Optical modulator

Details Optical modulator Optical modulator

2003-02-21

2004-07-27

Dung, Hung Xuan (Department: 2873)

Optical: systems and elements

Optical modulator

C359S245000, C359S278000, C359S322000, C385S002000, C385S008000

Reexamination Certificate

active

06768570

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to an optical modulator in which an element varying optical phase using the electrooptic effect is housed.
BACKGROUND OF THE INVENTION
An optical communication system has been applied for a large capacity broadband communication system. With increased demand for larger communication capacity, transmission at higher bit rate is required in such an optical communication system.
Meanwhile, an optical modulator is employed in the optical communication system. An element varying optical phase using the electrooptic effect is housed in the optical modulator, by which a refractive index is changed when electric field is applied on a ferroelectric crystal, etc.
Such an element varying the optical phase by the electrooptic effect (electrooptic effect element) to be housed in the optical modulator is provided with an optical waveguide formed on a wafer cut but of an electrooptic crystal of LiNbO
3
, LiTaO
2
, etc. with a metallic film of Ti, etc. produced thereon through patterning and thermal diffusion or proton exchange in benzoic acid by the IC production technique. Further a required electrode is formed in the vicinity of the optical waveguide.
The optical modulator has such a configuration that an optical signal is supplied from outside the electrooptic effect element to the optical waveguide, and that a high-frequency modulation signal of a microwave band is supplied to an electrode which is formed in the vicinity of the optical waveguide.
FIG. 1
shows one configuration example of the optical modulator, in which a top plan view of the uncovered optical modulator is illustrated. An electrooptic effect element
2
is housed in a shielding case
1
.
FIGS. 2A through 2C
are the schematic configuration diagrams of electrooptic effect element
2
.
To function as an optical modulator, an exemplary optical waveguide
10
formed on electrooptic effect element
2
is made to branch into two parallel waveguides I and II, which constitute a Mach-Zehnder waveguide, as schematically shown in FIG.
2
A.
FIG. 2B
is a cross-sectional view along line ‘a’ in the plan view shown in FIG.
2
A. Also
FIG. 2C
is a cross-sectional view along line ‘b’.
As an example, when using a Z-cut wafer for electrooptic effect element
2
cut out from an LiNbO
3
crystal in the Z-axis direction, constituting an electrode of a single electrode, and applying a modulation scheme of the intensity modulation, a signal electrode
20
is disposed right on top of either one of the parallel branch waveguides I, II (optical waveguide I in the case of
FIG. 2
A), while a ground electrode
22
is disposed right on top of the other optical waveguide (optical waveguide II in FIG.
2
A).
In addition, there is provided a buffer layer of 0.2-1 &mgr;m in thickness constituted of SiO
2
, etc. between the substrate and signal electrode
20
, as well as between the substrate and ground electrode
22
, so that the optical signal traveling in the two parallel waveguides I, II is prevented from being absorbed by signal electrode
20
and ground electrode
22
.
In
FIG. 2A
, an optical signal is input to an incident side (Opt In) of waveguide
10
. To function as an optical modulator, a rectangular microwave signal output from a signal source
25
is supplied to signal electrode
20
as a modulation signal in the same direction as the traveling direction of the optical signal.
Accordingly, the refractive indexes of branching optical waveguides disposed in parallel are varied corresponding to the polarity of the microwave signal, such as +&Dgr;na and −&Dgr;nb, respectively. This produces a varied optical phase difference between the phases in the parallel optical waveguides I, II. An intensity modulated optical signal is then output from an output side (Opt Out) shown in
FIG. 2A
of optical waveguide
10
.
Further, by altering the electrode section form, it becomes possible to control an effective refractive index caused by the microwave and match the velocities of the optical signal and the microwave, thus obtaining a wideband optical response characteristic.
Here, in the configuration of the optical modulator shown in
FIG. 1
, a high-frequency microwave signal as the modulation signal supplied from signal source
25
is supplied to the space between signal electrode
20
and ground electrodes
21
,
22
through an RF connector
3
. RF connector
3
is provided with a center conductor
30
and an external conductor
31
.
Center conductor
30
of RF connector
3
is inserted into a sliding contact member
32
and is connected to signal electrode
20
of electrooptic effect element
2
and to sliding contact member
32
by means of bonding. Also external conductor
31
of RF connector
3
is connected to ground electrodes
21
,
22
of electrooptic effect element
2
by means of wire bonding
23
.
In such a way, in the input portion of a high-frequency microwave signal, there are provided an interaction portion in which signal electrode
20
and ground electrodes
21
,
22
are disposed in parallel, and an extraction portion. A pad is formed on one end side of the extraction portion in which the electrode is widened.
A high-frequency signal input from the pad travels in the interaction portion through the extraction portion. The signal is output from another pad through the extraction portion of the output side, and thereafter the output signal is terminated.
In this configuration, in order to input a high-frequency signal efficiently by preventing the reflection of the microwave (traveling to the inside of the substrate of electrooptic effect element
2
), it is necessary to set the characteristic impedance of the extraction portion including the pads as 50 &OHgr;. For this purpose, conventionally, the gaps between signal electrode
20
and ground electrodes
21
,
22
in the extraction portion have been widened.
However, there has been a problem that when the aforementioned gaps are widened, the transmission characteristic becomes deteriorated because of an increase in a radiation component as a result of the diffused electric field between signal electrode
20
and ground electrodes
21
,
22
.
Namely, in the optical modulator of conventional configuration, when a high-frequency signal wavelength is sufficiently long compared to the electrode size of electrooptic effect element
2
, the transmission characteristic is not largely affected. However, the problem mentioned below has been recognized when the wavelength becomes short. In this case, the high-frequency characteristic of electrooptic effect element
2
is affected and, as a result, wideband transmission characteristic cannot be achieved.
FIG. 3
shows the high-frequency characteristic of the conventional optical modulator. In
FIG. 3
, RF signal frequency is shown in the horizontal axis, while attenuation S
21
of the optical signal traveling from the input side toward the output side is shown in the vertical axis. It is understood that, at the increased RF signal frequency in the vicinity of 36 GHz, a large dip is produced in the attenuation characteristic, instead of the attenuation being produced linearly. From this existence of the dip in the attenuation, it is to be understood that the wideband transmission characteristic is impeded.
Until recently, the cause of this attenuation dip in the transmission characteristic has not been investigated, and the inventor of the present invention has been studied to investigate this issue.
As a result of the study, the inventor of the present invention has found out the cause that, when the frequency of the microwave modulation signal becomes high, the radiation component of the microwave into electrooptic effect element
2
becomes increased, thus producing the coupling with the electric field which is formed between signal electrode
20
and ground electrode
21
.
SUMMARY OF THE INVENTION
Accordingly, it is an object of the present invention to provide a configuration of the optical modulator by which wideband characteristic can be obtained while maintaining a char

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