IR Fiber Optic Isolators with SM Fiber (1290 - 2010 nm)


  • Center Wavelengths at 1310, 1550, or 2000 nm
  • Minimum Isolation from 29 dB to 45 dB
  • Terminated or Unterminated SM Fiber
  • OEM and Build-to-Order Fiber Isolators Available

IO-H-1310

1310 nm, No Connectors

IO-K-2000

2000 nm, No Connectors

IO-H-1550APC

1550 nm, FC/APC Connectors

FC/APC

FC/PC

Related Items


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Selection Guide for Isolators
(Click Here for Our Full Selection)
Fiber Isolators
Spectral Region Wavelength Range Fiber Type
Visible 650 - 670 nm SM
NIR 770 - 1060 nm SM
PM
Nd:YAG 1064 nm SM
PM
IR 1290 - 2010 nm SM
PM
Fiber Isolators for Broadband SLDsa
Free-Space Isolators
Custom Isolators
  • Superluminescent Diodes

Custom Isolators

  • Customizable Wavelength, Aperture, Max Power, Housing, Polarizers, and Operating Temperature
  • Pricing Similar to Stock Units
  • Wide Range of OEM Capabilities
  • Please Contact Tech Support or See Our Custom Isolators Page

Features

  • Minimize Feedback into Optical Systems
  • Operating Wavelength Ranges of 1290 - 1330 nm, 1530 - 1570 nm, 1535 - 1565 nm, or 1990 - 2010 nm
  • 0.8 m to 1 m of Fiber Built into Each Side of the Isolator
  • Available with 2.0 mm Narrow Key FC/PC or FC/APC Connectors or Unterminated
  • Designed for CW Applications
  • Each Unit is Individually Tested
  • Custom Isolators Available (See the Custom Isolators tab)

Fiber isolators protect light sources from back reflections and signals that can cause intensity noise and optical damage. Optical isolators, also known as Faraday isolators, are magneto-optic devices that preferentially transmit light in the forward direction while absorbing or displacing light propagating in the reverse direction (see the schematic below). Please see the Isolator Tutorial tab for an explanation of the operating principles of a Faraday isolator.

Light Propagation Through a Polarization-Independent Isolator
Click for Details

This schematic shows a single-stage, polarization-independent isolator. Light is deflected away from the input path and stopped by the housing. See the Isolator Tutorial tab for more details and for a comparison to dual-stage isolators. Click the schematic to show polarization states.

The IOT-H-1550A dual-stage isolator includes an additional Faraday rotator, half-wave plate, and birefringent beam displacer compared to a single-stage isolator in order to achieve greater isolation.

Thorlabs' polarization-independent IR isolators, sold on this page, are compatible with single mode (SM) fibers. In contrast, our polarization-dependent IR isolators are designed to connect to polarization-maintaining (PM) fibers. Our high-power units are built using a specialized fiber end face process that increases the maximum power. There is 0.8 m to 1 m of fiber built into each side of the isolator, and an arrow on the body indicates the transmission direction. In addition, each unit is tested before shipment to ensure compliance with our specifications and a complete test report comes with every serialized part.

Thorlabs also manufactures free-space isolators and fiber isolators designed for the infrared range. Please use the Selection Guide table above for more information. If you do not see an isolator that suits your application, please refer to the Custom Isolators tab for information on our build-to-order options, or contact Tech Support.

Optical Isolator Tutorial

Function
An optical isolator is a passive magneto-optic device that only allows light to travel in one direction. Isolators are used to protect a source from back reflections or signals that may occur after the isolator. Back reflections can damage a laser source or cause it to mode hop, amplitude modulate, or frequency shift. In high-power applications, back reflections can cause instabilities and power spikes.

An isolator's function is based on the Faraday Effect. In 1842, Michael Faraday discovered that the plane of polarized light rotates while transmitting through glass (or other materials) that is exposed to a magnetic field. The direction of rotation is dependent on the direction of the magnetic field and not on the direction of light propagation; thus, the rotation is non-reciprocal. The amount of rotation β equals V x B x d, where V, B, and d are as defined below.

