Polarization insensitive semiconductor optical amplifier and an optical communication system using the same

A polarization insensitive optical amplifying apparatus having a semiconductor laser structure, and serving as an amplifier for imparting a gain to input light from outside the apparatus. In the optical amplifying apparatus, a second semiconductor layer is formed on at least a first semiconductor layer. The lattice constant of the second semiconductor layer is less than the lattice constant of the first semiconductor layer. The second semiconductor layer undergoes a biaxial tensile stress due to a lattice mismatch between the first and second semiconductor layers, and serves as a well layer of an active layer having a quantum well structure. A third semiconductor layer is also formed on at least the first semiconductor layer. The lattice constant of the third semiconductor layer is less than the lattice constant of the first semiconductor layer. The third semiconductor layer also undergoes a biaxial tensile stress due to a lattice mismatch between the first and third semiconductor layers, and serves as a barrier layer of the active layer having the quantum well structure.

BACKGROUND OF THE INVENTION 
1. Field of the Invention 
The present invention relates to a polarization insensitive semiconductor 
optical amplifier or amplifying apparatus and an optical communication 
system or network using this optical amplifier. 
2. Related Background Art 
Generally, a semiconductor optical amplifier or an amplifying apparatus 
comprises a semiconductor laser structure including an active layer and a 
cladding layer, and amplifies an input light by means of a bias current, 
below a threshold, injected into the laser structure. In the optical 
communication field, the optical amplifier has been developed as a device 
for compensating for an optical loss that occurs in optical fibers or at 
connections between optical fibers. 
However, there has been the problem of a polarization dependency of the 
optical amplification factor (i.e. the optical amplification factor 
differs depending on the different polarization modes of an input light) 
when a semiconductor optical amplifier is used in optical fiber 
communication systems. Generally, the state of polarization of an output 
light, which is transmitted through the optical fiber, is unstable, so the 
level of an output light from the optical amplifier will not be stable 
when such light from the optical fiber is input into such an amplifier 
having the above-discussed polarization dependency. Further, the 
fluctuation of such output burdens a light receiving system regarding its 
dynamic range and the like. This is a vital drawback which limits the 
scale of the communication system. 
Therefore, various conventional methods of fabricating a polarization 
insensitive optical amplifier have been performed. Among them, a method of 
using a strain quantum well structure is proposed as a method for solving 
the polarization dependency of optical gain in the active layer. The 
strain quantum well structure is used for both controlling the oscillation 
wavelength and reducing an oscillation threshold gain in the field of 
semiconductor lasers, and thus this structure is a remarkably useful 
technique. 
Generally, in order to utilize a strain quantum well structure as a 
polarization insensitive optical amplifier, the gain for TM mode light is 
equalized with or made larger than that for TE light. More in particular, 
the degeneracy in a valence band is solved by the effect of strain, and 
hence band structures of heavy and light holes are respectively shifted. 
Thus, the energy gap between the ground level of electrons in the 
conduction band and the level of heavy holes in the valence band is 
approximately made equal with or made slightly larger than the energy gap 
between the ground level of electrons in the conduction band and the level 
of light holes in the valence band. When there is no polarization 
dependency of gain other than that of the optical gain, those energy gaps 
are equalized with each other. When there exists a gain dependency on 
polarization that is other than that of the optical gain, the latter 
energy gap, concerning the light holes, is made smaller. In general, 
optical confinement for TE light is larger than that for TM light, so the 
latter energy gap, concerning the light holes, is made smaller when 
considering such difference in optical confinement. 
Several methods have been proposed for creating the strain necessary for 
obtaining the above-discussed desired energy levels. 
First, a method for imparting a biaxial tensile stress to a well structure 
is proposed as disclosed in Japanese Patent Laid-Open Application No. 
1-251685 (1989). On a reference first semiconductor layer (i.e. a 
substrate or a cladding layer), a second semiconductor layer, having a 
lattice constant smaller than that of the first semiconductor layer, is 
formed. Hence a biaxial tensile stress is imparted to the second 
semiconductor layer. The energy level of the light holes in the valence 
band is shifted in a direction for narrowing its band gap, by imparting 
the biaxial tensile stress to the well layer. As a result, the energy 
level of light holes in the valence band approaches the energy level of 
heavy holes in the valence band, and hence a desired energy level is 
obtained. 
Second, a method for imparting a biaxial tensile stress to a barrier layer 
is proposed as disclosed in Japanese Patent Laid-Open Application No. 
4-27183 (1992). Similar to the first method, an energy level of light 
holes in a valence band of the barrier layer is shifted. As a result, a 
well for the light holes is shallowed, leading to a shift in the energy 
level, and a desired level results. 
Third, a method of fabricating an active layer having a strained well layer 
(a biaxial tensile stress exists) and a non-strained well layer is 
proposed as described in Japanese Patent Laid-Open Application No. 
1-257386 (1989). 
However, those prior art methods have respectively their own advantages and 
disadvantages. The first prior art method has an advantage in that a 
relatively large amount of energy shift can be obtained by a slight strain 
amount and thus a desired effect can be achieved by a relatively small 
amount of strain. On the other hand, an energy shift of the conduction 
band occurs simultaneously with an energy shift of the valence band due to 
the effect of strain. Conversely, the second prior art method has a 
drawback in that a relatively large amount of strain is needed, compared 
to the first prior art method, to attain a desired effect, although the 
wavelength, at which a gain is obtained, hardly changes. 
The third prior art method has an advantage in that freedom in design is 
increased by the combination of two well layers and a desired effect can 
be readily obtained. However, the amount of strain needs to be increased, 
compared to the first prior art method. 
A semiconductor optical amplifier is used for amplifying a signal light 
generated by driving a semiconductor laser, and this amplifier can be 
replaced by a structure resembling the semiconductor laser. If a 
wavelength range of gain of the amplifier largely changes due to the 
effects of strain, its construction material has to be unfavorably 
changed. 
Further, dislocation in a strained lattice can be prevented by reducing its 
layer thickness to a value less than a critical thickness, but its life 
time under a long-term driven condition decreases as the amount of strain 
increases. Moreover, the growth condition for fabricating the strained 
lattice becomes severe as the amount of strain increases. Therefore, it is 
not advantageous to increase the amount of strain excessively. 
