Products> Isolators> Faraday Isolators> 115D/387 D-Band Isolators
Description:
Mi-Wave’s 115 series D-band isolator uses the Faraday principle of rotation in a broadband dielectric waveguide design to achieve high isolation across full waveguide bands. High-quality ferrite material is used in these isolators, and the magnetic field is produced by an integral permanent magnet. To ensure maximum reproducibility and performance, a combination of precise machining operations and refined assembly techniques are used.
Features
• Low insertion loss
• Full waveguide band
• Excellent isolation across the band
• Faraday rotation principle of operation
Applications
• Test Labs
• Sub-Assemblies
• Automotive Industry
• MMwave Test Systems
The standard models shown represent only part of Mi-Wave’s broader product capabilities. Custom configurations are available to support specific frequency bands, interfaces, and application requirements, enabling optimized solutions for specialized RF, microwave, and millimeter-wave systems.

* Images, Plots & Datasheets are for reference only.
* Outline Drawings keep enhancing which may alter dimensions, please contact us for latest specifications.
Features & Specifications
Broadband Operation Across Full Waveguide Bands
The 115 Series Faraday Isolators are designed to operate across the entire standard waveguide frequency band, rather than a narrow tuned region. This enables seamless integration into broadband systems where frequency agility, wideband testing, or multi-channel operation is required without performance degradation at band edges.
Low Insertion Loss for System Efficiency
Forward signal transmission is maintained with minimal insertion loss, preserving available power and ensuring that system gain and noise performance are not unnecessarily degraded. This is especially important in mmWave systems where every dB of loss directly impacts link margin and receiver sensitivity.
High Isolation for Source Protection
The isolator provides strong reverse signal suppression, preventing reflected power from reaching sensitive upstream components. This improves amplifier stability, reduces gain ripple, and protects oscillators, multipliers, and measurement equipment from mismatch-induced stress.
Passive Operation with Permanent Magnet Bias
Using an integral permanent magnet, the 115 Series requires no external biasing or control circuitry. This simplifies system design, improves reliability, and ensures consistent performance across varying environmental conditions without the need for active tuning.
Precision Mechanical Construction
Performance consistency across units is achieved through tight machining tolerances and controlled assembly processes. At microwave and millimeter-wave frequencies, even small dimensional variations can impact RF behavior, making precision manufacturing critical to repeatability and long-term reliability.
Ferrite-Based Non-Reciprocal Behavior
The use of high-quality ferrite materials enables stable Faraday rotation-based non-reciprocal operation, ensuring predictable directional performance across the operating band. This allows the isolator to maintain consistent isolation and insertion loss characteristics even in demanding RF environments.
How Faraday Isolators Work
Mi-Wave’s 115 Series Faraday Isolators operate by using the Faraday rotation effect, a non-reciprocal electromagnetic phenomenon that allows RF energy to pass efficiently in one direction while suppressing reflections in the opposite direction.
Forward Direction (Desired Signal Path)
- The incoming RF signal enters the isolator and passes through the ferrite section
- The polarization of the wave is rotated, typically by 45 degrees
- The wave then aligns with the output waveguide structure and continues with minimal insertion loss
Reverse Direction (Reflected Signal)
- A reflected signal re-enters the isolator from the output side
- It undergoes another 45° rotation in the same direction (non-reciprocal behavior)
- Total rotation becomes 90 degrees, misaligning the signal with the input waveguide
- The signal is directed into a lossy or absorbing section, where it is dissipated as heat
Inside the isolator, the signal travels through a magnetized ferrite element positioned within a broadband dielectric waveguide structure. As the forward-traveling wave passes through this ferrite, its polarization rotates by a controlled amount. The wave is then aligned with the output structure so it can continue through the device with relatively low insertion loss.
When a reflected signal attempts to travel backward through the isolator, it experiences additional rotation in the same rotational direction, rather than reversing as it would in a reciprocal device. This causes the reflected wave to become misaligned with the input path. Instead of returning to the source, the unwanted energy is directed into an internal absorptive region where it is dissipated.
This is what gives the isolator its directional behavior. Forward power is transmitted with minimal loss, while reverse power is strongly attenuated. In practical RF systems, this helps protect amplifiers, sources, and sensitive measurement equipment from reflected energy that could otherwise introduce instability, standing waves, gain ripple, or even damage.