 

Faraday Effect in an Isolator Drawing
Click to Enlarge

Figure 1. Faraday Rotator's Effect on Linearly Polarized Light

Faraday Rotation

β = V x B x d

V: the Verdet Constant, a property of the optical material, in radians/T • m.

B: the magnetic flux density in teslas.

d: the path length through the optical material in meters.

An optical isolator consists of an input polarizer, a Faraday rotator with magnet, and an output polarizer. The input polarizer works as a filter to allow only linearly polarized light into the Faraday rotator. The Faraday element rotates the input light's polarization by 45°, after which it exits through another linear polarizer. The output light is now rotated by 45° with respect to the input signal. In the reverse direction, the Faraday rotator continues to rotate the light's polarization in the same direction that it did in the forward direction so that the polarization of the light is now rotated 90° with respect to the input signal. This light's polarization is now perpendicular to the transmission axis of the input polarizer, and as a result, the energy is either reflected or absorbed depending on the type of polarizer.

 

Drawing of Light Propagation Through an Isolator
Click to Enlarge

Figure 2. A single-stage, polarization-dependent isolator. Light propagating in the reverse direction is rejected by the input polarizer.

Polarization-Dependent Isolators

The Forward Mode
In this example, we will assume that the input polarizer's axis is vertical (0° in Figure 2). Laser light, either polarized or unpolarized, enters the input polarizer and becomes vertically polarized. The Faraday rotator will rotate the plane of polarization (POP) by 45° in the positive direction. Finally, the light exits through the output polarizer which has its axis at 45°. Therefore, the light leaves the isolator with a POP of 45°.

In a dual-stage isolator, the light exiting the output polarizer is sent through a second Faraday rotator followed by an additional polarizer in order to achieve greater isolation than a single-stage isolator.

The Reverse Mode
Light traveling backwards through the isolator will first enter the output polarizer, which polarizes the light at 45° with respect to the input polarizer. It then passes through the Faraday rotator rod, and the POP is rotated another 45° in the positive direction. This results in a net rotation of 90° with respect to the input polarizer, and thus, the POP is now perpendicular to the transmission axis of the input polarizer. Hence, the light will either be reflected or absorbed.

 

Light Propagation Through a Polarization-Independent IsolatorClick for Details
Figure 3. A single-stage, polarization-independent isolator. Light is deflected away from the input path and stopped by the housing.

Polarization-Independent Fiber Isolators

The Forward Mode
In a polarization independent fiber isolator, the incoming light is split into two branches by a birefringent crystal (see Figure 3). A Faraday rotator and a half-wave plate rotate the polarization of each branch before they encounter a second birefringent crystal aligned to recombine the two beams.

In a dual-stage isolator, the light then travels through an additional Faraday rotator, half-wave plate, and birefringent beam displacer before reaching the output collimating lens. This achieves greater isolation than the single-stage design.

The Reverse Mode
Back-reflected light will encounter the second birefringent crystal and be split into two beams with their polarizations aligned with the forward mode light. The faraday rotator is a non-reciprocal rotator, so it will cancel out the rotation introduced by the half wave plate for the reverse mode light. When the light encounters the input birefringent beam displacer, it will be deflected away from the collimating lens and into the walls of the isolator housing, preventing the reverse mode from entering the input fiber.

 

General Information

Damage Threshold
With 25 years of experience and 5 U.S. patents, our isolators typically have higher transmission and isolation than other isolators, and are smaller than other units of equivalent aperture. For visible to YAG laser Isolators, Thorlabs' Faraday Rotator crystal of choice is TGG (terbium-gallium-garnet), which is unsurpassed in terms of optical quality, Verdet constant, and resistance to high laser power. Thorlabs' TGG Isolator rods have been damage tested to 22.5 J/cm2 at 1064 nm in 15 ns pulses (1.5 GW/cm2), and to 20 kW/cm2 CW. However, Thorlabs does not bear responsibility for laser power damage that is attributed to hot spots in the beam.

