Electro-optical element, and optical modulation element
By using a lithium niobate film with a c-axis oriented epitaxial structure and a specific X-ray intensity ratio, the optical modulation element significantly reduces DC drift, improving its stability and performance under applied voltage conditions.
Patent Information
- Application Number
- JP2023181573
- Authority / Receiving Office
- JP · JP
- Patent Type
- Applications
- Current Assignee / Owner
- Filing Date
- 2023-10-23
- Publication Date
- 2025-05-08
AI Technical Summary
Optical modulation elements with optical waveguides made of lithium niobate films epitaxially grown on single crystal substrates suffer from significant DC drift, which affects their performance over time.
The electro-optical element incorporates a lithium niobate film with a c-axis oriented epitaxial structure and a specific X-ray intensity ratio of LiNb3O8(60-2) to LiNbO3(006) of 0.02 or more, which suppresses DC drift when a voltage is applied.
This configuration effectively reduces DC drift by 50% or less when the electro-optical element is heated to 120°C and subjected to a DC voltage for one hour, enhancing the stability and reliability of the optical modulation element.
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Figure 2025071425000001_ABST
Abstract
Description
[Technical field]
[0001] The present invention relates to an electro-optical element and an optical modulation element. [Background technology]
[0002] Lithium niobate (LiNbO3, hereafter sometimes referred to as "LN") has a large electro-optic constant, making it suitable as a material for electro-optic elements. Electro-optic elements using LN single crystal substrates have excellent high-frequency response characteristics, and have been used in devices such as optical modulators and optical switches.
[0003] 2. Description of the Related Art Conventionally, electro-optical elements using an LN single crystal substrate include optical modulation elements having an optical waveguide formed by diffusing Ti (titanium) near the surface of an LN single crystal substrate. However, such optical modulation elements have a large cross-sectional shape of the optical waveguide, and the electric field efficiency is poor. For this reason, optical modulators having optical modulation elements using LN single crystal substrates have a long total length of about 10 cm.
[0004] In recent years, there has been a demand for miniaturizing electro-optical elements. One example of a small electro-optical element is an optical modulation element with an optical waveguide made of an LN film epitaxially grown on a single crystal substrate. In such optical modulation elements, good electric field efficiency can be obtained by making the cross-sectional shape of the optical waveguide small, making it possible to significantly reduce the size.
[0005] For example, Patent Document 1 discloses an optical waveguide element having a waveguide made of a lithium niobate film, which is an epitaxial film formed on a single crystal substrate, and a ridge portion having a ridge-shaped cross section. [Prior art documents] [Patent documents]
[0006] [Patent Document 1] JP 2015-230466 A Summary of the Invention [Problem to be solved by the invention]
[0007] An optical modulation element having an optical waveguide made of an LN film epitaxially grown on a single crystal substrate can be significantly smaller than an optical modulation element having an optical waveguide made by diffusing Ti (titanium) near the surface of an LN single crystal substrate. However, optical modulation elements having optical waveguides made of LN films epitaxially grown on single crystal substrates have a large DC drift.
[0008] In an optical modulation element having an optical waveguide made of an LN film epitaxially grown on a single crystal substrate, the modulated waveform moves according to the DC (direct current) voltage applied to the electrodes of the optical modulation element. The modulated waveform in an optical modulation element using an LN film changes with the time that the DC (direct current) voltage is applied. This change in the modulated waveform over time is called DC drift.
