Fusion splicing of highly rare-earth-doped optical fibers
A method and arrangement for achieving low splice-losses when connecting Highly Rare-Earth-Doped (HRED) optical fibers and dissimilar optical fibers having a large Mode Field Diameter (MFD) mismatch. Warm images are taken during a pre-fusion process to capture thermal light emissions and determine an arc-center position. The end-surfaces of the fibers are abutted and longitudinally offset from the arc-center, based on the light propagation direction and the MFD-mismatch. The fibers are then asymmetrically heated with different fusion temperatures during the main fusion processes. An MFD-match is achieved with well-defined fusion currents and fusion time. To maintain the same offset distance in a sequence of splices, the main-fusion arc-center position is determined by a process of direct arc-recentering. Variations of fusion temperature caused by changes of electrode conditions and the operating environment are monitored in real-time, and an arc-check process is invoked to compensate for the large variations of fusion temperature.
1. A method of splicing dissimilar optical fibers, comprising:
longitudinally positioning an end-surface of a first optical fiber adjacent to an end-surface of a second, dissimilar optical fiber so that a gap is formed between the two end-surfaces, wherein the end-surfaces are positioned in a splicer so that a center of the gap is aligned with the splicer electrodes;
cleansing micro-dust particles from the two end-surfaces with a low-power electric arc generated by the splicer electrodes;
capturing a warm image of the two end-surfaces and the gap during the cleansing step;
determining a pre-fusion arc-center position by analyzing thermal light emissions captured in the warm image;
determining an offset distance from the pre-fusion arc-center position based on a direction of light propagation and a degree of Mode Field Diameter (MFD) mismatch between the dissimilar optical fibers;
abutting the two end-surfaces;
longitudinally repositioning the two abutted end-surfaces by the offset distance with respect to the pre-fusion arc-center position; and
asymmetrically heating the repositioned abutted end-surfaces with a high-power electric arc generated by the splicer electrodes, thereby fusing the two dissimilar optical fibers.
2. The method of claim 1 , wherein the first optical fiber is a Highly Rare-Earth-Doped (HRED) optical fiber, and the second optical fiber is a None-Rare-Earth-Doped (NRED) fiber having a large Mode Field Diameter (MFD) mismatch with the HRED optical fiber.
3. The method of claim 2 , wherein the direction of light propagation is from the HRED fiber to the NRED fiber, and the step of longitudinally repositioning the two abutted end-surfaces by the offset distance includes longitudinally repositioning the two abutted end-surfaces in the direction of the HRED fiber so that a lower fusion temperature is generated in the HRED fiber when the asymmetrical heating step is performed.
4. The method of claim 2 , wherein the direction of light propagation is from the NRED fiber to the HRED fiber, and the step of longitudinally repositioning the two abutted end-surfaces by the offset distance includes longitudinally repositioning the two abutted end-surfaces in the direction of the NRED fiber so that a lower fusion temperature is generated in the NRED fiber when the asymmetrical heating step is performed.
5. The method of claim 1 , wherein a plurality of splices are performed, and the method is repeated for each splice in the plurality of splices so that a new offset distance is calculated for each splice.
6. The method of claim 5 , further comprising:
capturing a warm image of the two abutted end-surfaces during the asymmetrical heating step; and
determining a main-fusion arc-center position by analyzing thermal light emissions captured in the warm image.
7. The method of claim 6 , wherein the step of capturing a warm image of the two abutted end-surfaces during the asymmetrical heating step includes capturing a plurality of warm images by periodically capturing a warm image during the asymmetrical heating step.
8. The method of claim 7 , wherein the step of periodically capturing a warm image includes capturing a warm image approximately every 100 ms during the asymmetrical heating step.
9. The method of claim 8 , further comprising:
determining a main-fusion arc-center position for each of the plurality of warm images captured during the asymmetrical heating step;
for each of the determined main-fusion arc-center positions, determining a difference between the main-fusion arc-center position and the pre-fusion arc-center position;
comparing each of the determined arc-center differences with a difference threshold; and
if a determined arc-center difference exceeds the difference threshold, stopping the asymmetrical heating step.
10. The method of claim 9 , further comprising invoking an arc-check process to compensate for large variations of fusion temperature.
