Optical waveguide device

Abstract: An optical waveguide device is provided with a semiconductive layer (4) formed between a buffer layer (3) and a pair of electrodes (5, 6). In a first aspect of the present invention a part (P; Q) of the semiconductive layer (4a, 4b; 4c) corresponding to the gap between the pair of electrodes (5, 6) is of reduced or zero thickness, thereby to ensure that, when a low frequency electric signal is applied to the pair of electrodes (5, 6), the electric field is concentrated on that part (P; Q). In a second aspect of the present invention a second semiconductive layer (9a) is provided between the first semiconductive layer (4) and at least one of the electrodes (5, 6).

Description: The present invention relates to an optical waveguide device, and more particularly to an optical waveguide device such as a modulator, switch, distributor, or the like, used in optical communication apparatus. A typical optical waveguide device used in an optical switch, an optical modulator, or the like, is constituted such that an electric field is applied to an optical waveguide formed on a surface of a substrate consisting of electrooptical crystal such as lithium niobate (LiNbO 3 ), or the like, so as to change a refractive index, and thus switching or phase modulation of a light signal traveling through the optical waveguide can be carried out. In particular, an optical waveguide device typically includes an optical waveguide formed on a surface of a substrate having an electrooptical effect and a pair of electrodes formed on corresponding regions above the optical waveguide and receiving a driving electric signal thereacross. A distribution of electric field occurring in a vicinity of the optical waveguide by an application of the electric signal is greatly changed in accordance with a change in a frequency of the electric signal. As an example of the optical waveguide device, a Mach-Zehnder type modulator is well known. A modulator of this type includes at least an optical waveguide formed on a surface of a Z-cut LiNbO 3 substrate and a pair of asymmetrical electrodes formed on corresponding regions above the optical waveguide. In such a structure, charges collected on the surface of the LiNbO 3 substrate by the pyroelectric effect act on the asymmetrical structure of the electrodes and thus a disadvantage occurs in that the distribution of charges is made uneven and an adverse influence is exerted on characteristics of the device. Also, since the distribution of resistance, dielectric constant and capacitance of each portion of the structure or partial fine structure is delicately changed in accordance with the process conditions, the electrical equivalent circuit accordingly becomes complicated. This results in a problem in that a direct current (DC) component of an electric signal applied across the electrodes greatly changes an application manner of the electric field with a long-term time constant and the optical response is also accordingly changed. This phenomenon is called a DC drift. Both JP-A-62 073 207 and JP-A-1 302 325 disclose an optical waveguide device in which at least two metal electrodes are formed on a buffer layer overlying a LiNbO 3 substrate. It is therefore desirable to provide an optical waveguide device capable of suppressing a DC drift thereof to effectively compensate for fluctuation in operational characteristics due to the DC drift, stress, or the like. In the applicant's co-pending European patent application No. 91301729.9 there is proposed an optical waveguide device in which a third electrode other than the pair of driving electrodes is provided on a region spaced by a predetermined distance from the pair of driving electrodes formed on corresponding regions above the optical waveguide. The third electrode may receive a DC or low frequency voltage, or may be grounded under predetermined layout conditions of each electrode. In an optical waveguide device formed on an electrooptical crystal substrate having a pyroelectric effect, it is preferable that a semiconductive layer of, e.g., silicon (Si) is formed on a buffer layer so as to make uniform a distribution of charges occurring in the vicinity of the surface of the optical waveguide. In this case, in a structure having a narrow signal line electrode and a wide grounding electrode, a potential on the semiconductive (Si) region on the outside of the signal line electrode (i.e. on the opposite side of the grounding electrode) is uniformly made equal because the silicon (Si) layer acts as a conductor in a low frequency band. As a result, a drawback arises in that the electric field to be concentrated on the vicinity of the signal line electrode is dispersed into the outside semiconductive (Si) region and thus it is not effectively applied to the optical waveguide. To cope with this drawback, a third electrode may be provided on the outside of the signal line electrode, i.e. on the opposite side of the grounding electrode. By this structure, it is possible to cause a voltage drop in proportion to the distance between the signal line electrode and the third electrode and thus concentrate the dispersed electric field on the vicinity of the