SUMMARY OF THE INVENTION 
The object of the present invention is to provide, in view of the above 
problems, a polarization insensitive semiconductor optical amplifier or 
amplifying apparatus in which a change in a wavelength range of gain due 
to the effects of strain is small, and the amount of strain necessary for 
obtaining a desired effect does not need to be substantially increased, 
and an optical communication system using this optical amplifying 
apparatus. 
In the polarization insensitive optical amplifying apparatus of this 
invention, which imparts gain to a light signal input thereto, to achieve 
the above object, there are provided a first semiconductor layer having a 
first lattice constant; a second semiconductor layer, having a second 
lattice constant, and formed on at least the first semiconductor layer, 
the second lattice constant of the second semiconductor layer being less 
than the first lattice constant of the first semiconductor layer, and the 
second semiconductor layer undergoing a biaxial tensile stress because of 
a lattice mismatch between the first semiconductor layer and the second 
semiconductor layer and serving as a well layer for an active layer having 
a quantum well structure; and a third semiconductor layer, having a third 
lattice constant, and formed on at least the first semiconductor layer, 
the third lattice constant of the third semiconductor layer being less 
than the first lattice constant of the first semiconductor layer, and the 
third semiconductor layer undergoing a biaxial tensile stress because of a 
lattice mismatch between the first semiconductor layer and the third 
semiconductor layer and serving as a barrier layer of the active layer 
having a quantum well structure. This apparatus performs polarization 
insensitive type optical amplifying for imparting a gain to input light 
from outside. 
In the optical communication system of this invention, to achieve the above 
object, there are provided a transmitter station for transmitting optical 
signals; a receiver station for receiving the optical signals; a 
transmission line, upon which the optical signals travel, for connecting 
the transmitter station and the receiver station; and an optical 
amplifying apparatus, for amplifying the optical signals, disposed in at 
least one of the transmitter station and the receiver station. The optical 
amplifying apparatus is constructed as described above. 
In the optical communication system of this invention, to achieve the above 
object, there are provided a transmitter station for transmitting optical 
signals; a receiver station for receiving the optical signals; repeater 
equipment for amplifying the optical signals; a transmission line, upon 
which the optical signals travel, for connecting the transmitter station 
and the receiver station through the repeater equipment; and an optical 
amplifying apparatus, for amplifying the optical signals, disposed in at 
least one of the transmitter station, the receiver station and the 
repeater equipment. The optical amplifying apparatus is constructed as 
discussed above. 
In the bidirectional optical communication system of this invention to 
achieve the above object, there are provided a plurality of transceiver 
stations for transmitting and receiving optical signals; a transmission 
line, upon which the optical signals travel, for connecting the 
transceiver stations; and an optical amplifying apparatus disposed in at 
least one location of the transceiver stations. The optical amplifying 
apparatus, for amplifying the optical signals, is disposed in at least one 
of the transceiver stations. The amplifying apparatus is constructed as 
discussed above. 
In the bidirectional optical communication system of this invention, to 
achieve the above object, there are provided a plurality of transceiver 
stations for transmitting and receiving optical signals; repeater 
equipment for amplifying optical signals; a transmission line, upon which 
the optical signals travel, for connecting the transceiver stations 
through the repeater equipment; and an optical amplifying apparatus, for 
amplifying the optical signals, disposed in at least one of the 
transceiver stations and the repeater equipment. The optical amplifying 
apparatus is constructed as discussed above. 
In the bus-type optical communication system of this invention, to achieve 
the above object, there are provided a plurality of terminals which 
transmit and receive electrical signals; a plurality of transceiver 
stations, which are respectively connected to the terminals for 
transmitting and receiving the electrical signals to and from their 
respective one of the plurality of terminals, for performing optical 
communication among the terminals; at least one transmission line for 
connecting the plurality of transceiver stations; and an optical 
amplifying apparatus disposed in at least one of a light transmitting path 
from a light transmitter portion of any one of the plurality of 
transceiver stations to a light receiver portion of any one of the 
plurality of transceiver stations. The optical amplifying apparatus is 
constructed as discussed above. 
In the active bus-type optical communication system of this invention to 
achieve the above object, there are provided a plurality of terminals 
which transmit and receive electrical signals; a plurality of optical 
nodes, each of the optical nodes including, at least, a plurality of means 
for transmitting a light signal, a plurality of means for receiving the 
light signal and means for controlling communication, wherein the 
plurality of optical nodes transmit and receive the electrical signals to 
and from their respective one of the plurality of terminals; a 
transmission line for connecting the plurality of optical nodes; and an 
optical amplifying apparatus, for amplifying the light signal, disposed in 
at least one of light transmitting path from the light signal transmitting 
means in any one of the plurality of optical nodes to the light signal 
receiving means in any one of the plurality of optical nodes. The optical 
amplifying apparatus is constructed as described above. 
In the star-type optical communication network of this invention to achieve 
the above object, there are provided a plurality of transceiver stations, 
each of the transceiver stations including a light transmitter portion for 
transmitting optical signals and a light receiver portion for receiving 
optical signals; a star coupler which connects the optical signal between 
the plurality of transceiver stations; a transmission line, upon which the 
optical signals travel, for connecting the star coupler to the plurality 
of transceiver stations; and an optical amplifying apparatus, for 
amplifying the optical signals, disposed in at least one location on a 
light transmitting path within the plurality of transceiver stations and 
along the transmission line. The optical amplifying apparatus is 
constructed as discussed above. 
In the loop-type optical communication system of this invention, to achieve 
the above object, there are provided a plurality of stations, each one of 
the stations including a light transmitter portion and a light receiver 
portion; a transmission line for connecting the stations; and an optical 
amplifying apparatus disposed in at least one of a light transmitting path 
within the plurality of stations and along the transmission line. The 
optical amplifying apparatus is constructed as discussed above. 
In the polarization insensitive optical amplifying apparatus of the present 
invention, both well and barrier layers are respectively given biaxial 
tensile stresses and are strained, so that the amount of shifted peak 
wavelength with respect to the amount of shift in strain can be set to 
values between those of the first and second prior art methods. Thus, 
advantages of the first and second prior art methods can be utilized while 
the disadvantages thereof can be compensated for. 
