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JP5141632B2 - Wafer with inspection electrode and method of measuring refractive index - Google Patents
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JP5141632B2 - Wafer with inspection electrode and method of measuring refractive index - Google Patents

Wafer with inspection electrode and method of measuring refractive index Download PDF

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JP5141632B2
JP5141632B2 JP2009105195A JP2009105195A JP5141632B2 JP 5141632 B2 JP5141632 B2 JP 5141632B2 JP 2009105195 A JP2009105195 A JP 2009105195A JP 2009105195 A JP2009105195 A JP 2009105195A JP 5141632 B2 JP5141632 B2 JP 5141632B2
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electrode
inspection
wafer
electrodes
refractive index
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JP2010256541A (en
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将之 本谷
勝利 近藤
勇貴 金原
哲也 藤野
正明 須藤
潤一郎 市川
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Sumitomo Osaka Cement Co Ltd
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Description

本発明は、光導波路と電極が形成された光導波路素子の製造工程において前記電極の屈折率を測定する技術に関する。   The present invention relates to a technique for measuring a refractive index of an electrode in a manufacturing process of an optical waveguide element in which an optical waveguide and an electrode are formed.

電気光学効果を有する強誘電体基板にマッハツェンダー型光導波路と進行波型電極を形成した光変調器が開発され、光通信や光計測に利用されている(例えば、特許文献1参照)。この構成の光変調器を広帯域で動作可能とするためには、光導波路を伝搬する光信号と電極を進行するマイクロ波との速度整合をとる必要があり、そのために、光変調器の製造時において、電極のマイクロ波に対する屈折率を測定することは重要である。   An optical modulator in which a Mach-Zehnder type optical waveguide and a traveling wave type electrode are formed on a ferroelectric substrate having an electro-optic effect has been developed and used for optical communication and optical measurement (see, for example, Patent Document 1). In order to enable the optical modulator of this configuration to operate in a wide band, it is necessary to match the speed of the optical signal propagating through the optical waveguide and the microwave traveling through the electrode. It is important to measure the refractive index of the electrode with respect to microwaves.

特開平4−288518号公報JP-A-4-288518

上記の光変調器を製造する工程は、一般的には次のようになる。まず、1枚のウエハ上に、薄膜形成工程及びフォトリソグラフィ工程を用いて光導波路パターンと電極パターンを多数形成する。次に、このウエハ内の電極パターンの電気特性を検査する。例えば、この検査工程では、電極にマイクロ波を入力して上述のように電極のマイクロ波に対する屈折率を測定し、得られた屈折率の値によって良否判定を行う。次に、ウエハを個々の光変調器の形状に切断して光変調器1つ1つをチップ化する。次に、チップ化前の電気特性の検査結果と、チップ化後に行う光導波路の光学特性の検査結果とに基づいて、チップ化されたそれぞれの光変調器の良品と不良品を選別する。   The process of manufacturing the above optical modulator is generally as follows. First, a large number of optical waveguide patterns and electrode patterns are formed on a single wafer using a thin film forming process and a photolithography process. Next, the electrical characteristics of the electrode pattern in the wafer are inspected. For example, in this inspection process, microwaves are input to the electrodes, the refractive index of the electrodes with respect to the microwaves is measured as described above, and the quality is determined based on the obtained refractive index value. Next, the wafer is cut into individual optical modulator shapes, and each optical modulator is formed into a chip. Next, a non-defective product and a defective product of each of the optical modulators formed into chips are selected based on the electrical property inspection results before chip formation and the optical property inspection results of the optical waveguide performed after chip formation.

このように、従来は、ウエハ全面においてマイクロ波の屈折率が不良となっていた場合であっても電極パターンの全数検査を行っていたため、屈折率の測定回数が多く、検査に時間がかかっていた。また、電極の引き回し配線が長く形成された電極パターンでは、その部分が屈折率の測定に影響を及ぼし、実際にマイクロ波と光信号が相互作用する電極の電界印加部(光導波路と平行に配設されている部分)の屈折率を正確に測定することができなかった。また、引き回し配線は電界印加部と延伸方向が異なるため、ウエハの結晶異方性により、引き回し配線の屈折率は電界印加部の屈折率とは異なる値を示すが、このことも実際に知りたい電界印加部の屈折率を正確に測定できない一因となっていた。   As described above, conventionally, since all the electrode patterns are inspected even when the refractive index of the microwave is poor over the entire surface of the wafer, the number of times of measuring the refractive index is large and the inspection takes time. It was. Also, in the electrode pattern in which the electrode routing wiring is formed long, the portion affects the measurement of the refractive index, and the electric field application portion of the electrode where the microwave and the optical signal actually interact (arranged in parallel with the optical waveguide). The refractive index of the portion provided) could not be measured accurately. In addition, the drawing wiring has a different drawing direction from that of the electric field application part, so the refractive index of the drawing wiring shows a different value from the refractive index of the electric field application part due to the crystal anisotropy of the wafer. This is one of the reasons that the refractive index of the electric field application part cannot be measured accurately.

