U.S. patent number 3,602,845 [Application Number 05/006,085] was granted by the patent office on 1971-08-31 for slot line nonreciprocal phase shifter.
This patent grant is currently assigned to The United States of America as represented by the Secretary of the Army. Invention is credited to John P. Agrios, Nathan Lipetz.
United States Patent |
3,602,845 |
Agrios , et al. |
August 31, 1971 |
SLOT LINE NONRECIPROCAL PHASE SHIFTER
Abstract
A nonreciprocal microwave energy phase shifter utilizing a slot
line for propagating microwave energy and a ferrite member which is
magnetically biased to produce a magnetic field therein which is
orthogonal to and interacts with the RF magnetic field cyclically
generated along the slot line. The ferrite may be in the form of a
toroid to provide a closed-loop magnetic field and which is
produced by a latching current.
Inventors: |
Agrios; John P. (Long Branch,
NJ), Lipetz; Nathan (Oakhurst, NJ) |
Assignee: |
The United States of America as
represented by the Secretary of the Army (N/A)
|
Family
ID: |
21719232 |
Appl.
No.: |
05/006,085 |
Filed: |
January 27, 1970 |
Current U.S.
Class: |
333/24.1;
333/238 |
Current CPC
Class: |
H01P
1/195 (20130101) |
Current International
Class: |
H01P
1/18 (20060101); H01P 1/195 (20060101); H01p
001/32 () |
Field of
Search: |
;333/1.1,24.1,84M |
Other References
G H. Robinson et al., Slot Line Application to Miniature Ferrite
Devices, EEE Trans. on MTT, Dec. 1969, pp. 1097-1101 333-84 M .
G. H. Robinson et al., Application of Slot Line To Miniature
Ferrite Devices, 1969 PGMTT Symposium Record, pp. 106-109.
|
Primary Examiner: Saalbach; Herman Karl
Assistant Examiner: Gensler; Paul L.
Claims
What is claimed is:
1. A nonreciprocal microwave energy phase shifter comprising
a ferrite substrate,
a slot line on one surface of said substrate for propagating RF
microwave energy,
and means for producing in said ferrite substrate a magnetic bias
field orthogonally oriented to the RF magnetic field of said
propagated microwave energy.
2. The phase shifter in accordance with claim 1 wherein said slot
line comprises a pair of longitudinally spaced metal strips
separated by a very narrow slot, and wherein said RF magnetic field
is elliptically polarized along said narrow slot.
3. The phase shifter in accordance with claim 2 wherein said
ferrite substrate is in the form of a toroid having a substantial
longitudinal dimension.
4. The phase shifter in accordance with claim 3 wherein said slot
is along a line parallel to the longitudinal axis of said ferrite
toroid.
5. The phase shifter in accordance with claim 3 wherein the
magnetization of said ferrite toroid is characterized by a square
hysteresis loop.
6. The phase shifter in accordance with claim 4 wherein the
magnetization of said ferrite toroid is characterized by a square
hysteresis loop.
7. The phase shifter in accordance with claim 3 wherein said slot
line is on one outer surface of said ferrite toroid and said
magnetic-field bias-producing means is in circuit with a portion of
said ferrite toroid not including said slot line.
8. The phase shifter in accordance with claim 4 wherein said slot
line is on one inner surface of said ferrite toroid and said
magnetic-field bias-producing means is in circuit with a portion of
said ferrite toroid not including said slot line.
9. A nonreciprocal microwave energy phase shifter comprising
a substrate,
a slot line on one surface of said substrate for propagating RF
microwave energy,
a ferrite toroid positioned over said slot line,
and means for producing a closed magnetic-field loop in said
toroid, said magnetic field being characterized by a square
hysteresis loop.
10. The phase shifter in accordance with claim 9 wherein said
substrate is a dielectric.
11. The phase shifter in accordance with claim 10 and further
including a latching current-carrying conductor extending through
the aperture of said ferrite toroid.