These advantages and others will be more readily understood in connection 
with the following detailed description of the preferred embodiments in 
conjunction with the drawings.

DESCRIPTION OF THE PREFERRED EMBODIMENT 
First Embodiment 
FIGS. 1 and 2 illustrate a first embodiment of an optical amplifying 
apparatus. FIG. 1 shows the entire structure of the first embodiment, and 
FIG. 2 is a cross-sectional view (a right-hand half of the amplifier is 
illustrated) showing its layer structure and the manner in which the 
lattice constant changes. 
In the first embodiment, on a (100) substrate 1 comprising an n-type GaAs, 
an n-type GaAs buffer layer 2 whose thickness is 1 .mu.m, an n-type 
Al.sub.0.5 Ga.sub.0.5 As cladding layer 3 whose thickness is 1.5 .mu.m, an 
undoped strained quantum well active layer 4, which is a graded 
index-separate confinement heterostructure (GRIN-SCH) layer, a p-type 
Al.sub.0.5 Ga.sub.0.5 As cladding layer 5 whose thickness is 1.5 .mu.m, 
and a p-type GaAs cap layer 6 whose thickness is 0.5 .mu.m, are 
consecutively layered in this order. The layering is performed by the 
metal organic chemical vapor deposition (MOCVD) method. 
Next, as shown in FIG. 2, the layers are etched to the p-Al.sub.0.5 
Ga.sub.0.5 As cladding layer 5 with a stripe-shaped region of 3 .mu.m 
width being untouched. Then, after an insulating layer 7 of a silicon 
nitride has been deposited on the entire surface, the portion of 
insulating layer that is deposited on the stripe region is removed. Then, 
an upper electrode 8 of Au-Cr is deposited thereon and a lower electrode 9 
of Au-Ge is deposited on the bottom surface of the substrate 1. Thus, a 
ridge type laser structure is fabricated. 
Next, the wafer is cleaved at a length of 500 .mu.m in a direction 
perpendicular to the direction of the stripe. Finally, antireflection 
coatings 10a and 10b of ZrO.sub.2 are provided on both end surfaces of the 
apparatus by using the electron beam method. Lensed fibers 11a and 11b, 
whose tips are formed into a spherical shape, are disposed near the end 
surfaces of the device, so that signal light can be input into or output 
from the device. 
When the arrangement is thus achieved, as shown in FIG. 1, a traveling 
wave-type semiconductor amplifying apparatus has been constructed and gain 
can be imparted to an external signal light beam between the optical 
fibers 11a and 11b. 
The structure of the strained quantum well active layer 4 and its effect 
will be described. The active layer 4 comprises, viewed from the side of 
the substrate 1, a GRIN-Al.sub.x Ga.sub.1-x As layer 12a (the value x is 
gradually changed from 0.5 to 0.25) whose thickness is 0.2 .mu.m, a 
GaAs.sub.0.75 P.sub.0.25 barrier layer 13a whose thickness is 7 nm, a 
GaAs.sub.0.9 P.sub.0.1 well layer 14 whose thickness is 6 nm, a 
GaAs.sub.0.75 P.sub.0.25 barrier layer 13b whose thickness is 7 nm, and a 
GRIN-Al.sub.x Ga.sub.1-x As layer 12b (the value x is gradually changed 
from 0.25 to 0.5) whose thickness is 0.2 .mu.m. 
In this embodiment, the barrier layers 13a and 13b and the well layer 14 
are respectively composed of GaAs.sub.1-y P.sub.y whose lattice constant 
is smaller than that of the GaAs of the substrate 1, so both layers 13a 
and 13b and 14 are respectively undergoing biaxial tensile stresses. In 
the well layer 14, the value of y is equal to 0.1 and its amount of strain 
is -0.3%, while in the barrier layers 13a and 13b, the value of y is equal 
to 0.25 and their amount of strain is -0.9%. 
The structure of the first embodiment will be compared to that of the prior 
art methods. 
In order to obtain the same effect as the first embodiment, the amount of 
strain that the well layer must be set to is -0.5% in the first prior art 
method mentioned, in which strain is imparted only to the well layer. The 
amount of strain that the barrier layer must be set to is -1.5% in the 
second prior art method mentioned, in which the strain is imparted only to 
the barrier layer. 
A peak wavelength of the gain will be compared between the first embodiment 
and the prior art. The peak wavelength of the first embodiment is shifted 
by 5 nm toward a longer wavelength, that is compared to a case where the 
layer thicknesses are the same as those of the first embodiment and no 
strain is imparted (i.e. the well layer and barrier layer respectively 
consist of GaAs and Al.sub.0.25 Ga.sub.0.75 As). When the same comparison 
is made, the peak wavelength of gain is shifted by 15 nm toward a longer 
wavelength in the first prior art method, and shifted by 3 nm toward a 
longer wavelength in the second prior art method. 
As discussed above, in the first embodiment, the amount of shifted peak 
wavelength and the amount of strain can be respectively set to values 
between those of the first and second prior art methods. Therefore, the 
advantages of the first and second prior art methods can be made use of, 
and at the same time their disadvantages can be reduced or avoided. 
In more detail, the first embodiment can attain the following technical 
advantages: 
1) The amount of shift in the peak wavelength is small. As a result, its 
matching with other optical devices having similar compositions, such as 
semiconductor lasers, is excellent and the first embodiment is suitable 
for integration with optical devices. 
2) The amount of strain can be set to a relatively small magnitude. As a 
result, the devices lifetime is long and the first embodiment is 
advantageous in the procurement of a long-term reliability. Further, its 
growth condition can be moderately set, so the first embodiment is 
productive. 
The structure of the first embodiment is the most preferable for attaining 
the effects of the present invention. However, other examples of the 
combination of well and barrier layers for effectuating strains therein 
are possible. The design may be determined from a viewpoint of which 
effect, of the two important effects of the present invention, should be 
stressed. Therefore, the structure of the first embodiment should not be 
considered as restrictive. 
Second Embodiment 
FIG. 3 illustrates a second embodiment of an optical amplifying apparatus. 
The layer structure of the second embodiment is different from that of the 
first embodiment. 
