1. Field of the Invention
Apparatuses, devices, and methods consistent with the present invention relate to optical waveguides and, more particularly, to an optical waveguide sensor having a long period grating.
2. Description of the Related Art
In a related art optical waveguide, the characteristic of light transmission depends on the interface between a core and a cladding material and, more specifically, on the difference between the refractive index of the core and the refractive index of the cladding material. Recently, long period gratings (LPGs) have been added to manipulate the light resonance between the core and the cladding material. The LPG couples the core guided mode with the cladding modes, propagating in the same direction. When a coupling between the guided mode and the cladding mode occurs, a relationship between those modes is given by
λ0=(N0−Nm)Λ (1)
where λ0 is a resonance wavelength, at which the guided mode and m-th cladding mode are coupling, N0 is the effective refractive index of the guided mode, Nm is the effective refractive index of the cladding mode, and Λ is the grating period. The excitation of the cladding mode attenuates the light intensity of the guided mode after the LPG, which results in a resonant loss in the transmission spectrum.
The LPG is fabricated as either a phase grating, which periodically manipulates the material refractive index of the waveguide core by means of inscription, or by corrugation grating, which periodically creates geometrical features by means of material removal.
This fabrication process has a few disadvantages. For example, many different operations are involved, such as using laser inscription, laser cutting, thermal inscription, reactive ion beam (RIB) etching, and the like. Also, many different materials are involved, with each operation requiring a different equipment setup. Accordingly, the fabrication cycle time of the related art—optical waveguide is long and costly, and there are many constraints on the geometry of the optical waveguide.
Exemplary embodiments of the present invention address the above disadvantages and other disadvantages not described above. However, the present invention is not required to overcome the disadvantages described above, and thus, an exemplary embodiment of the present invention may not overcome any of the disadvantages described above.
According to an exemplary embodiment of the present invention, there is provided an optical waveguide comprising a first cladding layer; a first waveguide core formed on the first cladding layer, the first waveguide core comprising a first long period grating formed in at least one sidewall of the first waveguide core; and a second cladding layer formed over the first waveguide core.
According to another exemplary embodiment of the present invention, there is provided a process for forming an optical waveguide, the process comprising forming a first waveguide core on a surface of a first cladding layer; patterning the first waveguide core with a long period grating that is perpendicular to a surface of the first cladding layer; and forming a second cladding layer on the first cladding layer so as to cover the first waveguide core.
The above and other aspects of the present invention will become more apparent and more readily appreciated from the following description of exemplary embodiments of the present invention taken in conjunction with the attached drawings, in which:
Exemplary embodiments of the present invention will now be described with reference to the accompanying drawings. In the following description, like reference numerals refer to like elements throughout.
Turning now to
The first cladding layer 15 may be of any thickness as long as the cladding mode is confined to the second cladding layer 35. The waveguide core 20 shown in
The first cladding layer 15, the second cladding layer 35, and the waveguide core 20 are each made of a polymer material, which is sensitive to ultraviolet light. The polymer materials are selected based on the refractive indices of the materials. A relationship among the refractive indices of the waveguide core 20, the first cladding layer 15 and the second cladding layer 35 is n(core)>n(clad 2)>n(clad 1), where n(core) denotes the refractive index of the waveguide core 20, n(clad 1) denotes the refractive index of the first cladding layer 15, and n(clad 2) denotes the refractive index of the second cladding layer 35. Under this relationship for the refractive indices of the waveguide core 20, the first cladding layer 15 and the second cladding layer 35, the cladding mode propagates in the second cladding layer. Alternatively, the relationship of the refractive indicies may be n(core)>n(clad 1)>n(clad 2), in which case the cladding mode propagates in the first cladding layer.
Turning to
The first waveguide core 40 includes a first long period grating 43, and the second waveguide core 45 includes a second long period grating 47. In contrast to the first exemplary embodiment described above, the first long period grating 43 is provided in both sidewalls of the first waveguide core 40, and the second long period grating 47 is provided in both sidewalls of the second waveguide core 45. Alternatively, the first long period grating 43 and the second long period grating 47 may be provided in only one sidewall of the first waveguide core 40 and the second waveguide core 45, respectively. The period of the first long period grating 43 and the second long period grating 47 are substantially the same. However, alternatively, the periods may be different. Additionally, the depth of the first long period grating 43 and the second long period grating 47 are substantially the same. However, alternatively, the depths may be different.
