1x16 Polarization-Maintaining Fiber Optic Splitters

  • 1310/1550 nm Dual-Window Splitters
  • Split Input Evenly into 16 Ports
  • 2.0 mm Narrow Key FC/PC or FC/APC Connectors


FC/PC Connectors


FC/APC Connectors

Use for Splitting Signals

Related Items

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PANDA PM Fiber Cross Section

Panda Style Fiber
The connector key is aligned to the slow axis of the fiber.


  • 1310/1550 nm ± 40 nm Polarization-Maintaining Fiber Optic Splitters
  • Split Input Signal Evenly Into Sixteen Output Ports
  • 2.0 mm Narrow Key FC/PC or FC/APC Connectors
  • 0.8 m Long Fiber Leads with a Tolerance of +0.075 m / -0.0 m
  • Individual Test Report Included with Each Splitter (See the PER Measurement Tab; Click Here for a Sample Data Sheet)
  • Mount to an Optical Table with the FCQB Mounting Base (Available Below)
  • Contact Us for Custom Wavelength, Coupling Ratio, and Connector Options

Thorlabs' Polarization-Maintaining 1x16 Fiber Optic Planar Lightwave Circuit (PLC) Splitters allow a user to split a single input signal evenly into 16 output signals, which is ideal for high-channel-count applications. In contrast to fused fiber couplers, where light is coupled from one fiber core to the other, these devices operate as a continuous waveguide that splits the propagating signals. Each splitter features a ±40 nm bandwidth around both 1310 nm and 1550 nm center wavelengths. They cannot be used in reverse to combine light sources together into one output port.

These splitters are manufactured using PANDA fiber. As seen in the diagram to the right, stress rods run parallel to the fiber's core and apply stress that creates birefringence in the fiber's core, allowing polarization-maintaining operation. Linearly polarized light must be launched along the slow axis of the fiber to achieve the specified coupling ratio and maintain a high polarization extinction ratio (PER).

Thorlabs' PM Splitters provide a PER of ≥18.0 dB including connectors. Note that the PER will vary with temperature; see the Temperature Cycling Tests section in the PER Measurement tab for details. They have a maximum power handling of 300 mW with connectors or bare fiber and a maximum power handling of 500 mW when spliced (see the Damage Threshold tab for more details). They undergo extensive testing and verification of the PER; details of our testing procedures are provided on the PER Measurement tab. A sample data sheet for the 1310/1550 nm PM splitters can be viewed here.

Each polarization-maintaining splitter is contained in a compact 100.0 mm x 80.0 mm x 10.0 mm housing that includes four through holes for mounting the device to our FCQB mounting base (available separately below). Splitters are offered from stock with 2.0 mm narrow key FC/PC or FC/APC connectors. Five fiber caps are also included with every splitter. Fiber leads are jacketed in Ø900 µm Hytrel®* tubing and the leads are 0.8 m long. Custom configurations with other wavelengths, fiber types, coupling ratios, alignment axes, or port configurations are also available. Please contact Tech Support with inquiries.

*Hytrel® is a registered trademark of DuPont Polymers, Inc.

Alternative Fiber Coupler & Splitter Options
Double-Clad Couplers Single Mode Couplers Single Mode
PLC Splitters
Multimode Couplers Polarization-Maintaining
PLC Splitters
Wavelength Division
Multiplexers (WDM)
2x2 1x2 2x2 1x4 1x8 1x16 1x2 2x2 1x2 2x2 1x4 1x8 1x16

1x16 Fiber Optic PLC Splitter Definitions

This tab provides a brief explanation of how we determine several key specifications for our 1x16 planar waveguide splitters. These devices are fabricated waveguide splitters that split the input signal evenly among 16 outputs. These splitters are not recommended for light combining applications and should only be used to split light. For combining light of different wavelengths, Thorlabs offers a line of wavelength division multiplexers (WDMs).


Excess Loss

Excess loss in dB is determined by the ratio of the total input power to the total output power:

Excess Loss

Pinput is the input power, and the Pport is the output power at each port; when summed across all ports, this represents the total output power. All powers are expressed in mW.


