FIELD OF THE INVENTION
[0001] This invention relates to a magnetic device which utilizes an abrupt change in magnetization
that occurs in response to a change in an externally applied magnetic field. The invention
also relates to a process and an apparatus for producing the magnetic device.
BACKGROUND OF THE INVENTION
[0002] The magnetization behavior of magnetic materials has been extensively utilized in
various devices. Magnetic materials that are recently drawing the attention of researchers
include those which, when the strength of a magnetic field exceeds a certain critical
value, exhibit a sudden magnetic flux reversal as a discontinuous response. If a pickup
coil is placed in the neighborhood of such a magnetic material, a sharp voltage pulse
is induced by the discontinuous magnetic flux reversal in the magnetic material. The
resulting signal finds wide use in various magnetic devices for measuring magnetic
fields (e.g., the earth's field), rotational speeds and flow rates.
[0003] Electronic article surveillance systems for preventing the theft of merchandise and
article identification systems for enabling rapid delivery have recently gained in
popularity. In addition to oscillation circuits, LC resonant circuits, magnetostrictive
resonance materials and high permeability materials, magnetic materials which exhibit
the above-described discontinuous magnetic flux reversal are used as identification
markers. For example, Examined Japanese Patent Publication No. Hei-3-27958 (corresponding
to U.S. Patents 4,660,025, 4,686,516 and 4,797,658) teaches a marker in the form of
a filament of an Fe-based amorphous metal and a system using the marker.
[0004] The magnetization of the metal filament in a longitudinal direction is sufficiently
stable so as not to readily undergo magnetic flux reversal, but the moment an externally
applied magnetic field reaches a certain magnitude, a 180° magnetic flux reversal
occurs very abruptly. This property, which is also called a "large Barkhausen reversal",
is utilized in the anti-theft systems described above. If an alternating magnetic
field transmitted as an interrogating signal in the surveillance zone reaches a critical
value, the metal filament undergoes a discontinuous magnetic flux reversal and an
abrupt voltage pulse is induced in the detection coil. The waveform of the resulting
pulse is subjected to frequency analysis and in accordance with the intensity or proportion
of higher-order harmonic waves, the marker signal is used to determine whether an
alarm should be sounded. This system is advantageous in that the marker is inexpensive
and provides a highly discriminating performance.
[0005] In addition to the above-described amorphous metal filament, many other magnetic
materials have been found to exhibit a discontinuous magnetization response. For example,
Unexamined Published Japanese Patent Application No. Hei-1-150881 (corresponding to
U.S. Patent 4,980,670) and No. Hei-6-94841 (corresponding to U.S. Patent 5,313,192)
teach materials obtained by annealing elongated amorphous metal ribbons in a magnetic
field. According to Unexamined Published Japanese Patent Application No. Hei-4-218905
(corresponding to U.S. Patent 5,181,020), a thin film having a strong uniaxial magnetic
anisotropy which is formed on a flexible polymeric substrate such as a resin film
exhibits a discontinuous magnetic flux reversal and has good square hysteresis loop
characteristics similar to the metal filament.
[0006] The thin film described in Unexamined Published Japanese Patent Application No. Hei-4-218905
(corresponding to U.S. Patent 5,181,020) produces an abrupt and discontinuous magnetization
response similar to the amorphous metal filament if it is rendered in an elongated
form measuring, for example, 1 mm wide by 50 mm long by 0.5 µm thick along the axis
that is easily magnetized (the magnetic easy axis). However, the magnetic characteristics
of the thin film are highly sensitive to a demagnetizing field and have been found
to deteriorate markedly when provided in a shorter, wider and thicker form. Although
there is a strong need today for miniaturizing sensors and anti-theft markers, it
cannot be met by the above noted magnetic materials because they cannot provide an
abrupt and discontinuous magnetization response unless provided in an elongated form.
SUMMARY OF THE INVENTION
[0007] The present invention has been accomplished in view of the above problems of the
prior art.
[0008] It is therefore an object of the present invention to provide a magnetic device which
exhibits satisfactory magnetic characteristics despite its compact size. Another object
of the invention is to provide a process for easily producing the magnetic device.
A further object of the invention is to provide an apparatus for easily producing
the magnetic device.
[0009] The above objects have been achieved, in a first embodiment of the present inventions,
by providing a magnetic device comprising a soft magnetic thin film formed on a substrate,
said soft magnetic thin film includes a central area and a second area having a film
thickness that is smaller than that of the central area, and wherein said magnetic
device has a magnetic hysteresis loop which exhibits a discontinuous magnetization
reversal.
[0010] In a second embodiment of the present invention, the soft magnetic thin film of said
second area has a film thickness gradient.
[0011] In a third embodiment, the present invention provides a process for producing the
above-described magnetic device, which comprises:
positioning a mask member having an opening over said substrate with sufficient clearance
so as not to contact the substrate, and
depositing a magnetic thin film through the opening of said mask member and onto said
substrate.
