Building Your Custom Patch CableHave you looked through our broad selection of stocked patch cables to see if one of them meets your needs? If none of the stocked options are what you are looking for, a custom cable can be manufactured. Select a FiberThorlabs offers four major types of fiber: Single Mode (SM), Multimode (MM), Polarization Maintaining (PM), and Doped. Each fiber type is explained in detail below. You will also find a complete list of all the fibers that we offer for our custom patch cables along with key specifications that may help you decide which fiber is best for your application. We sell all of these fibers individually on our website as well, along with a wide variety of others. Click here to view all of the fiber options Thorlabs offers. Please contact Tech Support if you have any other questions about our fiber.  Light Propagation Down Single Mode Fiber Single Mode (SM) FiberSM fiber has small core sizes that only allow one mode, or ray, to propagate through the fiber. The mode defines how the light travels through space. Light propagates along the axis of the fiber in this single mode (see drawing to the right). In SM fiber, waves have the same mode but different frequencies. This type of fiber is useful in situations where the integrity of the incident pulse of light needs to be retained over long distances. SM fiber offers high bandwidth and low modal dispersion. Photosensitive SM Fiber
Photosensitive single mode fiber is designed to provide high photosensitivity for UV radiation. These fibers offer lower splice loss than standard SM fibers and are suitable for a range of applications. For more information about these fibers, click here. | Item # | Wavelength Range | NA | MFD | | PS1060 | 980 - 1060 nm | 0.13 | 6.2 µm @ 1060 nm | | GF3 | 1500 - 1600 nm | 0.16 | 8.3 µm @ 1550 nm | | GF1 | 1500 - 1600 nm | 0.13 | 10.5 µm @ 1550 nm | | GF4A | 1550 nm | 0.13 | 4.4 µm @ 1550 nm | | GF1B | 1550 nm | 0.13 | 10.4 µm @ 1550 nm |
| Item # | Dispersion | Effective Area | | DCF38 | -38 ps/nm*km | 27 µm2 | | DCF3 | -38 ps/nm*km | 48 µm2 |
| Item # | Wavelength Range | NA | MFD | | SM300 | 305 - 450 nm | 0.13 | 2.5 µm @ 350 nm | | S405-XP | 400 - 680 nm | 0.12 | 3.6 ± 0.5 µm @ 405 nm
5.0 ± 0.5 µm @ 630 nm | | 460HP | 450 - 600 nm | 0.13 | 3.5 µm @ 515 nm | | S460-HP | 460 - 600 nm | 0.12 | 3.4 µm @ 460 nm | | 630HP | 600 - 770 nm | 0.13 | 4.2 µm @ 630 nm | | SM600 | 600 - 800 nm | 0.12 | 4.3 µm @ 633 nm
4.6 µm @ 680 nm | | S630-HP | 630 - 860 nm | 0.12 | 4.2 µm @ 630 nm | | 780HP | 780 - 970 nm | 0.13 | 5.0 µm @ 850 nm | | SM800-5.6-125 | 830 nm | 0.12 | 5.6 µm @ 830 nm | | SM800-G80* | 830 nm | 0.16 | 4.2 µm @ 830 nm | | SM980-5.8-125 | 970 - 1650 nm | 0.13 | 5.8 µm @ 980 nm
6.2 µm @ 1064 nm
10.4 µm @ 1550 nm | | HI1060-J9** | 980 - 1060 nm | 0.14 | 5.9 µm @ 980 nm
6.2 µm @ 1060 nm | | 1060XP | 980 - 1600 nm | 0.14 | 5.9 µm @ 980 nm
6.2 µm @ 1060 nm
9.5 µm @ 1550 nm | | 980HP | 980 - 1600 nm | 0.2 | 4.2 µm @ 980 nm
6.8 µm @ 1550 nm | | SM980-G80** | 980 - 1650 nm | 0.18 | 4.5 µm @ 980 nm
7.5 µm @ 1550 nm | | SMF-28-J9* | 1260-1620 nm | 0.14 | 9.2 µm @ 1310 nm
10.4 µm @ 1550 nm | | CCC1310 - J9* | 1260 - 1625 nm | 0.14 | 8.6 µm @ 1310 nm
9.7 µm @ 1550 nm | | 1310BHP | 1300 - 1625 | 0.13 | 9.5 µm @ 1550 nm | | SM1250G80** | 1310 nm, 1550 nm | 0.12 | 9.0 µm @ 1310 nm
10.5 µm @ 1550 nm | | 1550BHP | 1460 - 1620 nm | 0.13 | 9.5 µm @ 1550 nm | | SM1500G80** | 1550 nm | 0.20 | 6.4 µm @ 1550 nm | | SM2000 | 1700 - 2100 nm | 0.11 | 13 µm @ 2000 nm |
* Ø900 µm Jacket
