voids were fully collapsed. Two years later, a Mach-Zehnder fiber interferometer was demonstrated as the temperature sensor, after a long fiber annealing [4], and a temperature sensitivity of about 8 pm/℃ was demonstrated. Similar to the interferometer presented here, many other research groups reported on fiber optic sensors to measure temperature. In 2009, Larrion et al. [5] reported an interferometer using a commercial PCF as the temperature sensor, but the low temperature range of operation and the necessity of nanoparticles deposition make the sensor impracticable for outdoor applications. In the same year, Peiró et al. [6] reported a temperature sensor using a suspended core fiber with the germanium doped core, the group filled the fiber with a liquid and found a high temperature sensitivity of 25 nm/℃, and the need to fill the fiber with liquid can make the production slow and increase costs.
Other sensors were reported as temperature sensors, using liquids inside of the PCF voids, such as ethanol [7] or a colloid [8]. The sensitivities found in these cases were 6.6 nm/℃ and 70 pm/℃, respectively.
However, until now, the devices that use the fiber filled with liquid have only a short operation range. Another temperature sensor reported used a combination of splices between multimode fiber-PCF-and single mode fibers [9], where a temperature sensitivity of 73 pm/℃ was demonstrated, but the device needed the 40-cm PCF for its preparation. In this paper, we report on a small and simple fiber interferometer as the temperature sensor which used a PCF with a high concentration of germanium inside its core. In contrast to the papers mentioned above, the device had a short length (< 2.0 mm) and did not require any fiber annealing to operate until 500 ℃. The device was designed for operation in reflection. The PCF was spliced between two single mode fibers in order to build an interferometer. In the splicing regions, the PCF voids were fully collapsed while the solid fiber core was conserved. A numerical simulation was performed in order to explain the interference of guided modes in the PCF.

Principle
A PCF with a specially doped germanium core as shown in Fig. 1 was used to build the interferometer. The fiber core consisted of a double refractive index structure. The highly doped central core with a diameter of 1.2 µm was surrounded by a pedestal-like structure with a diameter of 3.4 µm. As shown in Fig. 1(b), the core had a shaped concentration profile with approximately 32 mol% (right side) at its top and 13 mol% at the maximum of the pedestal. The PCF specifications are shown in Table 1.
The fiber was spliced between pieces of conventional single mode fibers (SMF). In the splicing region, the PCF voids were fully collapsed, as represented in Fig. 2. In the first splice (SMFPCF), the fundamental core mode and higher order cladding modes of the PCF got excited, and the second splice (PCFSMF) had the function of combining the excited modes. The advantage of having a PCF with a high refractive index in the core (germanium doped) is that the light can be guided in the cladding region (in particular in our case due to the device having the fully collapsed region and because the PCF core was smaller than the SMF core). The PCF allows the propagation of different modes in the cladding due to its specific structure as reported in [10,11]. In the microstructure cladding region, leaky modes can propagate with a (complex) refractive index below the value of the fundamental space filling mode. This effect is sometimes also called the pseudo-bandgap [12].  The power distribution between the interfering modes could be adjusted by an offset of the splice.
The second splice (PCFSMF) worked as the spatial filter which only collected the light from the PCF core. An interferometer with the same principle of the shifting core position was reported in [3,10]. The measured signal was an interference pattern in transmission. However, for practical measurement reasons, a reflection measurement concept is more advantageous. Therefore, we cleaved the second SMF one centimeter after the splice region and deposited a gold film with approximately 50-nm thickness on the fiber end face using a metal evaporation technique.
The gold film operated as a mirror in order to make the device operate in reflection and to improve the reflection signal in comparison to the Fresnel reflection in the silica-air interface (approximately 4%).
After the gold film deposition, the signal increased about 13 dB compared to the Fresnel reflection. Considering the operating wavelength around 1550 nm, which was used in the experimental setup, only the fundamental mode could propagate inside the fiber core [see Fig. 2(a)]. Nevertheless, the cladding was capable of guiding a high number of modes.
To determine the modes which could interfere with the fundamental core mode, the guided power was used with the first ring of air holes. The overlap of the fundamental mode [see Fig. 3(a)] with the doped core region was 71%, and the guided power within the first ring of air roles was 100%. The defect mode with the highest overlap in the first ring zone [see Fig. 3(b)] carried 6% of its power in the doped core and 35% within the first ring of air holes. These two modes interfered along their propagation inside the PCF. Generally, the interference of two modes can be described [4] as ( ) where I 1 and I 2 are the intensities of the fundamental mode and higher order cladding mode, respectively. L is the length of the PCF stub. The phase difference, θ , can be written as a function of the fiber length, the refractive index difference ∆n eff between the two interfering modes (∆n eff = n 1 -n 2 ), and the wavelength λ: where β 1 and β 2 are the propagation constants.
The refractive index difference between the modes can be calculated using the space between two consecutive peaks at the wavelengths λ 1 and λ 2 : The wavelength shifts a minimum of the interference pattern of (δλ n ) as a function of temperature variation (∆Τ ) of a single transmission dip can be written as a function of the refractive index: where ∆T is the temperature variation, and ∂∆n eff / ∂T is the variation of the effective refractive index difference of the guided modes with the temperature.
The influence of the thermally induced length change is equal for both modes and does not result in a wavelength shift. The value of the refractive index variation with the temperature depended strongly on the germanium doping level and was considerably higher than that for un-doped silica [6,7].
The thermo-optical coefficient of pure silica was 1.06×10 -5 K -1 [13]. The effect of germanium doping on the thermo-optical coefficient was reported in [14]. From these results, we could approximate a molar GeO 2 concentration slope on the thermo-refractive index of about 1.2×10 -7 K -1 mol% -1 . A variation of 15% Ge doping between the central core and the socket would result in a difference of the temperature coefficient of the modes of about ∂n eff / ∂T =1.6×10 -6 K -1 . The device had a length of 1.80 mm and a period of λ 2 −λ 1 , 44.39 nm. From these data, a wavelength sensitivity of 83 pm/K can be expected theoretically.
A temperature difference of 500 K would therefore result in an interference pattern shift of about 41 nm.