[0012] In a fourth embodiment, the present invention provides a process for producing the
above-described magnetic device, which comprises:
winding a substrate on a cylindrical can,
winding a mask member having an opening corresponding to the shape of said thin film
onto said substrate via a spacer so as not to contact the substrate, and
depositing a soft magnetic thin film through the opening of said mask member and onto
said substrate.
[0013] In a fifth embodiment, the present invention provides a process for producing the
above-described magnetic device, which comprises:
winding a substrate on a cylindrical can,
positioning a mask member having an opening corresponding to the shape of said thin
film over said substrate with sufficient clearance so as not to contact said substrate,
and
depositing a soft magnetic film through the opening of said mask member and onto said
wound substrate.
[0014] In a sixth embodiment, the present invention provides an apparatus for producing
the above-described magnetic device, which comprises:
means for superposing, in the following order, (1) a substrate, (2) a spacer and (3)
a mask member having an opening corresponding to the shape of said thin film around
a cylindrical can in such manner that the mask member does not contact the substrate,,
means for depositing a soft magnetic thin film through the opening of said mask member
and onto said substrate, and
means for winding the superposed substrate, spacer and mask member.
[0015] In a seventh embodiment, the present invention provides an apparatus for producing
the above-described magnetic device,
means for winding a substrate or a cylindrical can,
means for positioning a mask member having an opening corresponding to the shape of
said thin film over said substrate with sufficient clearance so as not to contact
said substrate, and
means for depositing a soft magnetic film through the opening of said mask member
and onto said wound substrate
[0016] In an eighth embodiment, the present invention provides a process for producing a
magnetic device comprising a thin film formed on a substrate, including a central
area and a second area having a film thickness that is smaller than that of the central
area, which comprises:
positioning a mask member between said substrate and a thin film deposition source,
to thereby selectively block deposition from said deposition source, and
depositing a thin film onto said substrate while moving said mask member and said
substrate relative to each other, to thereby vary the area blocked by said mask member
over time and form said second area having a reduced film thickness.
[0017] The magnetic device of the present invention has a discontinuous magnetization response
characteristic which is not overly sensitive to the shape of the magnetic device.
Hence, the magnetic device of the invention exhibits satisfactory magnetic characteristics
despite its compact size.
[0018] The process and apparatus of the present invention enable easy production of a compact
magnetic device having a discontinuous magnetization response characteristic.
BRIEF DESCRIPTION OF THE DRAWINGS
[0019] Fig. 1 is a simplified schematic diagram showing an example of the magnetic device
of the present invention.
[0020] Fig. 2 is a simplified schematic diagram showing another example of the magnetic
device of the present invention.
[0021] Fig. 3 is a simplified schematic diagram showing yet another example of the magnetic
device of the present invention.
[0022] Fig. 4 is a simplified schematic diagram showing an example of the apparatus for
producing the magnetic device of the present invention.
[0023] Fig. 5 shows a partially enlarged view of the film forming zone of the apparatus
of Fig. 4, and particularly the relative positions of a substrate, mask member and
spacer provided therebetween.
[0024] Fig. 6 is a simplified schematic diagram illustrating the operating principle of
the second production process of the present invention.
[0025] Fig. 7 is a simplified schematic diagram showing another example of the apparatus
for producing the magnetic device of the present invention.
[0026] Fig. 8 is a simplified schematic diagram showing two different ways to cut out the
magnetic device of the present invention from a substrate with a thin film produced
with the apparatus of Fig. 7.
[0027] Fig. 9 is a simplified schematic diagram showing an example of thin film deposition
with a mask member fixed on a substrate.
[0028] Fig. 10 is a simplified schematic diagram showing an example of thin film deposition
with a rod of a mask member set on a substrate such that its longitudinal direction
coincides with the direction of movement of the substrate.
[0029] Fig. 11 is a simplified schematic diagram showing an example of thin film deposition
with a rod of a mask member set obliquely on a substrate such that its longitudinal
direction forms a certain angle with the direction of movement of the substrate.
[0030] Fig. 12 is a simplified schematic diagram showing an example of thin film deposition
with a sawtooth edged a mask member set on a substrate.
[0031] Fig. 13 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Example 1.
[0032] Fig. 14 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Comparative Example 1.
[0033] Fig. 15 is a graph showing the thickness gradient of the thin film formed in Example
2.
[0034] Fig. 16 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Example 2.
[0035] Fig. 17 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Comparative Example 2.
[0036] Fig. 18 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Example 3.
[0037] Fig. 19 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Example 4.
[0038] Fig. 20 is a diagram showing the hysteresis loop of the magnetic device manufactured
in Comparative Example 3.
DETAILED DESCRIPTION OF THE INVENTION
[0039] The present invention will now be described in further detail with reference to the
accompanying drawings. The magnetic devices according to the first and second embodiments
of the present invention are described first.
[0040] The magnetic device of the present invention comprises a soft magnetic thin film
formed on a substrate comprising an area having a smaller film thickness than the
central area of the soft magnetic thin film. The soft magnetic thin film formed in
that area desirably has a film thickness gradient.
[0041] Fig. 1 is a simplified schematic diagram showing an example of the magnetic device
of the present invention. Fig. 1(a) is a plan view of the magnetic device and Fig.
