Ultra-high speed light transmission method making use of quasi-solitons in fibers
AssigneeJapan Science and Technology Corporation
InventorAkira Hasegawa
Life of this patent
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Abstract
There is disclosed a super-high speed light transmission method making use of quasi-solitons in a fiber. Chirped stationary pulses are transmitted through the fiber. At a position where the effect of the chirp becomes weak and the sign of the chirp reverses, the sign of the chirp is reversed by a dispersion compensation fiber or fiber grating connected to the fiber in order to recover the initial chirp. The dispersion profile of each of the fibers is properly controlled in order to produce stationary quasi-solitons having a stable pulse shape. The method can prevent widening of pulses, which would otherwise occur due to dispersion.
Claims4
An ultra-high speed light transmission method making use of quasi-solitons in a fiber, said method comprising the steps of:
- (a) transmitting stationary light pulses with a chirp in an optical fiber that has a dispersion profile such that an equivalent potential produced by the chirp reinforces the soliton effect;
- and
- (b) reversing the sign of the chirp at a position where the effect of the chirp becomes weak and the sign of the chirp reverses;
- (c) said reversion of the sign being performed, through use of a dispersion compensation fiber or fiber grating connected to the fiber, in order to recover the initial chirp;
- and
- (d) the dispersion profile of each of the fibers being properly controlled in order to produce stationary quasi-solitons having a stable pulse shape.
An ultra-high speed light transmission method making use of quasi-solitons in a fiber, said method comprising the steps of:
- (a) transmitting stationary light pulses with a chirp in an optical fiber whose dispersion profile d.sub.e (Z') is given by the equation:
- ##EQU16## wherein .delta.=.sqroot.K.sub.1 +C(0).sup.2 , C(0) is a chirp value, Z' is position along the fiber, and K.sub.1 is a constant, or approximately thereof for a given value of the chirp such that an equivalent potential that traps the pulse reinforces the soliton effect;
- and
- (b) reversing the sign of the chirp at a position where the pulse width regains the original value by means of a dispersion compensation fiber or fiber grating connected to the fiber, in order to recover the initial chirp;
- and
- (c) the dispersion profile of each of the fibers being properly controlled in order to produce stationary quasi-solitons having a stable pulse shape.
Dependencies are inferred from the claim text.