** Cladding: Ø80 µm | Item # | Wavelength Range | NA | MFD | | UHNA1 | 1100 - 1600 nm | 0.28 | 4.0 µm @ 1310 nm | | UHNA3 | 960 - 1600 nm | 0.35 | 3.3 µm @ 1310 nm | | UHNA4 | 1100 - 1600 nm | 0.35 | 3.3 µm @ 1310 nm |
 Light Propagation Down Step-Index Multimode Fiber  Light Propagation Down Graded-Index Multimode Fiber Multimode (MM) FiberThe larger core diameters of multimode (MM) fiber allow for the propagation of more than one mode. Light not only propagates along the axis of the fiber, as in SM fiber, but also travels away from the axis toward the cladding (see animations to the right). The total internal reflection that occurs at the core-cladding boundary helps reflect the light back towards the fiber axis. MM fiber tends to have a higher NA and larger core sizes than SM fiber, which allows it to gather larger beams of light at greater incident angles. It has lower bandwidth than SM fiber and is susceptible to modal dispersion. Modal dispersion is a distortion of the incident light pulse caused by the fact that the propagation velocity of the different modes varies. Due to the “zigzag” path the modes take to travel down the fiber, the modes that zigzag more take longer to reach the end than those that travel in a straighter path. When all modes, both fast and slow, combine again at the other end of the fiber, the pulse is widened. There are two main types of MM fiber: Step Index and Graded Index. The core in a step-index fiber has a uniform refractive index throughout. There is a sharp decrease in refractive index at the core-cladding boundary where the cladding refractive index is lower than that of the core. This results in the modes traveling down the fiber in a very jagged path (see animation to the right). Step-index fiber is generally made by doping the fiber with another material. The refractive index of the core in a graded-index fiber decreases as the distance to the center of the core increases. This results in a much smaller change in the refractive indice at the core-cladding interface. The smoother transition causes the modes to travel in sinusoidal paths down the fiber (see animation to the right). Graded-index fibers have much lower modal dispersion than step-index fibers. The parabolic wave profile of the modes continuously re-focuses the rays. Those traveling straight down the center of the fiber travel much slower than those traveling in a more sinusoidal path due to the differences in refractive index. The resulting pulse is less spread out and very close in profile to the incident one. Solarization-Resistant MM Fiber
Solarization-Resistant multimode fiber exhibits impressive performance and transmission from the UV to the NIR (180 to 1150 nm). With exceptional UV radiation resistance compared to standard fibers, these multimode fibers are ideal for use in applications such as spectroscopy for pollution analysis and chemical processing, UV photolithography, and medical diagnostics. The polyimide buffer allows this fiber to be used at temperatures up to 300 °C. For more information about these fibers, click here. | Item # | Wavelength Range | NA | Core Size | | HPSC10 | 280 - 750 nm | 0.1 | 10 µm | | HPSC25 | 25 µm |
