"; _cf_contextpath=""; _cf_ajaxscriptsrc="/cfthorscripts/ajax"; _cf_jsonprefix='//'; _cf_websocket_port=8578; _cf_flash_policy_port=1244; _cf_clientid='C004051E7FCF7CDACB3A38258DC943AC';/* ]]> */
Nd:YAG Free-Space Isolators (1020 - 1100 nm)
Removed from Saddle
Click to Enlarge
Our Adjustable Narrowband Isolators can be tuned to maximize the peak isolation for any wavelength within a narrow spectral range (shaded in this graph). See the Wavelength Tuning tab for more details. This plot shows data for the IO-3-1064-HP. Graphs showing the isolation and transmission for each isolator tuned to the center wavelength are provided on the Graphs tab.
Click to Enlarge
Isolator in Custom Package for FiberBench Systems
Click to Enlarge
IO-3-1064-HP Isolator Shown in Included SM1RC Saddle and Mounted to an Optical Table Using a BA1 Base and SD1 1/4"-20 to 8-32 Counterbore Adapter
Thorlabs is pleased to stock a variety of free-space optical isolators designed for use with Nd:YAG lasers (i.e., output at the fundamental wavelength of 1064 nm). Optical isolators, also known as Faraday isolators, are magneto-optic devices that preferentially transmit light along a single direction, shielding upstream optics from back reflections. Back reflections can create a number of instabilities in light sources, including intensity noise, frequency shifts, mode hopping, and loss of mode lock. In addition, intense back-reflected light can permanently damage optics. Please see the Isolator Tutorial tab for an explanation of the operating principles of a Faraday isolator.
For applications at Nd:YAG wavelengths, we offer four types of isolators. The first type, Fixed Narrowband Isolators, contains fixed, factory-aligned optics, for which peak isolation and peak transmission occurs at a pre-defined center wavelength. Any deviation from this wavelength will cause a dip in isolation and transmission. The second type, Adjustable Narrowband Isolators, offers the user the ability to adjust the alignment of the input and output polarizers, allowing tuning of the center wavelength within a 45 nm range. The third type, Tandem Narrowband Isolators, consists of two Faraday rotators in series, boosting the isolation to at least 55 dB at the expense of lower transmission. The fourth type, Polarization-Independent Isolators, achieves the same performance characteristics regardless of the input polarization, greatly simplifying alignment. Please see the Isolator Types tab for additional design details and representative graphs of the wavelength-dependent isolation.
The housing of each isolator shown here, except for the IO-D-1064-VLP, is marked with an arrow that indicates the direction of forward propagation. The input and output apertures of the IO-D-1064-VLP are indicated by the black and gold coloring of the cylinder, respectively. All isolators shown here (including the IO-D-1064-VLP) have engravings that indicate the alignment of the input and output polarizers.
Thorlabs also manufactures free-space and fiber-optic isolators for wavelengths from the UV to the infrared (see the Selection Guide table to the left). As indicated in the tables below and pictured to the right, many of our stock isolators can also be provided in a mount designed for our FiberBench systems. If Thorlabs does not stock an isolator suited for your application, please refer to the Custom Isolators tab for information on our build-to-order options, or contact Tech Support. Thorlabs' in-house manufacturing service has over 25 years of experience and can deliver a free-space isolator tuned to your center wavelength from 244 nm to 4.55 µm.
Blue shaded regions on a graph represent the center wavelength tuning range of the isolator (see the Wavelength Tuning tab for more information). With these isolators, the isolation and transmission curves will shift as the center wavelength shifts. If the graph is not blue shaded, then the isolator is non-tunable. Please note that these curves were made from theoretical data and that isolation and transmission will vary from unit to unit.
The IO-3-1064-VHP, IO-5-1064-VHP, and IO-10-1064-VHP are Fixed Narrowband Isolators for use at 1064 nm. For operation centered at 1053 nm, please contact us prior to ordering.