In the second embodiment, an n-type In.sub.x Ga.sub.1-x As.sub.1-y P.sub.y 
buffer layer 32, whose thickness is about 1 .mu.m, is initially layered on 
a substrate 31 comprising an n-type GaAs. In the buffer layer 32, the 
values of x and y are respectively changed from 0 to 0.2 and from 0 to 
0.1, and then the values of x and y are respectively maintained at 0.2 and 
0.1 up to a thickness of approximately 2 .mu.m. Thus, the lattice constant 
of the uppermost surface is about 1% larger than that of GaAs. Then, a 
superlattice layer 33, which is composed of ten alternately layered 
In.sub.0.5 Ga.sub.0.5 As.sub.0.28 P.sub.0.72 layers and ten In.sub.0.2 
Ga.sub.0.8 As.sub.0.9 P.sub.0.1 layers (each thickness is 30 .ANG.), is 
layered on the buffer layer 32. The lattice constant of the superlattice 
33 is matched with that of the nearest portion of the buffer layer 32, and 
the superlattice 33 consists of two kinds of layers having different band 
gaps. 
Then, an n-type In.sub.0.5 Ga.sub.0.5 As.sub.0.28 P.sub.0.72 cladding layer 
34 whose thickness is 1.5 .mu.m, an In.sub.0.2 Ga.sub.0.8 As.sub.0.9 
P.sub.0.1 SCH layer 35a whose thickness is 0.2 .mu.m, a 3-MQW 
(multi-quantum well) strained superlattice active layer 24, which consists 
of four alternately layered GaAs barrier layers 36a-36d (thickness: 7 nm) 
and three In.sub.0.07 Ga.sub.0.93 As well layers 37a-37c (thickness: 6 
nm), an In.sub.0.2 Ga.sub.0.8 As.sub.0.9 P.sub.0.1 SCH layer 35b whose 
thickness is 0.2 .mu.m, a p-type In.sub.0.5 Ga.sub.0.5 As.sub.0.28 
P.sub.0.72 cladding layer 38 whose thickness is 1.5 .mu.m, and a p-type 
In.sub.0.14 Ga.sub.0.86 As cap layer 39 whose thickness is 0.5 .mu.m, are 
consecutively layered in this order. 
Next, similar to the first embodiment, the layers are etched to form a 
ridge portion. Then, after an insulating layer 40 has been deposited on 
the entire surface, a portion of the insulating layer that is deposited 
along a stripe region is removed. Then, an upper electrode 41 is deposited 
thereon and a lower electrode 42 is deposited on the bottom surface of the 
substrate 31. Thus, a ridge type laser structure is fabricated. 
Next, the wafer is cleaved to a length of 500 .mu.m in a direction 
perpendicular to the direction of the stripe. Finally, antireflection 
coatings are provided on both end surfaces of the apparatus, and optical 
fibers are disposed near the end surfaces of the device. 
In the second embodiment, the non-strained reference layer is a layer 
formed on the substrate 31, but not the substrate 31 itself. As a result, 
the buffer layer 32 serves as a layer for adjusting or converting the 
lattice constant. If the buffer layer 32 is too thin, then the layer 32 
would contain strain therein. Therefore, the thickness of the buffer layer 
32 needs to be larger than 1 .mu.m. The superlattice (SL) layer 33 acts as 
a stopper layer so that the dislocation caused by the conversion of the 
lattice constant is not introduced into the upper layers. 
Although the composition of the active layer 24 in the second embodiment is 
different from that of the first embodiment, the amount of strain produced 
is approximately the same. Therefore, the same effects as those of the 
first embodiment can be obtained in the second embodiment. Furthermore, a 
multi-quantum well structure is adopted in the second embodiment, so a 
gain can be obtained that is than the first embodiment in which a single 
quantum well is used. 
As in the second embodiment, when a layer deposited on the substrate, but 
not the substrate itself (typically the cladding layer), is used as a 
reference layer, design freedom with regard to the strained quantum well, 
such as its material composition, can be increased and usefulness can be 
enhanced. In this case, however, the control of the oscillation wavelength 
can be readily performed, so the advantageousness over the first prior art 
method mentioned might be lessened in some cases. 
Yet, the second embodiment is still a useful example for constructing a 
polarization insensitive optical amplifier, for the freedom in designing 
the strained quantum well is enhanced in this embodiment. 
In the foregoing, a ridge type laser structure is exemplified, but any type 
of structure can be used in the present invention. In any case, gain may 
be controlled so that other polarization characteristics (polarization 
dependency on end-surface reflectivity and the like) caused by the laser 
structure can be compensated for, and the amount of strain, thicknesses of 
the well and barrier layers, and the like only need to be designed 
according to the adopted structure. 
Moreover, the material of the substrate is not limited to GaAs, and other 
III-V group compounds, which contain InP, and II-VI group compounds may be 
used as the substrate or other layers. 
Third Embodiment 
FIG. 4 shows an optical communication system in which the above discussed 
optical amplifying apparatus is used. In FIG. 4, reference numerals 101 
and 102 are transmitter stations, reference numerals 115 and 117 are 
branching-combining devices, reference numeral 106 is repeater equipment, 
reference numerals 103 and 104 are receiver stations, and reference 
numerals 118 and 119 are optical transmission lines. The transmitter 
stations 101 and 102, respectively, include light transmitters 111 and 
121, which are provided with a signal processing portion or processor and 
an electro-optical converting portion or transducer, and optical 
amplifying devices or amplifiers 112 and 122 for amplifying a light signal 
output from the light transmitters 111 and 121, respectively. The repeater 
equipment 106 comprises an amplifier 116. The receiver stations 103 and 
104, respectively, comprise optical amplifying devices or amplifiers 132 
and 142 for amplifying an input signal and their respective light 
receivers 131 and 141 which comprise an opto-electric transducer and a 
signal processing portion. 
