**4. Fabrication and experimental observations on properties of a LPG based on PCF [38]**

#### **4.1 Fabrication of a PCF-LPG**

Unlike conventional fibers, which contain at least two different glasses each with a different thermal expansion coefficient, thereby giving rise to a relatively high thermal expansion coefficient, PCFs are virtually insensitive to temperature because it is made of only one material (and air holes). This property can be utilized to obtain temperature-insensitive PCFbased devices, as demonstrated in [14]. However, the single material property of PCFs leads to non-photosensitivity to UV light, therefore FBGs and LPGs cannot normally be formed in PCFs by use of the conventional UV-written technique, unless a PCF with a Ge-doped photosensitive core is used [26]. Recently, several alternative methods for making LPGs in PCFs with non-photosensitive cores were introduced, including glass structure change [27], periodic structural and/ or residual stress relaxation induced by arc discharge or a CO2 laser [28-32], refractive index modulation by periodically applied mechanical pressure [33] or by the use of an acoustic wave [34, 35], and periodic drilling micro-holes with a femto-second laser [36].

LPGs fabricated by use of a CO2 laser are compact and stable because the perturbations are everlasting whereas in LPGs fabricated by UV light in conventional fibers, the refractive index modulation caused by UV light are prone to aging, therefore making LPGs in conventional fibers unstable over time. Here, we demonstrate the fabrication method by using a CO2 laser, which has been used widely [30, 32, 37, 38, 40].

7.827×10-6

ξcl = 7.85×10-6

7.8×10-6

7.75×10-6

Fig. 9. Theoretical temperature sensitivity at resonance wavelength vs. LPG period for

400 450 500 550 600 **Period of LPG (μm)**

**4. Fabrication and experimental observations on properties of a LPG based** 

Unlike conventional fibers, which contain at least two different glasses each with a different thermal expansion coefficient, thereby giving rise to a relatively high thermal expansion coefficient, PCFs are virtually insensitive to temperature because it is made of only one material (and air holes). This property can be utilized to obtain temperature-insensitive PCFbased devices, as demonstrated in [14]. However, the single material property of PCFs leads to non-photosensitivity to UV light, therefore FBGs and LPGs cannot normally be formed in PCFs by use of the conventional UV-written technique, unless a PCF with a Ge-doped photosensitive core is used [26]. Recently, several alternative methods for making LPGs in PCFs with non-photosensitive cores were introduced, including glass structure change [27], periodic structural and/ or residual stress relaxation induced by arc discharge or a CO2 laser [28-32], refractive index modulation by periodically applied mechanical pressure [33] or by the use of an acoustic wave [34, 35], and periodic drilling micro-holes with a femto-second

LPGs fabricated by use of a CO2 laser are compact and stable because the perturbations are everlasting whereas in LPGs fabricated by UV light in conventional fibers, the refractive index modulation caused by UV light are prone to aging, therefore making LPGs in conventional fibers unstable over time. Here, we demonstrate the fabrication method by

using a CO2 laser, which has been used widely [30, 32, 37, 38, 40].

various values of ξcl and with taken from Fig. 5.





**Temperature sensitivity (nm/ oC)**

0.02

0.04

0.06

0

**on PCF [38]** 

laser [36].

**4.1 Fabrication of a PCF-LPG** 

Fig. 10 shows the experimental setup of the PCF-LPG fabrication. The CO2 laser operates at a frequency of 10 kHz and has a maximum power of 10 W. The laser power is controlled by the width of the laser pulses. In the experiment, the pulse-width of the CO2 laser was chosen to be 3.8 μs. The laser beam was focused to a spot with a diameter of ~60 μm and scanned across the ESM-PCF transversely and longitudinally along the fiber by use of a two-dimensional optical scanner attached to the laser head. The scanning step of the focused beam was 1 μm and the delay time of each step was 350 μs. The LPG inscribed has a period of about 467 μm and a period number of 40. The process of the CO2 laser scanning is repeated 9 times, which results in a LPG with a deep transmission dip and no observable deformity in the fiber structure. The spectrum measurements were performed using a broadband light source (a light-emitting diode, LED, with the wavelength range of 1200 ~1700 nm) in combination with an optical spectrum analyzer (OSA, ADVANTEST Q8384) with a resolution of 0.5 nm.

Fig. 10. Schematic of the PCF-LPG fabrication setup

Fig. 11 shows the growing process of a PCF-LPG as a function of the number of scanning procedures. The resonant wavelengths of the PCF-LPG are about 1552.45 nm and 1363.3 nm which are due to coupling of the fundamental core mode to two different cladding modes. The dip at the wavelength 1552.45 nm is nearly 20 dB. The insertion loss of the LPG is about 1.5 dB. The resonance at 1552.45 nm is due to coupling of the core mode to the cladding mode shown in Fig. 2 (b) and is in good agreement with the theoretical result (1552.45 nm resonance wavelength corresponds 467.2 μm LPG period) in Fig. 4.

#### **4.2 Properties of a LPG based on PCF in experiment**

Fig. 12 shows the experimental setup for measuring the characteristics of the PCF-LPG. The spectrum measurements were performed by using a broadband LED and an OSA with a

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 235

temperature insensitivity is *cl* =7.827 ×10-6, this value is slightly larger than that of the core and agrees with the prediction at the end of Section 4.2. It should be noted that the difference between *co* and *cl* for the PCF is 6 times smaller than that of conventional Ge-

Fig. 13. Transmission spectra of the PCF-LPG for applied strain of (from right to 1eft) 0, 535,

1530 1540 1550 1560 1570 **Wavelength (nm)**

**intensity (dB**

)






**Transmission** 

Strain increasing

Fig. 14. Resonant wavelength and the intensity at the transmission dip as functions of

**Strain (με)** 

0 500 1000 1500 2000

By exploiting the PCF-LPG's large sensitivity to strain and insensitivity to temperature, temperature-insensitive strain sensors are realized. These sensors can be based on either wavelength or intensity measurement. In this part, we demonstrate a simple, low cost strain sensor based on the measurement of the transmitted light intensity at a wavelength close to

**5. Applications of an LPG in PCF in optical fiber sensors** 

**5.1 Temperature-insensitive strain sensor based on a PCF-LPG [38]** 

doped fiber and 18 times smaller than that of B-Ge co-doped fiber [48].


1546

1548

1550

**Wavelength (nm)**

1552

1554



**Transmission intensity (dB)**



936, and 1604 μm

applied strain

the LPG resonance.

