Hollow-Core Photonic Crystal Fiber and Method of Manufacturing thereof

Abstract

A hollow-core photonic crystal fiber (HC-PCF)(10) for guiding at least one mode of a light field(1) along a mode guiding section(11) of the HC-PCF(10), comprises an outer jacket(12), an inner cladding(13) and a hollow core(14), which extend along the HC-PCF(10), wherein the inner clad-ding(13) is arranged on an interior surface of the outer jacket(12) and comprises anti-resonant structures(15) surrounding the hollow core(14), and the hollow core(14) has a mode guiding core diameter(d) provided along the mode guiding section of the HC-PCF(10), and wherein at least one fiber end (16) of the HC-PCF(10) has a light field coupling section(17) in which the hollow core(14) is tapered over an axial coupling section length from a fiber end core diameter(D) at the at least one fiber end (16) to the mode guiding core diameter(d). Furthermore, methods of using the HC-PCF and manufacturing the HC-PCF are described.

Claims

1.-18. (canceled)

19. A hollow-core photonic crystal fiber (HC-PCF), being configured for guiding at least one mode of a light field along a mode guiding section of the HC-PCF, comprising: an outer jacket, an inner cladding and a hollow core, that extend along the HC-PCF, wherein the inner cladding is arranged on an interior surface of the outer jacket and comprises anti-resonant structures surrounding the hollow core, and the hollow core has a mode guiding core diameter (d) provided along the mode guiding section of the HC-PCF, characterized in that at least one fiber end of the HC-PCF has a light field coupling section in which the hollow core is tapered over an axial coupling section length from a fiber end core diameter (D) at the at least one fiber end to the mode guiding core diameter (d).

20. The hollow-core photonic crystal fiber of claim 19, wherein: the anti-resonant structures have a cross-sectional dimension that gradually increases in the light field coupling section towards the mode guiding section.

21. The hollow-core photonic crystal fiber of claim 19, wherein: the fiber end core diameter (D) and the axial coupling section length are selected such that an overlap of the inner cladding and the light field to be focussed to the hollow core for guiding by the HC-PCF is excluded or negligible at the fiber end.

22. The hollow-core photonic crystal fiber of claim 19, wherein: an axial transition length over which the fiber core diameter dimension reduces in the light field coupling section from the fiber end core diameter (D) to (0.5*(D+d)) is at least 0.5 times the mode guiding core diameter (d) and/or at most 0.5 times a transition dimension ((D.sup.2d.sup.2d.sup.4).sup.0.5/(4)), where is the central wavelength of the light field.

23. The hollow-core photonic crystal fiber of claim 22, wherein: the axial transition length is at least 10 m and/or at most 1000 m.

24. The hollow-core photonic crystal fiber of claim 19, wherein: the axial coupling section length of the light field coupling section is at least the mode guiding core diameter (d) and/or at most a transition dimension ((D.sup.2d.sup.2d.sup.4).sup.0.5/(4)), where is the central wavelength of the light field.

25. The hollow-core photonic crystal fiber of claim 24, wherein: the axial coupling section length of the light field coupling section is at least 20 m and/or at most 5000 m.

26. The hollow-core photonic crystal fiber of claim 19, wherein: the anti-resonant structures have rounded ends facing toward the at least one fiber end.

27. The hollow-core photonic crystal fiber of claim 19, wherein: the inner cladding extends to the opening of the at least one fiber end.

28. The hollow-core photonic crystal fiber of claim 19, wherein: the inner cladding does not extend to the opening of the at least one fiber end.

29. The hollow-core photonic crystal fiber of claim 19, wherein: the light field coupling section is provided at an incoupling end of the HC-PCF only.

30. The method of using the hollow-core photonic crystal fiber of claim 19, wherein: the HC-PCF is used for subjecting a light field to an optically non-linear process, in particular spectral broadening, or the HC-PCF is used for delivering a light field to an application site.

31. The method of manufacturing the hollow-core photonic crystal fiber of claim 19, comprising the steps of: providing a HC-PCF including the outer jacket and the inner cladding, and forming the light field coupling section by thermal treatment of the HC-PCF.

32. The method of claim 31, comprising the steps of: subjecting at least one fiber section of the HC-PCF to the thermal treatment, and cutting the HC-PCF in the at least one thermally treated fiber section and with a distance thereof to a predetermined fiber length for forming the light field coupling section at the at least one fiber end.

33. The method of claim 31, comprising the steps of: cutting the HC-PCF to a predetermined fiber length to be obtained, and subjecting at least one fiber end of the cut HC-PCF to the thermal treatment for forming the light field coupling section at the at least one fiber end.