Autocorrelation Measurement of Isolator IO-5-780-HP
Click to Enlarge

Figure 4. Pulse Duration Measurements Before and After an IO-5-780-HP Isolator

Magnet
The magnet is a major factor in determining the size and performance of an isolator. The ultimate size of the magnet is not simply determined by magnetic field strength but is also influenced by the mechanical design. Many Thorlabs magnets are not simple one piece magnets but are complex assemblies. Thorlabs' modeling systems allow optimization of the many parameters that affect size, optical path length, total rotation, and field uniformity. Thorlabs' US Patent 4,856,878 describes one such design that is used in several of the larger aperture isolators for YAG lasers. Thorlabs emphasizes that a powerful magnetic field exists around these Isolators, and thus, steel or magnetic objects should not be brought closer than 5 cm.

Temperature
The magnets and the Faraday rotator materials both exhibit a temperature dependence. Both the magnetic field strength and the Verdet Constant decrease with increased temperature. For operation greater than ±10 °C beyond room temperature, please contact Technical Support.

Pulse Dispersion
Pulse broadening occurs anytime a pulse propagates through a material with an index of refraction greater than 1. This dispersion increases inversely with the pulse width and therefore can become significant in ultrafast lasers.

τ: Pulse Width Before Isolator

τ(z): Pulse Width After Isolator

Example:
τ = 197 fs results in τ(z) = 306 fs (pictured to the right)
τ = 120 fs results in τ(z) = 186 fs

Optical Isolator in FiberBench Mount
Click to Enlarge

Custom Isolator Example
Custom Adjustable Narrowband Isolator with Different Input and Output Polarizers Optimized for 650 nm Wavelength and 40 °C Temperature.

OEM Application Services

  • Direct Integration to Laser Head Assemblies
  • Combination Isolator and Fiber Coupling Units
  • Minimum Footprint Packages
  • Filter Integration
  • Active Temperature Control and Monitoring
  • Feedback Monitoring
  • Environmental Qualification
  • Private Labeling
  • ITAR-Compliant Assembly

OEM and Non-Standard Isolators

In an effort to provide the best possible service to our customers, Thorlabs has made a commitment to ship our most popular free-space and fiber isolator models from stock. We currently offer same-day shipping on more than 90 isolator models. In addition to these stock models, non-stock isolators with differing aperture sizes, wavelength ranges, package sizes, and polarizers are available. In addition, we can create isolators tuned for specific operating temperatures and isolators that incorporate thermistors with heating or cooling elements for active temperature control and monitoring. These generally have the same price as a similar stock unit. If you would like a quote on a non-stock isolator, please fill out the form below and a member of our staff will be in contact with you.

Thorlabs has many years of experience working with OEM, government, and research customers, allowing us to tailor your isolator to specific design requirements. In addition to customizing our isolators (see the OEM Application Services list to the right), we also offer various application services.

 

Parameter Range
Wavelength Range From 365 - 4550 nma
Aperture Sizes  Up to Ø15 mm
Polarization Dependence Dependent or Independent
Max Powerb Up to 2 GW/cm²
Isolation Up to 60 dB (Tandem Units)
Operating Temperature 10 - 70 °C
  • Custom Faraday rotators, for use in the 365 to 5000 nm range, are also available.
  • The maximum power specification represents the maximum power for the combined forward and reverse directions. Therefore, the sum of the powers in the forward and reverse directions cannot exceed the maximum power specification.

Free-Space Isolators

We are able to provide a wide range of flexibility in manufacturing non-stock, free-space isolators. Almost any selection of specifications from our standard product line can be combined to suit a particular need. The table to the right shows the range of specifications that we can meet.

