Optical circulator

An optical circulator is a non-reciprocal, passive optical device with typically three or four ports that directs light signals unidirectionally from one port to the next sequential port, enabling the separation of forward- and backward-propagating signals in a single optical fiber. This functionality prevents back-reflections from interfering with the input signal while routing returned light to a designated output port, analogous to a microwave circulator but optimized for optical wavelengths. Unlike an optical isolator, which blocks backward-propagating light, a circulator routes it to another port.^[1] The core principle of operation involves the magneto-optic Faraday effect, where an applied magnetic field rotates the polarization of light in a non-reciprocal manner, combined with components such as polarization beam splitters and birefringent crystals to achieve directional routing.^[2] In a standard three-port configuration, light entering port 1 exits port 2 with minimal insertion loss (typically 0.7–1.0 dB), while light entering port 2 exits port 3; attempts to propagate in the reverse direction encounter high isolation (>30 dB).^[3] These devices support common wavelengths like 1310 nm and 1550 nm, with power handling up to 500 mW, and are available in forms such as inline fiber pigtails or polarization-maintaining variants.^[4] Optical circulators are indispensable in fiber-optic communication systems, including dense wavelength division multiplexing (DWDM) networks for signal routing and optical add-drop multiplexers (OADMs) for channel selection.^[3] They also play key roles in fiber Bragg grating applications, bidirectional pumping in fiber amplifiers, chromatic dispersion compensation, and fiber-optic sensors.^[2] In biomedical and sensing fields, they enhance optical coherence tomography (OCT) systems by isolating signals, and ongoing research in silicon photonics enables integrated, compact versions for photonic circuits.^[5]^[6]

Introduction

Definition and function

An optical circulator is a passive, non-reciprocal, multi-port optical device, typically featuring three or four ports, that routes incoming light signals sequentially from one port to the next in a single direction, thereby preventing backward propagation through the same path.^[1]^[7] This non-reciprocal behavior ensures that light travels only in the designated circulation direction, such as clockwise or counterclockwise, allowing for efficient signal management in optical networks without reversal.^[4] In a standard three-port configuration, light entering port 1 is directed to exit port 2 with minimal insertion loss, and light entering port 2 exits port 3, with high isolation suppressing reverse propagation.^[1]^[4] This port-specific routing enables the separation of signals traveling in opposite directions within the same optical pathway, such as in bidirectional transmission setups.^[7] The device's isolation properties further suppress unwanted reflections or counter-propagating signals, maintaining signal integrity across the ports.^[1] A basic use case for an optical circulator is in single-fiber bidirectional communication systems, where it separates forward-transmitted signals from backward-reflected or received signals, for example, by directing an input from port 1 through a fiber to a remote reflector and routing the reflection from port 2 to port 3 for detection.^[4]^[7] The standard schematic of a three-port optical circulator is often illustrated as a circular or triangular diagram with ports labeled 1, 2, and 3, connected by curved arrows indicating the unidirectional flow: an arrow from port 1 to port 2 and from port 2 to port 3, emphasizing the sequential routing without reverse paths.^[1]^[4] Optical circulators differ from optical isolators primarily in their handling of backward-propagating light: while isolators, which are typically two-port devices, transmit light in the forward direction but block or absorb it in the reverse direction to prevent feedback, circulators route the backward light to a separate output port, enabling potential reuse in systems like bidirectional communication links.^[8] This multi-port routing in circulators (usually three or four ports) allows for sequential directionality—light entering port 1 exits port 2, entering port 2 exits port 3, and so on—without dissipation of the reverse signal, contrasting the absorptive loss in isolators.^[4] Optical circulators draw an analogy to radiofrequency (RF) and microwave circulators, adapting the ferrite-based non-reciprocal principles of the latter—originally relying on magnetic biasing for directional signal routing—to optical frequencies using magneto-optic materials like yttrium iron garnet (YIG). However, optical circulators operate at much higher wavelengths, such as 1550 nm in telecommunications bands, where magneto-optic effects like Faraday rotation enable the non-reciprocal behavior scaled down from microwave regimes.^[9] In contrast to optical switches, which are generally active devices requiring electrical or optical control to route signals reciprocally between ports, circulators function passively without external actuation, relying solely on inherent non-reciprocity for fixed directional transfer.^[10]^[11]

