D behavior of solitons propagating through the D map is changed such that (1) solitons of modest bandwidths have adequate energy at or near D=to provide for error-free transmission over transoceanic distances at or near D=0, and (2) such that the path average pulse energy is nearly independent of D, at or near D=0 for solitons of various pulse widths. The transmission system having this D map is much more tolerant of variations in D and pulse width than the prior art. Another technique uses two different types of +D fiber in the +D section so that there is a step change in the ratio of D divided by the cross-sectional area of the fiber, or “Aeff”, as solitons propagate from one type of +D fiber to the other type of +D fiber in the +D section. This step change in <math overflow="scroll"><mfrac><mi>D</mi><msub><mi>A</mi><mi>eff</mi></msub></mfrac></math> nullifies the effects of the variation in pulse intensity thereby restoring the pulse breathing symmetry. Furthermore, through the use of intermediate Raman amplification, signal loss in transmission lines having very large amplifier periods, e.g., 80 km or 120 km, is overcome."/> Dispersion-managed soliton transmission system with guiding filters
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Dispersion-managed soliton transmission system with guiding filters

机译:具有导向滤波器的色散管理孤子传输系统

摘要

A new dispersion managed soliton transmission system where the D map period is the same as the amplifier period and the pulse breathing the in the +D sections of the D maps is approximately symmetrical. Pulse breathing symmetry by one or both of two techniques. In one technique a guiding filter is placed at the beginning of the D map period such that the guiding filter reduces the bandwidth of soliton pulses passing through it by a minimum amount. Consequently, pulse breathing symmetry is restored. The path average pulse energy vs. D behavior of solitons propagating through the D map is changed such that (1) solitons of modest bandwidths have adequate energy at or near D=to provide for error-free transmission over transoceanic distances at or near D=0, and (2) such that the path average pulse energy is nearly independent of D, at or near D=0 for solitons of various pulse widths. The transmission system having this D map is much more tolerant of variations in D and pulse width than the prior art. Another technique uses two different types of +D fiber in the +D section so that there is a step change in the ratio of D divided by the cross-sectional area of the fiber, or “Aeff”, as solitons propagate from one type of +D fiber to the other type of +D fiber in the +D section. This step change in <math overflow="scroll"><mfrac><mi>D</mi><msub><mi>A</mi><mi>eff</mi></msub></mfrac></math> nullifies the effects of the variation in pulse intensity thereby restoring the pulse breathing symmetry. Furthermore, through the use of intermediate Raman amplification, signal loss in transmission lines having very large amplifier periods, e.g., 80 km or 120 km, is overcome.
机译:一种新的色散管理孤子传输系统,其中D映射周期与放大器周期相同,并且D映射的+ D部分中的脉冲呼吸近似对称。通过两种技术中的一种或两种来实现脉冲呼吸对称。在一种技术中,将引导滤波器放置在D图周期的开始,使得引导滤波器将通过它的孤子脉冲的带宽减小最小量。因此,恢复了脉冲呼吸的对称性。改变通过D映射传播的孤子的路径平均脉冲能量与 D 行为,以使(1)中等带宽的孤子在 D =可在 D = 0或附近的跨洋距离上提供无错传输,并且(2)使得路径平均脉冲能量为对于各种脉冲宽度的孤子,在 D = 0或附近,几乎独立于 D 。具有该D图的传输系统比现有技术更能容忍 D 和脉冲宽度的变化。另一种技术是在+ D部分中使用两种不同类型的+ D纤维,以使D的比率除以纤维的横截面积即“ A eff ”存在阶跃变化。 ,因为孤子在+ D部分中从一种+ D光纤传播到另一种+ D光纤。这一步改变 <![CDATA [<数学溢出=“ scroll”> D A eff ]]> 消除了脉冲强度变化的影响,从而恢复了脉冲呼吸的对称性。此外,通过使用中间拉曼放大,克服了具有非常大的放大器周期,例如80km或120km的传输线中的信号损失。

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