[0009] The present invention has been made in consideration of the above-mentioned problems, and aims to provide an electro-optical element having an optical waveguide made of a lithium niobate film epitaxially grown on a substrate, in which DC drift is suppressed. [Means for solving the problem]
[0010] An electro-optical element according to one embodiment of the present invention comprises a single crystal substrate, an optical waveguide made of a dielectric thin film formed on and in contact with a main surface of the single crystal substrate, and electrodes for applying a voltage to the optical waveguide, wherein the dielectric thin film is made of a lithium niobate film which is a c-axis oriented epitaxial film, and the X-ray intensity ratio of LiNb3O8 to LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) is 0.02 or more. Effect of the Invention
[0011] The electro-optical element of the present invention has an optical waveguide made of a dielectric thin film formed on the main surface of a single crystal substrate, the dielectric thin film being made of a lithium niobate film that is an epitaxial film oriented along the c-axis, and the X-ray intensity ratio between LiNb3O8 and LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) is 0.02 or more. Therefore, the electro-optical element is one in which DC drift is suppressed when a voltage is applied to the optical waveguide by the electrodes. [Brief description of the drawings]
[0012] [Figure 1] FIG. 1 is a plan view showing a Mach-Zehnder type optical modulation element 200A, which is an example of the electro-optical element of the present invention. [Diagram 2] 2(a) is a cross-sectional view of the light modulation element 200A shown in FIG. 1 taken along line AA', and FIG. 2(b) is a cross-sectional view of the light modulation element 200A shown in FIG. 1 taken along line BB'. [Diagram 3] FIG. 3 is a process chart for explaining the method for manufacturing the optical modulation element 200A shown in FIG. 1, FIG. 2(a) and FIG. 2(b), and is a cross-sectional view showing the substrate 1 with the dielectric thin film. [Figure 4] FIG. 4 is a scanning transmission electron microscope (STEM) photograph of a lithium niobate film having an X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of 0.050, selected from the dielectric thin films of the 15 optical modulation elements 200A of Experimental Example 2. [Diagram 5] FIG. 5 is a chart showing the results of X-ray diffraction of a lithium niobate film having an X-ray intensity ratio of LiNb3O8 to LiNbO3 of 0.024 and a lithium niobate film having an X-ray intensity ratio of 0.050, which were selected from the dielectric thin films of the 15 optical modulation elements 200A in Experimental Example 2. [Figure 6] Figure 6 is a graph showing the relationship between the X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of the lithium niobate film on the dielectric thin film-coated substrate 1 used in the optical modulation element 200A of experimental example 2 and the DC drift of the optical modulation element 200A of experimental example 2 after one hour. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0013] The present inventors have solved the above problems and have studied to suppress DC drift when a voltage is applied to an electro-optical element having an optical waveguide made of a lithium niobate film epitaxially grown on a single crystal substrate. Specifically, the present inventors have determined that an electro-optical element is acceptable if the DC drift when heated to 120° C. is 50% or less when the application time of a DC (direct current) voltage reaches 1 hour, and have conducted extensive studies focusing on the relationship between the composition of the lithium niobate film forming the optical waveguide and the DC drift.
[0014] As a result, we found that by using an electro-optical element having an optical waveguide made of a lithium niobate film which is a c-axis oriented epitaxial film and has an X-ray intensity ratio between LiNb3O8 and LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) of 0.02 or more, DC drift when voltage is applied to the optical waveguide can be sufficiently suppressed.
[0015] More specifically, a lithium niobate film epitaxially grown by sputtering tends to have a composition with less Li than the stoichiometric composition, even if a target with a stoichiometric composition of Li2O:Nb2O5=0.50:0.50 is used. The present inventors have thoroughly studied epitaxially grown lithium niobate films and found that when a lithium niobate film with even less Li is epitaxially grown than a congruent composition (Li / (Li+Nb) of about 0.485) with less Li than the stoichiometric composition, minute LiNb3O8 crystals are likely to be generated together with LiNbO3 crystals.
[0016] The LiNb3O8 crystals that formed in the lithium niobate film together with the LiNbO3 crystals are so tiny that they cannot be clearly observed as a different phase by X-ray diffraction. These LiNb3O8 crystals can be confirmed by detailed analysis using a scanning transmission electron microscope (STEM).
[0017] Conventionally, it has been considered desirable for the lithium niobate film used in the optical waveguide of an electro-optical element to be a single phase consisting of the LiNbO3 phase in order to obtain an excellent electro-optical effect. For this reason, it has been considered that LiNb3O8 crystals should be controlled so as not to be generated during the epitaxial growth of the lithium niobate film, and the film formation conditions have been determined so as not to grow heterogeneous phases such as LiNb3O8 crystals when the lithium niobate film is epitaxially grown on a single crystal substrate.
[0018] However, as a result of intensive research by the present inventors, it was found that by forming an electro-optical element having an optical waveguide made of a lithium niobate film containing a sufficient amount of LiNb3O8 crystals, it is possible to suppress the DC drift when a voltage is applied to the optical waveguide. Although the reason why the DC drift of the electro-optical element is suppressed has not been clearly elucidated, it is presumed that the lithium niobate film containing LiNb3O8 and LiNbO3 and having an X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of 0.02 or more contains LiNb3O8 crystals, which prevents the movement of charged particles that cause DC drift when a voltage is applied.
[0019] The present invention includes the following aspects. [1] A single crystal substrate; an optical waveguide made of a dielectric thin film formed on and in contact with a main surface of the single crystal substrate; an electrode for applying a voltage to the optical waveguide; The electro-optical element, wherein the dielectric thin film is made of a lithium niobate film that is a c-axis oriented epitaxial film, and the X-ray intensity ratio of LiNb3O8 to LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) is 0.02 or more.
[0020] [2] The electro-optic element according to [1], wherein the single crystal substrate is a sapphire single crystal substrate, the main surface of which is a c-plane.