Device	Number of Ports	Reciprocity	Typical Applications
Optical Circulator	3 or 4	Non-reciprocal	Bidirectional transmission, signal separation in fiber links^[8]
Optical Isolator	2	Non-reciprocal	Laser protection from backreflections, amplifier isolation
Optical Switch	2×2 or more	Reciprocal	Dynamic signal routing in networks, multiplexing control^[11]

Operating Principles

Non-reciprocal behavior

In optics, reciprocity refers to the principle that electromagnetic wave propagation in passive media is reversible, meaning the transmission characteristics remain unchanged when the direction of light propagation is reversed. This behavior is governed by the Lorentz reciprocity theorem, which states that in a linear, time-independent system with symmetric constitutive optical tensors, the ratio between received and transmitted fields is identical for forward and time-reversed propagation directions.^[12] In passive media lacking external fields or asymmetries, light paths are thus bidirectional, allowing signals to traverse the same route in either direction without alteration.^[13] Non-reciprocity arises when this symmetry is disrupted, specifically by breaking time-reversal invariance, which prevents light from following the same path in reverse. This is commonly achieved through the introduction of external magnetic fields or structural asymmetries that render the system's response direction-dependent.^[12] Such interventions violate the conditions of the Lorentz theorem, leading to an asymmetric scattering matrix where transmission coefficients differ between forward and backward directions.^[13] In optical circulators, non-reciprocal behavior plays a pivotal role by enforcing unidirectional signal flow, ensuring that light entering an input port cannot return to it but instead routes to subsequent output ports, thereby providing isolation between ports.^[1] This isolation, often quantified in terms of decibels (typically >30 dB in commercial devices), prevents back-reflections and interference, enabling reliable sequential port routing as light progresses from one port to the next without reversal.^[4] To illustrate the distinction, consider the following conceptual representation of light paths in a three-port device: Reciprocal system (symmetric paths):

Input at Port 1 → Output at Port 2
Input at Port 2 → Output at Port 1 (reversible)

Non-reciprocal system (asymmetric paths, as in circulators):

Input at Port 1 → Output at Port 2
Input at Port 2 → Output at Port 3 (no return to Port 1)
Input at Port 3 → Output at Port 1

This asymmetry underpins the circulator's function, directing signals unidirectionally while blocking reverse propagation.^[1]

Faraday rotation mechanism

The Faraday effect, also known as Faraday rotation, is a magneto-optic phenomenon in which the plane of polarization of linearly polarized light rotates as it propagates through a transparent material subjected to an external magnetic field applied parallel to the direction of light propagation. This rotation is non-reciprocal, meaning that the sense of rotation remains the same regardless of whether the light travels parallel or antiparallel to the magnetic field, which is a key property enabling directional control in optical devices.^[14]^[15] The magnitude of the rotation angle \theta is given by the equation