Insertion Loss

The insertion loss is defined as the ratio of the input power to the output power for a given port of the splitter. Insertion loss is always specified in decibels (dB). It is generally defined using the equation below:

Insertion Loss

where Pin and Pout are the input and output powers (in mW). For our 1x16 PLC splitters, the insertion loss specification is provided for each output port. To define the insertion loss for a specific output (e.g., port 1 or port 2), the equation is rewritten as:

Insertion Loss

Insertion Loss

Insertion loss inherently includes both coupling (e.g., light transferred to the other output legs) and excess loss (e.g., light lost from the splitter) effects. The maximum allowed insertion loss for each output is specified. Because the insertion loss in each output is correlated to light coupled to the other outputs, no splitter will ever have the maximum insertion loss in all outputs simultaneously.

Calculating Insertion Loss using Power Expressed in dBm
Insertion loss can also be easily calculated with the power expressed in units of dBm. The equation below shows the relationship between power expressed in mW and dBm:


Then, the insertion loss in dB can be calculated as follows:

Insertion Loss


Optical Return Loss (ORL)

Optical return loss (ORL) is the fraction of light that is reflected back into the input port of the component.


Coupling Ratio

Insertion loss (in dB) is the ratio of the input power to the output power from each leg of the splitter as a function of wavelength. It captures both the coupling ratio and the excess loss. The coupling ratio is calculated from the measured insertion loss. Coupling ratio (in %) is the ratio of the optical power from each output port to the sum of the total power of all output ports as a function of wavelength. It is not impacted by spectral features such as the water absorption region because all output legs are affected equally.



The uniformity is also calculated from the measured insertion loss. Uniformity is the variation (in dB) of the insertion loss over the bandwidth as a function of wavelength. It is a measure of how evenly the insertion loss is distributed over the spectral range. The uniformity is defined as the difference between the insertion loss in one output leg at a given wavelength and the highest or lowest value of insertion loss over the specified wavelength range in that same output leg.

Item #a Description Qty.
Light Source (Not Shown)
S5FC1005P PM Benchtop SLD Source, 1550 nm 1
P1-1550PM-FC-1 Patch Cable, FC/PC, 1550 nm, PM Panda Style, 1 m 1
Linear Polarizer Module
PAF-X-11-PC-Cb FiberPort, FC/PC,
1050 nm - 1620 nm
CP08FP(/M) Cage Plates for Mounting FiberPorts 2
LPNIR050-MP2 Linear Polarizer 1
CRM1P(/M) Cage Rotation Mount 1
SM1A6T Adapter with External SM1 Threads and Internal SM05 Threads 1
ER2-P4 2" (50.8 mm) Long Cage Rods, 4 Pack 1
Analyzer Module
PAF-X-11-PC-Cb FiberPort, FC/PC,
1050 nm - 1620 nm
CP08FP(/M) Cage Plates for Mounting FiberPorts 1
LPNIR050-MP2 Linear Polarizer 1
CRM1P(/M) Cage Rotation Mount 1
SM1A6T Adapter with External SM1 Threads and Internal SM05 Threads 1
CP33(/M) SM1-Threaded (1.035"-40)
Cage Plate
PM122D Digital Power Meter, 700 - 1800 nm 1
ER2-P4 2" (50.8 mm) Long Cage Rods, 4 Pack 1
  • Item list does not include the posts, post holders, clamping forks, breadboard, or fiber component tray shown in the photo to the left.
  • This previous-generation FiberPort is no longer available. A suitable replacement is the PAF2P-11C FiberPort.

Click to Enlarge
Setup to Measure the Extinction Ratio of a
1550 nm PM Coupler

Measurement of Polarization Extinction Ratio (PER)

The polarization extinction ratio (PER) is a measure of how well a polarization-maintaining (PM) fiber or device can prevent cross coupling between the different polarization axes of the fiber. External stress on a fiber from sources such as heating, bending, or pulling can cause the PER to change.

There are two accepted techniques for measuring PER in a fiber coupler. The most common method uses a low-coherence (unpolarized or circularly polarized) broadband light source and measures the extinction ratio with a linear polarizer and power meter. An alternative method uses a narrowband, high-coherence light source and measures the PER with a polarimeter.

Thorlabs uses the power meter method to characterize the extinction ratio performance of the PM fiber couplers sold on this page. An example setup is shown in the image to the right with itemized component list in the table. A broadband light source is input into a linear polarizer module, which allows the user to set the polarization of light entering the input leg of the fiber coupler. The output from one of the legs is sent to the analyzer module, which contains another polarizer and the power meter for measuring the output. Alternatively, the analyzer module can be replaced with an extinction ratio meter.