Fig. 11. Transmission spectra of the PCF-LPG with various numbers of repeated scans

resolution of 0.5 nm as mentioned in Section 4.1. The strain characteristics of the PCF-LPG was tested by stretching the PCF-LPG by moving the translation stage shown in Fig. 10 from 0 to 0.5 mm in four steps (corresponding to a strain variation of from 0 to 1604 με), the center wavelength of the transmission dip shifts toward shorter wavelength as shown in Fig. 13. This is opposite to a LPG in a conventional SMF where the transmission dip shifts toward longer wavelengths [23]. The strain dependence of the resonance wavelength 1552.45 nm on axial strain is shown in Fig. 14. The strain sensitivity, which is the slope of the curve, is estimated to be -2.68 nm/ 1000 μm and shown in Fig.7 as a small circle. By varying the strain coefficient of the cladding material *cl* to fit the experimental data, we found the value of *cl* that best fits the experimental sensitivity is *cl* =-0.22115. The transmitted intensity at resonance wavelength was found increases with the applied axial strain, and this is also shown in Fig. 14.

Fig. 12. Experimental setup for measuring the temperature and strain characteristics of the PCF-LPG, where a broadband source and an OSA are used.

To test the temperature characteristics of the PCF-LPG, the ambient temperature of the LPG was varied by using a temperature chamber whose temperature can be controlled within the range of 25 oC to 100 oC. As shown in Fig.15, the transmission spectrum hardly changes when temperature was raised from 25 oC to 100 oC. The estimated sensitivity of the resonant wavelength to temperature is about 0.007 nm/ oC. Again, the temperature sensitivity of the PCF-LPG is marked as a circle in Fig.9. The cladding temperature coefficient *cl* that fits this

2

Number of repeated scans

Fig. 11. Transmission spectra of the PCF-LPG with various numbers of repeated scans

this is also shown in Fig. 14.

resolution of 0.5 nm as mentioned in Section 4.1. The strain characteristics of the PCF-LPG was tested by stretching the PCF-LPG by moving the translation stage shown in Fig. 10 from 0 to 0.5 mm in four steps (corresponding to a strain variation of from 0 to 1604 με), the center wavelength of the transmission dip shifts toward shorter wavelength as shown in Fig. 13. This is opposite to a LPG in a conventional SMF where the transmission dip shifts toward longer wavelengths [23]. The strain dependence of the resonance wavelength 1552.45 nm on axial strain is shown in Fig. 14. The strain sensitivity, which is the slope of the curve, is estimated to be -2.68 nm/ 1000 μm and shown in Fig.7 as a small circle. By varying the strain coefficient of the cladding material *cl* to fit the experimental data, we found the value of *cl* that best fits the experimental sensitivity is *cl* =-0.22115. The transmitted intensity at resonance wavelength was found increases with the applied axial strain, and

1200 1300 1400 1500 1600 1700 **Wavelength (nm)**

Fig. 12. Experimental setup for measuring the temperature and strain characteristics of the

Fixed

Movable

Glue LPG

PCF

To test the temperature characteristics of the PCF-LPG, the ambient temperature of the LPG was varied by using a temperature chamber whose temperature can be controlled within the range of 25 oC to 100 oC. As shown in Fig.15, the transmission spectrum hardly changes when temperature was raised from 25 oC to 100 oC. The estimated sensitivity of the resonant wavelength to temperature is about 0.007 nm/ oC. Again, the temperature sensitivity of the PCF-LPG is marked as a circle in Fig.9. The cladding temperature coefficient *cl* that fits this

PCF-LPG, where a broadband source and an OSA are used.

Broadband source


**Transmission (dB)**

Glue

Fixed Fixed temperature insensitivity is *cl* =7.827 ×10-6, this value is slightly larger than that of the core and agrees with the prediction at the end of Section 4.2. It should be noted that the difference between *co* and *cl* for the PCF is 6 times smaller than that of conventional Gedoped fiber and 18 times smaller than that of B-Ge co-doped fiber [48].

Fig. 13. Transmission spectra of the PCF-LPG for applied strain of (from right to 1eft) 0, 535, 936, and 1604 μm

**Strain (με)** 

Fig. 14. Resonant wavelength and the intensity at the transmission dip as functions of applied strain

#### **5. Applications of an LPG in PCF in optical fiber sensors**

#### **5.1 Temperature-insensitive strain sensor based on a PCF-LPG [38]**

By exploiting the PCF-LPG's large sensitivity to strain and insensitivity to temperature, temperature-insensitive strain sensors are realized. These sensors can be based on either wavelength or intensity measurement. In this part, we demonstrate a simple, low cost strain sensor based on the measurement of the transmitted light intensity at a wavelength close to the LPG resonance.

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 237

nm, and 1563 nm. Therefore, the setup shown in Fig. 16 converts directly the strain variation to intensity variation. Assume that we choose a DFB laser at 1553nm as source, and use an optical power meter with a resolution of 0.001 dB, we may achieve a strain resolution of ~0.3με.

Fig. 17. Strain dependence of the transmission intensity of the PCF-LPG at different

**5.2 Temperature-insensitive demodulator based on a PCF-LPG for a fiber Bragg** 

Fiber Bragg grating (FBG) is another kind of optical fiber grating, and is formed by a periodic modulation of the refractive index along an optical ber with ~0.5 μm pitch Λ, which causes the coupling between the forward-propagating core mode to the backwardpropagating core mode at the reflective wavelength satisfied with the phase matching condition 2 *B eff n* , where λB is the reflective wavelength, *neff* is the effective refractive index of the core mode, respectively. By fabricating FBG with different pitch, we can get different reflective wavelength of FBG. The bandwidth of FBG is narrow compared with that of LPG, because the coupling strength decreases rapidly when the wavelength departs from *λB*. FBGs have been applied widely in sensors. Because of the wavelength-encoded nature of the FBG sensors, it is necessary to convert the wavelength-encoded signal into

0 500 1000 1500 2000

1563 1560 1555.6

**Strain (με)** 

In this part, we present the use of PCF-LPG for the purpose of making a temperature insensitive sensor interrogation based on the PCF-LPG's much lower temperature sensitivity and realize a whole fiber Bragg grating (FBG) temperature sensor, including a sensor head and a PCF-LPG readout component, in one package. Utilizing the wavelength-dependent transmission loss of the LPG, the wavelength change of the FBG due to the temperature of the environment is translated to the intensity of the output. At the output, only a power meter is required to deduce the temperature of the environment and an expensive OSA would not be needed. The experimental results show that the interrogation based on the

wavelengths

**grating temperature sensor [45]** 




**Transmission Intensity (dB)**


1538 1542

1545

1547.7

electronic signals for easy reading and real time monitoring.

PCF-LPG works well under different environmental temperatures.

Fig. 15. Transmission spectra of the LPG in the ESM PCF at various ambient temperatures

Fig. 16 shows the proposed strain sensor that uses the PCF-LPG as the sensing element. A single wavelength light such as a DFB laser is used as a light source. The wavelength of the DFB laser is near the resonant wavelength of the LPG and hence the output light intensity from the LPG will be directly related to the LPG's transmission at the wavelength of the DFB laser. Since the LPG's transmission is insensitive to temperature, the output power will only be affected by the transmission spectrum change caused by the strain applied to the LPG. At the output, an optical power meter will be adequate to deduce the strain information and an expensive OSA would not be needed.