\theta = V B L,

where V is the material's Verdet constant (a measure of its magneto-optic sensitivity, typically in rad/(T·m)), B is the magnetic field strength (in tesla), and L is the optical path length through the material (in meters). This linear relationship allows precise control of the rotation by adjusting the field strength or material thickness, with typical designs targeting a 45° rotation for integration into circulators.^[14]^[16] In optical circulators, the Faraday rotator is integrated with polarization-sensitive components such as polarizing beam splitters (PBS) and half-wave plates to achieve unidirectional light routing across multiple ports. The rotator, consisting of a magneto-optic crystal within a permanent magnet providing the axial field, induces the necessary polarization transformation: a 45° rotation in the forward direction aligns the light with the transmission axis of the PBS for output to the next port, while the non-reciprocal nature ensures backward-propagating light experiences an additional 45° rotation in the same sense, resulting in a 90° total shift that redirects it to a subsequent port rather than reflecting it back. Common materials include yttrium iron garnet (YIG, Y₃Fe₅O₁₂) for near-infrared wavelengths in telecommunications applications due to its low optical losses and high Faraday rotation efficiency, and terbium gallium garnet (TGG, Tb₃Ga₅O₁₂) for visible and near-infrared ranges owing to its large Verdet constant (around -150 rad/(T·m) at 633 nm) and thermal stability; these are selected to provide exactly 45° rotation at the operating wavelength under a saturated magnetic field of approximately 0.1–0.3 T.^[17]^[18]^[19] A detailed step-by-step light path in a basic three-port polarization-dependent Faraday-based circulator illustrates this mechanism. Light enters Port 1 as unpolarized or partially polarized and is first incident on a PBS, which transmits the p-polarized component and reflects the s-polarized component; for simplicity, assume input light is aligned to be primarily p-polarized and transmitted. It then passes through the Faraday rotator, where the magnetic field induces a 45° clockwise rotation of the polarization plane (viewed in the direction of propagation). Next, a half-wave plate, oriented at 22.5° to the original polarization, compensates for this rotation, restoring the polarization to its initial state (net 0° rotation) while directing the beam via the PBS to exit Port 2. For light entering from Port 2 in the reverse direction, it is again split by the PBS (now entering as p-polarized relative to the splitter), passes through the half-wave plate (which rotates it by 45° due to the orientation), and then through the Faraday rotator, which adds another 45° clockwise rotation; the combined 90° total rotation misaligns the polarization with the PBS transmission axis, causing reflection to Port 3 instead of returning to Port 1. This sequential, non-reciprocal routing ensures isolation between ports and prevents back-reflection.^[18]^[20]^[1]

Types and Designs

Polarization-dependent circulators

Polarization-dependent optical circulators operate by exploiting the polarization state of the input light, typically requiring linearly polarized signals aligned with specific axes for effective routing. These devices commonly feature polarizing beam splitters (PBS) to separate orthogonal polarization components, half-wave plates to adjust polarization orientations, and Faraday rotators to induce non-reciprocal rotation via the magneto-optic Faraday effect. Birefringent crystals, such as calcite, are often integrated to enhance beam displacement and splitting without significant loss, enabling compact bulk-optic assemblies.^[1]^[21] The operational sequence begins with input light at the first port, polarized parallel to the transmission axis of the initial PBS, passing through to the Faraday rotator. The rotator induces a 45° clockwise rotation (for forward propagation), after which a half-wave plate may compensate or further align the polarization, allowing the light to transmit through a subsequent PBS and exit the second port. Reverse-propagating light from the second port experiences a counterclockwise -45° rotation in the same rotator due to the non-reciprocal nature of the Faraday effect, resulting in its polarization being orthogonal to the PBS transmission axis and thus deflected to the third port. This directional asymmetry ensures signal isolation while maintaining low insertion loss in properly aligned systems.^[1]^[20] These circulators offer advantages such as high port-to-port isolation exceeding 50 dB and relatively compact footprints, particularly when leveraging birefringent materials like calcite for precise polarization control and minimal beam walk-off.^[1]^[21] However, their performance is limited by the necessity for polarized input light; unaligned or randomly polarized signals lead to reduced efficiency and crosstalk. Additionally, they exhibit sensitivity to polarization fluctuations in single-mode fibers, where environmental factors can induce state-of-polarization drifts, compromising isolation and insertion loss stability.^[20] Early examples of such designs emerged in the 1970s as bulk-optic configurations using dielectric coatings on PBS components to achieve efficient polarization separation in fiber transmission setups.