We offer isolators suitable for both narrowband and broadband applications. The size of the housing is very dependent on the desired maximum power and aperture size, so please include a note in the quote form below if you have special requirements.

 

Faraday Rotators

We offer Faraday rotators center wavelengths from 532 nm to 1550 nm. These are the same components used to make our isolators and rotate the polarization of incoming light by 45°. Please contact Tech Support if you require a Faraday rotator with a rotation angle or center wavelength outside of the aforementioned specifications.

 

Parameter Range
Wavelength Range From 633 - 2050 nma
Polarization Dependence Dependent or Independent
Max Powerb (Fiber to Free-Space) 30 W
Max Powerb (Fiber to Fiber) 20 W
Operating Temperature 10 - 70 °C
  • For wavelengths shorter than 633 nm, we recommend using our free-space isolators in conjunction with our modular FiberBench accessories. Please contact Technical Support for more information.
  • The maximum power specification represents the maximum power for the combined forward and reverse directions. Therefore, the sum of the powers in the forward and reverse directions cannot exceed the maximum power specification.

Fiber Isolators

Thorlabs is uniquely positioned to draw on experience in classical optics, fiber coupling, and isolators to provide flexible designs for a wide range of fiber optic specifications. Current design efforts are focused on increasing the Maximum power of our fiber isolators at and near the 1064 nm wavelength. We offer models with integrated ASE filters and taps. The table to the right highlights the range of specifications that we can meet.

The fiber used is often the limiting factor in determining the Maximum power the isolator can handle. We have experience working with single mode (SM) and polarization-maintaining fibers (PM); single-, double- and triple-clad fibers; and specialty fibers like 10-to-30 µm LMA fibers and PM LMA fibers. For more information about the fiber options available with our custom isolators, please see the expandable tables below.

In the spectral region below 633 nm, we recommend mounting one of our free-space isolators in a FiberBench system. A FiberBench system consists of pre-designed modules that make it easy to use free-space optical elements with a fiber optic system while maintaining excellent coupling efficiency. Upon request, we can provide select stock isolators in an optic mount with twin steel dowel pins for our FiberBench systems, as shown to the left.

We are also in the process of extending our fiber isolator capabilities down into the visible region. For more information, please contact Technical Support.

Custom Fiber Isolator

Custom Free-Space Isolator for Wavelengths Below 633 nm

Optical Isolator in FiberBench Mount
Click to Enlarge

Twin Steel Pins Insert into FiberBench
Optical Isolator in FiberBench Mount
Click to Enlarge

Mounted Isolator
Polarization Independent Fiber
Polarization Maintaining Fiber

 

Make to Order Options

The expandable tables below provide information on some common isolator and rotator specials we have manufactured in the past. We keep the majority of the components for these custom isolators in stock to ensure quick builds, so these specials are available with an average lead time of only 2-4 weeks.  Please use the Non-Stock Isolator Worksheet below for a quote.

Adjustable Narrowband Isolators
Faraday Rotators
Fixed Narrowband Isolators
Fixed Broadband Isolators

 

Custom Request Form

Request a custom isolator quote using the form below or by contacting us for more information at (973) 300-3000.

Non-Stock Isolator Worksheet:
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Free-Space Input
Wavelength or Wavelength Range (nm):
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Max 1/e2 Beam Diameter (mm)*:
Isolation (dB):
% Transmission:
Notes:
Fiber Input
Wavelength or Wavelength Range (nm):
Power (W):
Polarization Sensitivity:  Dependent   |     Independent
Isolation (dB):
% Transmission:
Fiber:
Fiber Connector:   FC/PC   |     FC/APC   |     Other
Output:   Fiber   |     Free-Space
Notes:

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Thorlabs Lab Fact: Isolation & Transmission Properties of IO-F and IO-H Fiber Isolators

Light Propagation Through a Polarization-Independent Isolator
Click for Details

Figure 1: IO-H Series Polarization-Independent Isolator Schematic
Light Propagation Through a Polarization-Independent Isolator
Click for Details

