The present invention relates generally to the field of optical fiber sensors and, more particularly, to an optical fiber based polymer core sensor.
Without limiting the scope of the invention, its background is described in connection with optical fiber sensors and their applications.
Most optical fiber biochemical sensors are based on measuring the RI of bio/chemical liquids using various sensing schemes such as interferometry [1], fiber gratings [2-5], and specialty fibers [7-11]. Interferometer-based RI sensors usually consist of two arms of light; one arm of light is influenced by the external medium and thus serves as the sensing arm while the other arm of light is used as the reference. When these two arms are combined to generate an interference pattern, a change in the external RI alters the optical path length of the sensing arm and thus causes a shift in the interference pattern. Interferometric RI sensors often require a mechanism to split the incoming light into two arms, resulting in a more complicated sensor system. Two types of fiber gratings, i.e. Fiber Bragg Grating (FBG) and Long Period Fiber Grating (LPFG), are commonly exploited for RI measurement. RI changes are measured from the shifts of the transmission/reflectance spectra due to the influence of the external RI on the coupling conditions of the fiber gratings. Because an LPFG couples the light from the core mode to the cladding modes, its transmission spectrum is highly sensitive to the changes of the external RI [2]. In comparison, the FBG-based RI sensors are usually much less sensitive because the light is mainly confined within the fiber core region. In order to increase the sensitivity, the cladding surrounding a FBG is often etched or thinned [3-4]. RI sensors based on fiber grating are usually expensive because of the stringent grating fabrication processes. Specialty fibers such as tapered fiber [7-8], and D-shaped fiber [9], microstructured fiber [10], and cladding stripped fiber [11] have also been developed for biochemical sensing. These types of optical fiber biochemical sensors require accessing the evanescent field at the fiber core/cladding interface. As such, precision micromachining is required in order to remove a part of the fiber cladding. In addition, many of these RI sensors require a long interaction length of more than a few millimeters to achieve a high RI sensitivity better than or comparable to the reported RI sensors [1,3,5-8].
For example, United States Published Patent Application No. 20030112443 (Hjelme et al.) describes a chemical sensing probe that detects chemical contents based on the volume change or the refractive index change of the chemically sensitive sensing materials that fill a Fabry-Perot cavity. The sensor requires the chemically sensitive sensing materials to react with the chemical contents so that either its volume or refractive index is changed. The change in volume and/or refractive index gives a change in an optical path length through the probe which can be measured interferometrically.
United States Published Patent Application No. 20090074349 (Hjelme et al.) describes the fabrication of interferometric fiber optic probes employing hydrogel sensor material that is responsive to an analyte; and to probes produced thereby. The invention relates particularly to probes which are suitable for invasive measurements of analytes in a live body. The sensor is fabricated on one fiber while the UV light is delivered by a second fiber.
U.S. Pat. No. 5,277,872 (Bankert) describes an optical fiber pH microsensor that includes an optical fiber having a portion of the surface of a light conducting core covered with a layer of a pH sensitive dye material. The dye material is covalently bonded to a polymeric matrix which is in turn covalently bonded to the optical fiber core to prevent leaching of the indicator dye material during extended use. The dye material is crosslinked in situ over the tip of the optical fiber core to yield a hydrophilic, ion permeable pH sensor which can be used intravascularly to monitor blood pH.
In addition, optical fiber sensors have also been widely used for temperature sensing since they have many advantages than conventional temperature sensors, e.g., they can safely operate in strong electromagnetic fields, in explosive or chemically aggressive environment and at areas under high voltage [12]. Among various fiber optic sensors, Fabry-Perot interferometric (FPI) sensors have distinct advantages over the others such as compactness, high sensitivity, small size, and polarization independence. FPI-based fiber optic sensors can be grouped as extrinsic FPI (EFPI) sensors and intrinsic FPI (IFPI) sensors. For EFPI sensors, the light signal is delivered and collected by the optical fiber and the modulation of the light occurs outside of the fiber. While in the IFPI sensor, the modulation of the light takes place inside the fiber. As “all fiber” sensors, IFPI sensors can reduce or eliminate the bonding problems experienced with extrinsic sensors. IFPI sensors are also more versatile for installation and are more robust. On the other hand, IFPI sensors are usually more difficult and expensive to fabricate [13]. Most of the reported IFPI sensors are based on manufacturing thin-film mirrors on the cleaved fiber end-face through vacuum deposition, magnetron sputtering or electron-beam evaporation [14-15]. However, thin film mirrors can easily be damaged. Besides, it is difficult to control the film thickness and flatness with precision. Another method that is being used to manufacture IFPI sensors is splicing two fibers with different core diameters as a reflective mirror [16]. But in order to fabricate an IFPI sensor with this configuration, the ends of fibers have to be polished with four different polishing films beforehand to prevent large power losses, which is a long and tedious process [16].