The PER is measured using the following test procedure:

  • Prepare the fiber end faces of the PM coupler to connect to the measurement setup.
    • For bare fiber ends, strip and cleave the fibers. Use a bare fiber terminator, such as the BFT1, to create a temporary fiber termination.
    • For terminated fiber ends, clean and inspect the connector end faces.
    • Attach a fiber optic light trap to any fiber leads not being measured.
  • Adjust the polarizers in the linear polarizer and analyzer modules sequentially until a minimum power value is measured by the power meter. Record the measured value as Pmin.
  • Rotate the analyzer rotation mount by 90°. Then record the measured value as Pmax.

After Pmin and Pmax are measured, the extinction ratio can be calculated:

Click to Enlarge
7-hour temperature cycling test performed on a standard PN1550R5A1 PM fiber coupler shows that the PER measured for the white-white and white-red paths remains stable over a wide temperature range.

The White-White Path Follows the Input to Signal Output and the White-Red Path Follows the Input to Tap Output

Temperature Cycling Tests

Traditional PM couplers typically exhibit diminished polarization extinction ratio (PER) performance when used at sub-zero (°C) temperatures due to the contraction of the adhesives that are used to assemble the device. This effect disrupts the polarization state of light within the coupler and leads to a decrease in PER. Soft adhesives can be used to mitigate the impact of cold-temperature operation but can create reliability issues at higher temperatures. At high temperatures, adhesives can soften permanently, which changes the optical properties of the coupler.

Unlike traditional coupler manufacturing, Thorlabs uses a proprietary packaging process and design for our standard PM couplers as well as careful selection of adhesives to enable operation over a very wide temperature range (from -40 °C to 85 °C) without significant changes to PER and other optical specifications.

Laser-Induced Damage in Silica Optical Fibers

The following tutorial details damage mechanisms relevant to unterminated (bare) fiber, terminated optical fiber, and other fiber components from laser light sources. These mechanisms include damage that occurs at the air / glass interface (when free-space coupling or when using connectors) and in the optical fiber itself. A fiber component, such as a bare fiber, patch cable, or fused coupler, may have multiple potential avenues for damage (e.g., connectors, fiber end faces, and the device itself). The maximum power that a fiber can handle will always be limited by the lowest limit of any of these damage mechanisms.

While the damage threshold can be estimated using scaling relations and general rules, absolute damage thresholds in optical fibers are very application dependent and user specific. Users can use this guide to estimate a safe power level that minimizes the risk of damage. Following all appropriate preparation and handling guidelines, users should be able to operate a fiber component up to the specified maximum power level; if no maximum is specified for a component, users should abide by the "practical safe level" described below for safe operation of the component. Factors that can reduce power handling and cause damage to a fiber component include, but are not limited to, misalignment during fiber coupling, contamination of the fiber end face, or imperfections in the fiber itself. For further discussion about an optical fiber’s power handling abilities for a specific application, please contact Thorlabs’ Tech Support.

Power Handling Limitations Imposed by Optical Fiber
Click to Enlarge

Undamaged Fiber End
Power Handling Limitations Imposed by Optical Fiber
Click to Enlarge

Damaged Fiber End

Damage at the Air / Glass Interface

There are several potential damage mechanisms that can occur at the air / glass interface. Light is incident on this interface when free-space coupling or when two fibers are mated using optical connectors. High-intensity light can damage the end face leading to reduced power handling and permanent damage to the fiber. For fibers terminated with optical connectors where the connectors are fixed to the fiber ends using epoxy, the heat generated by high-intensity light can burn the epoxy and leave residues on the fiber facet directly in the beam path.

Estimated Optical Power Densities on Air / Glass Interfacea
Type Theoretical Damage Thresholdb Practical Safe Levelc
(Average Power)
~1 MW/cm2 ~250 kW/cm2
10 ns Pulsed
(Peak Power)
~5 GW/cm2 ~1 GW/cm2
  • All values are specified for unterminated (bare), undoped silica fiber and apply for free space coupling into a clean fiber end face.
  • This is an estimated maximum power density that can be incident on a fiber end face without risking damage. Verification of the performance and reliability of fiber components in the system before operating at high power must be done by the user, as it is highly system dependent.
  • This is the estimated safe optical power density that can be incident on a fiber end face without damaging the fiber under most operating conditions.

Damage Mechanisms on the Bare Fiber End Face

Damage mechanisms on a fiber end face can be modeled similarly to bulk optics, and industry-standard damage thresholds for UV Fused Silica substrates can be applied to silica-based fiber. However, unlike bulk optics, the relevant surface areas and beam diameters involved at the air / glass interface of an optical fiber are very small, particularly for coupling into single mode (SM) fiber. therefore, for a given power density, the power incident on the fiber needs to be lower for a smaller beam diameter.