Fig. 16. The proposed temperature insensitive strain sensor with a DFB laser and an optical power meter

Fig. 17 shows the measured relationship between the output intensity of the PCF-LPG sensor and the applied axial strain for various laser wavelengths. In the experiment, a tunable laser was used for easiness of wavelength adjustment. In practice, a DFB laser with appropriate wavelength would be a better for the purpose of reducing cost. As shown in Fig.17, for laser wavelengths of 1538 nm, 1542 nm, 1545 nm, and 1547.7 nm, which are shorter than the resonant wavelength (1552.45 nm) the LPG, the output intensity decreases with applied strain and the strain sensitivity is negative and respectively -1.41, -2.17, -2.80 and -2.41 dB/1000 με for 1538 nm, 1542 nm, 1545 nm, and 1547.7 nm. The relationship is approximately linear for strains from 0 to 1600 με. Similarly, for laser wavelength longer than the resonant wavelength (1552.45nm), the output intensity increases with applied strain and the intensity sensitivities are positive and respectively 3.25, 3.11, 2.01 and 1.53 dB/ 1000 με at 1553 nm, 1555.6 nm, 1560

Fig. 15. Transmission spectra of the LPG in the ESM PCF at various ambient temperatures

information and an expensive OSA would not be needed.




**Transmission intensity (dB)**




DFB Laser

Fixed

Movable

LPG Glue

power meter

Fig. 16 shows the proposed strain sensor that uses the PCF-LPG as the sensing element. A single wavelength light such as a DFB laser is used as a light source. The wavelength of the DFB laser is near the resonant wavelength of the LPG and hence the output light intensity from the LPG will be directly related to the LPG's transmission at the wavelength of the DFB laser. Since the LPG's transmission is insensitive to temperature, the output power will only be affected by the transmission spectrum change caused by the strain applied to the LPG. At the output, an optical power meter will be adequate to deduce the strain

1520 1540 1560 1580 **Wavelength (nm)**

Fig. 16. The proposed temperature insensitive strain sensor with a DFB laser and an optical

PCF

Glue

Power-meter

Fixed Fixed

Fig. 17 shows the measured relationship between the output intensity of the PCF-LPG sensor and the applied axial strain for various laser wavelengths. In the experiment, a tunable laser was used for easiness of wavelength adjustment. In practice, a DFB laser with appropriate wavelength would be a better for the purpose of reducing cost. As shown in Fig.17, for laser wavelengths of 1538 nm, 1542 nm, 1545 nm, and 1547.7 nm, which are shorter than the resonant wavelength (1552.45 nm) the LPG, the output intensity decreases with applied strain and the strain sensitivity is negative and respectively -1.41, -2.17, -2.80 and -2.41 dB/1000 με for 1538 nm, 1542 nm, 1545 nm, and 1547.7 nm. The relationship is approximately linear for strains from 0 to 1600 με. Similarly, for laser wavelength longer than the resonant wavelength (1552.45nm), the output intensity increases with applied strain and the intensity sensitivities are positive and respectively 3.25, 3.11, 2.01 and 1.53 dB/ 1000 με at 1553 nm, 1555.6 nm, 1560 nm, and 1563 nm. Therefore, the setup shown in Fig. 16 converts directly the strain variation to intensity variation. Assume that we choose a DFB laser at 1553nm as source, and use an optical power meter with a resolution of 0.001 dB, we may achieve a strain resolution of ~0.3με.

Fig. 17. Strain dependence of the transmission intensity of the PCF-LPG at different wavelengths

#### **5.2 Temperature-insensitive demodulator based on a PCF-LPG for a fiber Bragg grating temperature sensor [45]**

Fiber Bragg grating (FBG) is another kind of optical fiber grating, and is formed by a periodic modulation of the refractive index along an optical ber with ~0.5 μm pitch Λ, which causes the coupling between the forward-propagating core mode to the backwardpropagating core mode at the reflective wavelength satisfied with the phase matching condition 2 *B eff n* , where λB is the reflective wavelength, *neff* is the effective refractive index of the core mode, respectively. By fabricating FBG with different pitch, we can get different reflective wavelength of FBG. The bandwidth of FBG is narrow compared with that of LPG, because the coupling strength decreases rapidly when the wavelength departs from *λB*. FBGs have been applied widely in sensors. Because of the wavelength-encoded nature of the FBG sensors, it is necessary to convert the wavelength-encoded signal into electronic signals for easy reading and real time monitoring.

In this part, we present the use of PCF-LPG for the purpose of making a temperature insensitive sensor interrogation based on the PCF-LPG's much lower temperature sensitivity and realize a whole fiber Bragg grating (FBG) temperature sensor, including a sensor head and a PCF-LPG readout component, in one package. Utilizing the wavelength-dependent transmission loss of the LPG, the wavelength change of the FBG due to the temperature of the environment is translated to the intensity of the output. At the output, only a power meter is required to deduce the temperature of the environment and an expensive OSA would not be needed. The experimental results show that the interrogation based on the PCF-LPG works well under different environmental temperatures.

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 239

the output intensity of the PCF-LPG with the temperature on the FBG and that this relationship is virtually linear for temperature from 25 to 100 oC. In this temperature range (75 oC), the change in the reflected wavelength from the FBG is 0.75 nm, and the intensity change of the output power via the LPG is 1.2 dB. Thus the sensitivity of the proposed FBG temperature sensor is about -0.0165 dB/ oC. Because the slope of the transmission spectrum in the wavelength range from 1545 to 1548 nm is virtually constant as implied by Fig. 21, the linear dynamic range of this temperature sensor is at least 300 oC. Therefore, this setup converts the temperature variation to wavelength variation (FBG) and then it converts the

Fig. 19. The reflective spectrum of the FBG (curve 1) at room temperature and the

curve 1

1520 1540 1560

**wavelength (nm)**

curve 2

Fig. 20. The output spectra from PCF-LPG when a different temperature (25 oC, 30, 40, 50, 60,

wavelength variation to intensity variation (PCF-LPG).

transmission spectrum of the LPG (curve 2)




**Intensity (dB)**




70, 80, 90, 100 oC) is applied to the FBG.

Fig. 18 shows the schematic diagram and the experimental setup of the proposed fiber Bragg grating temperature sensor interrogation system using an LPG in a PCF. The sensor head was made of a FBG and was illuminated using a broadband LED via a 3-ports circulator. The sensor head was placed inside a temperature-controlled container in order to detect its sensitivity to temperature. The reflected light from the sensor head is returned to the circulator and enters the PCF-LPG. In the experiment, the central reflection wavelength of the FBG sensor head was chosen as shown in Fig. 19. The FBG was fabricated in a hydrogenloaded single-mode fiber using a phase mask illuminated by UV light. The phase mask had a constant period of 1068 nm (the corresponding grating period is 534 nm). The original centre wavelength of the FBG sensor is at 1546.3 nm, which is located at the middle of the wavelength range of the transmission spectrum of the LPG with the negative slope. The reflected light from the sensor head is transmitted partially by the PCF-LPG and the amount of transmission is a function of wavelength. The wavelength shift of the FBG sensor head with temperature is almost linearly related to the transmission function of PCF-LPG filter for the range of operation. The power at the output of the PCF-LPG is directly related to the temperature applied on the FBG because as the temperature increases, the wavelength of the light reflected by the FBG shifts more to a longer wavelength, which in tune causes the light to leading to PCF-LPG to decrease in intensity. At the output, only a power meter is enough to deduce the temperature of environment. Thus it is very feasible to monitor the variation in temperature by measuring the output power of the PCF-LPG in a relatively cheap manner.