Figure 2: IO-F Series Polarization-Independent Isolator Schematic

We present laboratory measurements of the isolation and transmission properties of our IO-H and IO-F series of fiber-coupled optical isolators. Generally, an isolator uses a Faraday rotator in conjunction with a half-wave plate, between two beam-displacement polarizers, to provide isolation from back reflections. While both series provide excellent isolation from optical feedback, they do so through different geometries. As a result, these two series offer different optimized performance specifications. The IO-H series (see Figure 1) is optimized for performance at a specific wavelength (e.g., 1550 nm for the IO-H-1550APC). The IO-F series (see Figure 2), however, is designed as a more versatile platform and offers customized performance over various wavelength bands. These bands are defined by the choice of half-wave plate and collimating lenses.

For this experiment the laser source was Thorlabs' TLK-L1550R Tunable Laser Kit, swept through 1505 – 1593 nm. The fiber-coupled laser beam was fed through a 99:1 fiber coupler, allowing 1% of the TLK's power to be sent to an OSA203 Optical Spectrum Analyzer to monitor and record the TLK's center wavelength at each data point. The remaining power was split in half by a 50:50 fiber coupler, which created two paths. One path was designated as a reference path and was fed directly into an integrating sphere; the other path was designated as the test path. The isolator was placed in the test path and then attached to an integrating sphere. For this experiment, the IO-H-1550APC and IO-F-1550APC isolators were tested. Either the transmission (when the isolator was integrated into the test path in the forward direction) or isolation (when the isolator was integrated into the path in the reverse direction) was measured. Since both reference and test path data were taken simultaneously, the exact transmission or isolation could be extracted along with peak wavelength data from the OSA.

Lab Facts Complete Summary

Figures 3 and 4 summarize the measured results for the IO-H series isolator and compare those results to those reported on our website. Figure 3 shows that for the two tested IO-H-1550APC isolators, the real transmission is a few percentage points higher than the specified value on the website (i.e., the performance exceeds the specification). It also shows a slight etalon effect caused by the front window of the OSA detector. Figure 4 details the isolation for the same set of isolators and shows a slight increase in isolation and similar bandwidth as the web specifications. Figures 5 and 6 summarize the measured results for the IO-F series isolator. The two tested isolators show a >5% increase over the specified transmission, and an additional etalon effect from the internal half-wave plate is observed as well. Figure 6 shows that the measured isolators again have higher isolation than specified but also have a variance in the peak isolated wavelength. For details on the experimental setup employed and the results summarized here, please click here.

Polarization through prism
Click to Enlarge

Figure 3: IO-H Series Transmission
Stress Induced Shifts
Click to Enlarge

Figure 4: IO-H Series Isolation
Stress Induced Shifts
Click to Enlarge

Figure 5: IO-F Series Transmission
Stress Induced Shifts
Click to Enlarge

Figure 6: IO-F Series Isolation

Posted Comments:
yunseokjun  (posted 2019-01-07 01:05:57.497)
Hello, I have a question about one of the polarization indepedent isolators : 'IO-H Fiber Isolators'. According to the experimental results posted on the website, It says this we can change 'the center wavelength of isolation peak' by rotating the half waveplate. I wonder if this is because the faraday rotator has wavelength dependency by which rotating angle of the half waveplate should be changed to make the 90 degree in total. If this is the case, I also wonder if the phase retardation in half waveplate is not changed which is supposed to introduce pi phase shift.
nbayconich  (posted 2019-02-07 10:42:13.0)
Thank you for contacting Thorlabs. Yes the amount of rotation the faraday rotator provides will be dependent on the source wavelength, therefore it is possible to compensate for this slight change in rotation by rotating the half waveplates used in these fiber isolators. Please note that the retardance induced by the half waveplates is also dependent on the operating wavelength meaning that as the source strays far from the design wavelength of the HWP, the half waveplate will induce some ellipticity in the source. This means that each isolator can only be used across such a broad wavelength range before the isolation & transmission becomes poor. The Isolation is typically more sensitive to a shift in the design wavelength of the system than transmission but you can achieve a relatively high isolation peak within a narrow bandwidth.
David.ljtao  (posted 2017-09-21 17:31:53.44)
Hello, I have two questions about your 1550nm polarization independent isolator with 300cw power. 1. Can your fiber isolator with FC/APC connector withstand 75W pulse peak power and 20~35mw average power? 2. Can you make a special isolator with 3dB insertion loss in forward and backward direction? The insertion loss can be induced only by rotating output wedge. And it must have the same inner structure with standard isolator.
tfrisch  (posted 2017-11-16 02:33:30.0)
Hello, thank you for contacting Thorlabs. While we do not currently have a source comparable to your that we could use in testing, I will contact you about sending a sample for your to test. I also have some questions on the insertion loss you've specified.

