Coupling device for connecting an optical waveguide to an associated optical waveguide connection

Abstract

A coupling device for an optical waveguide includes an optical waveguide connection for a first optical waveguide. The coupling device includes an optical filter arranged in a beam path between a laser light source and the optical waveguide connection which reflects light of a first wavelength range or a first polarization direction and transmits light of a second wavelength range or a second polarization direction.

Claims

1. A coupling device for at least one optical waveguide that is configured to detect overheating of the at least one optical waveguide, the coupling device comprising an optical waveguide connection for a first optical waveguide, wherein the coupling device further comprises an optical filter arranged in a beam path between a laser light source and the optical waveguide connection, wherein the optical filter reflects light of a first wavelength range and transmits light of a second wavelength range such that a beam path of laser light generated by the laser light source and a beam path of signal radiation generated by overheating of the optical waveguide connected to the optical waveguide connection are separated depending on a wavelength thereof, thereby causing the signal radiation to be detected separately and recognized as an indication of waveguide overheating.

2. The coupling device of claim 1, wherein a first light meter is arranged such that light reflected by the optical waveguide connection is directed to the optical filter and transmitted to the first light meter.

3. The coupling device of claim 2, wherein a second light meter is arranged such that at least a portion of light from the laser light source is transmitted to the second light meter via the optical filter.

4. The coupling device of claim 3, wherein the first light meter and/or the second light meter are respectively designed to measure the output of light of either the first or the second wavelength range.

5. The coupling device of claim 4, wherein the first light meter and/or the second light meter each comprise a photodiode and a light meter optical filter in the beam path between the photodiode and the optical filter, wherein the light meter optical filter of the first light meter transmits only light of the one of the first or the second wavelength range that the first light meter is designed to measure, and wherein the light meter optical filter of the second light meter transmits only light of the one of the first or the second wavelength range that the second light meter is designed to measure.

6. The coupling device of claim 1, wherein the first wavelength range comprises a wavelength range of at least one laser source outside the range of visible light.

7. The coupling device of claim 1, wherein the second wavelength range comprises visible light.

8. The coupling device of claim 3, wherein light bundling optics is provided between the optical filter and the first waveguide, between the optical filter and a second waveguide, between the optical filter and the first light meter and/or between the optical filter and the second light meter.

9. The coupling device of claim 1, wherein the coupling device comprises an optical waveguide inlet for a second optical waveguide, wherein the optical filter is arranged in the beam path between the optical waveguide inlet and the optical waveguide connection.

10. The coupling device of claim 1, wherein the coupling device for the signal light comprises a diffractive or dispersive filter spectrally distributing the signal light to different light meters.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The following is a detailed explanation of embodiments of the invention with reference to the drawings.

(2) In the Figures:

(3) FIG. 1 is a schematical illustration of a first embodiment,

(4) FIG. 2 is a diagram including the wavelength components of the first and the second wavelength range,

(5) FIG. 3 is a simplified illustration of the first embodiment,

(6) FIG. 4 shows a second embodiment in correspondence with the illustration in FIG. 3,

(7) FIG. 5 shows a third embodiment in correspondence with the illustration in FIG. 3,

(8) FIG. 6 shows a fourth embodiment in correspondence with the illustration in FIG. 3, and

(9) FIG. 7 illustrates a detail of another embodiment.

DESCRIPTION OF THE INVENTION

(10) FIG. 1 illustrates a laser device 10 of conventional design comprising a laser light source 11 in the form of a laser diode for generating laser light. The laser light has a working wavelength of about 980 nm that is outside the wavelength range of visible light of 380-780 nm. The laser light generated is coupled into a second optical waveguide 12 and is coupled into the coupling device 16 of the invention via the waveguide inlet 14. The laser light coupled in is directed onto the optical filter 20 through bundling optics 18, which filter is arranged in the beam path from the waveguide inlet 14 to the optical filter 20 under an inclination of about 45° relative to the propagation of the laser light.

(11) The optical filter 20 reflects light in a first wavelength range 22 of more than 850 nm, whereas light of the second wavelength range 24, which is less than 850 nm, is transmitted. Thus, the laser light coupled in, having a wavelength of 980 nm, is reflected by the optical filter by 90° towards the optical waveguide connection 26 and is coupled into the first optical waveguide 28 via the optical waveguide connection 26. The optical waveguide 28 is a laser cardiac catheter for application in cardiology in order to direct laser light with typical outputs of about 40 W to affected regions of the heart muscle for the treatment of cardiac insufficiency or disturbances of the heart muscle or the rhythm of the heart. In the event of a waveguide breakage or a breakage of a plurality of fibers of the waveguide, the energy is converted into heat at the breakage site. When used in a blood-filled heart or in the vascular system of a patient, the resulting temperature of up to 1,000° C. and beyond causes plasma to form which generates a signal radiation in the form of white light. The differentiation between laser light and signal radiation (white light) is based exclusively in dependence on the wavelength or, if applicable, in dependence on the polarization and is thus independent of output. Thereby, it is also possible to detect signal radiation with a significantly lower output with respect to laser light, which signal radiation is returned through the optical waveguide 28 to the optical waveguide connection 26.