Polarization-Maintaining (PM) FiberThe polarization of incident light is maintained during propagation through polarization-maintaining (PM) fiber. There are many types of PM fibers, but they all work the same way: stress is induced in the core via rods within the cladding. The stress aligns the fiber, and the light, to a particular polarization. Thorlabs offers two types of PM fiber: Panda style and Bow-Tie style. The types are named for the shape of the stress rods incorporated into the fiber (see drawing to the right). PM fiber is used in fiber optic sensing, interferometry, and quantum key distribution. It is also commonly found in telecommunications applications connecting a laser source and a modulator. PM fiber has higher attenuation than SM and MM fibers. It is important to note PM fiber does not polarize the incident light; rather, it just maintains the existing polarization of the light that is aligned with the stress rods. The fiber key is aligned during the manufacturing process to ensure high-quality output, as evidenced by the polarization extinction ratio (PER). A higher PER indicates that the light exiting the fiber has a polarization that is more consistent with that of what entered. | Item # | Wavelength Range | NA | MFD | | HB800G | 830 nm | 0.16 | 4.2 µm @ 830 nm | | HB980T | 980 nm | 0.14 | 6.0 µm @ 980 nm | | HB1250T | 1310 nm | 0.12 | 9.0 µm @ 1310 nm | | HB1500T | 1550 nm | 0.12 | 10.5 µm @ 1550 nm |
| Item # | Wavelength Range | NA | MFD | | PS-PM980 | 980 nm | | 6.6 ± 1.0 µm @ 980 nm |
| Item # | Wavelength Range | NA | MFD | | PM460-HP | 460 - 700 nm | 0.12 | 3.3 µm @ 515 nm | | PM630-HP | 620 - 850 nm | 0.11 | 4.5 µm @ 630 nm | | PM780-HP | 770 - 1100 nm | 0.12 | 5.3 µm @ 850 nm | | PM980-XP | 970 - 1550 nm | 0.12 | 6.6 µm @ 980 nm | | PM1300-HP | 1270 - 1625 nm | 0.13 | 9.5 µm @ 1300 nm | | PM1550-HP | 1440 - 1625 nm | 0.13 | 10.5 µm @ 1550 nm | | PM2000 | 1850 - 2200 nm | 0.2 | 8.0 µm @ 1950 nm | | Pure Silica Core | | PM-S350-HP | 350 - 460 nm | 0.12 | 2.3 µm @ 350 nm | | PM-S405-HP | 400 - 500 nm | 0.12 | 3.2 µm @ 405 nm
3.5 µm @ 460 nm |
| Item # | Wavelength Range | NA | MFD | | HB1060Z | 1064 ± 50 nm | 0.14 | 7.0 µm @ 1064 nm |
Doped Fiber* Designed to operate at 1530 nm
** Designed to operate from 900 - 970 nm Erbium-Doped SM Fiber
Our wide range of highly doped erbium fibers are suitable for fiber lasers and amplifiers operating in the 1530 to 1610 nm wavelength region. These fibers are utilized in a broad range of applications, ranging from telecommunication amplifiers (EDFAs) to high-power PON/CATV boosters and ultra-short pulse amplifiers used in instrumentation, industrial, and medical applications. For more information about these fibers, click here. Ytterbium-Doped MM Fiber
Thorlabs offers state-of-the-art Ytterbium doped optical fibers for optical amplifiers, ASE light sources, and high-power pulsed and CW fiber laser applications. These fibers are fabricated using the latest doped fiber production technology. For more information about these fibers, please click here. Ytterbium-Doped PM Fiber
Thorlabs' Ytterbium-doped PM fiber is manufactured using the latest technology. These fibers offer high birefringence, low nonlinear effects, and low photodarkening. For more information about these fibers, click here. Passive Double Clad Fiber
Thorlabs' passive large-mode-area (LMA) fibers are matched to the core diameters and numerical apertures of their active counterparts to maintain excellent beam quality throughout fiber laser or amplifier systems. The outer cladding diameter is designed to "round" the shaped active fibers, thereby achieving low pump coupling loss from passive to active fibers. The passive fibers are coated with low-index fluoroacrylate enabling active fibers to be pumped through them. For more information about these fibers, click here.
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Custom Fiber Patch Cables