1(b) is a section A-A' of Fig. 1(a). The magnetic device generally indicated by 1
in Fig. 1 is circular and an area 2 extending from position C to either end E has
a smaller film thickness than the central area 3, and the film thickness of the area
2 progressively decreases toward either end.
[0042] Fig. 2 is a simplified schematic diagram showing another example of the magnetic
device of the present invention. Similar to Fig. 1, Fig. 2(a) is a plan view of the
magnetic device, and Fig. 2(b) is a section A-A' of Fig. 2(a). The magnetic device
generally indicated by 1 in Fig. 2 is rectangular, and an area 2 extending from position
C to either end E has a smaller film thickness than the central area 3. Furthermore,
the film thickness of the area 2 decreases progressively toward either end of the
longer side.
[0043] Fig. 3 is a simplified schematic diagram showing yet another example of the magnetic
device of the present invention. Similar to Fig. 1, Fig. 3(a) is a plan view of the
magnetic device and Fig. 3(b) is a section A-A' of Fig. 3(a). The magnetic device
generally indicated by 1 in Fig. 3 is rectangular and two areas 2 extending from position
C to D have a smaller film thickness than the central area 3. Furthermore, the area
between position D and either end E has the same film thickness as the central area.
[0044] With an area or areas thus formed being a smaller film thickness than the central
area, the direction of magnetization of the magnetic device is reversed momentarily
in a critical magnetic field, whereupon an abrupt magnetic pulse is radiated to the
surroundings.
[0045] It should be noted that in the magnetic device of the invention, the soft magnetic
thin film is present even in the area or areas which have a smaller film thickness
than the central area. The magnetic device shown in Fig. 3 has a film thickness that
is controlled to be smaller not at opposite ends but in areas slightly offset toward
the center. If the film thickness of these areas is zero, the thin film is interrupted
in the middle, such that the first object of the invention is not attained. On the
other hand, the magnetic devices shown in Figs. 1 and 2 have a film thickness that
is controlled to be smaller at opposite ends such that the film thickness decreases
progressively toward either end until it becomes zero at the farthest end. These magnetic
devices produce sufficiently abrupt magnetic pulses to attain the first object of
the present invention.
[0046] In the case of controlling the film thickness at either end as shown in Figs. 1 and
2, the film thickness of the magnetic device preferably decreases progressively over
a length of about 1 to 20 mm, more preferably 2 to 10 mm, and it becomes almost zero
at the farthest end of the device. The gradient of such a decrease in film thickness
is desirably low.
[0047] In the case of controlling areas slightly offset from either end toward the center
as shown in Fig. 3, the film thickness of the magnetic device preferably changes over
a length of about 0.1 to 5 mm, more preferably 0.5 to 2 mm such that the smallest
thickness ranges preferably from about 10% to about 80% of the thickness in the central
area. This range is more preferably from about 20% to about 70%, and most preferably
about 30% to about 65%.
[0048] The composition of the magnetic device of the present invention is selected in consideration
of both the magnetic characteristics of the thin film
per se and the characteristics required by the magnetic device. For example, the soft magnetic
thin film either has uniaxial magnetic anisotropy or it may be isotropic. If the magnetic
device is to be manufactured using an isotropic thin film, satisfactory device characteristics
are easier to obtain with the circular shape shown in Fig. 1 than with the rectangular
shapes shown in Figs. 2 and 3. On the other hand, if the magnetic device is to be
manufactured using a thin film having uniaxial magnetic anisotropy, satisfactory device
characteristics can be easily obtained even if the thin film is rectangular as shown
in Figs. 2 and 3. In this case, the magnetic easy axis of the rectangular thin film
may be aligned with the direction A-A' such that the areas with a controlled thin
film cross the magnetic easy axis to cover the entire width of the magnetic device.
Preferably, the magnetic easy axis forms an angle of no more than 20°, more preferably
no more than 10°, with the lengthwise direction of the magnetic device. Most preferably,
the two directions are parallel to one another.
[0049] The areas of the magnetic device where the film thickness is controlled to be smaller
than in the central area may be at either end of the device as shown in Fig. 2 or
slightly offset therefrom toward the center as shown in Fig. 3. In the case of Fig.
3, the device characteristics thus obtained tend to be highly reproducible. On the
other hand, more abrupt magnetic pulses are sometimes obtained in the case of Fig.
2. Therefore, the areas of the magnetic device where the film thickness is controlled
to be smaller than in the central area may be determined as appropriate depending
on the intended application.
[0050] The general size of the magnetic device of the present invention is as follows. In
the case of the circular ones, the diameter is generally within the range of from
8 mm to 70 mm, preferably 20 mm to 40 mm. In the case of the rectangular ones, the
length of the shorter side is generally within the range of from 0.5 mm to 40 mm,
preferably from 1 mm to 20 mm, and the length of the longer side is generally within
the range of from 10 mm to 70 mm, preferably from 20 mm to 50 mm. Too short diameter
of the circular magnetic device or too short length of the shorter side of the rectangular
magnetic device is not preferable since the abrupt magnetization reversal would not
be obtained or the intensity of the signal radiated to the surroundings by the magnetization
reversal is not sufficient. On the other hand, too long diameter of the circular magnetic
device or too long length of the shorter side of the rectangular magnetic device is
not preferable since the abrupt magnetization reversal would not be obtained or the
large device is not easy to handle. In addition, too short length of the longer side
of the rectangular magnetic device is not preferable since the abrupt magnetization
reversal would not be obtained, and too long length of the longer side of the rectangular
magnetic device is not preferable since the large device is not easy to handle. In
addition to the circular magnetic devices and rectangular magnetic devices described
above, magnetic devices of other shapes have similar tendencies.