(12) The white light reflected by the optical waveguide connection 26 is directed through the bundling optics 30 between the optical waveguide connection 26 and the optical filter 20 to the optical filter 20 and is not reflected onto the waveguide inlet 14 by the same, but is transmitted towards the first meter means 32. The white light is transmitted and not reflected, because its wavelengths of a maximum of 780 nm fall into the second wavelength range 24 below 850 nm that is transmitted by the mirror 20, but not reflected. The first meter means 32 is arranged on the side of the optical waveguide connection 26 opposite the optical filter 20 such that a beam path follows a straight course from the optical waveguide connection 26 through the optical filter 20 to the photodiode of the first meter means 32.

(13) The first meter means 32 is further provided with an optical filter between the optical filter 20 and the photodiode of the meter means 32. The optical filter is a band pass filter with a passband in the range of visible light so that possible laser light with a wavelength of more than 900 nm does not reach the photodiode.

(14) A second light meter means 34 is arranged on the side of the optical waveguide inlet 14 opposite the filter 20 such that light from the optical waveguide inlet 14 impinges on the photodiode of the second meter means 34 via the optical filter 20. Thus, white light which, due to a breakage in the in-coupling second optical waveguide 12, impinges on the optical waveguide inlet 14 can be transmitted through the optical filter 20 and be measured by the photodiode of the second meter means 34. Moreover, the optical filter 20 is designed such that about 99.99% of the laser light of the first wavelength range 22 are reflected and about 0.01% of the output are transmitted. Thus, in normal operation with undamaged second waveguide 12, the second meter means 34 detects 0.01% of the laser output. If the laser light output differs significantly from 0.01%, because too little laser light reaches the coupling device 10, e.g. because of a waveguide breakage or fissure or a malfunction of the laser light source 11, or because, due to a malfunction of the laser light source 11, the laser light output coupled in is exceeded to an extent dangerous for a patient, the measuring signal can activate an emergency stop function for the deactivation of the laser source.

(15) FIG. 2 illustrates the two wavelength ranges 22 and 24 separated from each other by the optical filter 20. The laser light generated by the laser light source 11 has a maximum, standardized to the value 1, in the range of the working wavelength of the laser of 980 nm. As is exemplified by the transmission curve of the optical filter 20 (illustrated by the broken line), the laser light with the working wavelength of 980 nm is not transmitted, but is reflected. In the second wavelength range 24, a further local maximum in the range between 670 nm and 750 nm can be seen. The wavelength component results from the signal radiation in the range of visible light (white light) caused by a damage to the waveguide 28. This wavelength component of the signal radiation is transmitted almost completely by the optical filter 20, but is not reflected, as is represented by the overlap with the broken line for the transmitted wavelength components in FIG. 2.

(16) FIG. 3 is a simplified illustration of the basic principle of the first embodiment, wherein the laser light (shown as hatched lines) is reflected for the greater part from the optical waveguide inlet 14 to the optical waveguide connection 26 and is transmitted for a smaller part towards the second meter means 34. The optical filter 20 transmits the signal radiation (shown as dots), which is reflected in the optical waveguide 28, from the optical waveguide connection 26 completely towards the first meter means 32.

(17) The second embodiment illustrated in FIG. 4 differs from the first embodiment in FIG. 3 in that the optical waveguide inlet 14 and the optical waveguide connection 26 are arranged along a straight path on opposite sides of the optical filter 20, wherein a major part of the light of the first wavelength range 22 (laser light) is transmitted through the optical filter 20 towards the optical waveguide connection 26, while a lesser part of the light output in the first wavelength range 22 is reflected by the optical filter 20 towards the second meter means 34. The signal radiation (shown as dots) reflected in the optical waveguide 28 is reflected completely at the optical filter 20 from the optical waveguide connection 26 to the first meter means 32.

(18) The third embodiment illustrated in FIG. 5 differs from the first embodiment in FIG. 3 in that the light output of the first wavelength range 22 is reflected completely at the optical filter 20 from the optical waveguide inlet 14 towards the optical waveguide connection 26 without a part thereof being transmitted. No first meter means 32 is provided.

(19) The fourth embodiment illustrated in FIG. 6 differs from the second embodiment illustrated in FIG. 4 in that the light output of the first wavelength range 22 (laser light) is transmitted in its entirety from the optical waveguide inlet 14 through the optical filter 20 in the direction of the optical waveguide connection 26 without a part of the light output of the first wavelength range 22 being reflected. No second light meter means 34 is provided.

(20) Complementary to FIGS. 1 to 6, FIG. 7 describes an arrangement comprising a diffractive optical filter 20, wherein the signal light 22 is decomposed spectrally into different partial beams 24a, 24b, 24c by diffraction and is distributed to the light meter means 32a, 32b, 32c.