In the optical communication system of FIG. 4, light signals that are 
output from the light transmitters 111 and 121 are amplified by the 
amplifying devices 112 and 121, respectively, and are output from the 
transmitter stations 101 and 102. The output signals do not collide with 
each other along the transmission line 118 because they are controlled by 
a prescribed multiplexing system, such as time division multiplexing, 
frequency division multiplexing, CSMA/CD (carrier sense multiple 
access/collision detection), etc. The output signals are sent to the 
transmission line 118 through the branching-combining device 115. When the 
light signal is transmitted through the transmission line 118, the light 
signal is attenuated. Therefore, the light signal is amplified by the 
repeater equipment 106. In FIG. 4, only one of the repeater equipments 106 
is depicted, but if necessary, the repeater equipment 106 may be 
positioned at a plurality of locations. On the other hand, no repeater 
equipment need be used, if it is unnecessary. 
The light signal amplified by the repeater equipment 106 is input into the 
branching-combining device 117 through the light transmission line 119 and 
is separated by a separation method that corresponds to the prescribed 
multiplexing system and is input into the receiving stations 103 and 104. 
The light signal input to each receiver station 103 and 104 is amplified 
by the optical amplifiers 132 and 142, respectively, to compensate for 
losses generated in both the light transmission line 119 and the 
branching-combining device 117, and is input into the light receivers 131 
and 141, respectively. Thus, communications from the transmitter station 
101 to the receiver station 103 and from the transmitter station 102 to 
the receiver station 104 are conducted through the single light 
transmission line 118 and 119. 
In FIG. 4, there are two transmitter stations and two receiver stations, 
but the number of branches of the branching-combining devices 115 and 117 
may be increased to attain an N to N communication by using N number of 
transmitter stations and N number of receiver stations. Further, one to 
one communication is also possible without using the branching-combining 
devices 115 and 117. In FIG. 4, there is no need to position the optical 
amplifying apparatus in all the illustrated locations. This apparatus has 
only to be positioned in a location where signal attenuation at each part 
should be compensated for. 
When the polarization insensitive optical amplifying apparatus is used in 
the optical communication system, as shown in FIG. 4, the light receiver 
in the system will not substantially effect the dynamic range and the like 
because, even if the amplifying apparatus receives an unstable light 
signal in its state of polarization, the output therefrom is always 
supplied being amplified to a constant level. 
Further, a preferable optical communication system is attained, and there 
is no limitation as to the scale of the system since there is no power 
fluctuation in the light signal. Since the polarization dependency is 
solved without any degrading characteristics other than the gain 
characteristic, such as noise characteristic, the system is still 
preferable in this point. Moreover, there is no need to use means or 
apparatuses specially devised in coping with the fluctuation in the state 
of polarization, as signal processing means, E/O and O/E converting means, 
optical transmission line, etc., because a polarization insensitive 
amplifier is used in the system. As for those means for coping with 
fluctuation, conventional ones can be used. 
Fourth Embodiment 
FIG. 5 shows an example of a bidirectional optical communication system in 
which the polarization insensitive amplifying apparatus of the present 
invention is employed. In the optical communication system shown in FIG. 
5, reference numerals 201 and 202 are transceiving stations, reference 
numeral 203 is repeater equipment, and reference numerals 218 and 219 are 
optical transmission lines. The transceiving stations 201 and 202, 
respectively, include transmitters and receivers, and the transmitters are 
light transmitters 211 and 241, respectively, which comprise a signal 
processor and an E/O converting portion. The transceiving stations 201 and 
202 also comprise optical amplifiers 212 and 242, respectively, for 
amplifying the signal output from the light transmitters 211 and 241. The 
transceiver stations 201 and 202 have optical amplifiers 222 and 232, 
respectively, for amplifying the input light signal, and light receivers 
221 and 231, respectively, which include an O/E converting portion and a 
signal processor. In the transceiver stations 201 and 202, the transmitter 
and receiver are connected by branching-combining devices 215 and 217. The 
repeater equipment 203 includes an optical amplifier 213 and is connected 
to each transceiver stations 201 and 202 through the optical transmission 
lines 218 and 219. 
In the structure of FIG. 5, light signals output from the light transmitter 
211 in the transceiver station 201 and the light transmitter 241 in the 
transceiver station 202 are respectively amplified by the optical 
amplifiers 212 and 242 and are sent out from each transceiver station 201 
and 202 through the branching-combining devices 215 and 217, respectively. 
These output light signals are respectively transmitted in opposite 
directions through the optical transmission lines 218 and 219. The light 
signals are amplified by the repeater equipment 203 since the amount of 
light is attenuated when the light signals are transmitted through the 
transmission lines 218 and 219. 
In FIG. 5, the repeater equipment 203 is depicted as being in one location, 
but if necessary, it can be placed in a plurality of locations. If the 
repeater equipment 203 is not needed, it may be omitted. The light signals 
amplified by the repeater 203 are further transmitted through the 
transmission lines 219 and 218 and then input to the transceiver stations 
202 and 201 at the opposite side of the light signals origin. The input 
signals are branched off by the branching-combining devices 217 and 215 in 
the directions to the light receivers 231 and 221, respectively, and are 
amplified by the optical amplifiers 232 and 222, respectively, in order to 
compensate for losses caused in both the transmission lines 218 and 219 
and the branching-combining devices 215 and 217, and are input into the 
light receivers 231 and 221. Thus, bidirectional communication is 
performed between the transceiver stations 201 and 202 through single 
transmission lines 218 and 219. 
In FIG. 5, there is illustrated the example of a bidirectional 
communication in which two transceiver stations are provided, each having 
one transmitter and one receiver. However, such structures are possible 
wherein each transceiver station comprises a plurality of transmitters and 
receivers or wherein a plurality of transceiver stations are connected by 
the branching-combining device. There is no need to position the optical 
amplifiers in all the locations illustrated in FIG. 5, and the amplifier 
has only to be positioned where the attenuation of the light signal need 
be compensated for. For the rest, the system of FIG. 5 is the same as that 
of FIG. 4. 
Fifth Embodiment 
FIGS. 6 and 7 show a bus-type optical communication network in which a 
polarization insensitive type optical amplifying apparatus of the present 
invention is used. 