signal line electrode. Also, by suitably changing the thickness of the silicon (Si) layer between the signal line electrode and the third electrode, it is possible to change a distribution of resistance therebetween to regulate a distribution of the voltage drop and thus concentrate the electric field more effectively. On the other hand, when a high frequency electric signal is applied to the pair of driving electrodes, charges in the silicon (Si) layer cannot follow a change in the high frequency electric signal and thus the semiconductive layer functions as a dielectric. Also, by disposing the third electrode on a region spaced from the signal line electrode by a sufficient distance, it is possible to reduce the influence exerted on the characteristic impedance of the traveling wave electrode. In the afore-mentioned co-pending application the applicants propose the use of a semiconductor layer having a relatively low resistance in place of a conductor as the third electrode, thereby gaining the same effect as above and further reducing the influence exerted on the characteristic impedance. Although the above structure premises that the third electrode is grounded, the third electrode may receive a voltage signal. In this case, more effective advantages can be obtained. Namely, by applying a DC or low frequency voltage to the third electrode, it is possible to compensate for a fluctuation in operational characteristics occurring due to a DC drift, mechanical stress, or the like. In this case, it is preferable that a semiconductor layer consisting of material having a relatively high resistance, e.g. silicon (Si), is formed close to the signal line electrode. The semiconductor layer may receive a voltage directly from an external power source, or may receive the voltage via a conductor layer, which is formed on the semiconductor layer at a position spaced from the signal line electrode by a sufficient distance such that its presence does not greatly affect a characteristic impedance of the traveling wave electrode. By applying the voltage directly or indirectly to the semiconductor layer, it is possible to change a refractive index of the optical waveguide beneath the signal line electrode and thus compensate for a fluctuation in operational characteristics. In this case, the semiconductive layer functions as a conductor with respect to a low frequency voltage and functions as a dielectric with respect to a high frequency voltage. Accordingly, the presence of the semiconductive layer has less influence on the characteristic impedance in the high frequency band of the applied voltage. Also, another semiconductive layer may be formed all over the buffer layer so as to improve temperature characteristics. In this case, by decreasing the thickness of the semiconductive layer in the vicinity of the signal line electrode and concentrating the electric field on the thinly formed portion, it is possible to realise the same effect as above. In the present application the applicants propose an alternative solution which is an improvement of a conventional Mach-Zehnder type optical waveguide device and which is based on the principle described below. Electrodes constituting optical modulators, optical switches, or the like, are formed to have a low resistance and thus enable a high speed operation. To this end, it is preferabe to use a material having a high electric conductivity such as copper (Cu), gold (Au), or the like, and increase the thickness of the electrode. Where a material having a relatively high resistance such as a silicon (Si) layer is adjacent to the material having a high electric conductivity, it functions in different phases in accordance with the selection of the resistance value. Namely, when a DC or low frequency voltage is applied to the signal line electrode, the silicon (Si) layer is kept in a state of equal potential in the same manner as the conductor (electrode). Contrary to this, where the frequency of the signal propagating on the signal line electrode is gradually increased, charges in the silicon (Si) region cannot follow a high speed change in the signal, and thus, a region in which charges can follow the high speed change in the signal is gradually limited to the vicinity of the conductor (electrode). In other words, an effective shape of the electrode is greatly changed between the low frequency band and the high frequency band. By utilizing the change in the effective shape of the electrode, it is possible to constitute a device having various functions. To realize a high speed switching or modulation, a pair of electrodes for a traveling wave are normally employed. According to an improved structure, a semiconductive layer comprised of silicon (Si) is formed between the pair of electrodes and the buffer layer. The semiconductive layer is separated into two regions in the center of the corresponding region thereof between the electrode for signal line and the electrode for grounding. By this constitution, an electric field by a DC or low frequency component of the applied signal is concentrated on the separated portion and a component of the electric field in the vicinity of the optical waveguide is