Fig. 18. Schematic diagram of the proposed temperature sensor interrogation system based on a PCF-LPG, IMG: index matched glue, OC: optical circulator.

When the FBG sensor was put into a temperature chamber and the temperature was increased from 25 to 100 oC, the Bragg reflection of the FBG would shift to longer wavelengths due to the thermo-optic effect and the thermo-expansion effect of the optical fiber. Fig. 20 shows the output spectra. The intensity of the output changes in accordance with the transmission curve of the PCF-LPG, which is as the reflection wavelength of the FBG gets longer, the output of the PCF-LPG gets smaller. Fig. 21 shows the relationship of

Fig. 18 shows the schematic diagram and the experimental setup of the proposed fiber Bragg grating temperature sensor interrogation system using an LPG in a PCF. The sensor head was made of a FBG and was illuminated using a broadband LED via a 3-ports circulator. The sensor head was placed inside a temperature-controlled container in order to detect its sensitivity to temperature. The reflected light from the sensor head is returned to the circulator and enters the PCF-LPG. In the experiment, the central reflection wavelength of the FBG sensor head was chosen as shown in Fig. 19. The FBG was fabricated in a hydrogenloaded single-mode fiber using a phase mask illuminated by UV light. The phase mask had a constant period of 1068 nm (the corresponding grating period is 534 nm). The original centre wavelength of the FBG sensor is at 1546.3 nm, which is located at the middle of the wavelength range of the transmission spectrum of the LPG with the negative slope. The reflected light from the sensor head is transmitted partially by the PCF-LPG and the amount of transmission is a function of wavelength. The wavelength shift of the FBG sensor head with temperature is almost linearly related to the transmission function of PCF-LPG filter for the range of operation. The power at the output of the PCF-LPG is directly related to the temperature applied on the FBG because as the temperature increases, the wavelength of the light reflected by the FBG shifts more to a longer wavelength, which in tune causes the light to leading to PCF-LPG to decrease in intensity. At the output, only a power meter is enough to deduce the temperature of environment. Thus it is very feasible to monitor the variation in temperature by measuring the output power of the PCF-LPG in a relatively cheap

Fig. 18. Schematic diagram of the proposed temperature sensor interrogation system based

Broadband LED

FBG IMG

When the FBG sensor was put into a temperature chamber and the temperature was increased from 25 to 100 oC, the Bragg reflection of the FBG would shift to longer wavelengths due to the thermo-optic effect and the thermo-expansion effect of the optical fiber. Fig. 20 shows the output spectra. The intensity of the output changes in accordance with the transmission curve of the PCF-LPG, which is as the reflection wavelength of the FBG gets longer, the output of the PCF-LPG gets smaller. Fig. 21 shows the relationship of

on a PCF-LPG, IMG: index matched glue, OC: optical circulator.

Pout

OC

PCF-LPG

manner.

the output intensity of the PCF-LPG with the temperature on the FBG and that this relationship is virtually linear for temperature from 25 to 100 oC. In this temperature range (75 oC), the change in the reflected wavelength from the FBG is 0.75 nm, and the intensity change of the output power via the LPG is 1.2 dB. Thus the sensitivity of the proposed FBG temperature sensor is about -0.0165 dB/ oC. Because the slope of the transmission spectrum in the wavelength range from 1545 to 1548 nm is virtually constant as implied by Fig. 21, the linear dynamic range of this temperature sensor is at least 300 oC. Therefore, this setup converts the temperature variation to wavelength variation (FBG) and then it converts the wavelength variation to intensity variation (PCF-LPG).

Fig. 19. The reflective spectrum of the FBG (curve 1) at room temperature and the transmission spectrum of the LPG (curve 2)

Fig. 20. The output spectra from PCF-LPG when a different temperature (25 oC, 30, 40, 50, 60, 70, 80, 90, 100 oC) is applied to the FBG.

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 241

proposed sensor demodulation was used to read in optical power and an optical power meter (NF1112) with a resolution of 0.01 dB is used to monitor the output light intensity of the sensor. For monitoring transmission spectra of the FLM and the PCF-LPG, and explaining the principle of the sensor system, an OSA is used in experiments with a spectral

3dB coupler

PANDA Fiber

Tubular Oven

Fig. 22. Experimental setup of the proposed sensor, inset: micrograph of PCF.

PC Broadband

Filter

Source

Power meter

PCF LPG

in the experiment is the same one as mentioned above.

respectively, whose transmission spectra are shown in Fig.24.

The HiBi-FLM includes a 3 dB coupler, a 30.5 cm Panda PMF, and a polarization controller (PC). The Panda PMF has an attenuation of 1.0 dB/km, a measured birefringence of n = 6.24×10-4 at 1550 nm, and a core diameter~10 μm. Both ends of the Panda fiber were spliced to Corning SMF-28, and the combined loss of the two splicing points is 2.3 dB. The wavelength spacing between transmission peaks of the FLM is given by <sup>2</sup> / *n L* , where λ, Δn, and L are wavelength, birefringence and length of the HiBi fiber, respectively. The wavelength spacing between the transmission peaks of the FLM is about 13 nm at 1545 nm, as shown in Fig. 23. In the experiment, this value was chosen by considering the bandwidth of the PCF-LPG. When the PCF-LPG is given, a suitable wavelength spacing of the FLM can be obtained by choosing the length of the PMF. Thus by adjusting the state of the PC, one spectral peak of the FLM is located in a negative of the linear regions with the PCF-LPG at the initial state of the sensor. The temperature-insensitive of the PCF-LPG used

The band-pass filter is made of Metal-Dielectric-Metal (MDM), which is used to provide a narrow band light source. As shown the gray region in the Fig. 23, only the intensity in the band-pass of the filter is monitored by the optical power meter. In the experiment, several filters with the same center wavelength at 1545nm and different bandwidth are used to study the effect of the bandwidth of the filter on the sensing performance. The full width at half maximum (FWHM) of the band-pass filters is 12.66nm, 8.3 nm, 6.66 nm and 3 nm,

Fig.25 shows transmission spectra of the PCF-LPG, the HiBi-FLM, and the output signal at different temperature when the band-pass filter is not inserted. When temperature is increased, the transmission spectrum of the FLM blue-shifts due to thermally induced refractive index change and thermal expansion of the panda fiber, and the temperature sensitivity to wavelength is -0.772 nm/ oC. Due to the filtering function of the PCF-LPG, the

resolution of 0.02 nm.