[0021] [3] An optical modulation element comprising the electro-optical element according to [1] or [2].
[0022] The electro-optical element and the light modulation element of the present embodiment will be described in detail below with reference to the drawings as appropriate. The drawings used in the following description may show characteristic parts enlarged for the sake of convenience in order to make the features of the present invention easier to understand. Therefore, the dimensional ratios of each component may differ from the actual ones. The materials, dimensions, etc. exemplified in the following description are merely examples, and the present invention is not limited thereto, and may be appropriately modified and implemented within the scope of the present invention.
[0023] [Light modulation element] Fig. 1 is a plan view showing a Mach-Zehnder type light modulation element 200A which is an example of an electro-optical element of the present invention. Fig. 2(a) is a cross-sectional view of the light modulation element 200A shown in Fig. 1 taken along line AA', and Fig. 2(b) is a cross-sectional view of the light modulation element 200A shown in Fig. 1 taken along line BB'.
[0024] The optical modulation element 200A shown in Figures 1, 2(a) and 2(b) has a single crystal substrate 2, an optical waveguide 10 consisting of a dielectric thin film 3 formed on and in contact with the main surface of the single crystal substrate 2, and electrodes (first electrodes 7a, 7b and second electrodes 8a, 8b, 8c) that apply a voltage to the optical waveguide 10.
[0025] (Single crystal substrate 2) As the single crystal substrate 2, any known single crystal substrate can be used as long as it is capable of growing a c-axis oriented epitaxial film made of lithium niobate (LiNbO3). As the single crystal substrate 2, for example, a sapphire single crystal substrate, a silicon single crystal substrate, etc. can be used.
[0026] In the optical modulation element 200A of this embodiment, the single crystal substrate 2 preferably has a lower refractive index than LN. It is particularly preferable to use a sapphire single crystal substrate as the single crystal substrate 2. The sapphire single crystal substrate has a lower refractive index than LN. For this reason, for example, when the dielectric thin film 3 is used as the optical waveguide layer 10, it can play the role of a cladding layer. Therefore, when the single crystal substrate 2 is a sapphire single crystal substrate, the dielectric thin film 3 can be suitably used as the optical waveguide layer 10 of the optical modulation element 200A without providing a separate cladding layer between the single crystal substrate 2 and the dielectric thin film 3. When a silicon single crystal substrate is used as the single crystal substrate 2, it is necessary to provide a layer between the single crystal substrate 2 and the dielectric thin film 3, the refractive index of which is lower than that of LN, since the refractive index of silicon is higher than that of LN.
[0027] In the light modulation element 200A of this embodiment, the dielectric thin film 3 is made of an LN film, which is an epitaxial film oriented along the c-axis, and has three-fold symmetry. For this reason, it is desirable that the crystal orientation of the main surface (the surface on the dielectric thin film 3 side) of the single crystal substrate 2 has the same symmetry as that of the dielectric thin film 3. Therefore, when a sapphire single crystal substrate is used as the single crystal substrate 2, for example, it is preferable that the main surface is a c-plane. Furthermore, when a silicon single crystal substrate is used as the single crystal substrate 2, for example, it is preferable that the main surface is a (111) plane. The single crystal substrate 2 may have an off-angle.
[0028] In the light modulation element 200A of this embodiment, the dielectric thin film 3 formed on the single crystal substrate 2 is likely to be formed as a c-axis oriented epitaxial film for single crystal substrates 2 of various crystal orientations. Therefore, in the light modulation element 200A of this embodiment, the crystal orientation of the single crystal substrate 2 is not particularly limited.
[0029] (Dielectric Thin Film 3) The dielectric thin film 3 is made of an LN film, which is an epitaxial film oriented along the c-axis. Since LN has a large electro-optic constant, it is suitable as a material for the optical waveguide layer 10 of the optical modulation element 200A.
[0030] The LN film forming the dielectric thin film 3 may contain elements such as K, Na, Rb, Cs, Be, Mg, Ca, Sr, Ta, Ba, Ti, Zr, Hf, V, Cr, Mo, W, Fe, Co, Ni, Zn, Sc, and Ce.
[0031] The dielectric thin film 3 has an X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of 0.02 or more between LiNb3O8 and LiNbO3. Therefore, DC drift is suppressed when a voltage is applied to the optical waveguide 10. In order to further suppress DC drift in the optical modulation element 200A, the dielectric thin film 3 preferably has an X-ray intensity ratio of 0.03 or more between LiNb3O8 and LiNbO3.
[0032] When a lithium niobate film is epitaxially grown, it may grow epitaxially in a so-called twin crystal state in which crystals sharing a c-axis are bonded. There is no problem even if the lithium niobate film forming the dielectric thin film 3 in the optical modulation element 200A of this embodiment is a twin crystal.