In FIG. 6, showing the overall system, reference numeral 300 is an optical 
transmission line comprising optical fibers, reference numerals 311-319 
are respectively transceiver stations or units, which convert electric 
signals from terminals 321-329 to light signals to send them out to the 
transmission line 300, or convert the light signal on the transmission 
line to an electric signal to transfer it to the terminal. The transceiver 
stations or units 311-319 detect the condition of communication on the 
optical transmission line 300 and control the communication in such a 
manner that signals from other terminals will not collide with the signal 
from its own terminal. Further, reference numerals 331-339 are, 
respectively, optical couplers which are connected to the transmission 
line 300, and take out part of the signal on the optical transmission line 
300 to transmit it to the transceiver stations 311-319 and to send out the 
light signals from the transceiver stations 311-319 to the transmission 
line 300. Reference numerals 341 and 342 are, respectively, repeater 
optical amplifiers for amplifying the light signal on the transmission 
line 300. The polarization insensitive optical amplifying apparatus is 
used as those repeater optical amplifiers 341 and 342. 
FIG. 7 illustrates one example of the structure of the transceiver station 
312 in FIG. 6. In FIG. 7, reference numeral 350 is a light transmitter, 
which converts the electrical signal from the terminal 322 to an optical 
signal and transmits this light signal to the transmission line by 
controlling it in such a manner that the signals from the other terminals 
will not collide with that light signal when on the optical transmission 
line 300. Reference numeral 360 is an optical amplifier for amplifying the 
light signal from the light transmitter 350, reference numeral 370 is a 
light receiver which converts the light signal transmitted through the 
transmission line 300 to an electric signal and transmits this electric 
signal to its own terminal if the signal is addressed to that terminal (in 
this case, terminal 322) which is connected to its own transceiver station 
312, reference numeral 380 is an optical amplifier for amplifying the 
signal transmitted through the transmission line 300 to the light receiver 
370, and reference numeral 390 is a branching-combining device for sending 
out the optical signal from the amplifier 360 to the coupler (in this 
case, coupler 332) and transmitting the optical signal from the optical 
coupler 332 to the amplifier 380. The polarization insensitive type 
optical amplifying apparatus of the present invention is utilized as 
optical amplifiers 360 and 380. Here, only the structure of the 
transceiver station 312 is explained, but the transceiver stations 311-319 
also have similar structures. 
The operation of this embodiment will be explained, assuming that the 
communication is performed between the terminals 322 and 329. When the 
signal is to be transmitted from the terminal 322, first the light 
transmitter 350 controls the light signal from the terminal 322 such that 
it will not collide with the light signals from the other terminals on the 
optical transmission line 300. Such control is provided by using a 
prescribed multiplexing system such as time division multiplexing, 
frequency division multiplexing and CSMA/CD. The light transmitter 350 
converts the electrical signal from the terminal 322 to an optical signal 
to transmit it to the optical amplifier 360. This signal is amplified by 
the optical amplifier 360 to be sent out on the optical transmission line 
300 in opposite directions by the optical coupler 332 through the 
branching-combining device 390. This optical signal reaches the repeater 
optical amplifier 342 through the couplers 333, . . . , 338. At this time, 
part of this optical signal's power has been branched by each optical 
coupler and has been transmitted to the transceiver stations 313, . . . , 
318, and these transceiver stations recognize that this signal is not 
addressed to their own terminals 323, . . . , 328, respectively, and 
abandon this optical signal. The optical signal that arrives at the 
repeater optical amplifier 342 has been lowered in its signal intensity 
since part thereof has been branched at each optical coupler, but its 
intensity is regained by the amplification at the repeater optical 
amplifier 342 and thus the regained signal is transmitted to the optical 
coupler 339 through the transmission line 300. 
At the optical coupler 339, part of the optical signal is branched so as to 
be transmitted to the transceiver station 319, and the signal is sent to 
the light receiver through devices similar to the branching-combining 
device 390 shown in FIG. 7. In this light receiver, the transmitted 
optical signal is converted to an electric signal, and the light receiver 
recognizes that this signal is addressed to the terminal 329 and transmits 
it to the terminal 329. 
When the signal is transmitted from the terminal 329 to the terminal 322, 
the signal is transmitted on the transmission line 300 in opposite 
directions based on a process similar to that mentioned above. Here, the 
optical signal that reaches the transceiver station 312 passes through the 
optical couplers 338, . . . , 333, 332 and thereafter through the optical 
branching-combining device 390, so that the signal is attenuated at each 
part and its intensity has been weakened. However, the signal is amplified 
by the optical amplifier 380 before reaching the light receiver 370, and 
is transmitted to the light receiver 370 after its intensity has been 
regained. 
Thus, the amplifier 360 amplifies the light signal from the light 
transmitter 350 and transmits it to the transmission line 300, and the 
optical amplifiers 341, 342 and 380 compensate for the attenuation of 
light power that is caused along the path of light signal, including the 
optical node to amplify the optical signal, in such a manner that the 
optical signal has enough power to be received. Several advantages are 
achieved, which are similar to those found in the systems shown in FIGS. 4 
and 5. 
In this embodiment, the optical amplifiers are positioned right after the 
light transmitter 350, just before the light receiver 370, and on the 
optical transmission line 300. However, if the light transmitter 350 can 
transmit an optical signal having sufficient power, the optical amplifier 
360 is unnecessary. Further, if the output from the branching-combining 
device 390 has enough power to be received by the light receiver 370, the 
amplifier 380 is also dispensable. Further, if the number of optical 
couplers on the transmission line 300 is small, and the attenuation at the 
optical couplers is not critical, the optical amplifiers 341 and 342, on 
the transmission line 300, can also be omitted. Thus, all the amplifiers 
shown in FIGS. 6 and 7 are not necessary. When at least one of them is 
used, the bus-type optical communication network can achieve the 
above-mentioned advantages. 
In the system of FIG. 6, the repeater optical amplifiers 341 and 342 are 
positioned on the optical transmission line 300 separately from the 
optical couplers 331, . . . , 339. But also, when a repeater optical 
amplifier is contained in each optical coupler, the above-mentioned 
advantages can be attained only if the optical amplifying apparatus of the 
present invention is used in the system. 
In this embodiment, only a single transmission line 300 is used, but the 
above advantages can also be attained when a bidirectional communication 
or a multiplexing communication is performed using, for example, a 
plurality of optical fibers as optical transmission lines. 