12. The phase shifter in accordance with claim 11 wherein said
ferrite toroid is above said slot line.
13. The phase shifter in accordance with claim 10 wherein said
ferrite toroid surrounds said slot line and said dielectric
substrate.
14. The phase shifter in accordance with claim 13 and further
including a central aperture in said dielectric substrate and a
latching current conductor extending through said aperture.
15. The phase shifter in accordance with claim 12 wherein the slot
of said slot line is along a line parallel to the axis of said
ferrite toroid.
16. The phase shifter in accordance with claim 9 wherein said
substrate is a second ferrite toroid.
Description
BACKGROUND OF THE INVENTION
This invention relates to nonreciprocal microwave devices and more
particularly to nonreciprocal phase-shifting devices employing a
slot line for propagating microwave energy. A nonreciprocal
phase-shifting device is one which will shift by a given amount the
phase of microwave energy passing in one direction through the
device and will shift by a different amount the phase of the
microwave energy passing in the opposite direction through such
device. In the microwave region, miniaturization of components
becomes an absolute necessity, and since presently available
phase-shifting devices are rather complicated and bulky, such
devices have proved to be impractical for use in microwave
circuitry.
SUMMARY OF THE INVENTION
It is accordingly an object of the present invention to provide an
improved nonreciprocal phase-shifting device for microwave systems
which are extremely small and light in weight.
It is another object of the present invention to provide an
improved nonreciprocal phase-shifting device adapted for use with
slot lines.
In accordance with one embodiment of the invention, the
nonreciprocal phase shifter includes a ferrite substrate, a slot
line on one surface of the substrate for propagating RF microwave
energy, and means for producing in the substrate a magnetic bias
field orthogonally oriented to the RF magnetic field of the
propagated microwave energy. The ferrite substrate may be in the
form of a toroid having a substantial longitudinal dimension and
have a square hysteresis loop magnetization characteristic.
In another embodiment of the invention, the nonreciprocal phase
shifter includes a dielectric substrate with the slot line on one
surface of the substrate. Also included is a ferrite toroid
positioned over the slot line and means for producing a closed
magnetic field loop in the toroid which is characterized by a
square hysteresis loop.
BRIEF DESCRIPTION OF THE DRAWING
For a better understanding of the invention, together with other
and further objects thereof, reference is made to the following
description taken in connection with the accompanying drawing in
which:
FIG. 1 illustrates one embodiment of the invention;
FIG. 2 illustrates another embodiment of the invention wherein a
ferrite toroid is utilized to provide a latching-type phase
shifter;
FIG, 3 illustrates a modified version of the phase shifter shown in
FIG. 2; and
FIGS. 4 and 5 illustrate a phase shifter in accordance with the
invention wherein a dielectric substrate is utilized as the support
for the slot line.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring now to FIG. 1, there is shown at 10 a ferrite substrate
on which is deposited, by any suitable means well known in the art,
a slot line 12. Slot line 12 comprises a parallel pair of
longitudinally spaced metal strips 14 separated by a very narrow
slot 16. A variable DC magnetic bias field is applied transversely
to ferrite substrate 10 in the direction H by any suitable means
well known in the art. Microwave energy propagated along the slot
line 12 sets up an RF electric field across the slot 16 and an RF
magnetic field as at 17 whose field lines are orthogonal to the RF
electric field. Since the RF magnetic field lines curve and return
to the slot 16 at one-half-wave intervals they may be considered to
be elliptically polarized along the longitudinal dimension thereof.
