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 Fiber optic dye amplifier

Details
Inventors: Shaw, Herbert J.; Digonnet, Michel J. F.; Bergh, Ralph A.; Sorin, Wayne V.; Kolner, Brian H.;
Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford, CA)
Primary Examiner:
Assistant Examiner:
Attorney, Agent or Firm:

A fiber optic amplifier as disclosed, comprised of a fiber optic, monomode waveguide which has a core and cladding. Part of the cladding over a predetermined region is removed and replaced by an active medium capable of absorbing light energy at a first wavelength and emitting light energy at a second wavelength. The active medium is a lasing dye which has an index of refraction adjusted to be slightly less than the index of refraction of the fiber core. The amount of cladding which is removed is adjusted such that a predetermined amount of penetration of the evanescent field from a pump light signal coupled into an end of the fiber penetrates the active medium. A probe signal to be amplified causes stimulated emission from the excited dye molecules by penetration of its evanescent field into the dye in the region where the cladding is removed. In the preferred embodiment a recirculating pump is used to circulate dye through a cavity which is placed over the portion of the fiber where the cladding is removed. The dye molecules in contact with the surface caused by removal of the cladding are continually changed. A temperature control unit maintains the temperature of the dye such that its index of refraction remains tuned to an amount just less than the index of refraction of the core.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT Brief Description of the Drawings FIG.
1 is a drawing of the amplifier system of the invention.
FIG.
2 is a cross sectional view of the fiber 20 taken along the view line 2--2 in FIG.
1.
FIG.
3 is a perspective view of the fiber holder of the amplifier.
FIG.
4 is a graph of oil drop test results to determine the proper amount of cladding to remove.
FIG.
5 shows the effect of polishing into the core upon transmission losses.
FIG.
6 illustrates the wavelength dependence of the penetration of the evanescent field into the cladding.
FIG.
7 illustrates some of the chemical structures for dyes that are suitable for lasing and light amplification.
FIG.
8 illustrates the energy levels of a typical molecule of dye such as is shown in FIG.
7.
FIGS.
9 (a)-(c) illustrates the processes of absorption, spontaneous emission and stimulated emission occurring during changes in quantization levels.
FIG.
10 illustrates the mechanism of amplification by stimulated emission.
FIG.
11 shows the absorption and emission curves for a typical lasing dye such as Rhodamine 6G.
FIG.
12 illustrates the actual absorption curve for the Rhodamine 610 dye used in the preferred embodiment when placed on the fiber surface 72.
FIG.
13 illustrates the sensitivity of absorption of energy by the dye as a function of dye index of refraction and wavelength.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT Referring to FIG.
1 there is shown a drawing of the preferred embodiment of the invention and the dye amplifier itself.
A monomode fiber optic waveguide 20 is mechanically affixed to a fiber holder 22.
The purpose of the fiber holder 22 is to mechanically secure the fiber 20 and to expose a portion of the cladding of the fiber 20 for removal by polishing of the surface 26.
In the preferred embodiment, the fiber holder 22 is one-half of a directional coupler the structure of which is well known in the art.
Briefly, the structure is a quartz block having a groove formed therein of the approximate dimensions of the diameter of fiber 20



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