Sixth Embodiment 
FIGS. 8 and 9 show an example of an active bus-type optical communication 
network in which the polarization insensitive optical amplifying apparatus 
is used. In FIG. 8, illustrating the overall structure of the system, 
reference numerals 400 and 401 are optical transmission lines such as 
optical fibers, reference numerals 411, . . . , 419 are terminals for 
performing communication, reference numerals 421, . . . , 429 are active 
optical nodes for conducting light transmission, light receiving and 
communication control, and reference numeral 480 is a repeater optical 
amplifier for amplifying the optical signal. In FIG. 9, which shows, as an 
example, the structure of one active optical node 422, and reference 
numerals 450 and 451 are opto-electric converter (O/E) for converting an 
optical signal to an electric signal. Reference numerals 440 and 441 are 
electro-optical converters (E/O) for converting an electric signal to an 
optical signal, and reference numeral 430 is a communication controller. 
The controller 430 determines if the signal transmitted through the 
transmission lines 400 and 401, and converted to an electric signal, is 
addressed to the terminal 412, and if so, the controller 430 transmits the 
signal to the terminal 412 and if not so, the controller 430 again 
converts the signal to an optical signal using the E/O devices 440 and 441 
to transmit this signal to the optical transmission lines 400 and 401. 
Further, when the signal is transmitted to the controller 430 from the 
terminal 412, the controller 430 converts the electrical signal to an 
optical signal using the E/O devices 440 and 441 and transmits it to the 
transmission lines 400 and 401, respectively, under such control that the 
signal will not collide with the optical signals from the other terminals. 
The reference numerals 491-494 are optical amplifiers of the polarization 
insensitive type. 
The operation of this embodiment will be explained, taking a case in which 
the signal is transmitted from the terminal 412 to the terminal 419, as an 
example. When the signal is output from the terminal 412, the 
communication controller 430, in the active optical node, converts the 
electrical signal from the terminal 412 to an optical signal with the E/O 
devices 440 and 441. Then, the optical amplifiers 492 and 494 amplify the 
signal and it is transmitted on the optical transmission lines 400 and 401 
in opposite directions along the lines. The signal from the terminal 412 
will not collide with the signals from the other terminals on the 
transmission lines 400 and 401 because they are controlled using a 
prescribed multiplexing system such as time division multiplexing, 
frequency division multiplexing and CSMA/CD. This signal enters the active 
optical nodes 421 and 423, and is converted to an electric signal to be 
input into the communication controller in the active optical nodes 421 
and 423. However, this signal is not addressed to the terminal 411 and 
413, therefore, the signal is once again converted to an optical signal to 
be sent out to the optical transmission line. 
The distance between the terminals 423 and 429 is long. Therefore, the 
optical signal loses its intensity while traveling along the optical 
fiber. To amplify this signal and compensate for the loss, a repeater 
optical amplifier 480 is inserted in the transmission lines 400 and 401. 
The optical signal, amplified by the repeater optical amplifier 480, is 
further amplified by the optical amplifier in the active optical node 429 
and is then converted to an electric signal to reach the communication 
controller. The communication controller in the active optical node 429 
recognizes that this signal is addressed to the terminal 419, and 
transmits it to the terminal 419. On the other hand, the signal sent out 
to the active optical node 421 from the node 422 through the transmission 
line 401 consecutively passes the active optical nodes and reaches the 
left end of the communication system. There, the signal is abandoned. 
Thus, the optical transmission line 400 shares the signal transmission in 
the right direction in FIG. 8, and the line 401 shares that in the left 
direction. Therefore, signals output from any terminal are simultaneously 
transmitted in opposite directions, so they reach the addressed terminals 
without failure. 
In the above manner, the optical amplifiers 492 and 494 amplify the signals 
from the E/O devices 440 and 441, respectively, so as to transmit them on 
the transmission lines 400 and 401 respectively. The amplifiers 491 and 
493 amplify the optical signals so that the attenuation of light power in 
the transmission line is compensated for and the optical signals have 
enough power to be received. Further, the repeater amplifier 480 
compensates for light losses where the distance between the active optical 
nodes is long. The polarization insensitive amplifying apparatus of the 
present invention is used as the above optical amplifiers. 
In the system of this embodiment, several advantages can be attained, which 
are similar to those of the systems shown in FIGS. 6 and 7. 
In this embodiment, the optical amplifiers are disposed in several 
locations, as shown in FIGS. 8 and 9, but, for example, if the E/O devices 
440 and 441 can output an optical signal having adequate power, there is 
no need to use the amplifiers 492 and 494. If the active node receives 
enough power so that the O/E devices 450 and 451 can receive it, the 
optical amplifiers 491 and 493 can be omitted. Further, if the distance 
between the terminals is not so long as to make the losses in optical 
fibers considerable, the repeater optical amplifier 480 is dispensable. 
However, only if at least one amplifier is used, can the active bus-type 
optical communication network obtain the above-mentioned advantages. 
In the system of FIG. 8, there are two transmission lines between the 
active optical nodes to perform bidirectional communication. But also, in 
cases where bidirectional signal communication is performed with a single 
optical transmission line using the optical branching-combining device, as 
shown in FIG. 5, and where multiplexing signal communication is conducted 
using at least three transmission lines, the above mentioned advantages 
can be obtained if the polarization insensitive optical amplifying 
apparatus of the present invention, is used in each optical transmission 
line. 
Seventh Embodiment 
FIG. 10 shows the structure of a star-type optical communication network in 
which a polarization insensitive amplifying apparatus is used. In this 
embodiment, there are four transceiver stations, and the optical signals 
are transmitted in each optical fiber in opposite directions. 
In FIG. 10, reference numerals 601-604 are transceiver stations which 
connect terminals to the network, and reference numeral 605 is a star 
coupler, which connects inputs and outputs of the transceiver stations 
601-604 in the network in a matrix form. Reference numerals 606-613 are 
transmission lines which are optical fibers, reference numerals 614-617 
are light transmitters which convert electric signals to optical signals 
to transmit them to the network, and reference numerals 618-621 are light 
receivers which convert optical signals incident from the network to 
electric signals. Reference numerals 622-625 are optical 
branching-combining devices which connect the transmitters 614-617 and 
receivers 618-621 in the transceiver stations to the optical fibers 
610-613, respectively, and reference numerals 626-638 are the above 
optical amplifying apparatuses or amplifiers of the present invention 
which directly amplify the optical signals. These amplifying apparatuses 
626-638 are classified into booster amplifiers 626-629 for the light 
transmitters 614-617, respectively, pre-amplifiers 630-633 for the light 
receivers 618-621, respectively, a booster amplifier 634 of the star 
coupler 605, and repeater amplifiers 635-638 of the transmission line. 