There is, therefore, a need for an optical fiber sensor that provides improved sensitivity and does not require specialized or complex materials.
The fabrication, analysis, and evaluation of a compact refractive index (RI) and temperature sensor using a micro-sized polymer core fabricated at the end of an optical fiber that uses low-cost commercial products and simplified fabrication techniques is described herein. The refractive index of the polymer used is different from that of the optical fiber so that a part of the light traveling in the optical fiber can be reflected at the fiber/polymer interface. The polymer tip serves as a Fabry-Perot interferometric cavity so that a phase shift is introduced to the light propagating in it when the RI of the surrounding medium changes and thus causes a fringe shift in the interferometric fringe spectrum. With respect to temperature measurements, the optical path traveled by the light coupled into the polymer tip changes with the ambient temperature due to the combination of thermal expansion and thermo-optic effect. Because the polymer tip has a high thermo-optic coefficient compared to silica, the temperature sensitivity of the sensor when used for temperature measurements is higher than most of the reported sensors that works under the same principle. The sensitivity of the sensor can be adjusted or modified by changing the length or shape of the polymer tip length and/or tailoring the properties of the polymer material. Moreover, the present invention does not require the use of cladding materials, dyes, etching or complex fabrication techniques. As a result, the present invention provides greater sensitivity and overcomes many of the limitations of other optical fiber based sensors.
More specifically, the present invention provides an optical fiber based polymer core sensor that includes an optical fiber having a core and an end having a cured polymer core affixed to the core of the optical fiber. The cured polymer core extends outward from the end of the optical fiber and has a diameter approximately equal to the core of the optical fiber. Note the cured polymer core can be substantially cylindrical, tapered or geometrically shaped. The optical fiber based polymer core sensor can be used to measure a temperature, measure a strain, measure a distance, measure a refractive index, detect or measure an analyte, detect a toxin, detect a biological agent, monitor a chemical process, or a combination thereof.
In addition, the present invention provides a method for fabricating an optical fiber based polymer core sensor. An optical fiber having a core is provided. A flat reflective object is aligned with the core of the optical fiber to provide a gap between the core and the flat reflective object. The flat reflective object can be a second optical fiber, a mirror or other suitable object. A light-curable polymer is deposited within the gap. A light is transmitted through the core such that the light-curable polymer forms a cured polymer core connecting the core to the reflective object. The cured polymer core has a diameter approximately equal to the core. The reflective object is then removed such that the cured polymer core remains affixed to the optical fiber.
Moreover, the present invention provides a method for fabricating an optical fiber based polymer core sensor. An optical fiber having a core is provided. A flat reflective object is aligned with the core of the optical fiber to provide a gap between the core and the flat reflective object. The flat reflective object can be a second optical fiber, a mirror or other suitable object. A white light is transmitted through the optical fiber. The gap is measured using the optical fiber and the reflective object as a white light Fabry-Perot interferometric distance sensor. The gap is adjusted to provide a specified distance between the optical fiber and the reflective object. A light-curable polymer is deposited within the gap. A light is transmitted through the core such that the light-curable polymer forms a cured polymer core connecting the core to the reflective object. The reflective object is then removed such that the cured polymer core remains affixed to the optical fiber. Any uncured light-curable polymer is removed. The cured polymer core and a portion of the optical fiber are then packaged.