The table to the right lists two thresholds for optical power densities: a theoretical damage threshold and a "practical safe level". In general, the theoretical damage threshold represents the estimated maximum power density that can be incident on the fiber end face without risking damage with very good fiber end face and coupling conditions. The "practical safe level" power density represents minimal risk of fiber damage. Operating a fiber or component beyond the practical safe level is possible, but users must follow the appropriate handling instructions and verify performance at low powers prior to use.

Calculating the Effective Area for Single Mode Fibers
The effective area for single mode (SM) fiber is defined by the mode field diameter (MFD), which is the cross-sectional area through which light propagates in the fiber; this area includes the fiber core and also a portion of the cladding. To achieve good efficiency when coupling into a single mode fiber, the diameter of the input beam must match the MFD of the fiber.

As an example, SM400 single mode fiber has a mode field diameter (MFD) of ~Ø3 µm operating at 400 nm, while the MFD for SMF-28 Ultra single mode fiber operating at 1550 nm is Ø10.5 µm. The effective area for these fibers can be calculated as follows:

SM400 Fiber: Area = Pi x (MFD/2)2 = Pi x (1.5 µm)2 = 7.07 µm= 7.07 x 10-8 cm2

 SMF-28 Ultra Fiber: Area = Pi x (MFD/2)2 = Pi x (5.25 µm)2 = 86.6 µm= 8.66 x 10-7 cm2

To estimate the power level that a fiber facet can handle, the power density is multiplied by the effective area. Please note that this calculation assumes a uniform intensity profile, but most laser beams exhibit a Gaussian-like shape within single mode fiber, resulting in a higher power density at the center of the beam compared to the edges. Therefore, these calculations will slightly overestimate the power corresponding to the damage threshold or the practical safe level. Using the estimated power densities assuming a CW light source, we can determine the corresponding power levels as:

SM400 Fiber: 7.07 x 10-8 cm2 x 1 MW/cm2 = 7.1 x 10-8 MW = 71 mW (Theoretical Damage Threshold)
     7.07 x 10-8 cm2 x 250 kW/cm2 = 1.8 x 10-5 kW = 18 mW (Practical Safe Level)

SMF-28 Ultra Fiber: 8.66 x 10-7 cm2 x 1 MW/cm2 = 8.7 x 10-7 MW = 870 mW (Theoretical Damage Threshold)
           8.66 x 10-7 cm2 x 250 kW/cm2 = 2.1 x 10-4 kW = 210 mW (Practical Safe Level)

Effective Area of Multimode Fibers
The effective area of a multimode (MM) fiber is defined by the core diameter, which is typically far larger than the MFD of an SM fiber. For optimal coupling, Thorlabs recommends focusing a beam to a spot roughly 70 - 80% of the core diameter. The larger effective area of MM fibers lowers the power density on the fiber end face, allowing higher optical powers (typically on the order of kilowatts) to be coupled into multimode fiber without damage.

Damage Mechanisms Related to Ferrule / Connector Termination

Click to Enlarge
Plot showing approximate input power that can be incident on a single mode silica optical fiber with a termination. Each line shows the estimated power level due to a specific damage mechanism. The maximum power handling is limited by the lowest power level from all relevant damage mechanisms (indicated by a solid line).

Fibers terminated with optical connectors have additional power handling considerations. Fiber is typically terminated using epoxy to bond the fiber to a ceramic or steel ferrule. When light is coupled into the fiber through a connector, light that does not enter the core and propagate down the fiber is scattered into the outer layers of the fiber, into the ferrule, and the epoxy used to hold the fiber in the ferrule. If the light is intense enough, it can burn the epoxy, causing it to vaporize and deposit a residue on the face of the connector. This results in localized absorption sites on the fiber end face that reduce coupling efficiency and increase scattering, causing further damage.

For several reasons, epoxy-related damage is dependent on the wavelength. In general, light scatters more strongly at short wavelengths than at longer wavelengths. Misalignment when coupling is also more likely due to the small MFD of short-wavelength SM fiber that also produces more scattered light.

To minimize the risk of burning the epoxy, fiber connectors can be constructed to have an epoxy-free air gap between the optical fiber and ferrule near the fiber end face. Our high-power multimode fiber patch cables use connectors with this design feature.