[0051] The operating mechanism of the magnetic device of the present invention is discussed
below as follows. With respect to a magnetic material which experiences magnetic flux
reversal as a result of the motion of magnetic domain walls, when the walls of reverse
domains generated at either end of a sample of the magnetic material jump by moving
very fast the moment the applied magnetic field reaches a critical value, abrupt magnetic
pulses are radiated to the surroundings. On the other hand, the shorter and wider
the shape of the sample, the greater the demagnetizing field that works on the sample.
This makes the sample less likely to be magnetized but, at the same time, the discontinuous
behavior of reverse domains is suppressed. Because of this effect, it has been extremely
difficult to realize satisfactorily compact magnetic devices as discussed above.
[0052] In order to avoid the influence of the demagnetizing field, it would be effective
to constrain the magnetic walls of reverse domains by a certain kind of force, and
to have them jump by releasing the constraint the moment a magnetic field having a
particular strength is reached. This force which constrains the magnetic walls is
called a "pinning" force, and in the present invention, the film thickness is controlled
in selected areas to thereby provide an effect that is comparable to a pinning force.
The coercivity of the thin film largely depends on its thickness and increases with
an increasing film thickness. If the film thickness is reduced at either end, the
coercivity of that area becomes greater than that of the other areas. As a result,
the movement of the magnetic walls of the reverse domains present in that area is
restricted such that they will move slowly as the strength of the external magnetic
field increases. With the gradual increase in the external magnetic field, the tips
of the reverse domains move inwardly. The moment they reach the central area beyond
the areas having a controlled film thickness, the magnetic domain walls move fast
enough to complete a magnetic flux reversal. This is because the central area has
a smaller coercivity due to a sufficient film thickness. As a result of this rapid
movement of the magnetic flux domains, abrupt magnetic pulses are radiated to the
surroundings.
[0053] The above-described mechanism is realized in any of the magnetic devices shown in
Figs. 1 to 3. It should also be noted that in magnetic devices which have a controlled
film thickness at either end as in Figs. 1 and 2, an additional mechanism may come
into play depending on the composition of the device to thereby generate magnetic
pulses. For example, in a magnetic device having a geometry such that the film thickness
decreases progressively toward either end, the magnetic field leakage will act on
both ends. This produces a local distribution of the demagnetizing field which is
entirely different from what develops in a geometry having no changes in film thickness.
Because of these effects, the domain structure at the farthest ends of the magnetic
device becomes very stable and will not easily change. Ideally, such a magnetic device
does not develop a closure domain structure, but develop a single domain at the farthest
ends. Thus, upon the application of an external magnetic field, new reverse domains
will nucleate. If the nucleating magnetic field is greater than the coercivity of
the film, the magnetic domain walls will move very fast the moment the reverse domains
have nucleated and magnetic pulses subsequently radiate.
[0054] Specific examples of the alloy composition of the soft magnetic thin film of the
magnetic device of the present invention include crystalline materials such as NiFe,
FeAlSi, FeAl and FeSi, fine crystalline Fe or Co alloy materials containing B, C,
N, O, etc., and amorphous materials such as CoFeSiB, CoZrNb and FeC.
[0055] To form thin films of these materials, evaporation, plating and other commonly known
techniques may be employed. In the present invention, the use of a sputtering process
is particularly preferred.
[0056] Depending on its composition, the magnetic device of the invention may desirably
have uniaxial magnetic anisotropy. This property can be imparted by various methods
such as the application of stress to the magnetic device, annealing in a uniaxial
magnetic field, and annealing under an applied stress. An especially preferred sputtering
method is described in Unexamined Published Japanese Patent Application No. Hei-4-218905
(corresponding to U.S. Patent 5,181,020), in which thin-film forming particles impinge
on a substrate at an angle. According to this method, strong uniaxial magnetic anisotropy
is readily induced in the sputtered film as such, to thereby produce a soft magnetic
thin film having satisfactory magnetic characteristics.
[0057] Unexamined Published Japanese Patent Application No. Hei-7-220971 (corresponding
to EP-A-737,949) teaches another method of imparting uniaxial magnetic anisotropy.
According to this published patent application, a magnetostrictive thin film is formed
on a resin substrate having anisotropic thermal shrinkage under appropriate conditions.
As a result, not only is uniaxial magnetic anisotropy induced in compliance with the
anisotropic thermal shrinkage of the substrate, but a soft magnetic property is also
ensured.