本発明は上記の点に鑑みてなされたものであり、その目的は、光導波路と電極が形成された光導波路素子の製造工程において、電極の屈折率を簡便且つ正確に測定することが可能な検査用電極付きウエハ及び屈折率測定方法を提供することにある。   The present invention has been made in view of the above points, and an object of the present invention is to easily and accurately measure the refractive index of an electrode in a manufacturing process of an optical waveguide element in which an optical waveguide and an electrode are formed. An object of the present invention is to provide a wafer with an inspection electrode and a refractive index measurement method.

本発明は上記の課題を解決するためになされたものであり、電気光学効果を有するウエハに、複数の光導波路と、前記光導波路に沿ってホット電極及びアース電極が配置されてなる、該電極間に電気信号を進行させて該光導波路を伝搬する光を制御するための複数の進行波型制御電極と、前記ホット電極と同一断面形状及び同一延伸方向を有し、長さがそれぞれ異なる少なくとも2つの検査用電極と、を形成したことを特徴とする検査用電極付きウエハである。   The present invention has been made to solve the above-described problems, and includes a plurality of optical waveguides, and a hot electrode and a ground electrode arranged along the optical waveguide on a wafer having an electro-optic effect. A plurality of traveling-wave control electrodes for controlling the light propagating through the optical waveguide by passing an electric signal therebetween, and having the same cross-sectional shape and the same extending direction as the hot electrode, and at least different in length A wafer with inspection electrodes, characterized in that two inspection electrodes are formed.

また、本発明は、上記の検査用電極付きウエハにおいて、前記複数の進行波型制御電極の電界印加部は複数種類の断面形状を有し、前記断面形状の種類毎に前記少なくとも2つの検査用電極が設けられていることを特徴とする。   Further, the present invention provides the above-mentioned wafer with inspection electrodes, wherein the electric field application portions of the plurality of traveling wave type control electrodes have a plurality of types of cross-sectional shapes, and the at least two types of inspection use for each type of the cross-sectional shapes An electrode is provided.

また、本発明は、上記の検査用電極付きウエハにおいて、前記ホット電極と前記ウエハの間、及び前記検査用電極と前記ウエハの間は、同一の膜構成であることを特徴とする。   Further, the present invention is characterized in that, in the wafer with an inspection electrode, the same film configuration is formed between the hot electrode and the wafer and between the inspection electrode and the wafer.

また、本発明は、電気光学効果を有するウエハに、複数の光導波路と、前記光導波路に沿ってホット電極及びアース電極が配置されてなる、該電極間に電気信号を進行させて該光導波路を伝搬する光を制御するための進行波型制御電極と、前記ホット電極と同一断面形状及び同一延伸方向を有し、長さがそれぞれ異なる少なくとも2つの検査用電極と、を形成し、前記検査用電極の少なくとも2つに電気信号を入力して各電気信号がそれぞれ検査用電極を伝搬するのに要した遅延時間を測定し、前記各検査用電極の長さと前記測定された各遅延時間との傾きに基づいて前記検査用電極の電気信号に対する屈折率を求めることを特徴とする屈折率測定方法である。   Further, the present invention provides a wafer having an electro-optic effect, wherein a plurality of optical waveguides and a hot electrode and a ground electrode are disposed along the optical waveguide, and an electric signal is advanced between the electrodes to cause the optical waveguide to travel. A traveling-wave control electrode for controlling light propagating through the hot electrode, and at least two inspection electrodes having the same cross-sectional shape and the same extending direction as the hot electrode, and having different lengths, and the inspection An electrical signal is input to at least two of the test electrodes, and the delay time required for each electrical signal to propagate through the test electrode is measured. The length of each test electrode and the measured delay time The refractive index measurement method is characterized in that a refractive index with respect to an electric signal of the inspection electrode is obtained based on the inclination of the above.