Determining Power Handling with Multiple Damage Mechanisms

When fiber cables or components have multiple avenues for damage (e.g., fiber patch cables), the maximum power handling is always limited by the lowest damage threshold that is relevant to the fiber component. In general, this represents the highest input power that can be incident on the patch cable end face and not the coupled output power.

As an illustrative example, the graph to the right shows an estimate of the power handling limitations of a single mode fiber patch cable due to damage to the fiber end face and damage via an optical connector. The total input power handling of a terminated fiber at a given wavelength is limited by the lower of the two limitations at any given wavelength (indicated by the solid lines). A single mode fiber operating at around 488 nm is primarily limited by damage to the fiber end face (blue solid line), but fibers operating at 1550 nm are limited by damage to the optical connector (red solid line).

In the case of a multimode fiber, the effective mode area is defined by the core diameter, which is larger than the effective mode area for SM fiber. This results in a lower power density on the fiber end face and allows higher optical powers (on the order of kilowatts) to be coupled into the fiber without damage (not shown in graph). However, the damage limit of the ferrule / connector termination remains unchanged and as a result, the maximum power handling for a multimode fiber is limited by the ferrule and connector termination. 

Please note that these are rough estimates of power levels where damage is very unlikely with proper handling and alignment procedures. It is worth noting that optical fibers are frequently used at power levels above those described here. However, these applications typically require expert users and testing at lower powers first to minimize risk of damage. Even still, optical fiber components should be considered a consumable lab supply if used at high power levels.

Intrinsic Damage Threshold

In addition to damage mechanisms at the air / glass interface, optical fibers also display power handling limitations due to damage mechanisms within the optical fiber itself. These limitations will affect all fiber components as they are intrinsic to the fiber itself. Two categories of damage within the fiber are damage from bend losses and damage from photodarkening. 

Bend Losses
Bend losses occur when a fiber is bent to a point where light traveling in the core is incident on the core/cladding interface at an angle higher than the critical angle, making total internal reflection impossible. Under these circumstances, light escapes the fiber, often in a localized area. The light escaping the fiber typically has a high power density, which burns the fiber coating as well as any surrounding furcation tubing.

A special category of optical fiber, called double-clad fiber, can reduce the risk of bend-loss damage by allowing the fiber’s cladding (2nd layer) to also function as a waveguide in addition to the core. By making the critical angle of the cladding/coating interface higher than the critical angle of the core/clad interface, light that escapes the core is loosely confined within the cladding. It will then leak out over a distance of centimeters or meters instead of at one localized spot within the fiber, minimizing the risk of damage. Thorlabs manufactures and sells 0.22 NA double-clad multimode fiber, which boasts very high, megawatt range power handling.

A second damage mechanism, called photodarkening or solarization, can occur in fibers used with ultraviolet or short-wavelength visible light, particularly those with germanium-doped cores. Fibers used at these wavelengths will experience increased attenuation over time. The mechanism that causes photodarkening is largely unknown, but several fiber designs have been developed to mitigate it. For example, fibers with a very low hydroxyl ion (OH) content have been found to resist photodarkening and using other dopants, such as fluorine, can also reduce photodarkening.

Even with the above strategies in place, all fibers eventually experience photodarkening when used with UV or short-wavelength light, and thus, fibers used at these wavelengths should be considered consumables.

Preparation and Handling of Optical Fibers

General Cleaning and Operation Guidelines
These general cleaning and operation guidelines are recommended for all fiber optic products. Users should still follow specific guidelines for an individual product as outlined in the support documentation or manual. Damage threshold calculations only apply when all appropriate cleaning and handling procedures are followed.

  1. All light sources should be turned off prior to installing or integrating optical fibers (terminated or bare). This ensures that focused beams of light are not incident on fragile parts of the connector or fiber, which can possibly cause damage.

  2. The power-handling capability of an optical fiber is directly linked to the quality of the fiber/connector end face. Always inspect the fiber end prior to connecting the fiber to an optical system. The fiber end face should be clean and clear of dirt and other contaminants that can cause scattering of coupled light. Bare fiber should be cleaved prior to use and users should inspect the fiber end to ensure a good quality cleave is achieved.

  3. If an optical fiber is to be spliced into the optical system, users should first verify that the splice is of good quality at a low optical power prior to high-power use. Poor splice quality may increase light scattering at the splice interface, which can be a source of fiber damage.