Fig. 21. The measured output power for the temperature of the grating sensor

#### **5.3 A fiber loop mirror temperature sensor demodulation technique based on a PCF-LPG and a band-pass filter [46]**

Fiber loop mirrors (FLMs) have been demonstrated for a number of applications, for example wavelength filters and sensors [14, 15, 50]. In a FLM, two interfering waves counter-propagate through the same fiber, and are exposed to the same environment. This makes it less sensitive to environmental disturbance. Various kinds of sensors based on FLMs have been realized, such as temperature sensors, strain sensors, pressure sensors, liquid level sensors, biochemical sensors, UV detection, multi-parameter measurement and refractive index sensors. However, most HiBi-FLM sensors are based on monitoring the resonant wavelength variation of FLMs [15, 51], an expensive OSA is needed.

In this part, we present a HiBi-FLM temperature sensor using a PCF-LPG and a band-pass filter as a demodulator. For the sensing principle, only the HiBi-FLM acts as a sensor head, while the PCF-LPG serves as a filter to provide wavelength dependent optical power transmission and the band-pass filter is to provide a narrow band light source. By utilizing the stable filtering function of the PCF-LPG, the resonant wavelength variation of the FLM with temperature is transferred effectively to the intensity variation of the output light. When the optical intensity of the output is monitored, temperature applied on the FLM will be deduced. The experimental results show the demodulator based on the PCF-LPG and the band-pass filter works well. By choosing a filter with an appropriate bandwidth, the temperature sensitivity of the sensor with 1.742 dB/ oC is obtained.

Fig.22 shows the experimental setup. The configuration of the proposed sensor system includes a broadband light source, a band-pass filter, a HiBi-FLM, and a PCF-LPG. A broadband superluminescent LED (SLED) source with a flatten emission intensity in the wavelength range of 1530~1570 nm was used as an input light source, whose power is ~40 mW. The SLED with a band-pass filter launches the HiBi-FLM via a 3 dB coupler. The transmitted light from the HiBi-FLM then enters the temperature-insensitive PCF-LPG. The

0 20 40 60 80 100 120 **Temperature (oC)** 

Fig. 21. The measured output power for the temperature of the grating sensor

resonant wavelength variation of FLMs [15, 51], an expensive OSA is needed.

temperature sensitivity of the sensor with 1.742 dB/ oC is obtained.

**5.3 A fiber loop mirror temperature sensor demodulation technique based on a PCF-**

Fiber loop mirrors (FLMs) have been demonstrated for a number of applications, for example wavelength filters and sensors [14, 15, 50]. In a FLM, two interfering waves counter-propagate through the same fiber, and are exposed to the same environment. This makes it less sensitive to environmental disturbance. Various kinds of sensors based on FLMs have been realized, such as temperature sensors, strain sensors, pressure sensors, liquid level sensors, biochemical sensors, UV detection, multi-parameter measurement and refractive index sensors. However, most HiBi-FLM sensors are based on monitoring the

In this part, we present a HiBi-FLM temperature sensor using a PCF-LPG and a band-pass filter as a demodulator. For the sensing principle, only the HiBi-FLM acts as a sensor head, while the PCF-LPG serves as a filter to provide wavelength dependent optical power transmission and the band-pass filter is to provide a narrow band light source. By utilizing the stable filtering function of the PCF-LPG, the resonant wavelength variation of the FLM with temperature is transferred effectively to the intensity variation of the output light. When the optical intensity of the output is monitored, temperature applied on the FLM will be deduced. The experimental results show the demodulator based on the PCF-LPG and the band-pass filter works well. By choosing a filter with an appropriate bandwidth, the

Fig.22 shows the experimental setup. The configuration of the proposed sensor system includes a broadband light source, a band-pass filter, a HiBi-FLM, and a PCF-LPG. A broadband superluminescent LED (SLED) source with a flatten emission intensity in the wavelength range of 1530~1570 nm was used as an input light source, whose power is ~40 mW. The SLED with a band-pass filter launches the HiBi-FLM via a 3 dB coupler. The transmitted light from the HiBi-FLM then enters the temperature-insensitive PCF-LPG. The


**Intensity (dB)**

**LPG and a band-pass filter [46]** 

proposed sensor demodulation was used to read in optical power and an optical power meter (NF1112) with a resolution of 0.01 dB is used to monitor the output light intensity of the sensor. For monitoring transmission spectra of the FLM and the PCF-LPG, and explaining the principle of the sensor system, an OSA is used in experiments with a spectral resolution of 0.02 nm.

Fig. 22. Experimental setup of the proposed sensor, inset: micrograph of PCF.

The HiBi-FLM includes a 3 dB coupler, a 30.5 cm Panda PMF, and a polarization controller (PC). The Panda PMF has an attenuation of 1.0 dB/km, a measured birefringence of n = 6.24×10-4 at 1550 nm, and a core diameter~10 μm. Both ends of the Panda fiber were spliced to Corning SMF-28, and the combined loss of the two splicing points is 2.3 dB. The wavelength spacing between transmission peaks of the FLM is given by <sup>2</sup> / *n L* , where λ, Δn, and L are wavelength, birefringence and length of the HiBi fiber, respectively. The wavelength spacing between the transmission peaks of the FLM is about 13 nm at 1545 nm, as shown in Fig. 23. In the experiment, this value was chosen by considering the bandwidth of the PCF-LPG. When the PCF-LPG is given, a suitable wavelength spacing of the FLM can be obtained by choosing the length of the PMF. Thus by adjusting the state of the PC, one spectral peak of the FLM is located in a negative of the linear regions with the PCF-LPG at the initial state of the sensor. The temperature-insensitive of the PCF-LPG used in the experiment is the same one as mentioned above.

The band-pass filter is made of Metal-Dielectric-Metal (MDM), which is used to provide a narrow band light source. As shown the gray region in the Fig. 23, only the intensity in the band-pass of the filter is monitored by the optical power meter. In the experiment, several filters with the same center wavelength at 1545nm and different bandwidth are used to study the effect of the bandwidth of the filter on the sensing performance. The full width at half maximum (FWHM) of the band-pass filters is 12.66nm, 8.3 nm, 6.66 nm and 3 nm, respectively, whose transmission spectra are shown in Fig.24.

Fig.25 shows transmission spectra of the PCF-LPG, the HiBi-FLM, and the output signal at different temperature when the band-pass filter is not inserted. When temperature is increased, the transmission spectrum of the FLM blue-shifts due to thermally induced refractive index change and thermal expansion of the panda fiber, and the temperature sensitivity to wavelength is -0.772 nm/ oC. Due to the filtering function of the PCF-LPG, the

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 243

the peaks of the FLM shift to shorter wavelengths with temperature increasing. Therefore, the intensity of the output light changes periodically with temperature increasing. The change in the transmission wavelength of the FLM is 13nm corresponding to 16 oC temperature period, which is consistent with the wavelength spacing of 13 nm between the transmission peaks of the FLM. In order to certify the explaining, we take out the band-pass filter and measure the transmission spectra of the output signal at three different

Fig. 25. Transmission spectra of the FLM, the PCF-LPG and output signal when temperature

c

40 45 50 55 60 65 70 **Temperature(**℃**)**

Fig. 26. The relationship of the output power and temperature when the band-pass filter is

temperatures, which are marked in Fig.26.

is applied to the sensing head.