The following selection guide contains all of Thorlabs' Fiber Optical Isolators. Click the colored bars below to to see specifications and options for each wavelength range and isolator type. Please note that Thorlabs also offers free space optical isolators and custom optical isolators.

Optical_Isolator 940 nm PM
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1310 nm Polarization-Independent Isolators with SM Fiber

IO-H-1310 Mechanical Drawing
IO-H-1310x Simplified Mechanical Drawing
Click Image to Enlarge IO-H-1310
Item # IO-H-1310
IO-H-1310APC
IO-H-1310FC
Polarization Independent
Fiber Type SM
Isolator Design Single Stage
Center Wavelength 1310 nm
Operating Range 1290 - 1330 nm
Max Powera,b
(Without Connectors)
≤300 mW (CW)c
Isolationd 29 dB (Min)
Performance Graph
(Click for Plot)
Click to View
Insertion Loss (Without Connectors) 0.70 dB (Max)
Polarization Dependent Loss (PDL) ≤0.15 dB
Return Loss (Input/Output) ≥55/50 dB
Fiber SMF-28e+
  • The maximum power specification represents the maximum power for the combined forward and reverse directions. Therefore, the sum of the powers in the forward and reverse directions cannot exceed the maximum power specification.
  • The maximum power is quoted for the unterminated isolator and will be reduced by the addition of connectors.
  • This isolator is not recommended for high-power pulsed applications.
  • Isolation at Center Wavelength
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
IO-H-1310 Support Documentation
IO-H-1310Fiber Isolator, 1310 nm, SM, 300 mW, No Connectors
$198.38
Today
IO-H-1310APC Support Documentation
IO-H-1310APCFiber Isolator, 1310 nm, SM, FC/APC
$248.28
Today
IO-H-1310FC Support Documentation
IO-H-1310FCFiber Isolator, 1310 nm, SM, FC/PC
$223.34
Today
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1550 nm Polarization-Independent Isolators with SM Fiber