11. The method of claim 6 , wherein the step of determining a main-fusion arc-center position by analyzing thermal light emissions captured in the warm image includes:
defining an upper rectangular area within an upper portion of the fibers, said upper rectangular area extending longitudinally across the splice and over a portion of each of the fibers, said upper rectangular area being defined by coordinates {(x 1 , y 1 ), (x 2 , y 1 ), (x 2 , y 2 ), (x 1 , y 2 )};
analyzing light intensity-distributions in the upper rectangular area utilizing the warm image, said analyzing step including:
calculating an upper arc center position, X arc,up , utilizing the equations:
X
a
rc
,
up
=
∫
y1
y2
∫
x1
x2
xL
up
(
x
,
y
)
ⅆ
x
ⅆ
y
∫
y1
y2
∫
x1
x2
L
up
(
x
,
y
)
ⅆ
x
ⅆ
y
(
1
)
and
L up ( x,y )=max[ L min , L ( x,y )− L BG ] (2)
where, L(x,y) is the light intensity at coordinates (x, y); L BG is the average intensity of background light, which depends on settings of the imaging system; and L min is a pre-defined minimum value of light intensity to avoid divergence of the integrations defined in equation (1); and
repeating the defining and analyzing steps for a lower rectangular area within a lower portion of the fibers, said lower rectangular area extending longitudinally across the splice and over a portion of each of the fibers, thereby calculating a lower arc center position, X arc,down .
12. The method of claim 11 , further comprising:
determining an arc-walk distance in the upper rectangular area, Δ(up,0), utilizing the equation:
Δ(up,0)= X arc,up −X center
where, X center is a position aligned with the electrodes;
determining an arc-walk distance in the lower rectangular area, Δ(down,0), utilizing the equation:
Δ(down,0)= X arc,down −X center ;
and
calculating an initial average arc-walk distance, Δ(arc-walk,0), utilizing the equation:
Δ( arc -walk,0)=½[Δ(up,0)+Δ(down,0)].
13. The method of claim 1 , wherein the step of determining a pre-fusion arc-center position by analyzing thermal light emissions captured in the warm image includes:
defining an upper rectangular area above the fibers and the gap, said upper rectangular area extending longitudinally across the gap and over a portion of each of the fibers, said upper rectangular area being defined by coordinates {(x 1 , y 1 ), (x 2 , y 1 ), (x 2 , y 2 ), (x 1 , y 2 )};
analyzing light intensity-distributions in the upper rectangular area utilizing the warm image, said analyzing step including:
calculating an upper arc center position, X arc,up , utilizing the equations:
X
a
rc
,
up
=
∫
y1
y2
∫
x1
x2
xL
up
(
x
,
y
)
ⅆ
x
ⅆ
y
∫
y1
y2
∫
x1
x2
L
up
(
x
,
y
)
ⅆ
x
ⅆ
y
(
1
)
and
L up ( x,y )=max[ L min , L ( x,y )− L BG ] (2)
where, L(x,y) is the light intensity at coordinates (x, y); L BG is the average intensity of background light, which depends on settings of the imaging system; and L min is a pre-defined minimum value of light intensity to avoid divergence of the integrations defined in equation (1); and
repeating the defining and analyzing steps for a lower rectangular area below the fibers and the gap, said lower rectangular area extending longitudinally across the gap and under the portion of each of the fibers, thereby calculating a lower arc center position, X arc,down .
14. The method of claim 13 , further comprising:
determining an arc-walk distance in the upper rectangular area, Δ(up,0), utilizing the equation:
Δ(up,0)= X arc,up −X center
where, X center is a position aligned with the electrodes;
determining an arc-walk distance in the lower rectangular area, Δ(down,0), utilizing the equation:
Δ(down,0)= X arc,down −X center ;
and
calculating an initial average arc-walk distance, Δ(arc-walk,0), utilizing the equation:
Δ( arc -walk,0)=½[Δ(up,0)+Δ(down,0)].
15. A method of splicing dissimilar optical fibers, comprising:
determining during a pre-fusion process, an arc-center position by analyzing thermal light emissions captured in a warm image of a low-power electrical arc utilized to clean micro-dust particles from an end-surface of a first optical fiber and an end-surface of a second dissimilar optical fiber, wherein the two end-surfaces are longitudinally positioned adjacent to each other;
determining a longitudinal offset distance from the arc-center position;
abutting the two end-surfaces;
longitudinally positioning the two abutted end-surfaces at the offset distance from the arc-center position; and
asymmetrically heating the repositioned abutted end-surfaces with a high-power electric arc centered at the arc-center position, thereby fusing the two dissimilar optical fibers.
16. The method of claim 15 , wherein the step of determining a longitudinal offset distance from the arc-center position includes determining a longitudinal offset distance based on a direction of light propagation and a degree of Mode Field Diameter (MFD) mismatch between the dissimilar optical fibers.
17. The method of claim 16 , wherein the wherein the first optical fiber is a Highly Rare-Earth-Doped (HRED) optical fiber, and the second optical fiber is a None-Rare-Earth-Doped (NRED) fiber having a large Mode Field Diameter (MFD) mismatch with the HRED optical fiber.
18. The method of claim 17 , wherein the direction of light propagation is from the HRED fiber to the NRED fiber, and the step of longitudinally positioning the two abutted end-surfaces at the offset distance includes longitudinally repositioning the two abutted end-surfaces in the direction of the HRED fiber so that a lower fusion temperature is generated in the HRED fiber when the asymmetrical heating step is performed.