Polarization-independent circulators

Polarization-independent circulators enable reliable operation with input light of arbitrary polarization states, enhancing their utility in systems where polarization control is impractical or variable. Unlike polarization-dependent designs, these circulators split the incoming beam into orthogonal polarization components—typically ordinary and extraordinary rays—using birefringent elements, process each path through non-reciprocal Faraday rotation, and recombine them to maintain circulation functionality regardless of the input orientation. This approach leverages the non-reciprocal nature of the Faraday effect, where forward-propagating light experiences a consistent 45° rotation per stage, directing it to the next port, while backward light rotates oppositely and is routed to an isolation port.^[7]^[22] Designs often incorporate dual-stage polarization manipulation to achieve higher isolation, with each stage featuring separate Faraday rotators for the split components; for example, Terbium Gallium Garnet (TGG) crystals serve as robust rotators in high-power configurations, compensating for any residual birefringence via half-wave plates. Key components include birefringent prisms or beam displacers made from materials like rutile (titanium dioxide) or yttrium orthovanadate (YVO₄) for initial splitting and recombination, Yttrium Iron Garnet (YIG) or bismuth-substituted YIG as the Faraday elements providing the required rotation under magnetic bias, and compensating waveplates to align polarizations post-rotation. In a typical setup, the input from port 1 is separated by a rutile prism pair, each component rotated by 45° in YIG, adjusted by a quartz half-wave plate, and recombined to exit port 2, ensuring low polarization-dependent loss across the operational bandwidth.^[23]^[22]^[7] These circulators offer significant advantages for applications involving unpolarized or randomly polarized sources, such as multimode fiber systems, by providing isolation greater than 40 dB to effectively suppress unwanted reflections without polarization alignment. For instance, configurations with extended birefringent rhomboid displacers maintain this isolation level over wide spectral ranges, like 1.2–1.4 μm, while keeping insertion losses below 1 dB. Evolutionarily, designs transitioned in the 1990s from early polarization beam splitter (PBS)-based architectures, which achieved only about 20 dB isolation due to alignment sensitivities, to more efficient crystal-based systems using rutile or YVO₄ for compact, high-performance operation with improved directionality exceeding 50 dB.^[24]^[7]^[25]^[7] Fiber-pigtailed variants integrate these components with single-mode fibers via lens arrays or mode-field expansion techniques, enabling low-loss coupling (typically <0.8 dB) and rugged packaging suitable for telecommunications and sensing. This pigtailing uses fiber arrays positioned behind the birefringent-magneto-optic stack to align beams precisely, reducing overall device size by over an order of magnitude compared to free-space versions.^[7]^[26]

Applications

Telecommunications systems

Optical circulators can be used in certain configurations of passive optical networks (PONs) and fiber-to-the-home (FTTH) systems to enable bidirectional transmission over a single optical fiber by separating upstream and downstream signals, facilitating efficient duplexing. In these networks, upstream signals typically operate at around 1310 nm, while downstream data signals are at 1490 nm and video signals at 1550 nm, allowing the circulator to route incoming light from the central office to the end-user device via one port and direct returning signals to a receiver without interference.^[27]^[28] This configuration supports high-capacity data delivery to multiple households while minimizing fiber infrastructure costs, as the non-reciprocal routing prevents crosstalk between the counter-propagating signals.^[29] In wavelength-division multiplexing (WDM) and optical add-drop multiplexer (OADM) systems, optical circulators integrate seamlessly to route specific wavelengths to add-drop ports, enabling the selective insertion or extraction of channels without introducing significant crosstalk between adjacent wavelengths. By directing signals unidirectionally through the multiplexer, circulators ensure that dropped wavelengths are isolated from the main transmission line, supporting scalable network architectures in metro and access environments.^[30] This functionality is particularly vital in dense WDM (DWDM) setups, where achieving isolation greater than 30 dB across multiple channels maintains signal integrity for multi-terabit-per-second operations.^[7] Optical circulators can also be employed in erbium-doped fiber amplifiers (EDFAs) within telecommunications links to isolate backward-propagating signals and help prevent reflections from degrading amplification performance. In such configurations, the circulator aids in signal routing, while pump light is directed forward via wavelength-division multiplexers and backward reflections are typically managed by optical isolators, stabilizing gain and reducing noise accumulation in amplified spans.^[31] Since the 1990s, optical circulators have been indispensable for scaling bandwidth in long-haul fiber networks, particularly with the advent of WDM technologies that multiplied transmission capacities from gigabits to terabits per second on existing infrastructure. Their integration into OADMs and bidirectional systems addressed the explosive growth in data traffic driven by the Internet's expansion, enabling cost-effective upgrades without widespread fiber redeployment.^[32]