[0033] 1, 2(a) and 2(b) is a device that applies a voltage to a Mach-Zehnder interferometer formed of an optical waveguide 10 to modulate light propagating through the optical waveguide 10. As shown in Fig. 1, the optical waveguide 10 has a first optical waveguide 10a and a second optical waveguide 10b branched from a single input optical waveguide, and an output optical waveguide 10c in which the first optical waveguide 10a and the second optical waveguide 10b are combined.
[0034] As shown in Fig. 1 and Fig. 2(b), two first electrodes 7a and 7b are provided on the first optical waveguide 10a and the second optical waveguide 10b, respectively. Therefore, the light modulation element 200A has a dual electrode structure. The first electrodes 7a and 7b may be made of, for example, an Au film or a laminated film of a Ti film and an Au film.
[0035] The optical modulation element 200A shown in FIG. 1, FIG. 2(a) and FIG. 2(b) has a ridge portion 4 formed by processing a dielectric thin film 3 into a ridge shape (convex shape). In the optical modulation element 200A, the ridge portion 4 forms an optical waveguide 10. As shown in FIG. 2(b), a first electrode 7a is formed on the ridge portion 4 constituting the first optical waveguide 10a of the optical waveguide 10 via a buffer layer 5. Also, a first electrode 7b is formed on the ridge portion 4 constituting the second optical waveguide 10b of the optical waveguide 10 via a buffer layer 5. As shown in FIG. 2(b), the buffer layer 5 is formed so as to cover the upper surface and the side surface of the ridge portion 4. As the buffer layer 5, for example, one made of a SiO2 film, one made of a thin film in which an oxide of a metal element is added to SiO2, or the like can be used.
[0036] As shown in FIG. 1 and FIG. 2(b), the second electrodes 8a, 8b, 8c are provided spaced apart from each other via the first electrodes 7a, 7b. The second electrodes 8a, 8b, 8c are formed in contact with the upper surface of the slab portion made of the dielectric thin film 3. The second electrodes 8a, 8b, 8c may be made of, for example, an Au film or a laminated film of a Ti film and an Au film. The first electrodes 7a, 7b and the second electrodes 8a, 8b, 8c apply a voltage that changes the refractive index of the first optical waveguide 10a and the second optical waveguide 10b of the optical waveguide 10 in the in-plane direction from above the dielectric thin film 3. The slab portion made of the dielectric thin film 3 is obtained by thinning a part of the upper surface of the dielectric thin film 3 formed in contact with the main surface of the single crystal substrate 2 by etching or the like. As shown in FIG. 1, the first electrodes 7a, 7b and the second electrodes 8a, 8b, 8c are connected via a termination resistor 9.
[0037] [Method of manufacturing optical modulation element] The light modulation element 200A shown in Figures 1, 2(a) and 2(b) can be manufactured, for example, by the manufacturing method shown below. Figure 3 is a process diagram for explaining the manufacturing method of the light modulation element 200A shown in Figures 1, 2(a) and 2(b), and is a cross-sectional view showing the substrate 1 with the dielectric thin film.
[0038] 3, a dielectric thin film 3 is formed on and in contact with a main surface 2a of a single crystal substrate 2 to manufacture a substrate 1 with a dielectric thin film (dielectric thin film formation step). In the dielectric thin film formation step, the dielectric thin film 3 is formed on the main surface 2a of the single crystal substrate 2 by an epitaxial growth method.
[0039] The thickness of the dielectric thin film 3 epitaxially grown on the main surface 2a of the single crystal substrate 2 is preferably 0.2 μm to 2 μm. If the thickness of the dielectric thin film 3 is 0.2 μm or more, the dielectric thin film 3 of the substrate 1 with the dielectric thin film is applicable to a wide range of light from visible light to infrared light when used as the optical waveguide layer 10 of the optical modulation element 200A. If the thickness of the dielectric thin film 3 is 2 μm or less, the occurrence of cracks in the lithium niobate film forming the dielectric thin film 3 can be effectively suppressed.
[0040] The method for forming the dielectric thin film 3 may be any method that allows epitaxial growth on the main surface 2a of the single crystal substrate 2, and may be, for example, a sputtering method, a vacuum deposition method, a pulsed laser ablation (PLD) method, a chemical vapor deposition (CVD) method, a sol-gel method, or the like.
[0041] When sputtering is used as a method for depositing the dielectric thin film 3, a target having a composition in the range of Li / (Li+Nb)=48% to 51%, for example, can be used. The target can be produced, for example, by the following method. As the raw material, for example, a sintered body mainly composed of Li2CO3 and Nb2O5 with a purity of 3N or more is prepared. Next, the raw material is pulverized and mixed using a ball mill using balls made of ZrO2 to obtain a target powder material. The obtained target powder material is sintered using a known method to obtain a target.