Sensor packaging and measurement
The fiber was packaged inside the metal tubing with the outside diameter of 1.0 mm and the inside diameter of 400 µm (see Fig. 4) with the alumina ceramic glue 989, which resisted up to 1500℃. Such an arrangement as shown in Fig. 4 assures the good mechanical stability. The device was tested in an oven for a temperature range between the room temperature and 500 ℃, with the heating and cooling rate of 10 ℃/min.
The temperature was monitored with a thermocouple PT100 placed next to the fiber sensor.
For illumination of the sensor, the broadband source (ASE) was used, and the details of the temperature were acquired with an optical spectrum analyzer.
The result is shown in Fig. 5. The inset of Fig. 5 is the reflection spectrum of the interferometer before (black dots) and after (upper line) the gold deposition in the end of the fiber. The total wavelength shift with the temperature (∆λ/∆Τ) was measured as 78 pm/℃. This value was about 6 times higher than that for a fiber Bragg grating. A fiber Bragg grating in the same fiber achieved a thermal sensitivity of 13 pm/℃, as shown in Fig. 6. As for an additional parameter, the response time for a temperature difference between the room temperature (~22 ℃) and high temperature of 500 ℃ in the oven was investigated.
The device was put in the oven and removed after 25 seconds approximately. The spectral sensor responses of both sensor types were measured. Figure 7 shows the wavelength shifts of the PCF interferometer (upper line) and the FBG (lower line), which were measured with a commercial FBG interrogator (IBSEN I-MON E-USB 2.0). The temperature response time of about 3.0 s from the room temperature to the high temperature for both cases (PCF interferometer device and FBG device) was measured, and the temperature response time of the high temperature to low temperature of about 14.0 s was measured. These are comparable values for both types of the sensor and attractive parameters for commercial applications.

Conclusions
We demonstrated the use of a new type of structured optical fiber in a modal interferometer for a sensitive temperature measurement. A gold film deposition was made at the end of the SMF in order to operate the device in reflection. The temperature dependence had a high temperature sensitivity of 78 pm/℃. A package suitable for the high temperature measurement has been presented. The small size, the possibility of using reflected signals and the high temperature stability up to more than 500 ℃ make such a sensing element applicable for harsh environment conditions.