本発明によれば、ウエハに形成された長さがそれぞれ異なる検査用電極に電気信号を入力してその遅延時間を測定し、各検査用電極の長さと測定された各遅延時間との傾きを求めることによって、ウエハをチップ化する前に電極の屈折率を簡便に測定することができるとともに、電極の取り回し部分の影響を受けることなく電極の屈折率を正確に測定することができる。   According to the present invention, an electrical signal is input to inspection electrodes formed on wafers having different lengths and the delay time is measured, and the inclination between the length of each inspection electrode and the measured delay time is determined. As a result, the refractive index of the electrode can be easily measured before the wafer is made into chips, and the refractive index of the electrode can be accurately measured without being affected by the electrode handling portion.

本発明の一実施形態による検査用電極付きウエハの全体構成図である。1 is an overall configuration diagram of a wafer with inspection electrodes according to an embodiment of the present invention. 検査用電極の詳細構成図である。It is a detailed block diagram of the electrode for a test | inspection. 検査用電極を用いてマイクロ波に対する屈折率を測定した測定結果の一例である。It is an example of the measurement result which measured the refractive index with respect to a microwave using the electrode for a test | inspection.

以下、図面を参照しながら本発明の実施形態について詳しく説明する。
図1は、本発明の一実施形態による検査用電極付きウエハの全体構成図である。ウエハ1は、電気光学効果を有する材料、例えばニオブ酸リチウムで構成されている。ウエハ1の第1エリア10には、実際の製品である光導波路素子の光導波路パターン101と電極パターンが、行方向と列方向に複数配列して形成されている。光導波路パターン101は、平面形状がマッハツェンダー型光導波路をなしている。電極パターンは、図示を省略しているが、マッハツェンダー型光導波路のアームに沿ってホット電極とアース電極が配置された、進行波型電極をなしている。そして、ホット電極とアース電極は、電極間を進行するマイクロ波によって光導波路に電界が印加されるよう光導波路と平行に配設されている電界印加部と、外部との電気的接続をとるための端子までの引き回し配線部とからなっている。この1つのマッハツェンダー型光導波路とそれに対応する進行波型電極によって、1つの光変調器が構成される。ウエハ1から個々の光変調器をチップ化した後には、進行波型電極にマイクロ波を入力すると電界印加部から光導波路に電界が印加され、電気光学効果により光導波路の屈折率が変化し、マッハツェンダー型光導波路を伝搬する光に変調が施される。
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
FIG. 1 is an overall configuration diagram of a wafer with electrodes for inspection according to an embodiment of the present invention. The wafer 1 is made of a material having an electro-optic effect, for example, lithium niobate. In the first area 10 of the wafer 1, a plurality of optical waveguide patterns 101 and electrode patterns of optical waveguide elements which are actual products are arranged in the row direction and the column direction. The planar shape of the optical waveguide pattern 101 is a Mach-Zehnder type optical waveguide. Although not shown, the electrode pattern is a traveling wave electrode in which a hot electrode and a ground electrode are arranged along the arm of the Mach-Zehnder optical waveguide. The hot electrode and the ground electrode are connected to the outside of the electric field applying unit disposed in parallel with the optical waveguide so that the electric field is applied to the optical waveguide by the microwave traveling between the electrodes. It consists of a routing wiring part to the terminal. This one Mach-Zehnder type optical waveguide and the traveling wave type electrode corresponding thereto constitute one optical modulator. After the individual optical modulators are made into chips from the wafer 1, when a microwave is input to the traveling wave type electrode, an electric field is applied from the electric field applying unit to the optical waveguide, and the refractive index of the optical waveguide changes due to the electrooptic effect, The light propagating through the Mach-Zehnder type optical waveguide is modulated.

ウエハ1の第2エリア20には、2つの検査用電極201,202が形成されている。図2は、検査用電極201,202の詳細構成図である。検査用電極201,202は、直線電極部201a,202aと直線電極部201a,202aの両端のパッド電極部201b,202bから構成されている。直線電極部201a,202aは、第1エリア10に形成されている光変調器のホット電極と平行に設けられている。また、直線電極部201a,202aは、ホット電極の電界印加部と同一の断面形状、即ち、ホット電極の電界印加部と同一の膜厚及びパターンの幅を持つように形成されている。更に、一方の直線電極部201aの長さは、他方の直線電極部202aの長さより長く形成されている。また、パッド電極部201bとパッド電極部202bの形状は同一である。   Two inspection electrodes 201 and 202 are formed in the second area 20 of the wafer 1. FIG. 2 is a detailed configuration diagram of the inspection electrodes 201 and 202. The inspection electrodes 201 and 202 are composed of linear electrode portions 201a and 202a and pad electrode portions 201b and 202b at both ends of the linear electrode portions 201a and 202a. The straight electrode portions 201 a and 202 a are provided in parallel with the hot electrode of the optical modulator formed in the first area 10. The straight electrode portions 201a and 202a are formed to have the same cross-sectional shape as the electric field applying portion of the hot electrode, that is, the same film thickness and pattern width as the electric field applying portion of the hot electrode. Further, the length of one linear electrode portion 201a is longer than the length of the other linear electrode portion 202a. Further, the pad electrode portion 201b and the pad electrode portion 202b have the same shape.

