[0001] This invention relates to a permanent magnet magnetic circuit. Such permanent magnet
magnetic circuits are used in semiconductor manufacturing apparatus and similar apparatus
requiring a unidirectional magnetic field having linear lines of magnetic force in
a desired region and especially useful when restrictions are imposed on their attachment
or arrangement.
BACKGROUND OF THE INVENTION
[0002] Referring to FIG. 11, there is illustrated a first example of prior art permanent
magnet magnetic circuits. The circuit includes a U-shaped yoke 2 having opposed legs.
A pair of permanent magnets 1A and 1B are attached to the inside surfaces of the yoke
legs such that the N pole of one magnet 1A is opposed to the S pole of the other magnet
1 B. This arrangement creates a unidirectional magnetic field containing least of
unnecessary perpendicular magnetic field components.
[0003] In the first prior art circuit of FIG. 1, however, a region E1 where the unidirectional
magnetic field is produced is surrounded at three sides by the magnetic circuit. This
magnetic circuit is not useful where restrictions are imposed on its attachment or
location. For example, this first prior art circuit cannot be applied under the requirement
that the magnetic circuit should not protrude beyond the lower boundary line F1 of
the unidirectional magnetic field generating region E1. Such restrictions arise, for
example, when it is desired for a magnetic circuit located outside a vacuum vessel
to provide a region E1 of unidirectional magnetic field within the vacuum container
interior.
[0004] FIGS. 12 and 13 show a second example of the prior art, illustrating a most fundamental
magnetic circuit. A plate-shaped permanent magnet 5 has N and S poles disposed at
opposite edges. A region E2 of approximate unidirectional magnetic field is available
above (or below) one major surface of the plate-shaped permanent magnet 5 as seen
from FIG. 13. The magnetic circuit can be located only below (or above) the boundary
line F2 of the approximate unidirectional magnetic field region E2.
[0005] FIG. 14 shows the distribution of lines of magnetic force generated in the second
prior art circuit of FIGS. 12 and 13. In this example, the plate-shaped permanent
magnet 5 is a ferrite permanent magnet having a lateral dimension Lx of 250 mm, a
transverse dimension Ly of 300 mm and a thickness Lz of 24 mm.
[0006] Assume that X is a horizontal distance from the center of the plate-shaped permanent
magnet 5 and the vertical distance H from the major surface of the plate-shaped permanent
magnet 5 is fixed to 40 mm. In FIG. 6, broken line curves show horizontal and vertical
(or perpendicular) components Bx and Bz of the magnetic flux density as a function
of distance X in the range of from 0 to W/2 = 80 mm. It is understood from the broken
line curves in FIG. 6 and FIG. 14 that the second prior art circuit of FIGS. 12 and
13 produces a magnetic field which is far from an ideal unidirectional magnetic field
free of perpendicular components since the unnecessary vertical component Bz drastically
increases with the increasing distance X from the center of the plate-shaped permanent
magnet 5.
SUMMARY OF THE INVENTION
[0007] Therefore, an object of the present invention is to provide a permanent magnet magnetic
circuit capable of producing a unidirectional magnetic field free of perpendicular
components and of a simple structure which does not surround the unidirectional magnetic
field producing region.
[0008] In a first form of the present invention, the permanent magnet magnetic circuit includes
a magnet block having a pair of opposite edge surfaces and a pair of major surfaces
between the opposite edge surfaces. A pair of main magnetic poles of opposite polarities
are situated at the opposite edge surfaces. A channel is defined in one major surface.
A pair of auxiliary magnetic poles are situated at a pair of opposed inner surface
portions of the channel disposed inside the main magnetic poles. Each auxiliary magnetic
pole has opposite polarity to that of the corresponding main magnetic pole. The channel
may be recessed stepwise or continuously to define the opposed inner surface portions.
