Optical amplifying glass fiber

Details Optical amplifying glass fiber Optical amplifying glass fiber

2001-04-24

2003-05-06

Ngo, Hung N. (Department: 2874)

Optical waveguides

Optical fiber waveguide with cladding

C372S006000, C385S142000

Reexamination Certificate

active

06560392

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to an optical amplifying glass fiber which is operable within a wavelength range of from 1.5 to 1.6 &mgr;m.
2. Discussion of Background
For the purpose of application to an optical communication field, an optical amplifier using as an optical amplifying medium a glass fiber having a rare earth element added to the core, particularly an Er (erbium)-doped optical fiber amplifier, is being studied and developed, and its application to an optical communication system is actively being developed.
On the other hand, in order to cope with diversification of communication services expected in future, a wavelength division multiplexing optical communication system (WDM) has been proposed to increase the transmission capacity. In WDM, the transmission capacity increases as the number of wavelength division multiplexing channels increases. Application of “an optical amplifying glass fiber using an Er-doped fiber as a core” (EDF) to WDM has been studied. For example, EDF wherein the core is an Er-doped quartz type glass fiber (quartz type EDF) or EDF wherein the core is an Er-doped fluoride glass fiber (fluoride type EDF), has heretofore been proposed.
With the conventional quartz type EDF, it is known that the maximum gain with light within a wavelength range of from 1.5 to 1.6 &mgr;m, is obtainable when its length is from 10 to 30 m (the length at which the maximum gain is obtainable, varies depending upon the wavelength, the Er concentration, etc.). Accordingly, in a conventional optical amplifier employing the quartz type EDF, it is common to use e.g. a quartz type EDF of from 10 to 30 m wound into a bobbin having a diameter of about 5 cm in order to carry out the desired optical amplification and to accommodate the quartz type EDF in a container having a size of about 30 cm. However, if the quartz type EDF is wound into a bobbin as mentioned above, a bending stress is exerted to the quartz type EDF, and there has been a problem that the quartz type EDF is likely to be broken due to static fatigue during the use for a long period of time.
Further, with the conventional fluoride type EDF, it is known that the maximum gain with light within a wavelength range of from 1.5 to 1.6 &mgr;m can be obtained when its length is from 10 to 40 m, and also the optical amplifier employing such a fluoride type EDF has had the same problem as the optical amplifier employing a quartz type EDF.
Further, the quartz type EDF and the fluoride type EDF had a problem that the wavelength width within which a gain with light within a wavelength range of from 1.5 to 1.6 &mgr;m, is obtainable, is small.
In order to solve such problems, it is desired to develop EDF which can be accommodated in a container having a size of about 30 cm without being wound into a bobbin, and whereby the desired optical amplification can be obtained in a wide range.
SUMMARY OF THE INVENTION
It is an object of the present invention to provide EDF whereby the foregoing problems can be solved.
The present invention provides an optical amplifying glass fiber comprising a core glass and a clad glass, wherein a relation of:
0.0005≦(
n
1
−n
2
)/
n
1
≦0.1
where n
1
and n
2
are refractive indices of the core glass and the clad glass, respectively, is satisfied, the fiber has a length of at most 25 cm, the core glass contains Er, and the wavelength width wherein a gain is obtainable with light having a wavelength of from 1.50 to 1.59 &mgr;m, is at least 30 nm.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
The optical amplifying glass fiber of the present invention comprises a core glass and a clad glass. Usually, a protective resin is coated on the outer side of the clad glass. As such a resin, a silicone resin, an acrylic resin, an epoxy resin or a polyimide resin, may, for example, be mentioned.
Between the refractive index n
1
of the core glass and the refractive index n
2
of the clad glass, a relation represented by the following formula, is satisfied.
0.0005≦(
n
1
−n
2
)/
n
1
≦0.1
If (n
1
−n
2
)

1
is less than 0.0005, it tends to be difficult to confine light within the core glass. Preferably, it is at least 0.001, more preferably at least 0.003. If it exceeds 0.1, it tends to be difficult to transmit light in a single mode within the optical amplifying glass fiber. It is preferably at most 0.08, more preferably at most 0.05.
The core glass is one having Er added to a matrix glass. The amount of Er added to the matrix glass is preferably from 0.05 to 10 wt % (based on the matrix glass). If it is less than 0.05 wt %, it is likely that the desired optical amplification (the gain, and the wavelength width within which the gain can be obtained) may not be obtained. It is preferably at least 0.1 wt %, more preferably at least 0.2 wt %. If it exceeds 10 wt %, vitrification tends to be difficult. It is preferably at most 5 wt %, more preferably at most 3 wt %.
The above matrix glass preferably contains Bi
2
O
3
within a range of from 25 to 70 mol %. If it is less than 25 mol %, the desired optical amplification may not be obtained. If it exceeds 70 mol %, vitrification tends to be difficult. A preferred composition of the matrix glass is from 25 to 70 mol % of Bi
2
O
3
, from 5 to 74.79 mol % of B
2
O
3
+SiO
2
, from 0.1 to 30 mol % of WO
3
+TeO
2
+Ga
2
O
3
, from 0.01 to 10 mol % of CeO
2
, and from 0.1 to 30 mol % of Al
2
O
3
+Ga
2
O
3
.
The composition of the above clad glass is usually determined based on the composition of the above matrix glass, so that its refractive index n
2
satisfies the above-mentioned relation with the refractive index n
1
of the core glass.
The length of the optical amplifying glass fiber of the present invention is at most 25 cm. If it exceeds 25 cm, it tends to be difficult to accommodate it in a container having a size of about 30 cm without winding it into a bobbin shape. It is preferably at most 20 cm, more preferably at most 15 cm. Further, its length is preferably at least 0.5 cm. If it is less than 0.5 cm, handling or connection to another glass fiber tends to be difficult. More preferably, it is at least 1 cm.
Into the optical amplifying glass fiber, excitation light is introduced together with signal light. G calculated by the formula:
G=
10×log
10
(
I
out
/I
in
)
wherein I
in
is the intensity of the incident signal light, and I
out
is the intensity of the signal light coming out of the optical amplifying glass fiber, is referred to as the gain (unit: dB) in the present invention.
With the optical amplifying glass fiber of the present invention, the wavelength width wherein a gain is obtainable with light having a wavelength of from 1.50 to 1.59 &mgr;m (i.e. G>0) is at least 30 nm. If it is less than 30 nm, the number of channels in WDM tends to be too small. It is preferably at least 50 nm, more preferably at least 60 nm, particularly preferably at least 70 nm, most preferably at least 80 nm.
The minimum value of the gain with light having a wavelength of from 1.50 to 1.59 &mgr;m with the optical amplifying glass fiber of the present invention, is preferably at least 8 dB. If it is less than 8 dB, the desired optical amplification may not be obtained. It is more preferably at least 9 dB, particularly preferably at least 10 dB, most preferably at least 15 dB.
The gain with light having a wavelength of 1.53, of the optical amplifying glass fiber of the present invention, is preferably at least 8 dB. It is more preferably at least 9 dB, particularly preferably at least 10 dB, most preferably at least 15 dB.
The optical amplifying glass fiber of the present invention can be prepared, for example, as follows. The starting materials are mixed and put into a platinum crucible, an aluminum crucible, a quartz crucible or an iridium crucible and melted at a temperature of from 800 to 1,300° C. in air, and the obtained melt is cast in a mold to prepare a core glass and a clad glass. Then, the core glass and the clad glass are put together and subjected

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