The present invention is described in detail below with reference to the accompanying drawings.
The above and further advantages of the invention may be better understood by referring to the following description in conjunction with the accompanying drawings, in which:
While the making and using of various embodiments of the present invention are discussed in detail below, it should be appreciated that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed herein are merely illustrative of specific ways to make and use the invention and do not delimit the scope of the invention. The discussion herein relates primarily to optical fiber based polymer core sensors for refractive index and temperature sensor, but it will be understood that the concepts of the present invention are applicable to any optical fiber based sensors for strain measurement, distance measurement, toxin detection, biological agent detection, chemical process monitoring, pH measurement, analyte measurement, etc.
To facilitate the understanding of this invention, a number of terms are defined below. Terms defined herein have meanings as commonly understood by a person of ordinary skill in the areas relevant to the present invention. Terms such as “a”, “an” and “the” are not intended to refer to only a singular entity, but include the general class of which a specific example may be used for illustration. The terminology herein is used to describe specific embodiments of the invention, but their usage does not delimit the invention, except as outlined in the claims.
The fabrication, analysis, and evaluation of a compact refractive index (RI) and temperature sensor using a micro-sized polymer core fabricated at the end of an optical fiber that uses low-cost commercial products and simplified fabrication techniques is described herein. The refractive index of the polymer used is different from that of the optical fiber so that a part of the light traveling in the optical fiber can be reflected at the fiber/polymer interface. The polymer tip serves as a Fabry-Perot interferometric cavity so that a phase shift is introduced to the light propagating in it when the RI of the surrounding medium changes and thus causes a fringe shift in the interferometric fringe spectrum. With respect to temperature measurements, the optical path traveled by the light coupled into the polymer tip changes with the ambient temperature due to the combination of thermal expansion and thermo-optic effect. Because the polymer tip has a high thermo-optic coefficient compared to silica, the temperature sensitivity of the sensor when used for temperature measurements is higher than most of the reported sensors that works under the same principle. The sensitivity of the sensor can be adjusted or modified by changing the length or shape of the polymer tip length and/or tailoring the properties of the polymer material. Moreover, the present invention does not require the use of cladding materials, dyes, etching or complex fabrication techniques. As a result, the present invention overcomes many of the limitations of other optical fiber based sensors.
Now referring to
When light traveling inside the optical fiber 102 encounters the fiber/polymer interface 110, a portion of the light I1 is reflected due to the difference in RIs of the optical fiber 102 and the cured polymer core 108. The light transmitted into the polymer core 108 propagates along the polymer core 108 and are again partially reflected I2,j at the end 112 of the polymer core 108 due to the RI difference between the polymer core 108 and the surrounding medium 114. Tracing its path back, this reflected light I2,j reenters the optical fiber 102 and interferes with the light reflected at the SMF/polymer interface 110. As a result, the polymer core 108 serves as a Fabry-Perot interference (FPI) cavity, encoding the reflectance spectrum of the optical fiber sensor 100 with interference fringes. A change in the RI of the surrounding medium 114 alters the propagation constant of the light propagating inside the polymer core 108 and thus causes a shift of the fringe spectrum. By detecting the fringe shift using an optical spectrum analyzer, the correlation between the fringe shift and the RI change can be established. Note that depending on the intended use of the sensor 100, the polymer core 108 and a portion of the optical fiber 102 will typically be disposed within a package (not shown).
Referring now to
Now referring to
A more detailed description of a manufacturing process used to fabricate a sensor in accordance with the present invention will now be described. The polymer core is fabricated using the light-induced self-written (LISW) optical waveguide technology [23-24]. Unlike sensors previously reported in the literature and the prior art that uses a laser light and a custom-mixed resin to fabricate the waveguide, the present invention provides an economical technique that uses low-cost components, namely a UV light-emitting-diode (LED) and an UV-curable optical adhesive, to fabricate the polymer core. A UV LED (Nichia NSHU550A, wavelength 375 nm) is coupled to a single mode fiber (SMF). The cleaved SMF is mounted on a three-axis fiber alignment stage and is manually aligned with the LED. Different coupling mechanisms were studied. It was discovered that the maximum coupling from the LED to the SMF was achieved by removing the glass cover of the LED and directly butting the optical fiber against the LED chip. An optical power meter was employed to monitor the output power of the SMF during the alignment process in order to provide position feedbacks for the alignment. For a SMF of 0.5 m in length, the output power was 180 nW for a forward current of 50 mA. Even though the total output power was low, the power density of the UV light was sufficient to cure the epoxy in a few seconds.