[0058] The magnetic device of the invention comprises a soft magnetic thin film formed on
a substrate. The substrate is not limited to any particular type, and can be selected
from common types such as glass, metals and resins. The use of a polyethylene terephthalate
(PET) film is preferred since it is flexible and suited to large-scale production.
[0059] The magnetic device of the present invention has magnetic characteristics which exhibit
an abrupt magnetic flux reversal in magnetic hysteresis, and it is characterized in
that its discontinuous magnetization response characteristics are not so sensitive
to the device shape. As already noted, conventional materials are highly affected
by a demagnetizing field, and their characteristics have been found to abruptly deteriorate
when fabricated in a wider and shorter form. However, the magnetic device of the present
invention is less affected by the shape factor, and will effectively operate in sizes
of one inch or less to produce a discontinuous abrupt magnetic flux reversal even
if it is of a geometry having a high demagnetizing field coefficient. Consequently,
the present invention provides a very effective solution for meeting the need for
smaller sensors and markers which is sure to become more pressing in the years to
come.
[0060] Next, the process for producing the magnetic device of the present invention is described
below. The production of the magnetic device of the present invention starts with
preparing a thin film having a thickness difference in selected areas. This may be
effectively accomplished by plasma or acid etching of a thin film which is exposed
in only those areas where the film thickness needs to be controlled, but which is
covered in other areas. However, it is more advantageous from the viewpoint of productivity
and the like to cover a selected area of the substrate with a mask member during film
formation so that the deposition of particles in that area is restricted to reduce
the thickness of the film being formed in that area.
[0061] Thus, according to the first embodiment of the process for producing the magnetic
device of the present invention, a mask member having a shape which restricts the
inflow of particles deposited on a substrate is set with a sufficient clearance to
prevent contact with the substrate, and wherein said clearance effectively controls
the thickness gradient of the film that is formed.
[0062] It is a commonly adopted practice to form a patterned thin film on a substrate with
a mask member placed in contact with the substrate in order to restrict the inflow
of particles deposited on the substrate. However, according to this method, there
is no film deposition under the mask member, whereas a film of the same thickness
is deposited in those areas corresponding to the mask openings. Hence, cannot be used
to produce a thin film for the magnetic device of the present invention which has
a thickness difference in selected areas.
[0063] On the other hand, if a mask member having a desired shape in accordance with the
size and characteristics of the magnetic device is set with a sufficient clearance
to prevent contact with the substrate as a thin film is formed thereon, the vapourized
film-forming particles will pass around behind the shade of the mask member. This
results in a deposit on the corresponding areas of the substrate, to thereby form
a thin film having a thickness gradient which gradually decreases in thickness. By
cutting the substrate with the thus obtained thin film to a device shape such that
it has a smaller film thickness in areas other than the central area, the magnetic
device of the present invention can be produced which exhibits a discontinuous abrupt
magnetic flux reversal.
[0064] In the present invention, the gradient of film thickness is chiefly controlled by
the clearance (distance) between the substrate and the mask member. On the other hand,
the amount of particles that pass around behind the shade of the mask member to deposit
on corresponding areas of the substrate is largely influenced by the shape of the
apparatus employed and its characteristics such as the mean free path and the plasma
density which are determined by the operating pressure. Therefore, the distance between
the substrate and the mask member cannot be specified by any unique value, except
that a distance of about 0.1 to 5 mm is generally preferred.
[0065] If a thin film is formed with a flat substrate such as a glass plate that is successively
fed into the film forming stage, a flat plate mask member can be superposed on the
substrate with a spacer typically interposed therebetween to provide the necessary
clearance from the substrate. Hence, the production process of the present invention
is relatively easy to implement.
[0066] On the other hand, if a roll-to-roll apparatus is employed such that a highly flexible
resin film is fed into the film forming stage as it is wound in a roll and a deposited
film is then taken up, the mask member is not easy to set since the film is formed
on the substrate which is wound around a cylindrical can. Therefore, the present invention
also provides a process and an apparatus for efficiently producing the above-described
magnetic device of the present invention using a roll-to-roll apparatus. The process
and apparatus for attaining this aspect of the invention are described in detail below.
[0067] According to the first embodiment of the process of the present invention, a thin
film is formed on a continuous substrate which is wound onto a cylindrical can in
the roll-to-roll apparatus as follows. To produce the intended magnetic device by
this process, a mask member of a given shape and having an opening of a given shape
for restricting the inflow of particles deposited on the substrate is wound around
the can superposed on the substrate with a spacer provided therebetween to prevent
contact with the substrate. The thin film is formed on the substrate as the substrate,
the spacer and the mask member are taken up.
[0068] The mask member for use in the present invention may be selected from among metal
(e.g. stainless steel) foils, glass cloths, resin films, etc. The mask member is wrapped
around the cylindrical can with the interposed spacer to provide sufficient clearance
from the substrate and, hence, may occasionally fail to be thoroughly cooled with
the can. If, on account of this insufficient cooling, the mask member is heated during
deposition by sputtering, evaporation and the like methods, the mask member is preferably
made of a heat-resistant material such as glass, metal or a polyimide.