  4. Users should use low power when aligning the system and optimizing coupling; this minimizes exposure of other parts of the fiber (other than the core) to light. Damage from scattered light can occur if a high power beam is focused on the cladding, coating, or connector.

Tips for Using Fiber at Higher Optical Power
Optical fibers and fiber components should generally be operated within safe power level limits, but under ideal conditions (very good optical alignment and very clean optical end faces), the power handling of a fiber component may be increased. Users must verify the performance and stability of a fiber component within their system prior to increasing input or output power and follow all necessary safety and operation instructions. The tips below are useful suggestions when considering increasing optical power in an optical fiber or component.

  1. Splicing a fiber component into a system using a fiber splicer can increase power handling as it minimizes possibility of air/fiber interface damage. Users should follow all appropriate guidelines to prepare and make a high-quality fiber splice. Poor splices can lead to scattering or regions of highly localized heat at the splice interface that can damage the fiber.

  2. After connecting the fiber or component, the system should be tested and aligned using a light source at low power. The system power can be ramped up slowly to the desired output power while periodically verifying all components are properly aligned and that coupling efficiency is not changing with respect to optical launch power.

  3. Bend losses that result from sharply bending a fiber can cause light to leak from the fiber in the stressed area. When operating at high power, the localized heating that can occur when a large amount of light escapes a small localized area (the stressed region) can damage the fiber. Avoid disturbing or accidently bending fibers during operation to minimize bend losses.

  4. Users should always choose the appropriate optical fiber for a given application. For example, large-mode-area fibers are a good alternative to standard single mode fibers in high-power applications as they provide good beam quality with a larger MFD, decreasing the power density on the air/fiber interface.

  5. Step-index silica single mode fibers are normally not used for ultraviolet light or high-peak-power pulsed applications due to the high spatial power densities associated with these applications.

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1310 / 1550 nm 1x16 PM Fiber Optic Splitters

Item # Info Center
Bandwidth Coupling Ratioa
(Click for Plot)
Uniformityb Insertion
Fiberc,d Terminatione
TPS1315HF info 1310/1550 nm ±40 nm 6.25%
(Each Output Port)
≥18.0 dB (Typ.) ≤0.7 dB ≤14.5 dB
(Each Output Port)
Equivalent to
PM 15-U25D
TPS1315HA info FC/APC
  • Specified at each center wavelength for a linearly polarized slow-axis launch into the white input port without connectors and at room temperature.
  • Specified at each center wavelength for a linearly polarized slow-axis launch into the white input port with connectors and at room temperature. See the PER Measurement tab for more information on how extinction ratio is measured.
  • This splitter can be used with patch cables that incorporate PM1550-XP fiber (click for FC/PC and FC/APC versions).
  • Other fiber types may be available upon request. Please contact Tech Support with inquiries.
  • The connector keys are aligned to the slow axis of the fiber.
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
TPS1315HF Support Documentation
TPS1315HF1x16 PM Splitter, 1310 / 1550 ± 40 nm, 6.25% Split, ≥18.0 dB PER, FC/PC Connectors
TPS1315HA Support Documentation
TPS1315HA1x16 PM Splitter, 1310 / 1550 ± 40 nm, 6.25% Split, ≥18.0 dB PER, FC/APC Connectors
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Mounting Base

WDM mounted on FCQB Base
Click to Enlarge

The FCQB base is designed for the red package used to house Thorlabs' WDMs, 1x4 couplers, and splitters, as shown above.
  • Mounting Base for:
    • 3-Wavelength WDMs
    • 1x4 Couplers
    • 1x4, 1x8, or 1x16 Splitters
  • Four M2 Taps for Mounting Fiber Optic Component Housing
  • 2.25" Long Clearance Slots Accepts 1/4"-20 (M6) Screws
  • Four M2 Mounting Screws Included

The FCQB mounting base provides two 2.25" long clearance slots for 1/4" (M6) cap screws to secure the base to an optical table or other tapped surface. The two clearance slots are located 4" (101.6 mm) apart at opposite edges of the mounting base. Four M2 taps between the clearance slots are positioned to align with the through holes in Thorlabs' 3-Wavelength Wavelength Division Multiplexers (WDMs), 1x4 SM Couplers, 1x4 PM Splitters1x8 SM Splitters, 1x8 PM Splitters1x16 SM Splitters, or 1x16 PM Splitters. Four M2 screws are included.

Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
FCQB Support Documentation
FCQBMounting Base for Fiber Coupling Components