In order to control the length of the polymer tip, two SMFs facing each other were first aligned under a microscope. The alignment mechanism consists of two V-grooved fiber holders. One is stationary while the other is mounted on a three-axis translation stage. The fiber on which the polymer tip is to be fabricated was mounted on the stationary stage. A second fiber was placed in the V-groove mounted on a translation stage so that it can be aligned to face the original fiber using the translation stage. An optical microscope was used to view the alignment at a greater magnification and help performing finer adjustments of the fiber position. The gap between the two fibers can be changed by traversing the translational stage along the fiber axis. Since the two fibers form a Fabry-Perot cavity, the gap between the two fibers can be measured by connecting the second fiber to a whitelight reflectance spectrum measurement system as shown in
The schematic for the set-up 500 used in the sensor evaluation is shown in
Now referring to
Referring now to
where I1(r) and φ1 represent the intensity and the phase of the fundamental mode reflected at the SMF/polymer core interface while I1(2j) and φ2j are the intensity and the phase of {right arrow over (I)}12j. Expressing the incoming light ash {right arrow over (I)}1=I1exp(−jφ), I1(r) and φ1 are calculated as:
where R1 is the reflectivity of the SMF/polymer interface and is determined by the RIs of the polymer core npolymer and the SMF nSMF [17]. The reflection of {right arrow over (I)}2j at the end of the polymer core is equivalent to the transmission of {right arrow over (I)}2j to a mirror image of the RI sensor. The power evolution of {right arrow over (I)}2j, therefore, is similar to the large power transfer between the fundamental mode and the higher order modes in abruptly tapered fibers [18-19]. The light transmitted to the polymer core at the SMF/polymer interface is given by
{right arrow over (I)}1(t)=(1−R1)I1exp(−jφ). (3)
Denoting the percentage of light coupled from {right arrow over (I)}1(t) to {right arrow over (I)}2j as C1j, {right arrow over (I)}2j along the length of polymer core can be expressed as:
{right arrow over (I)}2j(z)=C1jI1(t)exp └−jφ−j∫0zβj(ζ)dζ┘, (4)
where βj(z) is the propagation constants of the jth mode inside the polymer core. The light after the reflection at the end of the polymer core is:
{right arrow over (I)}2j(z)=R2C1jIj(t)exp └−j(φ+π)−j∫0zβj(ζ)dζ┘, (5)
where the reflectivity R2 at the polymer/medium interface is calculated from the RIs of the polymer core and the surrounding medium, i.e.
A phase shift of π is introduced because it is a reflection instead of a transmission. Finally, the light re-entering the SMF is calculated as:
Cj1 represents the percent of light coupled from {right arrow over (I)}2j to {right arrow over (I)}1(2j) and L is the physical length of the polymer core. Assuming the polymer core has a uniform RI along its length, Eq. (6) can be simplified as:
Combining Eq. (1), (2) and (7), the reflectance spectrum of the RI sensor is:
A change of the external RI changes the propagation constants βj and thus shifts the reflectance spectrum. Based on Eq. (8), there are two effects that contribute to the phase shift. The
term is due to the Fabry-Perot interference between {right arrow over (I)}1(r) and {right arrow over (I)}2j while the
term is due to the beating of different local modes {right arrow over (I)}2j inside the polymer core [18].