The 115 Series achieves this using high-quality ferrite material, an integral permanent magnet for magnetic biasing, and a mechanically stable structure designed for repeatable broadband performance. The result is a passive waveguide component that improves system stability without requiring external bias power or active control circuitry.
Why This Matters
- Prevents standing waves and reflections
- Protects power amplifiers and sensitive front-end components
- Improves measurement accuracy in test systems
- Stabilizes gain and phase behavior in RF chains
Key Engineering Insight
Unlike reciprocal devices, Faraday isolators exhibit direction-dependent phase rotation, meaning:
- Forward and reverse signals do not behave symmetrically
- This is what enables true isolation rather than simple attenuation
Applications
RF and Millimeter-Wave Test Systems
In laboratory and production test environments, isolators are commonly placed between signal sources and devices under test to prevent reflected power from affecting measurement accuracy. By stabilizing the source impedance, they improve repeatability and reduce uncertainty in S-parameter and power measurements.
Amplifier Protection in RF Chains
Power amplifiers, particularly at microwave and mmWave frequencies, are highly sensitive to load mismatches. Integrating an isolator at the amplifier output helps prevent reflected energy from re-entering the device, reducing the risk of oscillation, compression artifacts, or long-term damage.
Automotive Radar and Sensing Systems
In automotive radar applications operating at high frequencies, isolators contribute to stable signal generation and reception by minimizing internal reflections. This supports more consistent detection performance and improved signal integrity in complex electromagnetic environments.
Sub-Assemblies and Integrated RF Modules
Isolators are frequently incorporated into multi-stage RF subsystems, including up/downconverter chains, transceiver front ends, and frequency generation modules. Their ability to enforce directional signal flow helps simplify system architecture and reduce unwanted interactions between stages.
Communication Systems and Signal Chains
In communication systems, particularly those operating in the microwave and millimeter-wave spectrum, isolators improve overall link performance by reducing standing waves and maintaining consistent impedance conditions. This results in more stable transmission characteristics and improved spectral purity.
Aerospace and Defense Systems
High-reliability applications such as radar, electronic warfare, and satellite communication systems rely on isolators to maintain consistent RF behavior under demanding conditions. The passive, magnetically biased design of the 115 Series makes it well suited for environments where robustness and predictability are critical.
Frequently Asked Questions (FAQ)
What is the purpose of a waveguide isolator?
An isolator allows RF energy to pass in one direction while blocking reflections in the opposite direction, protecting sensitive components like amplifiers and signal sources.
How is a Faraday isolator different from a circulator?
An isolator is essentially a two-port device derived from a circulator, typically with one port terminated. It provides simpler integration when only forward isolation is required.
Do these isolators require external power or biasing?
No. The 115 Series uses an integral permanent magnet, eliminating the need for external biasing.
Why is isolation important in RF systems?
High isolation prevents reflected signals from degrading performance, causing instability, or damaging components such as power amplifiers.
What frequency ranges are available?
Standard waveguide models are available from 18 GHz up to 325 GHz, covering microwave through millimeter-wave bands.
Can these be customized?
Yes. MI-Wave offers custom designs for specific frequency bands, power levels, and mechanical requirements.
Isolator Performance Calculators
These calculators help estimate forward loss, reflected power suppression, return loss behavior, and leakage levels when integrating Faraday isolators into microwave and millimeter-wave signal chains.
Reflected Power After Isolation
Estimate the reflected power that remains after the isolator suppresses reverse energy.
Output Power with Insertion Loss
Calculate forward output power after insertion loss through the isolator.
Return Loss to Reflected Power
Estimate reflected power from input power and return loss.
VSWR to Return Loss
Convert VSWR to return loss to evaluate impedance match quality.