[0069] An example of the spacer for use in the present invention is a beam-like element
consisting of a plurality of metal wires running parallel to each other. Metal wires
such as copper wires are preferred as the spacer because the distance from the substrate
can be controlled by the wire diameter and because the metal wires have a high heat
resistance. As discussed above, the preferred range of the wire diameter is not uniquely
determined since it depends on the apparatus used to produce the magnetic device of
the invention. Generally speaking, the range of the wire diameter is from about 0.5
to about 5 mm.
[0070] Fig. 4 is a simplified schematic diagram showing an example of the roll-to-roll apparatus
for producing the magnetic device of the present invention. Fig. 5 shows a partially
enlarged film forming zone of the apparatus of Fig. 4, particularly the relative positions
of the substrate 4, mask member 10 and spacer 9 provided therebetween.
[0071] As shown in Fig. 5, the mask member 10 has a circular opening 13 because the magnetic
device to be produced is of the circular type shown in Fig. 1; however, the present
invention is not so limited, and an opening of a desired shape may be provided in
the mask member 10.
[0072] Because vapourized film-forming particles will pass around behind the mask member
and deposit in corresponding areas of the substrate, the area where the particles
are deposited to form a thin film accordingly becomes larger than the opening in the
mask member. Considering this fact, the opening provided in the mask member may be
rendered somewhat smaller than the magnetic device that is to be finally produced.
As an example, a circular opening having a size of about 15 to 22 mm will suffice
if a magnetic device with a diameter of 25 mm is required.
[0073] In Fig. 5, only one opening is provided in the mask member but this is just for the
sake of convenience in explanation. In order to realize mass production of magnetic
devices, a plurality of openings are preferably arranged side by side so that many
magnetic devices can be simultaneously manufactured in one step. In this case, utmost
care must be exercised in determining the distance between openings provided in the
mask member. As discussed above, due to the clearance between the mask member and
the substrate, a thin film will be deposited considerably outward from the opening
in the mask member. If the distance between openings is unduly small, the individual
devices will overlap. Therefore, the distance between openings formed in the mask
is preferably as large as possible, and are generally spaced by at least 10 mm, possibly
at least 15 mm. As an example, if magnetic devices having a diameter of 25 mm are
to be manufactured on a film substrate having a width of 1 m, about 20 to 30 openings
can be provided per 1 m of the mask member in both horizontal and vertical directions.
Hence, about 400 to 900 magnetic devices can be manufactured simultaneously per square
meter of the mask member.
[0074] As shown in Figs. 4 and 5, metal wires as spacers 9 are placed on top of the substrate
4 and the mask member 10 having a circular opening 13 is placed on the spacers 9 such
that the substrate 4, the spacers 9 and the mask member 10 are wound around a can
11 in superposition on each other. Thin-film forming particles 14 pass through the
circular opening 13 to deposit on the substrate 4. Because the spacers 9 provide a
certain clearance between the substrate 4 and the mask member 10, the particles 14
will pass around behind the mask member in an area near the circular opening 13 to
deposit in a corresponding area of the substrate 4. As a result, a thin film is deposited
on the substrate 4 to a larger extent than the diameter of the circular opening 13,
and the area of the deposited thin film which is near the circumference decreases
in film thickness towards the peripheral edge thereof.
[0075] The apparatus for producing magnetic devices by the above method has both means for
winding the substrate, the spacer and the mask around the can in superposition, and
means for taking up the overlapping substrate, spacer and mask member. In order to
wind the respective materials for the substrate, spacer and mask member around the
can in superposition and to take them up after a thin film has been formed, a roll
of the respective superposed materials may be fed into the film coater unit. In the
film coater unit, the superposed materials are wound onto the can, and the substrate
is taken up together with the deposited film. Alternatively, the respective materials
may be separately fed into the film coater unit such that they are superposed on the
can 11 and, after a thin film has been formed, the respective materials are separately
taken up (this is the method illustrated in Fig. 4).
[0076] Referring to Fig. 4, the substrate 4, the spacer 9 and the mask member 10 are supplied
by associated feed rolls 8 and guide rolls 7, and are superposed on each other on
the peripheral surface of the can 11. As the can 11 rotates in the direction of the
arrow shown in Fig. 4, the superposed materials are fed onto a deposition source 12,
where a thin film is deposited on the substrate. Thereafter, the substrate with the
deposited film, the spacer and the mask member pass on associated guide rolls 6 and
are wound up by associated take-up rolls 5.
[0077] Thus, the mask member is supplied in a continuous form such as a film or a foil and
onto a deposition source simultaneously with the substrate on which a thin film is
being formed. This method provides great latitude in selecting the shape of the magnetic
device depending upon the shape of the opening in the mask member and, hence, is suitable
for producing circular magnetic devices. In addition, the clearance between the mask
member and the substrate can be held constant, and this is very effective for controlling
the film thickness.
[0078] If rectangular magnetic devices of the types shown in Figs. 2 and 3 are to be produced
by a roll-to-roll apparatus, a more simplified process and apparatus can be employed.
The process and the apparatus of this second embodiment are described below.