With the RF magnetic field and DC magnetic bias field orthogonally
oriented as shown, an interaction will occur between the RF
propagating wave and the electron spins of the ferrite to cause the
permeability of the ferrite to be different for the two directions
of microwave propagation. While the physical length of the slot
line 12 will introduce a delay or phase shift in the propagated
microwave energy, the change in permeability in the ferrite
superimposes on this phase shift a further phase shift hereinafter
referred to as a differential phase shift. By changing the
magnitude of the applied DC magnetic bias field across ferrite
substrate 10, the magnitude of the differential phase shift is
changed and hence a variable microwave phase shifter results. The
nonreciprocal characteristic of the phase shifter is due to the
orthogonal orientation of the RF magnetic field and the DC magnetic
bias field which may be varied by any suitable means as, for
example, by an electromagnet.
FIGS. 2-5 illustrate digital-latching-type phase shifters employing
the same principles of operation as that shown in FIG. 1. In these
figures like reference numerals refer to like elements. Referring
now to FIG. 2, at 20 there is shown a ferrite toroid having a
substantial longitudinal dimension and a square hysteresis loop
magnetization characteristic. The slot line 12 is longitudinally
and axially positioned on an outer surface of ferrite 20 such that
the slot 16 of slot line 12 is substantially along a line parallel
to the longitudinal axis of ferrite toroid 20. A single or multiple
wound conductor 22 extends longitudinally through the opening 24 of
ferrite toroid 20 and is looped around an inner and outer surface
of the toroid as shown. The terminals of conductor 22 are connected
to a pulsed DC current source 26. While the conductor 22 is shown
looped around the toroid surface distal the slot line 12, the
conductor loop 22 may also be wound around any other portions of
ferrite toroid 20 which does not include slot line 12. With the
pulsed DC current in the direction shown by arrow 27, the closed
magnetic field path produced in ferrite toroid 20 will be that
indicated at 28. As in FIG. 1, the DC magnetic bias field and the
RF magnetic field of a wave propagated along slot line 12 are
orthogonally oriented to provide the interaction for achieving a
nonreciprocal phase shift of the RF-propagated wave. Latching is
obtained by using the square loop hysteresis characteristic of the
ferrite toroid 20. Thus, after the DC energizing pulse is removed,
the magnetization will follow the square loop hysteresis curve of
the ferrite material so that ferrite toroid 20 will remain
magnetized at remanence. By changing the amplitude or the pulse
width of the current pulse from source 26, the remanent
magnetization of ferrite toroid 20 can be changed to yield a change
in the differential phase shift of the device.
In FIG. 3, slot line 12 is shown positioned longitudinally within
the ferrite toroid 20 along one inner surface thereof. As in FIG.
2, the slot 16 of slot line 12 is along a line parallel to the
longitudinal axis of the toroid 20 and the ferrite is energized by
passing a latching DC current pulse through a suitable wire
conductor 22. The latching and phase-shifting operation of the
device shown in FIG. 3 is similar to that shown in FIG. 2.
In FIG. 4, the slot line 12 is positioned on a dielectric substrate
30 and the ferrite toroid 20 is positioned above the slot line 12
such that the slot 16 is parallel to the longitudinal axis of the
toroid. The ferrite toroid 20 is energized by passing a DC current
pulse through a suitable wire conductor 22 to provide the
orthogonal magnetic bias means. RF energy propagated along slot
line 12 will produce an RF magnetic field which is elliptically
polarized along the longitudinal dimension of slot 12 so that it
interacts with the orthogonally oriented latching magnetic bias. If
desired, substrate 30 may be replaced by a second ferrite toroid
magnetized in a direction opposite to that shown for ferrite toroid
20.
FIG. 5 illustrates another embodiment which employs the same
principle of operation as that shown in FIGS. 1-4. Referring now to
FIG. 5, the substrate 30 on which slot line 12 is longitudinally
positioned is inclosed by ferrite toroid 32. A latching current is
provided by passing a DC pulse through wire conductor 22 which
extends longitudinally through a central aperture 34 provided
therefor in substrate 30.
We wish it to be understood that we do not desire to be limited to
the exact details of construction shown and described, for obvious
modifications will occur to a person skilled in the art.
* * * * *