19. The method of claim 15 , further comprising
monitoring variations of fusion temperature in real-time; and
invoking an arc-check process to adjust the high-power electric arc to compensate for detected variations of fusion temperature.
20. An arrangement for splicing dissimilar optical fibers, comprising:
means for longitudinally positioning an end-surface of a first optical fiber and an end-surface of a second dissimilar optical fiber adjacent to each other in a splicer;
means for applying a low-power electrical arc to the adjacent end-surfaces to clean micro-dust particles from the two end-surfaces;
a camera for capturing a warm image of thermal light emissions emitted from the low-power electrical arc and the optical fibers during the cleaning of the micro-dust particles;
means for determining a pre-fusion arc-center position by analyzing the thermal light emissions captured in the warm image;
means for determining a longitudinal offset distance from the pre-fusion arc-center position;
means for abutting the two end-surfaces and longitudinally positioning the two abutted end-surfaces at the offset distance from the pre-fusion arc-center position; and
means for asymmetrically heating the repositioned abutted end-surfaces with a high-power electric arc centered at the arc-center position, thereby fusing the two dissimilar optical fibers.
21. The arrangement of claim 20 , wherein the camera is also adapted to capture a warm image of the two abutted end-surfaces during the asymmetrical heating step, and the means for determining a pre-fusion arc-center position is also adapted to determine a main-fusion arc-center position by analyzing thermal light emissions captured during the asymmetrical heating step.
22. The arrangement of claim 21 , wherein the camera is adapted to capture a plurality of warm images by periodically capturing a warm image during the asymmetrical heating step.
23. The arrangement of claim 22 , wherein the camera is adapted to capture a warm image approximately every 100 ms during the asymmetrical heating step.
24. The arrangement of claim 23 , further comprising:
means for determining a main-fusion arc-center position for each of the plurality of warm images captured during the asymmetrical heating step;
means for determining a difference between the main-fusion arc-center position and the pre-fusion arc-center position for each of the determined main-fusion arc-center positions;
means for comparing each of the determined arc-center differences with a difference threshold;
means for stopping the asymmetrical heating step if a determined arc-center difference exceeds the difference threshold; and
means for invoking an arc-check process to compensate for large variations of fusion temperature.
25. The arrangement of claim 20 , further comprising:
means for monitoring variations of main-fusion temperature in real-time; and
means for adjusting the high-power electric arc to compensate for detected variations of main-fusion temperature.
26. A method of determining an arc-center position of an electrical arc formed between an upper electrode and a lower electrode of a splicer utilized to splice optical fibers, said method comprising:
longitudinally positioning an end-surface of a first optical fiber adjacent to an end-surface of a second optical fiber so that a gap is formed between the two end-surfaces, wherein the end-surfaces are positioned in the splicer so that a center of the gap is aligned with the splicer electrodes;
cleansing micro-dust particles from the two end-surfaces with a low-power electric arc generated by the splicer electrodes;
capturing a warm image of the gap, end-portions of the two fibers, and areas above and below the gap and the end-portions during the cleansing step utilizing an imaging system;
defining an upper rectangular area above the fibers and the gap, said upper rectangular area extending longitudinally across the gap and over a portion of each of the fibers, said upper rectangular area being defined by coordinates {(x 1 , y 1 ), (x 2 , y 1 ), (x 2 , y 2 ), (x 1 , y 2 )};
analyzing light intensity-distributions in the upper rectangular area utilizing the warm image, said analyzing step including:
calculating an upper arc center position, X arc,up , utilizing the equations:
X
a
rc
,
up
=
∫
y1
y2
∫
x1
x2
xL
up
(
x
,
y
)
ⅆ
x
ⅆ
y
∫
y1
y2
∫
x1
x2
L
up
(
x
,
y
)
ⅆ
x
ⅆ
y
(
1
)
and
L up ( x,y )=max[ L min , L ( x,y )− L BG ] (2)
where, L(x,y) is the light intensity at coordinates (x, y); L BG is the average intensity of background light, which depends on settings of the imaging system; and L min is a pre-defined minimum value of light intensity to avoid divergence of the integrations defined in equation (1); and
repeating the defining and analyzing steps for a lower rectangular area below the fibers and the gap, said lower rectangular area extending longitudinally across the gap and under the portion of each of the fibers, thereby calculating a lower arc center position, X arc,down .
27. The method of claim 26 , further comprising:
determining an arc-walk distance in the upper rectangular area, Δ(up,0), utilizing the equation:
Δ(up,0)= X arc,up −X center
where, X center is a position aligned with the electrodes;
determining an arc-walk distance in the lower rectangular area, Δ(down,0), utilizing the equation:
Δ(down,0)= X arc,down −X center ;
and
calculating an initial average arc-walk distance, Δ(arc-walk,0), utilizing the equation:
Δ( arc -walk,0)=½[Δ(up,0)+Δ(down,0)].