Optical sensing and measurement

Optical circulators play a crucial role in optical time-domain reflectometry (OTDR) systems by directing the input probe light into the fiber under test and routing the backscattered Rayleigh light from faults or discontinuities back to the detector, enabling precise fault location and characterization without signal interference.^[33] In coherent OTDR setups, the circulator ensures that reflected signals from fiber Bragg gratings or scattering events are efficiently separated from the outgoing pulse, supporting high-sensitivity distributed sensing over long distances.^[33] In fiber Bragg grating (FBG) sensor systems, optical circulators separate the reflected sensing signals, which carry information on parameters like strain or temperature, from the input probe light, allowing for accurate interrogation of the wavelength-shifted reflections.^[34] This unidirectional routing prevents back-reflections from contaminating the measurement, enabling high-resolution detection in applications such as structural health monitoring.^[34] For dispersion compensation in high-speed optical links, circulators facilitate a double-pass configuration through dispersion-compensating fibers (DCF), where light enters the DCF via one port, reflects off a return element like a mirror, and exits through another port, effectively halving the required DCF length while mitigating chromatic dispersion.^[35] This setup maintains signal integrity over extended transmission distances by compensating for pulse broadening without introducing excessive loss.^[35] In laboratory settings, optical circulators are employed in interferometric and laser systems to isolate counter-propagating signals and suppress noise, such as in Pound-Drever-Hall frequency stabilization where they route light into high-finesse cavities while minimizing parasitic reflections.^[36] By leveraging their non-reciprocal properties, these devices reduce intensity fluctuations and pointing errors, achieving stabilities on the order of 10^{-16} in compact fiber-coupled setups.^[36] Polarization-maintaining optical circulators are particularly valuable in fiber optic gyroscopes, where they enable the Sagnac effect by directing counter-propagating beams through the sensing coil without crosstalk, allowing precise rotation rate measurement via phase differences induced by angular velocity.^[37] In dual-polarization interferometric fiber optic gyroscopes (IFOGs), four-port circulators manage polarization coupling to enhance bias stability and scale factor accuracy for inertial navigation.^[37]

Performance Characteristics

Key metrics and specifications

Optical circulators are evaluated based on several key performance metrics that quantify their efficiency in directing optical signals unidirectionally while minimizing losses and unwanted reflections. These metrics include isolation ratio, insertion loss, bandwidth, and return loss, each critical for ensuring reliable operation in optical systems.^[1] The isolation ratio measures the device's ability to suppress backward-propagating signals, defined as the ratio of forward to backward transmission power expressed in decibels: Isolation (dB) = 10 \log_{10} (P_{\text{forward}} / P_{\text{backward}}), where P_{\text{forward}} and P_{\text{backward}} are the optical powers in the forward and backward directions, respectively.^[38] Typical values range from 20 to 60 dB, with commercial devices often achieving greater than 40 dB to prevent crosstalk in multi-port configurations.^[7]^[4] Insertion loss quantifies the power attenuation experienced by the signal traveling from the input to the designated output port, ideally kept below 1 dB in high-performance units.^[1] This loss arises primarily from factors such as coupling efficiency between optical elements and absorption in the materials, with typical values around 0.8 dB for telecom-grade circulators.^[4]^[18] Bandwidth refers to the operational wavelength range over which the circulator maintains its specified performance, often tailored to standard telecom bands like the C-band (1525-1565 nm).^[4] For example, devices operating in the 1550 nm region may cover 1520-1580 nm or broader spans up to 1525-1610 nm, depending on the design.^[39]^[4] Return loss indicates the suppression of reflections back to the input port, typically exceeding 50 dB in quality devices to avoid signal degradation from echoes.^[1] Commercial specifications often specify values greater than 50 dB, ensuring minimal feedback in fiber optic networks.^[4]^[18]