**Intensity(dB)**


a

b

with a central a wavelength 1545 nm and FWHM 12.66nm.



intensity of the resonant peak1 increases while the resonant peaks shift to shorter wavelength with temperature increasing. Therefore, when a band-pass filter is used, as shown in Fig.23, the part of the output light outside the band of the filter is attenuated owing to the function of the band-pass filter. And the intensity of the remainder will change with the transmission peak of the HiBi-FLM shifting. Therefore, converting the wavelength variation of the HiBi-FLM into intensity variation at the output directly is realized.

Fig. 23. Transmission spectra of the FLM, the PCF-LPG and the output signal. Gray region is transmission spectra of the sensor with band-pass filter.

Fig. 24. Transmission spectra of the band-pass filters used in the experiment.

Fig.26 shows the relationship of the output intensity of the sensing system with temperature applied on the FLM, when the filter was chosen with a FWHM 12.66 nm and a center wavelength at 1545 nm. The output intensity is approximately a periodic function of temperature. The period is 16 oC and temperature increases from 45.5 oC to 61.5 oC in a period. This behavior can be explained by the periodic property of the FLM. Since the transmission spectrum of the FLM is approximately a periodic function of the wavelength, the peaks of the FLM enter, then shift outside the pass-band of the filter one by one when

intensity of the resonant peak1 increases while the resonant peaks shift to shorter wavelength with temperature increasing. Therefore, when a band-pass filter is used, as shown in Fig.23, the part of the output light outside the band of the filter is attenuated owing to the function of the band-pass filter. And the intensity of the remainder will change with the transmission peak of the HiBi-FLM shifting. Therefore, converting the wavelength

Fig. 23. Transmission spectra of the FLM, the PCF-LPG and the output signal. Gray region is

Fig. 24. Transmission spectra of the band-pass filters used in the experiment.

Fig.26 shows the relationship of the output intensity of the sensing system with temperature applied on the FLM, when the filter was chosen with a FWHM 12.66 nm and a center wavelength at 1545 nm. The output intensity is approximately a periodic function of temperature. The period is 16 oC and temperature increases from 45.5 oC to 61.5 oC in a period. This behavior can be explained by the periodic property of the FLM. Since the transmission spectrum of the FLM is approximately a periodic function of the wavelength, the peaks of the FLM enter, then shift outside the pass-band of the filter one by one when

transmission spectra of the sensor with band-pass filter.

variation of the HiBi-FLM into intensity variation at the output directly is realized.

the peaks of the FLM shift to shorter wavelengths with temperature increasing. Therefore, the intensity of the output light changes periodically with temperature increasing. The change in the transmission wavelength of the FLM is 13nm corresponding to 16 oC temperature period, which is consistent with the wavelength spacing of 13 nm between the transmission peaks of the FLM. In order to certify the explaining, we take out the band-pass filter and measure the transmission spectra of the output signal at three different temperatures, which are marked in Fig.26.

Fig. 25. Transmission spectra of the FLM, the PCF-LPG and output signal when temperature is applied to the sensing head.

Fig. 26. The relationship of the output power and temperature when the band-pass filter is with a central a wavelength 1545 nm and FWHM 12.66nm.

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 245

Fig. 27. Transmission spectra of the HiBi-FLM, the PCF-LPG and the output signal when

FWHM=12.66nm FWHM=8.3nm FWHM=6.66nm FWHM=3nm

40 45 50 55 60 65 70 **Temperature(**℃**)**

Fig. 28. The relationships of the output power and temperature when different lters are

temperature applied on the sensor element is (a) 40°C, (b) 45.5°C, and (c) 53.5°C.


used.




**Intensity(dB)**



0

Fig.27 shows the transmission spectra of the HiBi-FLM, the PCF-LPG, and the output signal without the band-pass filter when temperature is applied at 40 oC, 45.5 oC and 53.5 oC, respectively. The region between the dotted lines is the bandwidth of the band-pass filter. It is clear that the peaks of the FLM shift inside and outside the filter with temperature increasing. Due to the filtering function of the PCF-LPG, the intensity of the output is decided by the location of the FLM's peak in the band of the filter. When the peak is located within a shorter wavelength of the LPG's transmission spectrum, in which a higher transmission is provided, the intensity of the output is larger, as shown in Fig.27 (a) and (c). Obviously, Fig.27 (b) shows the opposite situation. In this case, the peak of the FLM in the filter is near to the transmission dip of the PCF-LPG, thus the intensity of the output is lowest. As shown in Fig.26, the relationship is virtually proportional for temperature from 45.5 oC to 53.5 oC. In this temperature range (8 oC), the intensity change of the output power is 4.137 dB and the change in the transmission wavelength of the FLM is ~6.52 nm which is about half period of the FLM. The fitting function can be written as 3 2 *yx x x* 0.0227 3.3477 163.52 2636.6 with the fitting degree of <sup>2</sup> *R* 0.9978 . The average sensitivity of the proposed FLM temperature sensor is about 0.783 dB/ oC. When using a power meter with the resolution of 0.01dBm, the temperature resolution is obtained 0.013 oC. The measured temperature range is decided by the wavelength spacing between transmission peaks of the FLM which is given by λ2/ΔnL, where λ, Δn, and L are the wavelength, the birefringence and the length of the HiBi fiber, respectively. So we can widen the measured temperature range by shortening the length of the FLM. At the same time, a shorter sensor head is convenient in some applications, even though the sensitivity of the sensor will be decreased.

In order to study the effect of the band-pass filter on the sensing performance, several band-pass filters with a center wavelength 1545 nm are used, whose FWHM are 8.3 nm, 6.66 nm and 3 nm, respectively. A serial of experiments are carried out in the same way. Fig.28 shows the relationships of the output intensity and temperature when different filters are used. It is clear that all of them are periodic function and temperature period is 16 oC. The working range of the positive variation region is 8 oC, which is consistent with that of the filter with FWHM 12.66nm. This is because that the wavelength spacing between the transmission peaks of the FLM is not changed all the times. However, they have shown two marked differences: monotone interval and the output intensity range. Table I shows the properties of the proposed FLM temperature sensor when different filters are used.

From Table I, it can be concluded that the average sensitivity of the sensor is higher and the starting temperature of the monotone interval is lower when a filter with a narrower bandwidth is chosen. The reason is that, the transmission peak of the FLM shifts outside the filter band earlier and faster, the monotonicity of the relationship curve will change earlier and the output intensity range will vary larger, and the average sensitivity is also lager because of the same temperature range. When the filter is chosen a FWHM 3 nm with a center wavelength at 1545nm, the average sensitivity of the proposed FLM temperature sensor is about 1.742dB/oC. When a power meter with the resolution of 0.01dBm is used, the temperature resolution is obtained 0.006 oC.