An analysis of a sensor for temperature measurements in accordance with the present invention will now be described. As previously stated the polymer core serves as a FPI cavity, i.e. it introduces two reflective interfaces; one at the SMF/polymer interface and the other at the polymer/air interface. The light traveling in the fiber core is first partially reflected at the fiber/polymer interface due to the difference between the refractive indices of the optical fiber and the polymer. The transmitted light then travels inside the polymer core and again is partially reflected at the polymer/air interface. When these two reflected lights are recombined in the optical fiber, they interfere with each other due to the different optical paths they have traveled. The interference spectrum contributed by the light reflected at the SMF/polymer interface I1 and the light reflected at the polymer/air interface I2 can be expressed as:
I=I1+I2+2√{square root over (I1I2)} cos(φ12). (9)
The phase shift φ12 is determined by the optical path difference (OPD) traveled by I1 and I2. Because the polymer tip does not have a cladding region, it operates as a multi-mode fiber (ncore=1.54, nclad=1.0, V=23 at 1310 nm) with multiple higher-order modes propagating inside it. When these higher-order modes reenter the optical fiber, they are partially coupled back to the fundamental mode due to the mode-coupling effect of the SMF/polymer interface. As a result, the interference spectrum is a summation of the interferences between the fundamental mode reflected at the SMF/polymer interface and the fundamental mode converted from the higher order modes propagating in the polymer tip [20], i.e.:
where I12,j is the intensity of the light converted from the jth mode to the fundamental mode and φ12,j is the phase shift between the fundamental mode I1 traveling in the fiber and the jth-order mode I2,j traveling in the polymer tip. For the fundamental mode I2,1, the phase shift φ12,1 can be expressed as:
φ12,1=2β1L, (11)
where L is the physical length of the polymer core. The propagation constant of the fundamental mode β1 can be calculated from the wavelength λ, the refractive index of the polymer core ncore, the V number V, and the polymer core radius ρ [21], i.e.:
where the modal parameter of the LP0j mode, Uj∞, is given by the root of the Bessel function of zero order, i.e.:
J0(Uj∞)=0. (13)
For the higher order modes, the phase shift φ12,j can be calculated as [21]:
φ12,j=2(β1+Δβ1j)L, (14)
where Δβ1j is the difference between the propagation constants of the fundamental mode LP01 and the jth order mode LP0j. At a large V number, Δβ1j can be approximated as [22]:
Since Δβ1j is much smaller than β1 for large V numbers, it only introduces a small phase shift to the interference spectrum I12. Therefore, the OPD of the two interfering lights is mainly determined by 2β1L. Combining Eq. (3) and (4), we can express the OPD as:
where χ is the wave number. Equation (8) indicates that the OPD is a function of the refractive index and the length of the polymer core. Since temperature affects these two parameters, a change in the ambient air temperature will cause a change in the OPD, and thus results in a shift in the reflectance spectrum.
The effect of temperature change on the OPD can be found by differentiating equation (16) with respect to temperature, i.e.:
Expressing the thermal expansion coefficient and thermo-optic coefficient of the polymer core material as
we can establish the relationship between the OPD changes and the temperature variations as:
As a result, the temperature variation is defined by:
Now referring to
The reflectance spectra of the sensor 100 with two different external RIs are shown in
The mode coupling at the SMF/polymer interface has a strong influence on the sensitivity of the RI sensor. Based on the calculation of βj, the higher order modes are more sensitive to the RI changes. To achieve the RI sensitivity observed by the experiment, we estimated at least four local modes should be presented in the polymer core with the power transfer coefficients C1j=Cj1=[0.5, 0.3, 0.12, 0.08] (see
Referring now to
The whitelight reflectance spectrum measurement system shown in
The performance of the sensor is evaluated with a 42 μm long polymer core using a central wavelength of 1310 nm. The results can be summarized with the graph shown in
Now referring to
The measured sensitivity versus the theoretical sensitivity was:
When the present invention is used for distance measurement, there is no limit on the minimum measurement distance. Note that the minimum distance actually measured was 4 microns. The fringe spacing is directly related to the OPD:
An example of using the present invention as a strain sensor is shown in
The sensor provided by the present invention can be designed for the range/sensitivity required.