[0079] The simplified process for producing the magnetic device of the invention with a
roll-to-roll apparatus is realized. A thin film is formed on a substrate as it is
wound onto a cylindrical can. A mask of a given shape for restricting the inflow of
particles deposited on the substrate is set below the can with a sufficient clearance
to prevent contact with the substrate, and where the thin film is formed as the substrate
is taken up.
[0080] Fig. 6 is a simplified schematic diagram illustrating the operating principle of
this production process. A thin film is deposited on the substrate 4 using deposition
source 12 such as a sputtering cathode. As shown, a mask member 10 is placed in a
selected area below the can, preferably just underneath it, with sufficient clearance
to prevent contact with the substrate 4. In those areas of the substrate 4 which are
not covered with the mask member 10, vapourized film-forming particles 14 travel directly
to the substrate 4, thereby forming a thin film (having a greater thickness as indicted
by 15), whereas in the area of the substrate which is just above the mask member 10,
the particles 14 are blocked by the mask member 10 and fail to form a thin film. However,
in the neighborhood of either end of the mask member 10, the particles 14 pass around
behind the mask and are deposited in the corresponding areas of the substrate, to
form a thin film (having a smaller thickness as indicated by 2) which progressively
decreases in thickness. This effect is utilized by the subject production method of
the invention.
[0081] Fig. 7 is a simplified schematic diagram showing an example of a (roll-to-roll) apparatus
for producing the magnetic device of the invention by the method described above.
In Fig. 7, the substrate 4 is wound onto can 11 after passing on guide roll 7, and
a thin film is deposited on the substrate 4 by deposition source 12. In the apparatus
shown in Fig. 7, a plurality of linear mask members 10 (four mask members are shown
in Fig. 7) are set just beneath the can 11 such that they do not contact the substrate
4, and films having a smaller thickness 2 similar to the one shown in Fig. 6 are formed
in those areas of the substrate which correspond to the shades of the mask members
10. The substrate having the thin film formed thereon is sent to a take-up roll via
guide roll 6. The thin film on the substrate 4 wound up by the take-up roll consists
of alternating bands of the thicker portion 15 and the thinner portion 2, and the
magnetic device of the invention is cut out from the substrate 4.
[0082] Fig. 8 is a simplified schematic diagram showing two deferent ways to cut out the
magnetic device of the present invention from the substrate with the thin film that
was manufactured with the apparatus of Fig. 7. As described above, the thin film formed
on the substrate 4 consists of alternating bands of the thicker portion 15 and the
thinner portion 2. If a magnetic device of the shape indicated by 16 is cut out from
this substrate, the device 1 has a thin film of the smaller thickness 2 at each of
the farthest ends as shown in Fig. 8(a) and this is the magnetic device shown in Fig.
2. If, on the other hand, a magnetic device of the shape indicated by 17 is cut out
from the substrate, the device 1 has a thin film having a smaller thickness in areas
slightly offset toward the center as shown in Fig. 8(b) and this is the magnetic device
shown in Fig. 3.
[0083] As seen from Fig. 8, the width of the mask member 10 determines the shape of the
areas 2 of the thin film having a controlled thickness, and it ranges preferably from
0.1 to 30 mm, with the range of 0.5 to 10 mm being more preferred. If the width of
the mask member 10 is less than 0.1 mm, it is too narrow to provide the intended film
thickness gradient. On the other hand, if the width of the mask member 10 exceeds
30 mm, the overall size of the magnetic device increases to the extent that a compact
magnetic device is not realized which is a primary objective of the invention.
[0084] As described above, the distance between the mask member 10 and the substrate 4 cannot
be uniquely determined because it varies with the characteristics of the specific
film coater unit that is employed. However, in most cases, a range of from about 0.1
to about 5 mm is preferred.
[0085] The mask member 10 may be rectangular or in the form of a round bar. Alternatively,
it may assume any cross-sectional shape such as a triangle or an ellipse. A suitable
shape may be selected as appropriate in consideration of the gradient of the film
thickness of the magnetic device or the shape of the areas of the thin film which
are to have a controlled thickness. Fig. 7 shows the case of using linear masks. Because
the surface of the can is curved, the clearance between the mask member and the can
increases progressively with increasing distance from the center line of the can and
this may occasionally deteriorate the film thickness control. If this possibility
exists, it is effective to install a protector to ensure that a thin film is formed
only in the neighborhood of the central position of the can.
[0086] Forming a mask member having the same curvature as the can is a very effective means
because it permits the clearance between the mask member and the substrate to be held
constant.
[0087] In addition to the first process described above, the magnetic device of the invention
can also be produced by a second process which is described below.
[0088] In this second process, the magnetic device comprising a substrate and a thin film
formed thereon including a central area and an area having a film thickness that is
smaller than that of the central area is preferably produced by either evaporation
or sputtering. In order to prepare this thin film on the substrate, a mask member
for selectively blocking the deposition of a thin film is used. The second process
for producing the magnetic device of the invention is characterized in that the mask
member for selective blocking of the deposition of the thin film is provided between
the substrate and an evaporation source or a sputtering cathode. In this case, either
the substrate or the mask member is moved such that the region of the substrate which
is shaded by the mask member varies over time.