weakened. Accordingly, even if the DC or low frequency component is changed due to a DC drift, it is possible to suppress a fluctuation in operational characteristics. On the other hand, where a high frequency electric signal is applied to the pair of electrodes, charges in the silicon (Si) layer cannot follow a change in the high frequency electric signal and thus the silicon layer functions as a dielectric. In this case, since the electric field is applied across the pair of electrodes, it effectively acts on the optical waveguide. Also, even in the case that a thinly formed conductive layer is substituted for the above-mentioned semiconductive layer, it is possible to realize the same effect as above. This is because even the conductor has a larger volume resistivity than zero and the resistance value is increased with a decrease in the thickness of the conductive layer. Thus, according to a first aspect of the present invention there is provided an optical waveguide device comprising: an optical waveguide formed on a surface of a substrate having an electro-optical effect; a pair of electrodes operatively connected and arranged to receive a driving electric signal thereacross; a buffer layer formed all over the said surface of said substrate including the optical waveguide; and a semiconductive layer formed between the buffer layer and the pair of electrodes, a part of the said semiconductive layer which corresponds to the gap between the pair of electrodes being of reduced or zero thickness; wherein a change in frequency of the driving electric signal applied across the pair of electrodes when the device is in use brings about a corresponding change in a distribution of an electric field which occurs in the vicinity of the optical waveguide, and wherein, when a low frequency electric signal is applied to the pair of electrodes, the electric field is concentrated on the said part of the said semiconductive layer. According to a second aspect of the present invention there is provided an optical waveguide device comprising: an optical waveguide formed on a surface of a substrate having an electro-optical effect; a pair of electrodes operatively connected and arranged to receive a driving electric signal thereacross; a buffer layer formed all over said surface of said substrate including the optical waveguide; and a first semiconductive layer, formed between the buffer layer and the pair of electrodes, and a second semiconductive layer, formed between the first semiconductive layer and a signal line electrode of the pair of electrodes, the second semiconductive layer having a specific resistance different from that of the first semiconductive layer and having a broader width than that of the signal line electrode; wherein a change in frequency of a driving electric signal applied therebetween when the device is in use brings about a corresponding change in a distribution of an electric field which occurs in the vicinity of the optical waveguide. Reference will now be made, by way of example, to the accompanying drawings, in which: Figs. 1A and 1B show plan and sectional views, respectively, of a structure of a prior art Mach-Zehnder type modulator; Figs. 2A and 2B show plan and sectional views, respectively, of an optical waveguide device (optical modulator) embodying the first aspect of the present invention; Fig. 3 shows a sectional view of a first modification of the structure shown in Figs. 2A and 2B; Fig. 4 shows a sectional view of a second modification of the structure shown in Figs. 2A and 2B; Fig. 5 shows a sectional view of a third modification of the structure shown in Figs. 2A and 2B; Figs. 6 shows a sectional view of an optical waveguide device (optical modulator) embodying the second aspect of the present invention; Fig. 7 shows a sectional view showing a first modification of the structure shown in Fig. 6; and Figs. 8A and 8B show plan and sectional views, respectively, of a second modification of the structure shown in Fig. 6. Figures 1A and 1B show a structure of a prior art Mach-Zehnder type modulator. Note, Fig. 1B shows a sectional structure along the line A-A' in Fig. 1A. The illustrated structure shows an example using asymmetrical electrodes for a traveling wave. In the drawings, reference 1 denotes a Z-cut LiNbO 3 substrate and reference 2 denotes an optical waveguide including two-forked optical waveguides 2a and 2b. The optical waveguide 2 (2a, 2b) is formed by effecting a striplike patterning of a Titanium (Ti)-deposited layer formed on a surface of the substrate 1 and then effecting a thermal diffusion of the Titanium into the substrate 1. Thus, the optical waveguide 2 (2a, 2b) has a larger refractive index than that of the substrate 1. Also, to prevent light propagating through the optical waveguide from being absorbed in driving electrodes (a signal line electrode 5 and grounding electrode 6), a dielectric buffer layer 3 is formed between the electrodes 5, 6 and the optical waveguide 2. The buffer layer 3 is translucent and has a smaller refractive index than that of the optical waveguide 2. The buffer layer 3 is comprised of, for example, silicon dioxide (SiO 2 ). The dielectric layer 3 electrically functions as a