Fig.27 shows the transmission spectra of the HiBi-FLM, the PCF-LPG, and the output signal without the band-pass filter when temperature is applied at 40 oC, 45.5 oC and 53.5 oC, respectively. The region between the dotted lines is the bandwidth of the band-pass filter. It is clear that the peaks of the FLM shift inside and outside the filter with temperature increasing. Due to the filtering function of the PCF-LPG, the intensity of the output is decided by the location of the FLM's peak in the band of the filter. When the peak is located within a shorter wavelength of the LPG's transmission spectrum, in which a higher transmission is provided, the intensity of the output is larger, as shown in Fig.27 (a) and (c). Obviously, Fig.27 (b) shows the opposite situation. In this case, the peak of the FLM in the filter is near to the transmission dip of the PCF-LPG, thus the intensity of the output is lowest. As shown in Fig.26, the relationship is virtually proportional for temperature from 45.5 oC to 53.5 oC. In this temperature range (8 oC), the intensity change of the output power is 4.137 dB and the change in the transmission wavelength of the FLM is ~6.52 nm which is about half period of the FLM. The fitting function can be written as 3 2 *yx x x* 0.0227 3.3477 163.52 2636.6 with the fitting degree of <sup>2</sup> *R* 0.9978 . The average sensitivity of the proposed FLM temperature sensor is about 0.783 dB/ oC. When using a power meter with the resolution of 0.01dBm, the temperature resolution is obtained 0.013 oC. The measured temperature range is decided by the wavelength spacing between transmission peaks of the FLM which is given by λ2/ΔnL, where λ, Δn, and L are the wavelength, the birefringence and the length of the HiBi fiber, respectively. So we can widen the measured temperature range by shortening the length of the FLM. At the same time, a shorter sensor head is convenient in some applications, even though the sensitivity of the sensor will be

In order to study the effect of the band-pass filter on the sensing performance, several band-pass filters with a center wavelength 1545 nm are used, whose FWHM are 8.3 nm, 6.66 nm and 3 nm, respectively. A serial of experiments are carried out in the same way. Fig.28 shows the relationships of the output intensity and temperature when different filters are used. It is clear that all of them are periodic function and temperature period is 16 oC. The working range of the positive variation region is 8 oC, which is consistent with that of the filter with FWHM 12.66nm. This is because that the wavelength spacing between the transmission peaks of the FLM is not changed all the times. However, they have shown two marked differences: monotone interval and the output intensity range. Table I shows the properties of the proposed FLM temperature sensor when different

From Table I, it can be concluded that the average sensitivity of the sensor is higher and the starting temperature of the monotone interval is lower when a filter with a narrower bandwidth is chosen. The reason is that, the transmission peak of the FLM shifts outside the filter band earlier and faster, the monotonicity of the relationship curve will change earlier and the output intensity range will vary larger, and the average sensitivity is also lager because of the same temperature range. When the filter is chosen a FWHM 3 nm with a center wavelength at 1545nm, the average sensitivity of the proposed FLM temperature sensor is about 1.742dB/oC. When a power meter with the resolution of 0.01dBm is used, the

decreased.

filters are used.

temperature resolution is obtained 0.006 oC.

Fig. 27. Transmission spectra of the HiBi-FLM, the PCF-LPG and the output signal when temperature applied on the sensor element is (a) 40°C, (b) 45.5°C, and (c) 53.5°C.

Fig. 28. The relationships of the output power and temperature when different lters are used.

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 247

same path and input to the monitor. By use of the differential processing ΔW= (W1-W2) / (W1+ W2), the measurement is free from the effect of power fluctuations of the light source

PCF LPG

3dB coupler

SLED

Filter1

Filter2

PC

Panda fiber

Tubular Oven

3dB coupler

1530 1535 1540 1545 1550 1555 1560 1565 1570 **Wavelength(nm)**

Fig.31 shows the relationship of the intensity signal W1 located within a negative linear region of the LPG's transmission spectrum with temperature applied on the FLM. When temperature changes from 47°C to 55°C, the intensity signal W1 will increase with temperature increasing, the sensitivity of the intensity signal W1 to temperature is about 0.01034 mw/°C, and the fitting function can be written as Y=0.0003X3-0.0468X2+2.3668X-39.652 with the fitting degree of R2 = 0.9984. While the intensity signal W2 will decrease when temperature increasing, the sensitivity of which is about -0.00882 mw/°C, and the fitting function can be written as Y= - 0.0004X3 + 0.0572X - 2.8888 + 48.448 with the fitting degree of R2 = 0.9982, as shown in Fig. 32. Fig. 31 and Fig. 32 also show the relationship of the intensity signal W1 and W2 with temperature when the power of the light source

Fig. 30. Transmission spectra of the FLM, the PCF-LPG and the two band-pass filters

W1 W2

and any other noises.

Output

Signal processing units

Fig. 29. Experimental setup of the proposed sensor

PD1

PD2


FLM PCF-LPG

**Intensity(dB)**


Table 1. Properties of the proposed FLM temperature sensor when different filters are used

#### **5.4 Demodulation based on a PCF-LPG with differential processing for a fiber loop mirror temperature sensor [47]**

Demodulation systems based on intensity measurement are widely used in optical sensors with simple structures and low costs. However, the sensing accuracy may be decreased since fiber sensor systems often include some noises due to light source fluctuations and all of power fluctuations in the system. In this part, the demodulation based on a PCF-LPG with differential processing for FLM temperature sensor was demonstrated to eliminate the noise of the sensor and raise the sensor accuracy. Utilizing the two linear regions of the transmission spectrum of the PCF-LPG, the variations of the FLM's two resonant wavelengths, which are located respectively within the positive and negative linear region of the LPG's transmission spectrum, are transferred effectively to the intensity variations at the same time. By differential processing of the two signals separated by two band-pass filters, the noise of the sensor is eliminated effectively since the two signals (also including the noise of fiber sensors) transmit through the same path. Experimental results show that the FLM temperature sensor with demodulation based on differential processing of the PCF-LPG is stable.