[0042] In the target manufacturing process, when the raw material is pulverized using the ball mill, the balls made of ZrO2 are scraped off, and several hundred ppm or less of Zr is mixed into the target. However, since the amount of Zr mixed into the target is small, the dielectric thin film 3 can be epitaxially grown on the main surface 2a of the single crystal substrate 2 by sputtering using the target containing Zr.
[0043] There is no particular limitation on the shape of the target used for forming the dielectric thin film 3. In addition, the target preferably has a planar area twice or more the single crystal substrate 2 so that the dielectric thin film 3 having a uniform thickness can be obtained.
[0044] When sputtering is used as the method for depositing the dielectric thin film 3, the deposition conditions can be, for example, a mixture of Ar and O2 gas as the sputtering gas, the O2 ratio in the sputtering gas is set to 20% to 60%, the gas pressure is set to 0.1 Pa to 2 Pa, the temperature of the single crystal substrate 2 is set to 400°C to 700°C, a power of 500 W to 2000 W is applied, and the deposition rate is set to 2 nm / h to 15 nm / h. This allows the deposition of the dielectric thin film 3 made of a lithium niobate film, which is an epitaxial film with a c-axis orientation.
[0045] When the sputtering method is used as the method for forming the dielectric thin film 3, a lithium niobate film in which the X-ray intensity ratio between LiNb3O8 and LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) is 0.02 or more can be obtained by appropriately adjusting the above-mentioned film formation conditions. If the above-mentioned film formation conditions are not satisfied, a lithium niobate film in which the X-ray intensity ratio between LiNb3O8 and LiNbO3 is 0.02 or more cannot be formed. However, since the situation differs depending on the equipment used to form the dielectric thin film 3, it is not necessarily the case that a lithium niobate film in which the X-ray intensity ratio between LiNb3O8 and LiNbO3 is 0.02 or more can be obtained even if the above-mentioned film formation conditions are satisfied.
[0046] Next, the dielectric thin film 3 in the substrate 1 with the dielectric thin film shown in FIG. 3 is processed into a ridge shape (convex shape) using a known method such as an etching method, to form an optical waveguide 10 consisting of a ridge portion 4 and a slab portion consisting of the dielectric thin film 3, as shown in FIGS. 2(a) and 2(b).
[0047] Next, a buffer layer 5 is formed so as to cover the top and side surfaces of the ridge portion 4 using a known method such as sputtering, vacuum deposition, pulsed laser ablation (PLD) or chemical vapor deposition (CVD). Thereafter, using a known method such as sputtering or vacuum deposition, second electrodes 8a, 8b, and 8c are formed in contact with the upper surface of the slab portion made of the dielectric thin film 3, and first electrodes 7a and 7b are formed on the buffer layer 5. Through the above steps, the light modulation element 200A shown in FIG. 1, FIG. 2(a) and FIG. 2(b) is obtained.
[0048] [Operation principle of light modulation element] Next, the operating principle of the light modulation element 200A will be described. 1, the two first electrodes 7a, 7b and the second electrodes 8a, 8b, 8c are connected by a termination resistor 9 to function as traveling wave electrodes. The first electrodes 7a, 7b are used as signal electrodes, and the second electrodes 8a, 8b, 8c are used as ground electrodes. So-called complementary signals, which have the same absolute value, different positive and negative phases, and are not shifted, are input to the two first electrodes 7a, 7b from the input sides 15a, 15b of the first electrodes 7a, 7b of the optical modulation element 200A.
[0049] In this embodiment, when a signal is input from the input side 15a, 15b, a DC (direct current) voltage is applied in a superimposed manner in the in-plane direction of the dielectric thin film 3 from the first electrodes 7a, 7b toward the second electrodes 8a, 8b, 8c. This causes the refractive indexes of the first optical waveguide 10a and the second optical waveguide 10b of the optical waveguide 10 to change in proportion to the DC voltage, and output light having a modulated waveform is output from the output optical waveguide 10c. The modulated waveform of the output light output from the optical modulation element 200A changes with the application time of the DC (direct current) voltage. This change in the modulated waveform over time is called DC drift.