34. The method of claim 32, wherein: the thermal treatment comprises a heating of the HC-PCF such that the resonant structures of the inner cladding are softened and the light field coupling section is formed by the effect of surface tension in the softened anti-resonant structures.

35. The method of claim 32, wherein: the thermal treatment comprises a heating of the HC-PCF such that the resonant structures of the inner cladding are softened and the light field coupling section is formed by the combined effect of surface tension in the softened anti-resonant structures and an applied vacuum in at least one of the anti-resonant structures.

36. The method of claim 32, wherein: the thermal treatment comprises a heating of the HC-PCF such that the resonant structures of the inner cladding are softened and the light field coupling section is formed by the combined effect of surface tension in the softened anti-resonant structures and an applied pressure in the mode guiding core.

Description

[0031] Further details and advantages of the invention are described in the following with reference to the attached drawings, which show in:

[0032] FIG. 1: a schematic cross-sectional view of a HC-PCF according to a preferred embodiment of the invention;

[0033] FIG. 2: a schematic cross-sectional view of a HC-PCF according to a further embodiment of the invention with an illustration of the pump light field;

[0034] FIG. 3: images of a fiber end of an inventive HC-PCF, including an optical micrograph (A) and a SEM image (B);

[0035] FIG. 4: SEM images of the input side of degraded conventional HC-PCFs;

[0036] FIG. 5: experimental results of measuring a HC-PCF output power of an inventive HC-PCF (curve A) and a conventional HC-PCF (curve B);

[0037] FIG. 6: a schematic illustration of a light source device including a HC-PCF according to the invention;

[0038] FIG. 7: a measured output spectrum of a HC-PCF according to the invention; and

[0039] FIGS. 8 and 9: a schematic illustration of a HC-PCF based light source including a conventional HC-PCF and an SEM image of the input side of a conventional HC-PCF.

[0040] Features of preferred embodiments of the invention are described in the following with reference to the provision of a light field coupling section at the input fiber end of a HC-PCF. The invention can be correspondingly implemented with a light field coupling section at the output fiber end or at both ends of the HC-PCF. Exemplary reference is made to a HC-PCF, wherein the inner cladding is formed by a single ring arrangement of tube-shaped capillaries. The invention can be correspondingly implemented with other anti-resonant structures, like Kagome-type or nested structures.

[0041] FIGS. 1 and 2 show schematic enlarged cross-sectional views of HC-PCFs 10 according to preferred embodiments of the invention. FIG. 2 illustrates a Gaussian beam (input light field 1) being focused and coupled to the HC-PCFs 10 (shown with the input fiber end only). For practical applications, the HC-PCFs 10 have a longer axial extension than shown in FIGS. 1 and 2, which, depending on the function of the HC-PCF 10, is selected in a range from e. g. 1 cm to 5 m or even more.

[0042] The HC-PCF 10 comprises an outer jacket 12 being made of e. g. quartz glass with a thickness of e. g. 30 m and an inner diameter 1 of e. g. 60 m, an inner cladding 13 comprising anti-resonant structures 15, and a hollow core 14 being provided by the space between the anti-resonant structures. The anti-resonant structures comprise e. g. a single ring arrangement of five capillaries as illustrated with reference to the conventional technique in FIG. 9. The capillaries are made of quartz glass with a thickness of e. g. 0.1 m to 1 m or even more. The inner cladding 13 is supported by the interior surface of the outer jacket 12. The HC-PCF 10 includes a mode guiding section 11 wherein the hollow core 14 has a mode guiding core diameter d, e. g. 30 m.

[0043] At the input fiber end 16 of the HC-PCF 10, a light field coupling section 17 is provided. The light field coupling section 17 has an axial coupling section length L, along which the inner diameter of the HC-PCF 10 is reduced from the fiber end core diameter D to the mode guiding core diameter d. With an example of a HC-PCF 10 with a mode guiding core diameter of 30 m, the axial coupling section length preferably is equal to or below 300 m. For larger mode guiding core diameters, e. g. equal to or above 50 m, the axial coupling section length can be at least 1 mm, in particular some mm. The inner cladding 14 capillaries 15 form a smooth transition from partially collapsed (FIG. 3B) to their dimensions in the untreated fiber structure (FIG. 9).