capacitance containing relatively high resistance material. In an optical waveguide device using a substrate of Z-cut LiNbO 3 , a disadvantage occurs in that charges collected on the surface of the substrate by the pyroelectric effect act on the asymmetrical structure of the electrodes formed on the buffer layer and thus an uneven distribution of charges is formed, which has an adverse influence on characteristics of the optical waveguide device. In view of this, a semiconductive layer 4 comprised of, for example, silicon (Si) is formed between the buffer layer 3 and the electrodes 5, 6 and all over the buffer layer 3 (see Fig. 1B). By this structure, it is possible to make uniform the distribution of surface charges occurring due to a change in temperature or the like and stabilize the characteristics of the optical waveguide device. Furthermore, since the optical waveguide 2 is formed by diffusing the Titanium with high temperature into the LiNbO 3 substrate 1, its resistance, dielectric constant and capacitance are different from those of the bulk portion of the substrate 1. Additionally, a resistance of the surface of the LiNbO 3 substrate 1 is different from that of the bulk portion thereof due to the diffusing process. In view of the complicated distribution of the resistance, dielectric constant and capacitance of the above layers and partial fine structure, the electrical equivalent circuit also becomes complicated. As a result, a problem occurs in that a DC component of an electric signal applied across the electrodes 5, 6 greatly changes an application manner of the electric field with a long-term time constant in accordance with the process conditions and the optical response characteristics are also accordingly changed. Namely, a DC drift is caused. To cope with the problem, there have been taken measures to connect the electrodes 5, 6 of the modulator to an external power source by way of capacitance coupling and thus prevent a DC component of the power source from being directly applied to the modulator, or measures to connect a biasing DC power source to the electrode for signal line 5 by means of capacitance coupling and thus compensate a DC drift occurring due to some causes. According to the measures to employ an external power source by way of capacitance coupling, however, a drawback occurs in that the device is brought to an electrically open state seen from the power source and thus an adverse influence is exerted on the operation of the power source. A disadvantage also occurs in that an available frequency band of the power source is limited in dependence on the capacity thereof. On the other hand, according to the measures to employ a biasing DC power source by way of capacitance coupling, a drawback occurs in that a characteristic impedance of the traveling wave signal line electrode fluctuates and thus it is impossible to satisfactorily carry out the modulation operation. Also, where a stress is applied to the optical waveguides for some reason, the refractive index of the optical waveguides normally changes resulting in a fluctuation in operational characteristics of the modulator. To cope with this disadvantage, there has been heretofore taken measures to add a DC voltage to the application voltage so as to cancel a change in the refractive index occurring due to the stress. However, to take the measures to add a DC voltage to the application voltage is often difficult from a viewpoint of the limit of the dielectric strength of the DC power source. In view of the above problems, a structure or means other than the electrodes provided for switching or modulation needs to be provided for suppressing a DC drift and compensating for a fluctuation in operational characteristics due to the DC drift, stress, or the like. As shown in Figs. 2A and 2B, the structure illustrated in Figs. 1A and 1B may be modified in accordance with the first aspect of the present invention so as to have a semiconductive layer (4a, 4b) formed between the buffer layer 3 and the electrodes 5 and 6. The semiconductive layer is comprised of silicon (Si) and has a thickness of approximately 0.2 µ m, and is separated into two regions 4a and 4b in the center of the corresponding region thereof between the electrodes 5 and 6. The gap between the separated portions 4a, 4b, indicated by reference P, is selected to be 1 to 4 µ m. Note, each semiconductive layer 4a, 4b has a broader width than that of the corresponding electrode 5, 6. In this case, a specific resistance of the semiconductive layer (4a, 4b) can be designed and selected over a wide range from 0.001 to 100000 Ωm. Where the present optical modulator is used in a frequency of 5 to 6 MHz or more, the specific resistance is preferably selected to be 100 Ωm. Of course, the specific resistance is altered in accordance with a thickness of each layer, a layer-to-layer distance, a distance between each electrode, and the like. By adopting the above structure, components of a DC voltage or a low frequency voltage of 50 to 60 Hz applied across the electrodes 5, 6 are concentrated on the separated portion P and thus do not substantially affect the characteristic impedance of the optical waveguide 