Metric	Polarization-Maintaining (PM) Typical Specs	Polarization-Independent (Non-PM) Typical Specs
Isolation	≥40 dB (e.g., 1550 nm range)	≥40 dB (e.g., 1550 nm range)
Insertion Loss	≤0.9 dB (e.g., 1520-1580 nm)	0.8 dB typical (e.g., 1525-1610 nm)
Bandwidth	1520-1580 nm (C-band example)	1525-1610 nm (C-band example)
Return Loss	≥50 dB	≥50 dB

These representative values are drawn from commercial devices at 1550 nm, highlighting similar performance across types with PM variants offering enhanced polarization control.^[39]^[4]

Limitations and trade-offs

Optical circulators exhibit temperature sensitivity primarily due to the thermal expansion and contraction of Faraday materials, which can alter the precise rotation angle required for non-reciprocal operation, as well as the inherent temperature dependence of the Faraday rotation constant itself. This effect can lead to shifts in performance metrics like isolation over temperature variations, necessitating compensation strategies such as athermal designs that incorporate materials with balanced thermo-optic coefficients or specialized packaging to stabilize the optical path.^[40] Bulk optical circulators are typically large and costly because of the need for substantial magnets, high-quality crystals, and precise alignment, making them less suitable for compact systems.^[41] In contrast, integrated versions on platforms like silicon photonics offer significantly reduced size and potential cost savings through wafer-scale fabrication, but they often incur higher insertion losses—sometimes exceeding 2 dB—due to challenges in integrating magneto-optic materials with waveguides and managing interface reflections.^[42] Polarization-dependent loss (PDL) in optical circulators can reach up to 0.5 dB in polarization-dependent types, arising from variations in transmission for different input polarizations, which impacts signal integrity in systems with arbitrary polarization states.^[7] Polarization-independent designs mitigate this issue, achieving PDL values below 0.2 dB through symmetric birefringence compensation or depolarizing elements.^[43] Many optical circulators are designed for specific wavelength bands, such as the C-band (approximately 40 nm wide), with operational ranges often spanning 50-100 nm around 1550 nm, limited by the dispersion in Faraday rotation and material absorption.^[1] Using broadband materials such as terbium gallium garnet (TGG) extends this to wider ranges, often exceeding 100 nm, by providing low wavelength-dependent Verdet constants and minimal absorption across the near-infrared spectrum.^[44] A key trade-off in optical circulator design is the inverse relationship between isolation and insertion loss: higher isolation ratios, such as >50 dB, generally require thicker magneto-optic elements or stronger magnetic fields, which increase scattering and absorption losses, potentially raising insertion loss above 1 dB.^[45] This balance is application-specific; telecommunications systems prioritize low insertion loss (<0.8 dB) for minimal signal degradation over long distances, while sensing applications may tolerate higher losses for enhanced isolation to improve measurement accuracy.^[20]