In summary, the present invention describes a low cost fabrication technique to produce a compact optical fiber RI and temperature sensor. The sensitivity of the sensor to external RI changes was evaluated using RI standards. The RI resolution of the sensor is estimated to be 1.5e-5, assuming the measurement system has a spectral resolution of 1 pm. The design of the RI sensor, such as the RI and the length of the polymer core, can be easily adjusted using the fabrication technique of the present invention. The polymer tip sensor of the present invention was also evaluated for temperature measurements. Due to the high thermo-optic coefficient of the polymer material, a highly sensitive sensor was demonstrated. The sensitivity of the sensor can be further improved by tailoring the length of polymer tip or using a different polymer material.
All publications and patent applications mentioned in the specification are indicative of the level of skill of those skilled in the art to which this invention pertains. All publications and patent applications are herein incorporated by reference to the same extent as if each individual publication or patent application was specifically and individually indicated to be incorporated by reference.
The use of the word “a” or “an” when used in conjunction with the term “comprising” in the claims and/or the specification may mean “one,” but it is also consistent with the meaning of “one or more,” “at least one,” and “one or more than one.” The use of the term “or” in the claims is used to mean “and/or” unless explicitly indicated to refer to alternatives only or the alternatives are mutually exclusive, although the disclosure supports a definition that refers to only alternatives and “and/or.” Throughout this application, the term “about” is used to indicate that a value includes the inherent variation of error for the device, the method being employed to determine the value, or the variation that exists among the study subjects.
As used in this specification and claim(s), the words “comprising” (and any form of comprising, such as “comprise” and “comprises”), “having” (and any form of having, such as “have” and “has”), “including” (and any form of including, such as “includes” and “include”) or “containing” (and any form of containing, such as “contains” and “contain”) are inclusive or open-ended and do not exclude additional, unrecited elements or method steps.
The term “or combinations thereof” as used herein refers to all permutations and combinations of the listed items preceding the term. For example, “A, B, C, or combinations thereof” is intended to include at least one of: A, B, C, AB, AC, BC, or ABC, and if order is important in a particular context, also BA, CA, CB, CBA, BCA, ACB, BAC, or CAB. Continuing with this example, expressly included are combinations that contain repeats of one or more item or term, such as BB, AAA, MB, BBC, AAABCCCC, CBBAAA, CABABB, and so forth. The skilled artisan will understand that typically there is no limit on the number of items or terms in any combination, unless otherwise apparent from the context.
All of the compositions and/or methods disclosed and claimed herein can be made and executed without undue experimentation in light of the present disclosure. While the compositions and methods of this invention have been described in terms of preferred embodiments, it will be apparent to those of skill in the art that variations may be applied to the compositions and/or methods and in the steps or in the sequence of steps of the method described herein without departing from the concept, spirit and scope of the invention. All such similar substitutes and modifications apparent to those skilled in the art are deemed to be within the spirit, scope and concept of the invention as defined by the appended claims.
It will be understood that particular embodiments described herein are shown by way of illustration and not as limitations of the invention. The principal features of this invention can be employed in various embodiments without departing from the scope of the invention. Those skilled in the art will recognize, or be able to ascertain using no more than routine experimentation, numerous equivalents to the specific procedures described herein. Such equivalents are considered to be within the scope of this invention and are covered by the claims.
This application claims benefit of U.S. Provisional application Ser. No. 61/094,467 filed on Sep. 5, 2008, which is incorporated herein by reference in its entirety.
This invention was made with U.S. Government support under Contract No. CMS-0650716 awarded by the NSF. The government has certain rights in this invention.
Number | Name | Date | Kind |
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5028395 | Sebille et al. | Jul 1991 | A |
5277872 | Bankert et al. | Jan 1994 | A |
5747348 | Jaduszliwer et al. | May 1998 | A |
7343060 | Ohtsu et al. | Mar 2008 | B2 |
20030112443 | Hjelme et al. | Jun 2003 | A1 |
20090074349 | Hjelme et al. | Mar 2009 | A1 |
20100111136 | Huang et al. | May 2010 | A1 |
Number | Date | Country |
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WO 2010028319 | Mar 2010 | WO |
Number | Date | Country | |
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20100111136 A1 | May 2010 | US |
Number | Date | Country | |
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61094467 | Sep 2008 | US |