[0009] In a second form of the invention, the permanent magnet magnetic circuit includes
a magnet block having a pair of opposite edge surfaces, with a magnetic pole of one
polarity at one edge surface and a magnetic pole of opposite polarity at the other
edge surface for creating a magnetic field having lines of magnetic force extending
from the one edge surface to the other edge surface. Compensating magnetic poles are
situated between the edge surfaces for controlling the vectorial direction of the
magnetic field.
[0010] In a third form of the invention, the permanent magnet magnetic circuit includes
a magnet block having a pair of opposite edge surfaces. Main magnetic means is provided
for creating a loop pattern of lines of magnetic force extending from the one edge
surface to the other edge surface. Compensating magnetic means is provided for controlling
a middle portion of the lines of magnetic force to be linear. Preferably, the main
magnetic means is comprised of a magnetic pole of one polarity at one edge surface
and a magnetic pole of opposite polarity at the other edge surface, and the compensating
magnetic means is comprised of auxiliary magnetic poles.
[0011] In the permanent magnet magnetic circuit of the present invention, a vertical component
contained in the magnetic field produced between the main magnetic poles (a magnetic
field component perpendicular to the desired unidirectional magnetic field component)
can be offset by a vertical component of opposite orientation contained in the magnetic
field produced between the main and auxiliary (or compensating) magnetic poles. There
can be formed a unidirectional magnetic field free of unnecessary vertical component
over a wide area. The unidirectional magnetic field region is spaced from the magnet
block so that the magnetic circuit does not surround the unidirectional magnetic field
region. The circuit is thus best suited as the unidirectional magnetic field producing
means associated with semiconductor manufacturing apparatus.
BRIEF DESCRIPTION OF THE DRAWINGS
[0012]
FIGS. 1 and 2 are perspective and front elevational views of a permanent magnet magnetic
circuit according to a first embodiment of the present invention, respectively.
FIG. 3 illustrates the distribution of lines of magnetic force near the right edge
of the magnet block in FIG. 2.
FIG. 4 is an enlarged view of a portion of FIG. 3.
FIG. 5 illustrates a vector of the magnetic field between main magnetic poles, a vector
of the magnetic field between a main magnetic pole and a compensating magnetic pole,
and a resultant vector in the first embodiment.
FIG. 6 is a diagram showing the magnetic flux density in horizontal and vertical directions
relative to the distance from the magnet block center in the first embodiment of the
present invention and the second example of the prior art.
FIGS. 7 and 8 are perspective and front elevational views of a permanent magnet magnetic
circuit according to a second embodiment of the present invention, respectively.
FIGS. 9 and 10 are plan and fragmental cross- sectional views of a permanent magnet
magnetic circuit according to a third embodiment of the present invention, respectively.
FIG. 11 is a front elevation of a first example of the prior art magnetic circuit.
FIGS. 12 and 13 are perspective and front elevational views of a second example of
the prior art magnetic circuit, respectively.
FIG. 14 illustrates the distribution of lines of magnetic force near the right edge
of the magnet block in FIG. 13.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0013] Referring to FIGS. 1 and 2, there is illustrated a permanent magnet magnetic circuit
according to a first embodiment of the present invention. The circuit include a rectangular
magnet block 20 of a suitable permanent magnet material such as ferrite or rare earth
permanent magnet. The block 20 has a pair of first and second opposite edge or outer
surfaces and a pair of major surfaces joining the first and second opposite edge surfaces
and extending substantially perpendicular to the edge surfaces. Main magnetic poles
21A and 21B are formed in the first and second opposite edge surfaces by magnetization.
In the illustrated embodiment, the main magnetic poles 21 A and 21 B are N and S poles,
respectively. A channel 22 is defined in one (upper in the illustrated embodiment)
major surface. The channel 22 illustrated herein is a transverse trough extending
throughout the block 20 in a transverse direction and recessed stepwise at the right
and left sides in a symmetrical manner as viewed in the front elevation of FIG. 2.