Historical Development

Early inventions and principles

The Faraday effect, discovered by Michael Faraday in 1845, laid the foundational principle for non-reciprocal optical devices by demonstrating that the plane of polarization of light rotates when passing through a material in the presence of a magnetic field. This magneto-optical phenomenon, initially observed with visible light and heavy glass, provided the non-reciprocal rotation essential for directing light unidirectionally, analogous to concepts in radiofrequency circulators.^[15] The advent of the laser in 1960 enabled practical optical applications of the Faraday effect by supplying coherent, monochromatic light ideal for polarization control experiments. Early concepts for optical circulators emerged in this era, adapting microwave circulator principles to optics. In 1965, William B. Ribbens described the first optical circulator prototype using a Nicol prism as a polarizing beam splitter combined with a Faraday rotator to achieve non-reciprocal routing of light between ports, suitable for laboratory demonstrations of signal isolation.^[46] These bulk optic designs relied on polarizing elements and magnetic rotators to separate and redirect orthogonally polarized beams, marking initial steps toward devices that could handle light in a circulating manner without reflection back to the source. By the 1970s, advancements focused on materials like yttrium iron garnet (YIG) films for near-infrared wavelengths, improving compactness and efficiency for emerging fiber optic systems. A seminal 1979 development by Atsushi Shibukawa and Morio Kobayashi introduced a compact circulator using a YIG single crystal as a 45° Faraday rotator paired with Glan-Taylor prisms, achieving insertion losses of 1.5–2.3 dB at 1.32 μm and supporting any polarization state for bidirectional transmission.^[47] This work, conducted at Japanese institutions such as NTT, built on RF adaptations by integrating magneto-optical films to minimize size while maintaining high isolation. Patent milestones in the early 1980s advanced fiber-compatible designs, with Takao Matsumoto's 1981 U.S. patent (filed 1979) from Nippon Telegraph and Telephone Corporation describing a four-port circulator using Faraday and compensating rotators between polarizing prisms to eliminate polarization dependency.^[48] Concurrently, research at Bell Laboratories contributed through William L. Emkey's 1984 U.S. patent (filed 1982), which detailed a polarization-independent bulk optic circulator employing birefringent plates, a Faraday rotator, and a half-wave plate for low-loss port routing in fiber systems. These prototypes, primarily bulk configurations with polarizing beam splitters and rotators, facilitated lab testing of non-reciprocal light directionality, paving the way for telecommunications integration.

Modern advancements and commercialization

The 1990s marked a significant boom in the development and adoption of optical circulators, driven by the rapid expansion of wavelength-division multiplexing (WDM) in telecommunications systems. As dense WDM (DWDM) networks emerged to increase fiber optic capacity, optical circulators became essential for routing signals in bidirectional transmission setups, enabling efficient add-drop functionality without crosstalk.^[21]^[49] Polarization-maintaining variants gained prominence for their role in erbium-doped fiber amplifiers (EDFAs), where they separated forward signal and backward pump light to enhance amplification efficiency, and in optical add-drop multiplexers (OADMs), facilitating selective channel extraction in DWDM links.^[50]^[51] By the 2000s, integration trends shifted toward more compact and scalable designs, with fiber-pigtailed circulators becoming standard for seamless coupling to single-mode fibers in telecom modules, reducing alignment losses and improving packaging density.^[52] Concurrently, advances in planar waveguide technologies enabled monolithic integration on platforms like lithium niobate (LiNbO3) and silicon photonics, leveraging thin-film LiNbO3 for electro-optic modulation compatibility and silicon for CMOS-compatible fabrication.^[53] These developments addressed the need for on-chip nonreciprocal devices in photonic integrated circuits (PICs), transitioning from bulk optics to hybrid and fully integrated solutions.^[54] Performance enhancements in the 2000s and beyond focused on broadband operation spanning over 100 nm and insertion losses as low as 0.4 dB, achieved through advanced magneto-optical crystals such as terbium gallium garnet (TGG) and bismuth-substituted iron garnet (BIG) for improved Faraday rotation and reduced polarization-dependent loss.^[32]^[55]^[56] For instance, silicon nitride-based designs have demonstrated ultra-broadband circulators with losses under 3 dB across C- and L-bands, supporting wider spectral ranges for next-generation networks.^[57] Market drivers in the 2000s were propelled by telecom infrastructure expansion, with DWDM deployments fueling demand for reliable circulators in long-haul and metro networks.^[49] In the 2020s, emerging applications in quantum optics—such as routing single photons in chiral interfaces—and high-speed fronthaul for 5G/6G have further accelerated commercialization, integrating circulators into PICs for low-latency, secure communications.^[58]^[59] Key milestones include the commercial availability of fiber-based circulators from companies like JDS Uniphase (now Viavi Solutions) in the late 1990s, which supplied components for early DWDM systems.^[60] A pivotal patent, US5909310A granted in 1999, advanced fiber coupling efficiency in three-port circulators, enabling lower losses and broader adoption in integrated modules.^[61]