Tuning an Adjustable Narrowband Isolator
Click to Enlarge
When the isolator is tuned away from its design wavelength, the maximum transmission falls because the output polarizer's transmission axis is not parallel to the polarization direction of the output light. This plot shows transmission data for the IO-3-1064-HP. Graphs showing the transmission when each isolator is tuned to the center wavelength are provided on the Graphs tab.
Click to Enlarge
Our Adjustable Narrowband Isolators can be tuned to maximize the peak isolation for any wavelength within a narrow spectral range (shaded in this graph). This plot shows isolation data for the IO-3-1064-HP. Graphs showing the isolation when each isolator is tuned to the center wavelength are provided on the Graphs tab.
Click for Details
Light Not at the Design Wavelength is Partially Transmitted
Click for Details
Light at the Design Wavelength is Rejected
Operating Principles of Optical Isolators
The magnitude of the rotation caused by the Faraday rotator is wavelength dependent. This means that light with a different wavelength than the design wavelength will not be rotated at exactly 45°. For example, if 1064 nm light is rotated by 45° (that is, 1064 nm is the design wavelength), then 1054 nm light is rotated by 46.3°. If 1054 nm light is sent backward through an isolator designed for 1064 nm without any tweaking, it will have a net polarization of 45° + 46.3° = 91.3° relative to the axis of the input polarizer. The polarization component of the light parallel to the input polarizer's axis will be transmitted, and the isolation will therefore be significantly reduced.
Since the net polarization needs to be 90° to obtain high isolation, the output polarizer is rotated to compensate for the extra rotation being caused by the Faraday isolator. In our example, the new polarizer angle is 90° - 46.3° = 43.7°. This adjustment increases the isolation back to the same value as at the design wavelength.
Consequences of Wavelength Tuning Procedure
Here, θ is the angle between the polarization direction of the light after the Faraday rotator and the transmission axis of the polarizer, I0 is the incident intensity, and I is the transmitted intensity. For small deviations from the center wavelength, the decrease in transmission is very slight, but for larger deviations, the decrease becomes noticeable. In our example (a 10 nm difference between the design wavelength and the usage wavelength), θ = 46.3° - 43.7° = 2.6°, so I = 0.998 I0. This case is shown in the graphs above.
In applications, the decrease in transmission caused by the tuning procedure is usually less important than the significantly enhanced isolation gained by tuning. For example, if the 1064 nm isolator shown in the graphs above were used at 1044 nm without tuning, the transmission would be 92.2% (instead of 92.0%), but the isolation would be only 26 dB (instead of 42 dB). This case is also shown in the graphs above.
Thorlabs' isolator housings make it easy to rotate the output polarizer without disturbing the rest of the isolator. Our custom isolator manufacturing service (see the Custom Isolators tab) can also provide an isolator specifically designed for a particular center wavelength, which can eliminate or strongly mitigate the transmission losses that occur at the edges of the tuning range. These custom isolators are provided at the same cost as their equivalent stock counterparts. For more information, please contact Technical Support.
Illustrated Tuning Procedure
To optimize the isolation curve for a specific wavelength within the tuning range, the alignment of the output polarizer may be tweaked following the simple procedure outlined below. Only a minor adjustment is necessary to cover a range of several nanometers. The procedure differs slightly for different isolator packages, but the principle remains the same across our entire isolator family, and complete model-specific tuning instructions ship with each isolator.
Use the included 5/64" hex key to loosen the isolator from its saddle.
The isolator is mechanically stable in this position as long as the isolator has not been brought forward too much. (The amount shown in the image to the left is safe by several millimeters.) It should therefore not be necessary to reinsert the isolator at the end of the tuning procedure.
As long as the isolator was not brought forward too much at the end of Step 2, the isolator will be mechanically stable in this position. Attempting to reinsert the isolator at this point may cause misalignment.
