FCC FibreCableConnect GmbH develops and manufactures fiber optic cables for laser beam delivery up to 1 kW laser power for industrial and medical applications, based on standarded connectors like SMA or D80. In addition, fiber bundles, probes for spectroscopy and optical fiber couplers as well as customer and application-specific special solutions.
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Execution with ZrO2 ferrules for single and multimode fibers up to 128μm cladding diameter and metal ferrules for fibers with a cladding diameter from 128μm. APC version with bevel cut of 8 °.
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Laser cables High Power D80 Passive cooling – up to 500 W are mainly used in the area of material processing such as laser cutting or laser welding. The passive heat sink as well as 4mm copper ferrule allow a high thermal efficiency due to a very good heat dissipation. Optionally available with end caps and mode stripping. The complete structure is torsion- and stress-free mounted, but mechanically extremely stable.
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Laser cables High Power D80 Active cooling – up to 1 KW are used as well as passively cooled high power connectors in the field of material processing: laser welding, laser cutting. Due to the active cooling of the connector body, however, an even higher optical power condition is possible by very efficient heat dissipation. Optional versions with mode stripping and end cap are available. The complete structure is torsion- and stress-free mounted, but mechanically extremely stable.
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Laser cables High Power D80 fiber breakage monitoring are used in particularly critical applications, where a defect in the fiber can have particularly serious consequences. Apart from the fiber break, the plug temperature is also detected. The system shuts off automatically in the event of a defect, thus preventing uncontrolled leakage of the laser beam. Optionally, fiber breakage monitoring is also available for HP-SMA connectors.
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When coupling of the laser beam, it is focused into the fiber core, while a high power density occurs on the front surface. Although the anti-reflective (AR) coating of this surface reduces the Fresnel loss, it does not tolerate high power density even despite a large core diameter. A fiber end face without AR coating allows greater performance, but simultaneously leads more heat into the connector on the output side. This must be considered in terms of heat management.
For small fiber core Diameters with high power density dominate fiber connectors with a cylindrical end cap made of quartz glass currently. This end cap is larger than the fiber core and is spliced to the optical fiber. In doing so, the laser beam is focused onto the fiber core via the end surface of the quartz cap, where, at the same laser power, the power density is significantly lower. When, for instance, coupling 500 W of laser power in a 200 micron fiber, a 3 mm long quartz cap changes the energy density at the surface by the factor of 30. This allows the use of AR coating also in the kilowatt range. The method requires robust and low-loss splicing that guarantees a high damage threshold at the border between the end cap and the fiber.
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During coupling into a singlemode fiber, the laser beam is focused into the fiber core, resulting a high power density on the facet. This is higher the smaller the fiber core and larger the laser power. To reduce the power density, an end cap will be spliced on the fiber facet. The laser beam is focused on the fiber core over the end face of this end cap, where at the same laser power, the power density is significantly lower.
The length of the end cap is adjusted exactly to the fiber core. For singlemode fibers this starts at 100 μm. The diameter of the end cap is adjusted to the cladding diameter of the fiber. The singlemode fibers with spliced end cap are terminated with standard connectors (SMA, FC …) but also with application-specific ferrules.
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To obtain a good transfer performance, the beam must be optimally coupled into the fiber.
This requires that the focus on the fiber core generally should not to be more than 85% to 90% of the fiber core diameter. At the same time its divergence angle must be less than numerical aperture of the fiber. This is especially important for diode lasers that have a rectangular beam profile. If the laser beam couples not in the core only, but also in the cladding, the modes are also guided in the cladding. In order to remove them from the cladding, the specially developed for this purpose mode stripping is used. This mode stripper is installed in the connector body and removes the cladding modes over a certain length. The required length is defined according to the coupling properties (spot size and NA-difference). The mode stripper ensures that the beam profile looks perfect at the fiber output. The removed cladding modes are converted into the heat in the connector body. If, in this case, the connector is not sufficiently cooled, the fiber might burn off in the connector.
For this reason, different requirements may be imposed on the length of the mode stripper. This is why FCC has developed its own software to determine the mode stripper length.
To monitor the temperature of the fiber, the connectivity and the fiber break, a double-wound copper wire is used. Over connectivity of the fiber connector the circuit is closed. The principle is based on applying voltage at temperature-dependent resistors, which is proportional to the respective resistance. If the voltage falls below the lower or the upper limit, a relay switches, interrupting power transfer to the laser. In monitoring the fiber, the upper limit voltage serves to protect against fiber breakage, while the lower limit voltage bridges the contacts for connectivity. In monitoring the fiber connector temperature, only the lower limit voltage is used to prevent the fiber connector from overheating.
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