[0050] The lithium niobate film forming the dielectric thin film 3 in the substrate 1 with the dielectric thin film has an electro-optic effect. Therefore, the refractive indexes of the first optical waveguide 10a and the second optical waveguide 10b change to +Δn and -Δn, respectively, depending on a DC (direct current) voltage applied to the first optical waveguide 10a and the second optical waveguide 10b. As a result, the phase difference between the first optical waveguide 10a and the second optical waveguide 10b changes. Signal light having a modulated waveform that is intensity-modulated by this change in phase difference is output to the output side 12 from the output optical waveguide 10c in which the first optical waveguide 10a and the second optical waveguide 10b are multiplexed.
[0051] The optical modulation element 200A of this embodiment shown in FIG. 1, FIG. 2(a) and FIG. 2(b) has an optical waveguide 10 made of a dielectric thin film 3 formed on the main surface 2a of a single crystal substrate 2, the dielectric thin film 3 being made of a lithium niobate film which is an epitaxial film with a c-axis orientation, and the X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) between LiNb3O8 and LiNbO3 is 0.02 or more. Therefore, the optical modulation element 200A is formed in which DC drift is suppressed when a DC (direct current) voltage is applied in the in-plane direction from above the optical waveguide 10 by the first electrodes 7a, 7b and the second electrodes 8a, 8b and 8c. Therefore, the optical modulation element 200A of this embodiment is highly reliable and can be suitably used as, for example, an optical communication device.
[0052] When the optical modulation element 200A of this embodiment is heated to 120°C and a signal is input from the input sides 15a, 15b of the first electrodes 7a, 7b, a DC (direct current) voltage is applied from the first electrodes 7a, 7b toward the second electrodes 8a, 8b, 8c in the in-plane direction of the dielectric thin film 3 in a superimposed manner. It is preferable that the DC drift is 50% or less when the application time of the DC (direct current) voltage reaches 1 hour. The DC drift is a numerical value calculated using the following formula (I).
[0053] DC drift (%) = (shift voltage (V) / applied DC voltage (V)) x 100 (I) (In formula (I), the shift voltage (V) is a DC (direct current) voltage that indicates the amount of phase shift (amount of drift) of the modulated waveform relative to the modulated waveform at the time when the DC (direct current) voltage is applied.)
[0054] When the above DC drift of the light modulation element 200A of this embodiment when heated to 120° C. is 50% or less when the application time of the DC (direct current) voltage reaches 1 hour, the inventors consider that the characteristic is sufficiently practical for the device they are considering. This is because the light modulation element 200A is provided with a feedback driver (control circuit) that controls the DC (direct current) voltage applied from the first electrodes 7a, 7b to the second electrodes 8a, 8b, 8c, and the amount of shift in the phase of the modulation waveform can be easily compensated by applying a DC voltage corresponding to the shift voltage (V) by the feedback driver.
[0055] Although the preferred embodiment of the present invention has been described above, the present invention is not limited to the above embodiment. The present invention can be modified in various ways without departing from the spirit of the present invention, and it goes without saying that such modifications are also included within the scope of the present invention. For example, in the above-described embodiment, an optical modulation element has been described as a preferred example of the electro-optical element of the present invention, but the electro-optical element of the present invention is not limited to an optical modulation element and may be any electro-optical element that performs operating point control by applying a DC voltage, such as an optical switch. EXAMPLES
[0056] "Experimental Example 1" Fifteen substrates 1 with dielectric thin films as shown in FIG. 3 were manufactured by the method described below. First, as the single crystal substrate 2, a 4-inch sapphire single crystal substrate having a c-plane main surface 2a was prepared.
[0057] (Dielectric thin film deposition process) In the dielectric thin film formation step, the dielectric thin film 3 made of a lithium niobate film was formed on the main surface 2a of the single crystal substrate 2 by epitaxial growth using a sputtering method. The target used was a circle having a diameter of 8 inches and a composition of Li / (Li+Nb)=50%.
[0058] The target was produced using the following method. The raw materials were prepared as sintered bodies mainly composed of Li2CO3 and Nb2O5 with a purity of 3N or higher. The raw materials were then pulverized and mixed in a ball mill using balls made of ZrO2 to produce target powder. The obtained target powder was sintered to obtain the target.
[0059] The dielectric thin film 3 was formed by arranging the target thus obtained coaxially with the single crystal substrate 2 so that the distance from the main surface 2a of the single crystal substrate 2 was 70 mm. In addition, the dielectric thin film 3 was formed by using a mixed gas of Ar and O2 as the sputtering gas, setting the O2 ratio in the sputtering gas to 35% to 60%, the gas pressure to 0.1 Pa to 0.5 Pa, setting the temperature of the single crystal substrate 2 to 450°C to 700°C, and applying a power of 1500 W to 2000 W so that the film formation rate was 2 nm / h to 15 nm / h. By the above steps, 15 substrates 1 with dielectric thin films of Experimental Example 1 were obtained.