Next, the operation of this embodiment will be explained, assuming that 
communication is performed from the transceiver station 601 to the 
transceiver station 603. An electric signal is converted into an optical 
signal in the transmitter 614 of the transceiver station 601, and this 
light signal is amplified by the optical amplifier 626 and transmitted to 
the optical fiber 610 of the network through the branching-combining 
device 622. The optical signal incident on the optical fiber 610 is 
amplified by the optical amplifier 635 and is transmitted to the star 
coupler 605 through the optical fiber 606. The optical signal is amplified 
by the optical amplifier 634 in the star coupler 605, and is sent out to 
the optical fibers 606-609, which are connected to the star coupler 605. 
The optical signals incident on the optical fibers 606-609 are amplified 
by the optical amplifiers 635-638, are branched by the branching-combining 
devices 622-625, and parts thereof are amplified by the optical amplifiers 
630-633 to be transmitted to the receivers 618-621, respectively. 
The receivers 618-621 convert the optical signals to electric signals. The 
transceiver stations 601-604 then respectively discriminate whether the 
signal is addressed to itself from those converted electric signals. This 
signal is addressed to the transceiver station 603, so that the 
transceiver station 603 identifies this signal and receives it. Thus, the 
communication is completed. Also in the star-type system, in order to 
transmit optical signals from any transceiver station to all the 
transmission lines, the communication is conducted in such a manner that 
the optical signals will not collide with one another on the transmission 
line by using time division multiplexing, frequency division multiplexing, 
etc. 
In this embodiment, the optical amplifying apparatuses of the present 
invention are positioned in all paths along which the optical signals are 
transmitted in the network, but it is possible to position the optical 
amplifying apparatus in only part of those paths. Further, in this 
embodiment, the transmitter and receiver are connected by the 
branching-combining device and bidirectional communication is performed 
using one optical fiber for one transceiver station. But, such a system is 
possible when two optical fibers, one for transmitting and one for 
receiving, are used for one transceiver station. 
Also in this embodiment, there are the above-mentioned technical advantages 
that are similar to those of the networks shown in FIGS. 6 and 8, since 
the optical amplifying apparatus of the present invention is used. 
Eighth Embodiment 
FIG. 11 shows the structure of a loop-type optical communication network in 
which a polarization insensitive type optical amplifying apparatus of the 
present invention is used. In this embodiment, there are four transceiver 
stations and an optical signal is transmitted in a clockwise direction in 
the loop network. In FIG. 11, reference numerals 701-704 are transceiver 
stations for connecting terminals to the network, reference numerals 
705-712 are optical fibers, reference numerals 713-716 are transmitters 
for converting an electric signal to an optical signal so as to transmit 
it to the network, reference numerals 717-720 are receivers for converting 
the optical signal input from the network to the electric signal, and 
reference numerals 721-732 are optical amplifiers of the present invention 
for directly amplifying the optical signal. The optical amplifiers 721-732 
are classified as booster amplifiers 721-724 for the transmitters 713-716, 
respectively, pre-amplifiers 725-728 for the receivers 717-720, 
respectively, and repeater amplifiers 729-732 located along the optical 
transmission line. 
Next, the operation of this embodiment will be explained, assuming that the 
communication is conducted from the transceiver station 701 to the 
transceiver station 703. An electric signal is converted to an optical 
signal in the transmitter 713 of the transceiver station 701, and is 
amplified by the optical amplifier 721 to be transmitted to the optical 
fiber 705 in the network. This optical signal is amplified by the optical 
amplifier 729, transmitted through the optical fiber 706, amplified by the 
optical amplifier 726 in the transceiver station 702 and converted to an 
electric signal in the receiver 718. Since this signal is addressed to the 
transceiver station 703, the signal is converted to an optical signal in 
the transmitter 714 of the transceiver station 702 and this light signal 
is amplified by the optical amplifier 722 to be input into the optical 
fiber 707 in the network. This optical signal is amplified by the optical 
amplifier 730, transmitted through the optical fiber 708, amplified by the 
optical amplifier 727 of the transceiver station 703, and converted to an 
electric signal in the receiver 719. Since this signal is addressed to the 
transceiver station 703, the transceiver station 703 identifies this 
signal and receives it. Thus, communication is completed. 
In this embodiment, there are optical amplifiers positioned in all the 
paths in the network along which light signals are transmitted, but it is 
possible to position the optical amplifier in only part of the paths in 
the network. Further, this embodiment is an active type in which the 
signal in the transceiver station is re-generated and repeated. But, it is 
possible to construct a passive-type system in which the optical 
branching-combining device is used to connect the transceiver station to 
the optical fiber which is the transmission line. 
Also in this embodiment, since the optical amplifying apparatus of the 
present invention is used, the above discussed advantages of the networks 
shown in FIGS. 6 and 8 can be similarly obtained. 
As described in the foregoing, according to the present invention, a 
so-called polarization insensitive optical amplifying apparatus, in which 
its amplification gain would not vary even if the polarization state of an 
input light changes, can be attained. By using such a polarization 
insensitive optical amplifying apparatus, an optical communication network 
or system, in which communication quality is excellent, and in which there 
is no limit to its size, and in which its system structure is relatively 
simple, can be realized. 
Except as otherwise disclosed herein, the various components shown in 
outline or in block form in the Figures are individually well known in the 
field of optical amplifying apparatuses or amplifiers and the optical 
communication systems arts, and their internal construction and operation 
are not critical either to the making or using of this invention or to a 
description of the best mode of the invention. 
While the present invention has been described with respect to what is 
presently considered to be the preferred embodiments, it is to be 
understood that the invention is not limited to the disclosed embodiments. 
The present invention is intended to cover various modifications and 
equivalent arrangements included within the spirit and scope of the 
appended claims.