[0044] The theoretical maximum axial coupling section length L of the light field coupling section 17 can be derived from the focusing properties of a Gaussian laser beam (input light field 1) as follows. The focused laser beam is characterized by its beam diameter w(z) (z: beam propagation direction and axial direction of HC-PCF 10, see FIG. 2 in the region where z<0), its central wavelength , and its focal diameter w.sub.0=w(0). w(z) can be calculated via:

w(z)=w.sub.0(1+(z/z.sub.R).sup.2).sup.0.5,

[0045] where z.sub.R=w.sub.0.sup.2/(4) is the Rayleigh length.

[0046] To reduce the light overlap at the fiber end, the axial coupling section length L and the end diameter D of the light field coupling section have to be chosen such that w(L)<D, i.e.

D>W(L)d(1+(L/z.sub.R).sup.2).sup.0.5d(1+(4L/(d.sup.2)).sup.2).sup.0.5

[0047] where dw.sub.0. Solving this equation for L yields:

L<(D.sup.2d.sup.2d.sup.4).sup.0.5/(4)

[0048] The length restriction preferably is extended with a length limit for section that is facing the fiber end and where the initial core diameter D is reduced to 0.5*(D+d), i.e. to 50% of the total reduction. Preferably, this length (so called axial transition length) is shorter than 0.5 times (D.sup.2d.sup.2d.sup.4).sup.0.5/(4).

[0049] FIG. 3 shows images of a practical example of an inventive HC-PCF. FIG. 3A is an optical micrograph of the input fiber end 16, wherein the in the light field coupling section has a length of approx. 250 m. FIG. 3B is a SEM image of the input face with the outer jacket 12 and the anti-resonant structures 15. The essential advantage of the invention is represented by FIG. 3B: the anti-resonant structures 15 are shown after a lifetime test (see also FIGS. 4 and 5), and there is no visible sign of degradation.

[0050] The power induced degradation of conventional HC-PCFs and the advantageously longer life time of the inventive HC-PCF are further illustrated in FIGS. 4 and 5. FIGS. 4A and 4B show SEM images of the input side of conventional HC-PCFs that have been exposed for about >100 Wh to a pump light field. The inventors have found that this pronounced degradation of the cladding structure results from plasma-enhanced erosion, wherein the plasma is formed because of field enhancement at the sharp gas-glass-interfaces at the fiber input side. As a consequence of the degradation, the average output power of the conventional HC-PCF strongly decreases already after several 10's of Wh (see FIG. 5, dashed curve B). Testing the inventive HC-PCF in a nonlinear experiment, a dramatic improvement of the lifetime is obtained (see FIG. 5, solid curve A).

[0051] According to FIG. 5, that exposures >1000 Wh are feasible, with extrapolated values of several 1000 Wh.

[0052] An embodiment of a broadband, high-brightness light source 100 including the inventive HC-PCF 10 is illustrated in FIG. 6. Such light sources 100 preferably are used in applications where long lifetime is highly desired, such as optical metrology (e.g. for semiconductor industry), UV microscopy or spectroscopy.

[0053] The light source 100 comprises a pump source 20, an optional stabilization unit 21, the HC-PCF 10 placed in a gas cell 30 and optional additional output optics 22. The pump source 20 is a pulse laser creating the pulsed light field 1, e. g. with energy and sub-ps pulse duration, in particular 10 J energy and 300 fs pulse duration with a central wavelength 1030 nm. The stabilization unit 21 is provided for stabilizing the spatial position of the pulse output from the pump source 20. The pump pulses are launched into the gas-filled inventive HC-PCF 10. The gas cell includes e. g. Ar at 30 bar. The pulses are subjected to spectral broadening in the HC-PCF 10 and the broadband output 2 is collimated with the output optics 22 and delivered to an application. An example spectrum 3 of such a light source is shown in FIG. 7, ranging from about 240 to 1700 nm. The inset of FIG. 7 shows the measured beam cross-section of the output 2 (1/e.sup.2 diameter 3.9 mm at 570 nm), indicating a very high beam quality.

[0054] Alternatively, the HC-PCF 10 can be used for a linear light transmission, e. g. from a laser source creating cw or pulsed laser light for material processing to an application site, e. g. a work piece.

[0055] The HC-PCF 10, e. g. according to FIG. 1, is manufactured by heating a fiber section of a HC-PCF with a fusion splicer for a heating time of 300 ms to a temperature above the glass transition temperature of e. g. 1200 C. (for fused silica). The fiber section has a length of e. g. 500 m. The taper shape is formed by reducing the temperature from the centre of the heated fiber section to the ends thereof or simply by the temperature field created by a centre heating of the fiber section. Subsequently, the fiber section is cut after cooling.

[0056] The features of the invention disclosed in the above description, the drawings and the claims can be of significance individually, in combination or sub-combination for the implementation of the invention in its different embodiments.