Linear Leakage from Isolation
Estimate the remaining reverse leakage as a linear ratio from isolation in dB.
| Model Number | Frequency min. (GHz) | Frequency max. (GHz) | Isolation (dB) | Insertion Loss (dB) typical | VSWR max. | Power Handling CW (Watts max.) | Input Port | Output Port | LINK |
|---|---|---|---|---|---|---|---|---|---|
| 115K/595 | 18 | 26.5 | 25 | 1 | 1.30:1 | 2 | WR-42 Waveguide, UG-595/U Flange | WR-42 Waveguide, UG-595/U Flange | |
| 115(34)/595 | 22 | 33 | 25 | 1 | 1.30:1 | 2 | WR-34 Waveguide, UG-595/U Square Flange | WR-34 Waveguide, UG-595/U Square Flange | |
| 115(34)/381 | 22 | 33 | 25 | 1 | 1.30:1 | 2 | WR-34 Waveguide, UG-381/U Round Flange | WR-34 Waveguide, UG-381/U Round Flange | |
| 115A/599 | 26.5 | 40 | 25 | 1.2 | 1.30:1 | 2 | WR-28 Waveguide, UG-599/U Square Flange | WR-28 Waveguide, UG-599/U Square Flange | |
| 115B/383 | 33 | 50 | 25 | 1.3 | 1.30:1 | 1.5 | WR-22 Waveguide, UG-383/U Round Flange | WR-22 Waveguide, UG-383/U Round Flange | |
| 115U/383 | 40 | 60 | 25 | 1.5 | 1.30:1 | 1.5 | WR-19 Waveguide, UG-383/U-M Round Flange | WR-19 Waveguide, UG-383/U-M Round Flange | |
| 115V/385 | 50 | 75 | 25 | 1.7 | 1.30:1 | 1 | WR-15 Waveguide, UG-385/U Round Flange | WR-15 Waveguide, UG-385/U Round Flange | |
| 115E/387 | 60 | 90 | 25 | 2 | 1.35:1 | 1 | WR-12 Waveguide, UG-387/U Round Flange | WR-12 Waveguide, UG-387/U Round Flange | |
| 115W/387 | 75 | 110 | 25 | 2.2 | 1.40:1 | 1 | WR-10 Waveguide, UG-387/U-M Round Flange | WR-10 Waveguide, UG-387/U-M Round Flange | |
| 115F/387 | 90 | 140 | 22 | 2.7 | 1.50:1 | 0.4 | WR-08 Waveguide, UG-387/U-M Round Flange | WR-08 Waveguide, UG-387/U-M Round Flange | |
| 115D/387 | 110 | 170 | 20 | 3.1 | 1.50:1 | 0.2 | WR-06 Waveguide, UG-387/U-M Round Flange | WR-06 Waveguide, UG-387/U-M Round Flange | |
| 115G/387 | 140 | 220 | 20 | 3.5 | 1.50:1 | 0.2 | WR-05 Waveguide, UG-387/U-M Round Flange | WR-05 Waveguide, UG-387/U-M Round Flange | |
| 115H/387 | 170 | 260 | 20 | 5 | 1.50:1 | 0.1 | WR-04 Waveguide, UG-387/U-M Round Flange | WR-04 Waveguide, UG-387/U-M Round Flange | |
| 115J/387 | 220 | 325 | 20 | 5 | 1.50:1 | 0.1 | WR-03 Waveguide, UG-387/U-M Round Flange | WR-03 Waveguide, UG-387/U-M Round Flange |
*All data presented is collected from a sample lot.
* Actual data may vary unit to unit, slightly.
*All testing was performed under +25 °C case temperature.
*Consult factory to confirm if material, plating, size, shape, orientation and any electrical parameter is critical for the application as website information is for reference only.
*Millimeter Wave Products, Inc. reserves the right to change the information presented on website without notice as we continue to enhance the performance and design of our products.
D-Band Isolators
Our D-band Isolators are for the spectrum in the millimeter wave range of frequencies from 110GHz – 170GHz.
Designed for full waveguide band operation, the 115 series isolator is used in swept frequency applications. These components provide a high degree of isolation between signal sources and mismatched loads by attenuating the reflected signals. The insertion loss in the forward direction is minimized to allow for the full available power from the signal source-isolator combination. Typical applications for these broadband isolators include laboratory setups as well as millimeter wave test sets and automotive radar
Ready to Order or Have a Question?
Our sales engineers are standing by.
See datasheets, outline drawings and band specific info.
Click on the links below.

