Circulator

For other uses, see Circulator (disambiguation).

A waveguide circulator used as an isolator by placing a matched load on port 3. The label on the permanent magnet indicates the direction of circulation

A circulator is a passive non-reciprocal three- or four-port device, in which microwave or radio frequency power entering any port is transmitted to the next port in rotation (only). Thus, to within a phase-factor, the scattering matrix for an ideal three-port circulator is

$S = \begin{pmatrix} 0 & 0 & 1\\ 1 & 0 & 0 \\ 0 & 1 & 0 \end{pmatrix}$

When one port of a three-port circulator is terminated in a matched load, it can be used as an isolator, since a signal can travel in only one direction between the remaining ports.^[1]

There are circulators for LF, VHF, UHF, microwave frequencies and for light, the latter being used in optical fiber networks. Circulators fall into two main classes: 4-port waveguide circulators based on Faraday rotation of waves propagating in a magnetised material, and 3-port "Y-junction" circulators based on cancellation of waves propagating over two different paths near a magnetised material. Waveguide circulators may be of either type, while more compact devices based on striplines are of the 3-port type. Sometimes two or more Y-junctions are combined in a single component to give four or more ports, but these differ in behaviour from a true 4-port circulator.

In radar, circulators are used to route outgoing and incoming signals between the antenna, the transmitter and the receiver. In a simple system, this function could be performed by a switch that alternates between connecting the antenna to the transmitter and to the receiver. The use of chirped pulses and a high dynamic range may lead to temporal overlap of the sent and received pulses, however, requiring a circulator for this function.

Radio frequency circulators are composed of magnetised ferrite materials. A permanent magnet produces the magnetic flux through the waveguide. Ferrimagnetic garnet crystal is used in optical circulators.

There have also been investigations into making "active circulators" which are based on electronics rather than passive materials. However, the power handling capability and linearity and signal to noise ratio of transistors is not as high as those made from ferrites. It seems that transistors are the only (space efficient) solution for low frequencies.

References

1. ^ For a description of a circulator, see Jachowski (1976)

• Bosma, H. (1964), "On Stripline Y-Circulation at UHF", IEEE Transactions on Microwave Theory and Techniques 12 (1): 61–72, doi:10.1109/TMTT.1964.1125753 
• Chait, H. N.; Curry, T. R. (1959), "Y-Circulator", Journal of Applied Physics Supplement 30 (4): 1525, 1535, doi:10.1063/1.2185863 
• Hogan, C. L. (1953), "The Ferromagnetic Faraday Effect at Microwave Frequencies and its Applications", Reviews of Modern Physics 25 (1): 253–262, doi:10.1103/RevModPhys.25.253 
• US 3935549, Jachowski, Ronald E., "Ferrite Circulator", issued January 27, 1976 
• Ohm, E. A. (1956), "A Broad-Band Microwave Circulator", IRE Transactions on Microwave Theory and Techniques 4 (4): 210–217, doi:10.1109/TMTT.1956.1125064 
• Wenzel, C. (1991), "Low Frequency Circulator/Isolator Uses No Ferrite or Magnet", RF Design, http://www.wenzel.com/pdffiles1/pdfs/RFDesign3.pdf 
• Circulators and Isolators [1]