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Increas<strong>in</strong>g the relative-<strong>in</strong>dex difference<br />

between the core <strong>and</strong> the cladd<strong>in</strong>g results<br />

<strong>in</strong> decreas<strong>in</strong>g a bend<strong>in</strong>g loss but decreas<strong>in</strong>g<br />

a MFD. If two fibers with Gaussian<br />

electric fields <strong>and</strong> with MFDs of 2W <strong>and</strong> 1<br />

2W , the connection loss <strong>in</strong> dB, Ls,<br />

2<br />

between the fibers can be calculated by<br />

Eq. (3).<br />

(3)<br />

Obviously, the connection loss is m<strong>in</strong>imized when<br />

W =W . When an optical fiber with an enhanced<br />

1 2<br />

Feature Articles: <strong>Optical</strong> <strong>Fiber</strong> Communications<br />

IV. NEW OPTICAL FIBER IN<br />

DEVELOPMENT FOR FURTHER<br />

BENDING LOSS IMPROVEMENT<br />

We so far have described fibers with a simple refractive-<strong>in</strong>dex<br />

profile called as the step-<strong>in</strong>dex profile as<br />

shown <strong>in</strong> Fig.2 (b). In addition to the requirements<br />

<strong>for</strong> an <strong>in</strong>door cable as described <strong>in</strong> section 2, the<br />

cable is desired to be able to be h<strong>and</strong>led without<br />

worry<strong>in</strong>g about bend<strong>in</strong>g just like a metal<br />

cable [11] core refractive <strong>in</strong>dex <strong>for</strong><br />

reduction of bend<strong>in</strong>g loss<br />

is connected with C-<br />

SMF, connection loss <strong>in</strong>creases<br />

accord<strong>in</strong>g as the<br />

MFD difference between<br />

those two fibers.<br />

A fiber with improved<br />

bend<strong>in</strong>g loss <strong>for</strong> an <strong>in</strong>door<br />

cable should be connected<br />

with C-SMF applied <strong>in</strong> a<br />

drop cable <strong>and</strong> an optical<br />

network unit (ONU) <strong>in</strong> a<br />

subscriber. <strong>The</strong>re<strong>for</strong>e, we<br />

should consider not only<br />

bend<strong>in</strong>g loss but also MFD of the fiber so as to<br />

ma<strong>in</strong>ta<strong>in</strong> its MFD as large as that of C-SMF, 9.2 µm.<br />

We have proposed an improved bend<strong>in</strong>g loss fiber<br />

with a refractive <strong>in</strong>dex profile as shown <strong>in</strong> Fig.6<br />

. In this section, we <strong>in</strong>troduce the<br />

fiber which has a new refractive-<strong>in</strong>dex<br />

profile so as to achieve advanced bend<strong>in</strong>g<br />

loss properties.<br />

[12] Table 2. Attenuations of FutureGuide<br />

.<br />

<strong>The</strong> feature of the profile is that "trench" with a lower<br />

refractive-<strong>in</strong>dex than that of the fused silica locates<br />

between the <strong>in</strong>ner cladd<strong>in</strong>g around the core <strong>and</strong> the<br />

outer cladd<strong>in</strong>g. <strong>The</strong> <strong>in</strong>dex trench at the edge of the<br />

mode field works to conf<strong>in</strong>e the mode field stronger<br />

® -SR15E.<br />

Fig�� Fig�� Fig�� Fig�� Fig�� Schematic Schematic of of trench trench trench <strong>in</strong>dex <strong>in</strong>dex profile� profile� profile� profile� profile�<br />

than the step <strong>in</strong>dex profile even if MFD of the fiber is<br />

the same as that <strong>for</strong> a fiber with the step <strong>in</strong>dex profile.<br />

As a result, a fiber with optimized parameters of 1 ~<br />

3 <strong>and</strong> r2 ~r shown <strong>in</strong> Fig.6 can achieve improved<br />

3<br />

bend<strong>in</strong>g loss <strong>and</strong> connection loss properties com-<br />

Ch<strong>in</strong>a Communications December 2005 63

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