[0060] For the multiple dielectric thin film-attached substrates 1 of Experimental Example 1 thus obtained, an out-of-plane 2θ-θ scan was performed using an X-ray diffraction measuring device (manufactured by Rigaku Corporation) to check whether or not they had a c-axis orientation according to the following criteria. As a result, it was confirmed that for all of the dielectric thin film-attached substrates 1 of Experimental Example 1, the dielectric thin films 3 were epitaxial films having a c-axis orientation.
[0061] "standard" In the 2θ-θ scan of the out-of-plane measurement, a strong peak of the (006) plane, which is the c-axis orientation, was observed, and the peak intensity of the plane other than the (006) plane was 10% or less of the maximum peak intensity of the (006) plane, so the specimen was deemed to have a c-axis orientation.
[0062] Furthermore, lattice images were observed using a scanning transmission electron microscope (STEM) (manufactured by FEI) for the 15 substrates 1 with dielectric thin films in Experimental Example 1. As a result, it was confirmed that the dielectric thin films 3 made of lithium niobate films in the 15 substrates 1 with dielectric thin films in Experimental Example 1 all contained LiNb3O8 crystals and LiNbO3 crystals.
[0063] "Experimental Example 2" [Manufacturing of light modulation elements] Fifteen optical modulation elements 200A shown in FIG. 1, FIG. 2(a) and FIG. 2(b) were manufactured using the fifteen substrates 1 with dielectric thin films of Experimental Example 1 by the manufacturing method described below.
[0064] First, the dielectric thin film 3 in the substrate 1 with the dielectric thin film was processed into a ridge shape (convex shape) by etching to form an optical waveguide 10 consisting of a ridge portion 4, and a slab portion consisting of the dielectric thin film 3. Next, a buffer layer 5 made of a thin film containing SiO 2 as a main component and an oxide of In was formed so as to cover the upper and side surfaces of the ridge portion 4 by using a sputtering method.
[0065] Thereafter, a sputtering method was used to form a Ti film and an Au film in this order to become second electrodes 8a, 8b, and 8c in contact with the upper surface of the slab portion made of the dielectric thin film 3, and a Ti film and an Au film in this order to become first electrodes 7a and 7b were formed on the buffer layer 5. Using the obtained Ti film and Au film as seed layers, an Au film was further formed by plating, to form second electrodes 8a, 8b, and 8c and first electrodes 7a and 7b made of a laminated film of the Ti film and the Au film. Through the above steps, 15 light modulation elements 200A of Experimental Example 2 shown in FIG. 1, FIG. 2(a) and FIG. 2(b) were obtained.
[0066] For each of the dielectric thin films of the 15 optical modulation elements 200A in Experimental Example 2, the X-ray intensity ratio between LiNb3O8 and LiNbO3 was examined by the method described below.
[0067] "X-ray intensity ratio between LiNb3O8 and LiNbO3" An X-ray diffraction measurement device (manufactured by Rigaku) was used to perform 2θ-θ scans of out-of-plane measurements. From the charts of the X-ray diffraction results, the following analysis software PeakFit (manufactured by Hulinks) was used to obtain the following: <1> ~ <7> The LiNb3O8(60-2) peak and the LiNbO3(006) peak were separated and their areas were calculated using the calculation results. The ratio of the LiNb3O8(60-2) peak area to the LiNbO3(006) peak area (LiNb3O8(60-2) / LiNbO3(006)) was calculated as the X-ray intensity ratio between LiNb3O8 and LiNbO3.
[0068] "Calculation procedure for the peak area of LiNb3O8(60-2) and the peak area of LiNbO3(006)" <1> Read data in the 2θ range of 36 to 41 degrees. <2> Analyze using Gaussian Deconvolution (AutoFit Peaks III Deconvolution). <3> Enable Vary Width. <4> Use AI Expert to automatically set filter values. <5> Two peaks are selected: one in the 2θ range of about 38.2 to 38.5 degrees, and the other in the range of about 38.8 degrees. <6> Perform Addl Adjust with Full Peak Fit with Graphical Update. <7> The area value of the peak near 38.2 to 38.5 degrees is calculated and used as the peak area of LiNb3O8(60-2). Also, the area value of the peak near 38.8 degrees is calculated and used as the peak area of LiNbO3(006).
[0069] FIG. 4 is a scanning transmission electron microscope (STEM) photograph of a lithium niobate film selected from the dielectric thin films of 15 optical modulation elements 200A in Experimental Example 2, the X-ray intensity ratio of LiNb3O8 to LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) being 0.050. As shown in FIG. 4, it was confirmed that the lithium niobate film, which is the dielectric thin film of the optical modulation element 200A of Experimental Example 2, is composed of LiNbO3 crystals dotted with minute LiNb3O8 crystals.