上記の検査用電極201,202のマイクロ波に対する屈折率を測定する方法は、次のとおりである。屈折率の測定は、ウエハ1を切断しチップ化する前の1枚のウエハの状態で行う。このウエハの状態において、検査用電極201のパッド電極部201bに検査用プローブを接続し、ネットワークアナライザを用いてこの検査用プローブから測定信号を入力しタイムドメイン法によりその反射信号の遅延時間を測定する。このとき、遅延時間t1は、t1=Nm・2・(L1+ΔL)/cと表される。但し、Nmは検査用電極のマイクロ波に対する屈折率、L1は直線電極部201aの長さ、ΔLはパッド電極部201bの長さ、cは光速である。同様に、検査用電極202についても遅延時間を測定する。このとき、遅延時間t2は、t2=Nm・2・(L2+ΔL)/cと表される。但し、L2は直線電極部202aの長さである。   A method of measuring the refractive index of the inspection electrodes 201 and 202 with respect to the microwave is as follows. The refractive index is measured in the state of one wafer before the wafer 1 is cut into chips. In this wafer state, an inspection probe is connected to the pad electrode portion 201b of the inspection electrode 201, a measurement signal is input from the inspection probe using a network analyzer, and the delay time of the reflected signal is measured by the time domain method. To do. At this time, the delay time t1 is expressed as t1 = Nm · 2 · (L1 + ΔL) / c. Where Nm is the refractive index of the inspection electrode with respect to the microwave, L1 is the length of the straight electrode portion 201a, ΔL is the length of the pad electrode portion 201b, and c is the speed of light. Similarly, the delay time is also measured for the inspection electrode 202. At this time, the delay time t2 is expressed as t2 = Nm · 2 · (L2 + ΔL) / c. However, L2 is the length of the linear electrode part 202a.

この2つの測定結果を、横軸を直線電極部の長さ、縦軸を遅延時間とするグラフ上にプロットする。図3に測定結果の一例を示す。プロットされた2点を結ぶ直線の傾きをαとすると、検査用電極のマイクロ波に対する屈折率Nmは、
Nm=(α/2)・c
により求めることができる。
These two measurement results are plotted on a graph with the horizontal axis representing the length of the straight electrode portion and the vertical axis representing the delay time. FIG. 3 shows an example of the measurement result. When the slope of the straight line connecting the two plotted points is α, the refractive index Nm of the inspection electrode with respect to the microwave is
Nm = (α / 2) · c
It can ask for.

このように、本発明によれば、ウエハをチップ化する前に電極の屈折率を簡便に測定することができる。また、2つの検査用電極における遅延時間を測定し、図3のグラフの傾きから屈折率を求めているので、電極の取り回し部分やパッド電極の影響を受けることなく電極の屈折率を正確に測定することができる。   Thus, according to the present invention, the refractive index of the electrode can be easily measured before the wafer is chipped. In addition, the delay time of the two test electrodes is measured, and the refractive index is obtained from the slope of the graph of FIG. 3, so that the refractive index of the electrode can be accurately measured without being affected by the electrode handling portion or the pad electrode. can do.