2 (2a, 2b). On the other hand, where a high frequency voltage of approximately 5 to 6 MHz is applied across the electrodes 5, 6, charges cannot easily follow a change in the voltage and thus the semiconductive layer (4a, 4b) functions as a dielectric. Namely, since the high frequency voltage is applied between the electrodes 5 and 6, it is possible to effectively change the refractive index of the optical waveguide 2 (2a, 2b). Therefore, according to the present example, it is possible to disregard a DC component of the applied voltage and thus suppress the influence of DC drift. Figure 3 shows a first modification of the embodiment shown in Figs. 2A and 2B. In the present example, the semiconductive layer 4a is formed only in the vicinity of the electrode for signal line 5. Since the width of the semiconductive layer 4a formed under the electrode 5 can be arbitrarily designed and selected, it is possible to realize better frequency characteristics. Figure 4 shows a structure of a second modification. In the present example, in place of the separated semiconductive layers 4a, 4b shown in Figs. 2A and 2B, a semiconductive layer 4c comprised of silicon (Si) is formed between the buffer layer 3 and the electrodes 5 and 6 and all over the buffer layer 3. The semiconductive layer 4c has a thinly formed portion Q in the center of the corresponding region thereof between the electrodes 5 and 6. By this structure, a DC component or a low frequency component of the voltage applied across the electrodes 5, 6 is concentrated on the thinly formed portion Q and thus it is possible to gain the same effect as in Figs. 2A and 2B. Figure 5 shows a structure of a third modification, which is a combination of the example of Fig. 3 and the example of Fig. 4. In the present example, since the semiconductive layer 4c is formed only in the vicinity of the signal line electrode 5, it is possible to realize better frequency characteristics as in the example of Fig. 3. As shown in Fig. 6, the structure illustrated in Figs. 1A and 1B may be modified alternatively in accordance with the second aspect of the present invention so as to have a first semiconductive layer 4 and a second semiconductive layer 9a provided in place of the separated semiconductive layers 4a, 4b shown in Figs. 2A and 2B. The semiconductive layer 4 is comprised of silicon (Si) and formed between the buffer layer 3 and the electrode 6 and all over the buffer layer 3. The semiconductive layer 9a is comprised of silicon (Si) and formed between the semiconductive layer 4 and the electrode 5. Also, the semiconductive layer 9a has a specific resistance different from that of the semiconductive layer 4 and has a broader width than that of the corresponding electrode 5. In the device using the asymmetrical electrodes 5, 6 for a traveling wave, the electric field in the vicinity of the optical waveguide 2b beneath the grounding electrode 6 is relatively weak. Therefore, even if a DC electric field is concentrated on the region between the electrodes 5 and 6, it is possible to suppress the influence exerted on the refractive index of the optical waveguide 2b beneath the electrode 6 and thus gain the same effect as above. Figure 7 shows a structure of a first modification, which is an improvement of the example of Fig. 6. In the present example, a semiconductive layer 9b comprised of silicon (Si) is added to the structure shown in Fig. 6. The semiconductive layer 9b is formed between the semiconductive layer 4 and the electrode 6. Also, the semiconductive layer 9b has a specific resistance different from that of the semiconductive layers 4, 9a and has a broader width than that of the corresponding electrode 6. Since the present device has a number of design parameters, it is possible to design and optimize the device more effectively and thus gain a better effect. Figures 8A and 8B show a structure of a second modification. In addition to the features of the Fig. 7 structure, the structure of Figs. 8A and 8B has a semiconductive layer 9c, comprising silicon (Si), on which a third electrode 10 is formed, the layer 9c being separated from the layer 9a in a region between the electrodes 5 and 10. The semiconductive layer 9c has a specific resistance different from that of the semiconductive layer 4 and has a broader width than that of the electrode 10. According to this structure, it is possible to suppress a DC drift of the device and thus effectively compensate for a fluctuation in operational characteristics due to the DC drift, stress, or the like. Although, in the above embodiments and the associated modifications, the explanation is given by way of reference to a Mach-Zehnder type modulator, the present invention is applicable to other optical waveguide devices such as optical switches, or the like. Also, the present invention can be applied to an optical waveguide device to which a low frequency signal and a high frequency signal are fed independently. Although the present invention has been disclosed and described by way of various embodiments and the associated modifications, it is apparent to those skilled in the art that other embodiments and modifications of the present invention are possible.