A flat bottom is connected to the stepwise side walls. The channel includes at least
one pair, three pairs in the illustrated embodiment, of steps defining opposed inner
surface portions disposed inward of the opposite edge surfaces (21A, 21B). Auxiliary
magnetic poles in the form of compensating magnetic poles 23Ai, 23A
2 and 23A3 are formed by magnetization in the inner surface portions on the left side
disposed inward of the main magnetic pole 21A. Similarly, auxiliary magnetic poles
in the form of compensating magnetic poles 23B
i, 23B
2 and 23B
3 are formed by magnetization in the inner surface portions on the right side disposed
inward of the main magnetic pole 21 B. The auxiliary magnetic poles have opposite
polarity to that of the main magnetic poles. The compensating magnetic poles 23Ai,
23A
2 and 23A3 are S poles and the compensating magnetic poles 23B
i, 23B
2 and 23B
3 are N poles.
[0014] If the magnet block 20 is of uniform material, the main and auxiliary magnetic poles
21 and 23 have equal surface magnetic flux density, but the main magnetic poles have
a substantially larger total quantity of magnetic flux. The compensating magnetic
poles 23 function to compensate for magnetic force for tailoring the lines of magnetic
force produced by the main magnetic poles 21 to be linear.
[0015] FIG. 3 shows the distribution of lines of magnetic force generated in the magnetic
circuit embodiment of FIGS. 1 and 2. FIG. 4 is an enlarged view of a portion of FIG.
3. In this embodiment, the magnet block 20 is a ferrite permanent magnet having a
lateral dimension Lx of 250 mm, a transverse dimension Ly of 300 mm and a thickness
Lz of 60 mm and the channel 22 defined therein includes three pairs of opposed steps
each having a lateral width of 20 mm and a height of 10 mm.
[0016] Assume that X is a horizontal distance from the center (depicted by a phantom line)
of the magnet block 20 and the vertical distance H from the upper major surface of
the magnet block 20 is fixed to 40 mm. In FIG. 6, solid line curves show horizontal
and vertical (or perpendicular) components Bx and Bz of the magnetic flux density
as a function of distance X in the range of from 0 to W/2 = 80 mm.
[0017] It is understood from FIGS. 3 and 4 and the solid line curves in FIG. 6 that the
first embodiment of FIGS. 1 and 2 produces a magnetic field whose unnecessary vertical
component Bz is substantially equal to zero over a substantial portion of the X range.
The reason is given below. As shown in FIG. 5 taken together with FIG. 2, at a point
P in the region where a unidirectional magnetic field is to be produced, the magnetic
field has a vector V1 directing from the main N pole toward the main S pole and a
vector V2 extending between each main magnetic pole (N or S pole) and each compensating
magnetic pole (S or N pole). The magnetic poles are arranged such that the resultant
magnetic field vector VO may become substantially horizontal.
[0018] Consequently, the first embodiment of FIGS. 1 and 2 produces a nearly ideal unidirectional
magnetic field substantially free of unnecessary perpendicular components over a wide
range. The magnetic circuit may be located on one side of the unidirectional magnetic
field region because the magnetic circuit does not enclose the unidirectional magnetic
field.
[0019] FIGS. 7 and 8 show a second embodiment of the present invention. This embodiment
is similar to the first embodiment except the channel geometry. Instead of the stepwise
side wall channel, the magnet block 20 includes a continuously or smoothly recessed
channel 30 in one major surface between the opposite edge surfaces. The continuous
channel used herein means that the opposed inner side walls are curvilinear or rectilinear
slant walls joining to a flat bottom. The inner side walls are symmetrical as viewed
in the elevation of FIG. 8. Compensating magnetic poles 23A and 23B are formed by
magnetization in the opposed inner side walls disposed inward of the main magnetic
poles 21A and 21B, respectively. In the illustrated embodiment, the main magnetic
poles 21A and 21 B are N and S, and the compensating magnetic poles 23A and 23B are
S and N, respectively.
[0020] In this embodiment, the magnet block 20 is a ferrite permanent magnet having a lateral
dimension Lx of 250 mm, a transverse dimension Ly of 300 mm and a thickness Lz of
60 mm and the channel 30 defined therein includes a flat bottom having a lateral dimension
of 130 mm and a thickness of 30 mm.