The refractive indices of the first waveguide core 40 and the second waveguide core 45 are substantially the same. As in the first exemplary embodiment described above, the materials are polymer materials selected to satisfy the relationship n(core)>n(clad 2)>n(clad 1). Alternatively, the polymer materials may be selected to satisfy the relationship n(core)>n(clad 1)>n(clad 2).
As shown in
The optical waveguide 200 further includes a third waveguide core 60 and a fourth waveguide core 70. The third waveguide core 60 and the fourth waveguide core 70 are each substantially the same as the optical waveguide core 20 of the first exemplary embodiment. The third waveguide core 60 and the fourth waveguide core 70 are formed on top of the second cladding layer 35. A third cladding layer 80 is formed over the second cladding layer 35, and covers the third waveguide core 60 and the fourth waveguide core 70. Thus, the third waveguide core 60, the fourth waveguide core 70, and the third cladding layer 80 form a second optical layer, that is stacked on top of a first optical layer, which includes the first cladding layer 15, the first and second waveguide cores 40, 45, and the second cladding layer 35.
As shown in
The third waveguide core 60 and the fourth waveguide core 70 are formed in parallel over the first waveguide core 40 and the second waveguide core 45, respectively, such that each of the first waveguide core 40, the second waveguide core 45, the third waveguide core 60 and the fourth waveguide core 70 run in parallel to one another in the length direction. However, the second optical layer may alternatively be deviated by a certain angle from the first optical layer such that the third and fourth waveguide cores 60, 70 are deviated from the first and second waveguide cores 40, 45.
The polymer materials of the first cladding layer 15, the second cladding layer 35, the third cladding layer 80, and the first, second, third, and fourth waveguide cores 40, 45, 60, 70 are selected based on their respective refractive indexes. The materials for the first, second, third, and fourth waveguide cores 40, 45, 60, 70 are selected such that the refractive index of the first, second, third, and fourth waveguide cores 40, 45, 60, 70 are the same. The materials are selected to satisfy the following relationship: n(core)>n(clad 2)>n(clad 1)≧n(clad 3) or n(core)>n(clad 2)>n(clad 3)≧n(clad 1), where n(core) denotes the refractive index of the waveguide cores, n(clad 1) denotes the refractive index of the first cladding layer 15, and n(clad 2) denotes the refractive index of the second cladding layer 35, and n(clad 3) denotes the refractive index of the third cladding layer 80. Under this relationship of the refractive indexes, the cladding-mode propagates in the second cladding layer. Alternatively, the polymer materials may be selected according to the following relationship in which the cladding-mode propagates in the third cladding layer: n(core)>n(clad 3)>n(clad 2)≧n(clad 1) or n(core)>n(clad 3)>n(clad 1)≧n(clad 2).
While the third exemplary embodiment is shown with two waveguide cores in each of the first optical layer and the second optical layer, the number of waveguide cores in each layer may be more than two. Thus, as shown in
As in the preceding exemplary embodiments, the polymer materials of the first cladding layer 15, the second cladding layer 35, the third cladding layer 80, and the waveguide cores 20 are selected based on their respective refractive indexes. The materials are selected to satisfy the following relationship: n(core)>n(clad 2)>n(clad 1)≧n(clad 3) or n(core)>n(clad 2)>n(clad 3)≧n(clad 1), where n(core) denotes the refractive index of the waveguide cores, n(clad 1) denotes the refractive index of the first cladding layer 15, and n(clad 2) denotes the refractive index of the second cladding layer 35, and n(clad 3) denotes the refractive index of the third cladding layer 80. Under this relationship of the refractive indexes, the cladding-mode propagates in the second cladding layer. Alternatively, the polymer materials may be selected according to the following relationship in which the cladding-mode propagates in the third cladding layer: n(core)>n(clad 3)>n(clad 2)≧n(clad 1) or n(core)>n(clad 3)>n(clad 1)≧n(clad 2).
Turning now to
As shown in
In
The photolithography mask 605 is then removed, as shown in
In
Although the process has been described with respect to forming only one waveguide core 606, the process may be applied to produce a core array of a plurality of waveguides, each having a long period grating. In such a case, the photolithography mask is formed to correspond to the core array of a plurality of waveguides, and the core array is formed at one time using the mask. Each successive optical waveguide layer may then be formed by iterative application of the process.
While the present invention has been shown and described with reference to certain exemplary embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims.
This application claims the benefit of priority of U.S. Provisional Application No. 61/038,483, filed in the U.S. Patent and Trademark Office on Mar. 21, 2008, the entire contents of which is herein incorporated by reference.
Number | Date | Country | |
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61038483 | Mar 2008 | US |