Claims: An optical waveguide device comprising: an optical waveguide (2, 2a, 2b) formed on a surface of a substrate (1) having an electro-optical effect; a pair of electrodes (5, 6) operatively connected and arranged to receive a driving electric signal thereacross; a buffer layer (3) formed all over the said surface of said substrate (1) including the optical waveguide (2, 2a, 2b); and a semiconductive layer (4) formed between the buffer layer (3) and the pair of electrodes (5, 6), a part (P; Q) of the said semiconductive layer (4a, 4b; 4c) which corresponds to the gap between the pair of electrodes (5, 6) being of reduced or zero thickness; wherein a change in frequency of the driving electric signal applied across the pair of electrodes (5, 6) when the device is in use brings about a corresponding change in a distribution of an electric field which occurs in the vicinity of the optical waveguide (2, 2a, 2b), and wherein, when a low frequency electric signal is applied to the pair of electrodes (5, 6), the electric field is concentrated on the said part (P; Q) of the said semiconductive layer (4a, 4b; 4c). An optical waveguide device as claimed in claim 1, wherein the semiconductive layer (4c) has a thinly-formed portion (Q) and is formed only in the vicinity of the pair of electrodes (5, 6). An optical waveguide as claimed in claim 1, wherein when the thickness of said semiconductive layer (4a, 4b) at said part (P) is zero the semiconductive layer (4a, 4b) comprises two regions separated from one another at a part of said layer corresponding to the gap between the said pair of electrodes (5, 6), each separated region of the semiconductive layer (4a, 4b) having a broader width than that one of the said pair of electrodes (5, 6) under which it lies. An optical waveguide device as claimed in claim 3, wherein that one (4a) of the separated regions (4a, 4b) of the semiconductive layer which underlies a signal line electrode (5) of the pair of electrodes (5, 6) is formed only in the vicinity of the signal line electrode (5). An optical waveguide device comprising: an optical waveguide (2, 2a, 2b) formed on a surface of a substrate (1) having an electro-optical effect; a pair of electrodes (5, 6) operatively connected and arranged to receive a driving electric signal thereacross; a buffer layer (3) formed all over said surface of said substrate (1) including the optical waveguide (2, 2a, 2b); and a first semiconductive layer (4), formed between the buffer layer (3) and the pair of electrodes (5, 6), and a second semiconductive layer (9a), formed between the first semiconductive layer (4) and a signal line electrode (5) of the pair of electrodes (5, 6), the second semiconductive layer (9a) having a specific resistance different from that of the first semiconductive layer (4) and having a broader width than that of the signal line electrode (5); wherein a change in frequency of a driving electric signal applied therebetween when the device is in use brings about a corresponding change in a distribution of an electric field which occurs in the vicinity of the optical waveguide (2, 2a, 2b). An optical waveguide device as claimed in claim 5, wherein a second semiconductive layer (9b) is also formed between the first semiconductive layer (4) and a grounding electrode (6) of the pair of electrodes (5, 6) such that there are two semiconductive layer regions (9a, 9b) separated from one another at a location corresponding to the gap between the pair of electrodes (5, 6), each separated region (9a, 9b) having a broader width than that one of the said pair of electrodes (5, 6) under which it lies. An optical waveguide device as claimed in claim 6, further comprising a third electrode (10), wherein a second semiconductive layer (9c) is also formed between the first semiconductive layer (4) and the said third electrode (10) such that there are three semiconductive layer regions (9a, 9b, 9c) separated from one another at respective locations corresponding to the gaps between the three electrodes (5, 6, 10), each separated region (9a, 9b, 9c) having a broader width than that one of the said electrodes (5, 6, 10) under which it lies. An optical waveguide device as claimed in any preceding claim, wherein the buffer layer (3) comprises dielectric material and has a smaller refractive index than that of the optical waveguide (2, 2a, 2b). An optical waveguide device as claimed in claim 8, wherein the dielectric material comprises silicon dioxide. An optical waveguide device as claimed in any preceding claim, wherein the or each semiconductive layer (4; 9a, 9b) comprises silicon.

Inventors: DOI MASAHARU, KUBOTA YOSHINOBU, MEKADA NAOYUKI, NAKAZAWA TADAO, SEINO MINORU, DOI,MASAHARU, KUBOTA, YOSHINOBU, MEKADA,NAOYUKI, NAKAZAWA, TADAO, SEINO,MINORU, DOI,MASAHARU, C/O FUJITSU LIMITED, MEKADA,NAOYUKI, C/O FUJITSU LIMITED, SEINO,MINORU, C/O FUJITSU LIMITED
Applicants: FUJITSU LTD, FUJITSU LIMITED
Application year: 1991
Main classification: G02F1
IPC codes: G02F1