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Topic 3 Dielectric Waveguides and Optical Fibers 2-1 Symmetric ...

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α B (m -1 ) for 10 cm of bend<br />

10 2<br />

10 −1<br />

10 −2<br />

10 −3<br />

901 37500 光電導論 ?1999 S.O. Kasap, Optoelectronics (Prentice Hall)<br />

901 37500 光電導論<br />

10<br />

1<br />

λ = 633 nm<br />

V ≈ 2.08<br />

λ = 790 nm<br />

V ≈ 1.67<br />

0 2 4 6 8 10 12 14 16 18<br />

Radius of curvature (mm)<br />

Measured microbending loss for a 10 cm fiber bent by different amounts of radius of<br />

curvature R. Single mode fiber with a core diameter of 3.9 μm, cladding radius 48 μm,<br />

Δ = 0.004, NA = 0.11, V ≈ 1.67 <strong>and</strong> 2.08 (Data extracted <strong>and</strong> replotted with Δ correction<br />

from, A.J. Harris <strong>and</strong> P.F. Castle, IEEE J. Light Wave Technology, Vol. LT14, pp. 34-<br />

40, 1986; see original article for discussion of peaks in αB vs. R at 790 nm).<br />

77<br />

Example 2.9.1: Rayleigh scattering limit<br />

What is the attenuation due to Rayleigh scattering at around the<br />

λ = 1.55μm window given that pure silica (SiO 2 ) has the following<br />

properties: T f = 1730°C (softening temperature);<br />

β T = 7 x 10 -11 m 2 N -1 (at high temperatures);<br />

n = 1.4446 at 1.5μm.<br />

α<br />

≈<br />

3<br />

=<br />

R<br />

8π<br />

≈<br />

3λ<br />

3<br />

4<br />

2 ( n −1)<br />

3<br />

8π<br />

2 2 −11<br />

−23<br />

( 1.<br />

4446 −1)<br />

( 7×<br />

10 )( 1.<br />

38×<br />

10 )( 1.<br />

730 + 273)<br />

−6<br />

4<br />

( 1.<br />

55×<br />

10 )<br />

3.<br />

27×<br />

10<br />

−5<br />

Attenuation<br />

α<br />

dB<br />

= 4.<br />

34α<br />

m<br />

R<br />

−1<br />

=<br />

2<br />

=<br />

β<br />

T<br />

k<br />

B<br />

T<br />

3.<br />

27×<br />

10<br />

f<br />

−2<br />

km<br />

−1<br />

−2<br />

−1<br />

−1<br />

( 4.<br />

34)(<br />

3.<br />

27×<br />

10 km ) = 0.<br />

142dBkm<br />

79<br />

Example 2.9.1: Rayleigh scattering limit<br />

What is the attenuation due to Rayleigh scattering at around the<br />

λ = 1.55μm window given that pure silica (SiO 2) has the following<br />

properties: T f = 1730°C (softening temperature);<br />

β T = 7 x 10 -11 m 2 N -1 (at high temperatures);<br />

n = 1.4446 at 1.5μm.<br />

901 37500 光電導論<br />

Example 2.9.2: Attenuation along an optical fiber<br />

The optical power launched into a single-mode fiber from a laser<br />

diode is approximately 1 mW. The photodetector at the output<br />

required a minimum power of 10 nW to provide a clear signal (above<br />

noise). The fiber operates at 1.3μm <strong>and</strong> has an attenuation coefficient<br />

of 0.4 dB km -1 . What is the maximum length of fiber that can be used<br />

without inserting a repeater (to regenerate the signal)?<br />

α<br />

dB<br />

1<br />

L =<br />

α<br />

901 37500 光電導論<br />

1 ⎛ P<br />

= 10log<br />

L ⎜<br />

⎝ P<br />

dB<br />

in<br />

out<br />

⎛ P<br />

10log<br />

⎜<br />

⎝ P<br />

in<br />

out<br />

⎞<br />

⎟<br />

⎠<br />

−3<br />

⎞ 1 ⎛10<br />

⎞<br />

⎟ = 10log<br />

= 125km<br />

8<br />

0.<br />

4 ⎜<br />

10 ⎟ −<br />

⎠ ⎝ ⎠<br />

The signal has to be amplified after a distance of about 50 ~<br />

100km, <strong>and</strong> eventually regenerated by using a repeater.<br />

78<br />

80

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