[0021] Also in the second embodiment of FIGS. 7 and 8, the magnetic poles are arranged such
that the resultant magnetic field vector VO between a vector V1 directing from the
main N pole toward the main S pole and a vector V2 directing from each main magnetic
pole (N or S pole) toward each compensating magnetic pole (S or N pole) in the region
where a unidirectional magnetic field is to be produced as shown in FIG. 5 becomes
substantially horizontal.
[0022] FIGS. 9 and 10 show a third embodiment of the present invention. This embodiment
is similar to the first embodiment except the block geometry. Used in this embodiment
is a disk-shaped magnet block 40 having a pair of opposite edge surface segments,
that is, arcuate segments included within angles 81 and 02 where main magnetic poles
41A and 41B are formed by magnetization. The main magnetic poles 41A and 41B are N
and S poles, respectively, in the illustrated embodiment. The magnet block 40 has
a pair of major surfaces joining the opposite edge surface segments (41A and 41 B)
and extending substantially perpendicular to the segments (in the cross section of
FIG. 10). A transverse channel 42 is defined in one major surface. The channel 42
has symmetric steps defining pairs of opposed inner surface portions disposed inward
of the opposite edge surface segments. As seen from FIG. 10, in the opposed inner
surface portions disposed inward of the main magnetic pole 41B of one polarity are
formed compensating magnetic poles 43Bi, 43B
2 and 43B
3 of opposite polarity by magnetization. Similarly, in the opposed inner surface portions
disposed inward of the main magnetic pole 41A of opposite polarity are formed compensating
magnetic poles of one polarity.
[0023] The results of the third embodiment are equivalent to those of the first embodiment.
[0024] In all the embodiments, the magnet block may be either a unitary permanent magnet
block or an assembly of a plurality of permanent magnet pieces.
[0025] There has been described a permanent magnet magnetic circuit capable of producing
a unidirectional magnetic field substantially free of unnecessary perpendicular magnetic
force components without surrounding the region where the unidirectional magnetic
field is to be produced. The magnetic circuit is advantageously applicable to semiconductor
fabricating apparatus and similar apparatus where restrictions are imposed on the
attachment or location of the circuit.
[0026] While we have shown and described particular embodiments of our invention, it will
be obvious to those skilled in the art that various changes and modifications may
be made without departing from the invention in its broader aspects.
1. A permanent magnet magnetic circuit comprising
a magnet block having a pair of opposite edge surfaces and a channel defined between
said opposite edge surfaces, said channel including a pair of opposed inner surface
portions disposed inward of said opposite edge surfaces,
a pair of main magnetic poles of opposite polarities situated at said opposite edge
surfaces,
a pair of auxiliary magnetic poles situated at said opposed inner surface portions,
each auxiliary magnetic pole having opposite polarity to that of the corresponding
main magnetic pole.
2. The magnetic circuit of claim 1 wherein said channel is recessed stepwise to define
said opposed inner surface portions.
3. The magnetic circuit of claim 1 wherein said channel is continuously recessed to
define said opposed inner surface portions.
4. The magnetic circuit of claim 1 wherein said magnet block is of rectangular shape.
5. The magnetic circuit of claim 1 wherein said magnet block is of circular shape.
6. A permanent magnet magnetic circuit comprising
a magnet block having a pair of opposite edge surfaces,
a magnetic pole of one polarity at one edge surface and a magnetic pole of opposite
polarity at the other edge surface for creating a magnetic field having lines of magnetic
force extending from the one edge surface to the other edge surface, and
compensating magnetic poles situated between said edge surfaces for controlling the
vectorial direction of said magnetic field.
7. A permanent magnet magnetic circuit comprising
a magnet block having a pair of opposite edge surfaces,
a magnetic pole of one polarity at one edge surface and a magnetic pole of opposite
polarity at the other edge surface for creating a loop pattern of lines of magnetic
force extending from the one edge surface to the other edge surface, and
compensating magnetic pole means for controlling a middle portion of said lines of
magnetic force to be linear.