Click Image to Enlarge IO-H-1550 IOT-H-1550A IO-F-1550 IO-K-1550
Item #a IO-H-1550
IO-H-1550APC
IO-H-1550FC
IOT-H-1550A IO-F-1550
IO-F-1550APC
IO-K-1550
Polarization Independent Independent Independent Independent
Fiber Type SM SM SM SM
Isolator Design Single Stage Dual Stage Single Stage Single Stage
Center Wavelength 1550 nm 1550 nm 1550 nm 1550 nm
Operating Range 1530 - 1570 nm 1535 - 1565 nm 1530 - 1570 nm 1530 - 1570 nm
Max Powerb,c
(Without Connectors)
300 mW (CW)d 300 mW (CW)d 5 W (CW)d 10 W (CW)e
Isolationf 29 dB (Min) 45 dB (Min)
55 dB (Peak)
35 dB (Min)
36 dB (Typ.)
35 dB (Min)
36 dB (Typ.)
Performance Graph
(Click for Plot)
Click to View Click to View Click to View Click to View
Insertion Loss (Without Connectors) 0.7 dB (Max) ≤0.85 dB 0.6 dB (Typ.)
0.8 dB (Max)
0.9 dB (Typ.)
1.2 dB (Max)
Polarization Dependent Loss (PDL) ≤0.15 dB <0.10 dB ≤0.20 dB ≤0.25 dB
Return Loss ≥55/50 dB
(Input/Output)
>55/50 dB
(Input/Output)
≥50 dB ≥50 dB
Fiber SMF-28e+ SMF-28 Ultra SMF-28e+ SMF-28e+
  • Alternative connector options are available by contacting Tech Support.
  • The maximum power specification represents the maximum power for the combined forward and reverse directions. Therefore, the sum of the powers in the forward and reverse directions cannot exceed the maximum power specification.
  • The maximum power is quoted for the unterminated isolator and will be reduced by the addition of connectors.
  • This isolator is not recommended for high-power pulsed applications.
  • Ideal for High-Power CW or Pulsed Applications
  • Isolation at Center Wavelength
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
IO-H-1550 Support Documentation
IO-H-1550Fiber Isolator, 1550 nm, SM, 300 mW, No Connectors
$198.38
Today
IO-H-1550APC Support Documentation
IO-H-1550APCFiber Isolator, 1550 nm, SM, FC/APC
$248.28
Today
IO-H-1550FC Support Documentation
IO-H-1550FCFiber Isolator, 1550 nm, SM, FC/PC
$223.34
Today
IOT-H-1550A Support Documentation
IOT-H-1550ADual-Stage Fiber Isolator, 1550 nm, SM, FC/APC
$281.03
Today
IO-F-1550 Support Documentation
IO-F-1550Fiber Isolator, 1550 nm, SM, 5 W, No Connectors
$1,531.23
Today
IO-F-1550APC Support Documentation
IO-F-1550APCFiber Isolator, 1550 nm, SM, FC/APC
$1,579.94
Today
IO-K-1550 Support Documentation
IO-K-1550Fiber Isolator, 1550 nm, SM, 10 W, No Connectors
$2,381.77
Today
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2000 nm Polarization-Independent Isolators with SM Fiber

Click Image to Enlarge IO-F-2000 IO-K-2000
Item #a IO-F-2000 IO-K-2000
Polarization Independent Independent
Fiber Type SM SM
Isolator Design Single Stage Single Stage
Center Wavelength 2000 nm 2000 nm
Operating Range 1990 - 2010 nm 1990 - 2010 nm
Max Powerb,c
(Without Connectors)
3 W (CW)d 10 W (CW)e
Isolationf 28 dB (Min)
30 dB (Typ.)
28 dB (Min)
30 dB (Typ.)
Performance Graph
(Click for Plot)
Click to View Click to View
Insertion Loss 0.9 (Typ.)
1.0 dB (Max)
1.6 dB (Typ.)
1.6 dB (Max)
Polarization Dependent Loss (PDL) ≤0.20 dB ≤0.20 dB
Return Loss ≥50 dB ≥50 dB
Fiber SM2000 SM2000
  • Alternative connector options are available by contacting Tech Support.
  • The maximum power specification represents the maximum power for the combined forward and reverse directions. Therefore, the sum of the powers in the forward and reverse directions cannot exceed the maximum power specification.
  • The maximum power is quoted for the unterminated isolator and will be reduced by the addition of connectors.
  • This isolator is not recommended for high-power pulsed applications.
  • Ideal for High-Power CW or Pulsed Applications
  • Isolation at Center Wavelength
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
IO-F-2000 Support Documentation
IO-F-2000Customer Inspired! Fiber Isolator, 2000 nm, SM, 3 W, No Connectors
$3,049.40
Today
IO-K-2000 Support Documentation
IO-K-2000Customer Inspired! Fiber Isolator, 2000 nm, SM, 10 W, No Connectors
$3,656.42
Today