以上、図面を参照してこの発明の一実施形態について詳しく説明してきたが、具体的な構成は上述のものに限られることはなく、この発明の要旨を逸脱しない範囲内において様々な設計変更等をすることが可能である。
例えば、検査用電極の本数は3本以上であってもよい。この場合、図3のグラフにおけるプロット点は3点以上となるが、統計的な処理を行うことで屈折率の測定精度を向上させることができる。
また、検査用電極の遅延時間の測定は、一端側のパッド電極部から他端側のパッド電極部へ透過する信号の遅延時間を測定してもよい。この場合、屈折率を求める式は、Nm=α/cとなる。
また、1つのウエハ内にホット電極の電界印加部の断面形状が複数種類存在している場合は、検査用電極を電界印加部の断面形状の種類毎に設けることが好ましい。
また、ホット電極とウエハの間、及び検査用電極とウエハの間は、同一の膜構成(同じ材質で同じ膜厚)であることが望ましい。
As described above, the embodiment of the present invention has been described in detail with reference to the drawings. However, the specific configuration is not limited to the above, and various design changes and the like can be made without departing from the scope of the present invention. It is possible to
For example, the number of inspection electrodes may be three or more. In this case, the number of plot points in the graph of FIG. 3 is three or more, but the measurement accuracy of the refractive index can be improved by performing statistical processing.
In addition, the measurement of the delay time of the inspection electrode may be performed by measuring the delay time of a signal transmitted from the pad electrode portion on one end side to the pad electrode portion on the other end side. In this case, the equation for obtaining the refractive index is Nm = α / c.
In addition, when there are a plurality of types of cross-sectional shapes of the electric field application portion of the hot electrode in one wafer, it is preferable to provide an inspection electrode for each type of cross-sectional shape of the electric field application portion.
Further, it is desirable that the hot film and the wafer and the inspection electrode and the wafer have the same film configuration (the same material and the same film thickness).

1…ウエハ 101…光導波路パターン 201,202…検査用電極 201a,202a…直線電極部 201b,202b…パッド電極部   DESCRIPTION OF SYMBOLS 1 ... Wafer 101 ... Optical waveguide pattern 201, 202 ... Inspection electrode 201a, 202a ... Linear electrode part 201b, 202b ... Pad electrode part

Claims (4)

電気光学効果を有するウエハに、
複数の光導波路と、
前記光導波路に沿ってホット電極及びアース電極が配置されてなる、該電極間に電気信号を進行させて該光導波路を伝搬する光を制御するための複数の進行波型制御電極と、
前記ホット電極と同一断面形状及び同一延伸方向を有し、長さがそれぞれ異なる少なくとも2つの検査用電極と、
を形成したことを特徴とする検査用電極付きウエハ。
For wafers with electro-optic effect,
A plurality of optical waveguides;
A plurality of traveling-wave control electrodes for controlling light propagating through the optical waveguide by advancing an electrical signal between the electrodes, wherein a hot electrode and a ground electrode are disposed along the optical waveguide;
At least two inspection electrodes having the same cross-sectional shape and the same extending direction as the hot electrode, each having a different length;
A wafer with an inspection electrode, characterized in that is formed.
前記複数の進行波型制御電極の電界印加部は複数種類の断面形状を有し、
前記断面形状の種類毎に前記少なくとも2つの検査用電極が設けられている
ことを特徴とする請求項1に記載の検査用電極付きウエハ。
The electric field application portions of the plurality of traveling wave type control electrodes have a plurality of types of cross-sectional shapes,
The wafer with inspection electrodes according to claim 1, wherein the at least two inspection electrodes are provided for each type of the cross-sectional shape.
前記ホット電極と前記ウエハの間、及び前記検査用電極と前記ウエハの間は、同一の膜構成であることを特徴とする請求項1又は請求項2に記載の検査用電極付きウエハ。   The wafer with an inspection electrode according to claim 1 or 2, wherein the film structure is the same between the hot electrode and the wafer and between the inspection electrode and the wafer. 電気光学効果を有するウエハに、複数の光導波路と、前記光導波路に沿ってホット電極及びアース電極が配置されてなる、該電極間に電気信号を進行させて該光導波路を伝搬する光を制御するための進行波型制御電極と、前記ホット電極と同一断面形状及び同一延伸方向を有し、長さがそれぞれ異なる少なくとも2つの検査用電極と、を形成し、
前記検査用電極の少なくとも2つに電気信号を入力して各電気信号がそれぞれ検査用電極を伝搬するのに要した遅延時間を測定し、
前記各検査用電極の長さと前記測定された各遅延時間との傾きに基づいて前記検査用電極の電気信号に対する屈折率を求める
ことを特徴とする屈折率測定方法。
A plurality of optical waveguides and a hot electrode and a ground electrode are arranged along the optical waveguide on a wafer having an electro-optic effect, and an electric signal is advanced between the electrodes to control light propagating through the optical waveguide. A traveling wave type control electrode, and at least two inspection electrodes having the same cross-sectional shape and the same extending direction as the hot electrode, and different lengths from each other,
An electrical signal is input to at least two of the inspection electrodes, and a delay time required for each electrical signal to propagate through the inspection electrode is measured.
A refractive index measurement method, wherein a refractive index with respect to an electrical signal of the inspection electrode is obtained based on a slope between the length of each inspection electrode and each measured delay time.
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