[0070] Figure 5 is a chart of X-ray diffraction results for lithium niobate films selected from the dielectric thin films of the 15 optical modulation elements 200A in Experimental Example 2, the lithium niobate films having an X-ray intensity ratio between LiNb3O8 and LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) of 0.024 and 0.050.
[0071] Figures 5(a) and 5(b) are charts of the X-ray diffraction results of a lithium niobate film with an X-ray intensity ratio of 0.024, where the vertical axis is logarithmic in Figure 5(b), and Figures 5(c) and 5(d) are charts of the X-ray diffraction results of a lithium niobate film with an X-ray intensity ratio of 0.050, where the vertical axis is logarithmic in Figure 5(d). As shown in Figures 5(b) and 5(d), the lithium niobate film, which is the dielectric thin film of the optical modulation element 200A of Experimental Example 2, shows a shoulder due to the peak of LiNb3O8(60-2) in the 2θ range of approximately 38.2 to 38.5 degrees, and a peak of LiNbO3(006) in the 2θ range of approximately 38.8 degrees.
[0072] "DC drift evaluation" The fifteen light modulation elements 200A of Experimental Example 2 were each subjected to a DC drift evaluation by the method described below. That is, the optical modulation element 200A was heated to 120°C, and a signal was input from the input sides 15a, 15b of the first electrodes 7a, 7b. At that time, a DC (direct current) voltage of 8 V was superimposed and applied from the first electrodes 7a, 7b to the second electrodes 8a, 8b, 8c in the in-plane direction of the dielectric thin film 3. Then, for one hour from the time when the DC (direct current) voltage was applied in the in-plane direction of the dielectric thin film 3, the modulated waveform of the output light output from the output optical waveguide 10c of the optical modulation element 200A to the output side 12 was observed by an oscilloscope.
[0073] Then, when the application time of the DC voltage reached 1 hour, the DC drift (DC drift after 1 hour) was calculated using the above formula (I) from the phase shift (drift amount) of the modulated waveform relative to the modulated waveform at the time of application of the DC voltage. The results are shown in Figure 6.
[0074] 6 is a graph showing the relationship between the X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of the lithium niobate film in the substrate 1 with the dielectric thin film used in the optical modulation element 200A of Experimental Example 2 and the DC drift after one hour of the optical modulation element 200A of Experimental Example 2. In FIG. 6, the DC drift after one hour exceeding 50% is evaluated as failing, and the DC drift of 50% or less is evaluated as passing.
[0075] As shown in FIG. 6, the optical modulation elements 200A in which the X-ray intensity ratio (LiNb3O8(60-2) / LiNbO3(006)) of the lithium niobate film LiNb3O8 to LiNbO3 was 0.02 or more had a DC drift of 50% or less after one hour. In contrast, the optical modulation element 200A, in which the X-ray intensity ratio of the lithium niobate film is less than 0.02, exhibited a DC drift of more than 50% after one hour.
[0076] From these findings, it has been confirmed that DC drift can be suppressed by using an optical modulator 200A in which an optical waveguide 10 consisting of a dielectric thin film 3 formed in contact with the main surface 2a of a single crystal substrate 2 is made of a lithium niobate film, which is an epitaxial film oriented along the c-axis, and the X-ray intensity ratio of LiNb3O8 to LiNbO3 (LiNb3O8(60-2) / LiNbO3(006)) is 0.02 or more. [Explanation of symbols]
[0077] 1 substrate with dielectric thin film, 2 single crystal substrate, 2a main surface, 3 dielectric thin film, 4 ridge portion, 5 buffer layer, 7a, 7b first electrode, 8a, 8b, 8c second electrode, 9 termination resistor, 10 optical waveguide, 10a first optical waveguide, 10b second optical waveguide, 10c output optical waveguide, 12 output side, 15a, 15b input side, 200A optical modulation element.
Claims
1. A single crystal substrate; an optical waveguide made of a dielectric thin film formed on and in contact with a main surface of the single crystal substrate; an electrode for applying a voltage to the optical waveguide; The dielectric thin film is made of a lithium niobate film, which is an epitaxial film oriented along the c-axis. 3 O 8 and LiNbO 3 X-ray intensity ratio (LiNb 3 O 8 (60-2) / LiNbO 3 (006)) is 0.02 or more.
2. 2. The electro-optic element according to claim 1, wherein the single crystal substrate is a sapphire single crystal substrate, the main surface of which is a c-plane.
3. 3. An optical modulation element comprising the electro-optic element according to claim 1.
Citation Information
Patent Citations
Optical waveguide element and optical modulator using the same
JP2015230466A