Fig.29 shows the experimental setup of a HiBi-FLM temperature sensor with the proposed demodulation system based on the PCF-LPG with differential processing. A broadband SLED launches into the HiBi-FLM sensor head. The transmitted light from the HiBi-FLM enters the PCF-LPG, and the output light is split into two beams by a 3 dB coupler, then the two beams enters the signal processing units via two band-pass filters, respectively. The demodulation system is constructed using a PCF-LPG, a 3 dB coupler and two band-pass filters with the full width at half maximum (FWHM) 6.66nm whose center wavelength are 1542nm and 1561.77nm. By utilizing the stable filtering function of the PCF-LPG, the variations of the FLM's resonant wavelengths with temperature, which are located within the positive and negative linear regions of the LPG's transmission spectrum, respectively are transferred effectively to the intensity variations simultaneously. The intensity signals provided by the PCF-LPG are separated effectively by the two band-pass filters whose transmission spectra are shown as the gray regions in Fig. 30. Both signals W1 and W2 are related with the measurand, while they also may include the all of fluctuation of the sensor system. When monitoring W1 or W2, we can obtain the information of temperature applied on the FLM sensor, but the accuracy will be low due to the effect of noises. W1 and W2 are gotten at the same condition since the light from the broadband source passes through the

Table 1. Properties of the proposed FLM temperature sensor when different filters are used

**5.4 Demodulation based on a PCF-LPG with differential processing for a fiber loop** 

Demodulation systems based on intensity measurement are widely used in optical sensors with simple structures and low costs. However, the sensing accuracy may be decreased since fiber sensor systems often include some noises due to light source fluctuations and all of power fluctuations in the system. In this part, the demodulation based on a PCF-LPG with differential processing for FLM temperature sensor was demonstrated to eliminate the noise of the sensor and raise the sensor accuracy. Utilizing the two linear regions of the transmission spectrum of the PCF-LPG, the variations of the FLM's two resonant wavelengths, which are located respectively within the positive and negative linear region of the LPG's transmission spectrum, are transferred effectively to the intensity variations at the same time. By differential processing of the two signals separated by two band-pass filters, the noise of the sensor is eliminated effectively since the two signals (also including the noise of fiber sensors) transmit through the same path. Experimental results show that the FLM temperature sensor with demodulation based on differential processing of the PCF-

Fig.29 shows the experimental setup of a HiBi-FLM temperature sensor with the proposed demodulation system based on the PCF-LPG with differential processing. A broadband SLED launches into the HiBi-FLM sensor head. The transmitted light from the HiBi-FLM enters the PCF-LPG, and the output light is split into two beams by a 3 dB coupler, then the two beams enters the signal processing units via two band-pass filters, respectively. The demodulation system is constructed using a PCF-LPG, a 3 dB coupler and two band-pass filters with the full width at half maximum (FWHM) 6.66nm whose center wavelength are 1542nm and 1561.77nm. By utilizing the stable filtering function of the PCF-LPG, the variations of the FLM's resonant wavelengths with temperature, which are located within the positive and negative linear regions of the LPG's transmission spectrum, respectively are transferred effectively to the intensity variations simultaneously. The intensity signals provided by the PCF-LPG are separated effectively by the two band-pass filters whose transmission spectra are shown as the gray regions in Fig. 30. Both signals W1 and W2 are related with the measurand, while they also may include the all of fluctuation of the sensor system. When monitoring W1 or W2, we can obtain the information of temperature applied on the FLM sensor, but the accuracy will be low due to the effect of noises. W1 and W2 are gotten at the same condition since the light from the broadband source passes through the

**mirror temperature sensor [47]** 

LPG is stable.

same path and input to the monitor. By use of the differential processing ΔW= (W1-W2) / (W1+ W2), the measurement is free from the effect of power fluctuations of the light source and any other noises.

Fig. 29. Experimental setup of the proposed sensor

Fig. 30. Transmission spectra of the FLM, the PCF-LPG and the two band-pass filters

Fig.31 shows the relationship of the intensity signal W1 located within a negative linear region of the LPG's transmission spectrum with temperature applied on the FLM. When temperature changes from 47°C to 55°C, the intensity signal W1 will increase with temperature increasing, the sensitivity of the intensity signal W1 to temperature is about 0.01034 mw/°C, and the fitting function can be written as Y=0.0003X3-0.0468X2+2.3668X-39.652 with the fitting degree of R2 = 0.9984. While the intensity signal W2 will decrease when temperature increasing, the sensitivity of which is about -0.00882 mw/°C, and the fitting function can be written as Y= - 0.0004X3 + 0.0572X - 2.8888 + 48.448 with the fitting degree of R2 = 0.9982, as shown in Fig. 32. Fig. 31 and Fig. 32 also show the relationship of the intensity signal W1 and W2 with temperature when the power of the light source

Long-Period Gratings Based on Photonics Crystal Fibers and Their Applications 249

Fig. 33. Relationship of ΔW and temperature when the power of light source changes.

In this chapter, we have presented the basic operation principle of LPGs, and demonstrated the special properties of PCF-LPGs. By use of a dispersion factor , a deeper understanding of the behavior of LPG in the ESM-PCF has been achieved. Both the theoretical and experimental results clearly reveal the significant effect of the waveguide dispersive characteristics of the cladding modes on the strain and temperature characteristics of the LPG in the ESM-PCF. By selecting proper grating period, it is possible to design a LPG with

47 48 49 50 51 52 53 54 55 **Temperature(**℃**)**

Power constanting Power increasing Power decreasing

We have shortly reviewed PCF-LPG fabrication methods and mainly described the fabrication method by using a CO2 laser. The PCF-LPG fabricated under the theoretical design shows a good agreement with the theoretical predictions. Finally, applications of the

[1] T. A. Birks, J. C. Knight, and P. St. J. Russell, "endlessly single-mode photonic crystal

[2] J. C. Knight, J. Broeng, and T. A. Birks, "Photonic band gap guidance in optical fibers"

[3] J. C. Knight. T. A. Birks, R. F. Cregan, P. St. J. Russell, And J. –P. de Sandro, " Large mode area photonic crystal fiber", *Electon. Lett*. vol. 43, no. 13, pp. 1347, Jul. 1998. [4] Ortigosa-Blanch, J. C. Knight, W. J. Wadsworth, J. arriaga, B. J. ManganT. A. Birks, and P.

St. J. Russell, "Highly birefringent photonic crystal fibers", *Optics Lett*., vol. 25, no.

PCF-LPG in optical fiber sensors have been demonstrated and discussed fully.

fiber", *Opt. Lett*. vol. 22, no. 13, pp. 961-963, Jul. 1997.

*Science*, vol. 282, no. 5393, pp.1476-1478, Nov. 1998.

**6. Summary** 


△**W(a.u.)**

**7. References** 

specific strain and temperature properties.

18, pp. 1325-1327, Sep. 2000.

increases 10% and decreases 10%. It is clear that the measurement will deviate from true value and the accuracy of temperature sensor is low.

Fig. 31. Relationship of W1 and temperature when the power of light source changes

Fig. 32. Relationship of W2 and temperature when the power of light source changes.

Fig.33 shows the relationship of the differential ΔW with temperature. The fitting function can be written as Y= -0.0075X3 + 1.138X2 - 57.382X + 959.39 with the fitting degree of R2 = 0.9976 when temperature rises from 47°C to 55°C. When the power of the light source increases 10%, keeps constant and decreases 10%, the relationship of the differential ΔW with temperature remains stable and the differential algorithm based on a PCF-LPG eliminates the noises effectively. When the power of the light source changes ±10%, the measured temperature is 49.83 °C and the relative error is 0.34%. Compared with the result without the differential ΔW, the accuracy of the HiBi-FLM sensor rises from ~90.5% to ~99.7%.

Fig. 33. Relationship of ΔW and temperature when the power of light source changes.