Fixed Narrowband Isolator
The isolator is set for 45° of rotation at the design wavelength. The polarizers are non-adjustable and are set to provide maximum isolation at the design wavelength. As the wavelength changes the isolation will drop; the graph shows a representative profile.
Adjustable Narrowband Isolator
The isolator is set for 45° of rotation at the design wavelength. If the usage wavelength changes, the Faraday rotation will change, thereby decreasing the isolation. To regain maximum isolation, the output polarizer can be rotated to "re-center" the isolation curve. This rotation causes transmission losses in the forward direction that increase as the difference between the usage wavelength and the design wavelength grows.
Adjustable Broadband Isolator
The isolator is set for 45° of rotation at the design wavelength. There is a tuning ring on the isolator that adjusts the amount of Faraday rotator material that is inserted into the internal magnet. As your usage wavelength changes, the Faraday rotation will change, thereby decreasing the isolation. To regain maximum isolation, the tuning ring is adjusted to produce the 45° of rotation necessary for maximum isolation.
Fixed Broadband Isolator
A 45° Faraday rotator is coupled with a 45° crystal quartz rotator to produce a combined 90° rotation on the output. The wavelength dependences of the two rotator materials work together to produce a flat-top isolation profile. The isolator does not require any tuning or adjustment for operation within the designated design bandwidth.
Tandem isolators consist of two Faraday rotators in series, which share one central polarizer. Since the two rotators cancel each other, the net rotation at the output is 0°. Our tandem designs yield narrowband isolators that may be fixed or adjustable.
Polarizer Types, Sizes, and Power Limits
Thorlabs designs and manufactures several types of polarizers that are used across our family of optical isolators. Their design characteristics are detailed below. The suffix of the part number of a given isolator identifies the type of polarizer that isolator contains.
Optical Isolator Tutorial
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 Q equals V x L x H, where V, L, and H are as defined below.
Figure 1. Faraday Rotator's Effect on Linearly Polarized Light
Q = V x L x H
V: the Verdet Constant, a property of the optical material, in minutes/Oersted-cm.
L: the path length through the optical material in cm.
H: the magnetic field strength in Oersted.
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.
Figure 2. A polarization-dependent isolator. Light propagating in the reverse direction is rejected by the input polarizer.
The Forward Mode
The Reverse Mode
Click for Details
Figure 3. A polarization independent isolator. Light is deflected away from the input path and stopped by the housing.
Polarization-Independent Fiber Isolators
The Forward Mode
The Reverse Mode
Figure 4. Pulse Dispersion Measurements Before and After an IO-5-780-HP Isolator
τ: Pulse Width Before Isolator
τ(z): Pulse Width After Isolator
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 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.
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.
We can also offer Faraday rotators which rotate the polarization of incoming light by 45° ± 3°. These are similar to our isolators but with the polarizers at each end removed. They are available with center wavelengths from 244 to 5000 nm.
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.
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.
Request a custom isolator quote using the form below or by contacting us for more information at (973) 300-3000.
The IO-1.2PI-1064-PBB is a polarization-independent isolator that is based on a fiber-coupled isolator design. Unlike the other free-space isolators on this page, its transmission and isolation do not depend on the input polarization. This makes the isolator ideal for applications where the polarization state is indeterminate or variable.
This isolator is excellent for system development projects where new fiber optic systems are being built and tested. The polarization-independent nature of the isolator allows users to experiment with different collimators and couplers as power levels increase in the fiber optic system.
Please see our Nd:YAG Fiber Optic Isolators web page for our fiber-to-free-space isolators.
These adapters provide mechanical compatibility between our isolator bodies and SM1 (1.035"-40) lens tubes, SM2 (2.035"-40) lens tubes, SM3 (3.035"-40) lens tubes, 30 mm cage systems, Ø1/2" posts, Ø1" posts, and our FiberBench systems.
Click for Details
IO-5-532-HP Mounted in CP12 30 mm Cage Plate