[0089] Consider the case shown in Fig. 9, where masks 19 are fixed on a stationary substrate
18 and particles are deposited on the substrate to form a thin film. No film is deposited
at all in the areas of the substrate which are beneath the mask members 19. However,
in the open areas which are not covered with the mask members 19, a film of uniform
thickness is deposited on the substrate 18. As a result, the deposited thin film is
interrupted at areas 20 where no film is formed, and the film has a discontinuous
thickness profile in which the thickness of the film changes discontinuously from
one region to another. Hence, this method is not capable of producing a thin film
having a thickness gradient that is needed for the magnetic device of the invention
which should exhibit an abrupt magnetic flux reversal when the strength of an external
magnetic field reaches a critical value.
[0090] If a thin film is formed by moving either of the substrate or the mask member, the
thickness of the thin film thus formed is affected by the relative positions of the
mask member and the substrate. Consider the case shown in Fig. 10, where rods of mask
member 19 are set such that their lengthwise direction is aligned with the direction
of movement of the substrate 18. The substrate travels in the direction shown by the
arrow in Fig. 10. Even if the mask member 19 or the substrate 18 move relative to
each other, a given point on the substrate 18 is at all times in a position such that
it is shaded or not shaded by the mask members 19. In this case, the film formed on
the substrate 19 is of the same type as shown in Fig. 9 and no thin film will form
that has the desired thickness gradient.
[0091] However, if, as in the present invention, the substrate or the mask member is moved
such that the region of the substrate which is shaded by the mask member varies with
time, a film is obtained which has an area of continuously ranging thickness. Even
if the mask member 19 consists of rods as shown in Fig. 10, they may be set obliquely
as shown in Fig. 11 such that their lengthwise axes form an angle with the direction
of movement of the substrate 18. The substrate travels in the direction shown by the
arrow in Fig. 11. If this requirement is met, the region of the substrate which is
shaded by the mask member 19 varies with time and the thickness of the film thus formed
can be adjusted by the length of time over which the substrate 18 is covered by the
mask member 19. As a result, the thin film is provided with areas 2 having the desired
thickness gradient. The extent of the areas 2 is determined by the angle that the
lengthwise axis of the mask member 19 forms with the direction of movement of either
the substrate 18 or the mask member 19.
[0092] The film thickness gradient can be adjusted more precisely by using a nonlinear mask
member, for example, one having a sawtooth edge as indicated by 19 in Fig. 12. The
substrate travels in the direction shown by the arrow in Fig. 12. If the substrate
18 or the mask member 19 having such a nonlinear shape is moved, the length of time
over which the substrate is covered by the shade of the sawtooth edge 21 varies continuously,
to thereby form areas 2 having a film thickness gradient. In this case, the lengthwise
axis of the mask member 19 may be in complete alignment with the direction of movement
of the substrate 18 or the mask member 19.
[0093] The foregoing description has been directed to a method of forming a thin film on
a substrate that is held in a flat state. Flexible substrates such as resin films
or metal foils can be processed by the roll-to-roll method in which a roll of the
substrate is unwound and passed around a cylindrical can so that a thin film is continuously
formed on the substrate as it is wound by a take-up roll, and the invention is also
effective for this method. In this case, the mask member is set below the can around
which the substrate has been wound. In order to achieve more precise adjustment of
the film thickness, it is more effective to bend the mask member in conformance with
the curvature of the can so that the mask member maintains a constant clearance from
the substrate.
[0094] The following Examples and comparative Examples are provided for the purpose of further
illustrating the present invention. However, the present invention should not be construed
as being limited thereto.
Example 1
[0095] A fluororesin impregnated glass cloth 75 µm thick (product of Yodogawa Kasei Co.,
Ltd.) was punched to form circular holes (15 mm⌀) at intervals of 30 mm, and the thus
prepared sheet was used as a mask member. A roll-to-roll apparatus was used in the
coating process. A PET (polyethylene terephthalate) film 100 µm thick was wrapped
as a substrate onto a water-cooled can, and copper wires 0.9 mm in diameter were placed
as spacers on top of the substrate. The separately prepared mask member was superposed
on the copper wires. Thus, the mask member was set on the substrate with a clearance
of about 0.9 mm provided therebetween. Using a DC magnetron sputtering apparatus of
the type described in Unexamined Published Japanese Patent Application No. Hei-4-218905
(corresponding to U.S. Patent 5,181,020), in which magnets are positioned below a
target and the magnetic flux from the magnets is guided by yokes to generate a high-density
plasma on the target surface, an amorphous thin film having the composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed in a thickness of 0.5 µm on the substrate,
which was taken up continuously together with the spacers and the mask member. The
substrate with the thin film formed thereon was cut out in a specified geometry to
manufacture magnetic device samples of the invention. Each sample was circular with
a diameter of about 25 mm, and in the area extending over the range of 7.5 to 12.5
mm from the center of the circle, the film thickness decreased continuously to provide
a thickness gradient.
[0096] The magnetic characteristics of each sample were measured with an ac B-H tracer (AC,
BH-100K of Riken Denshi Co., Ltd.) at 60 Hz. Since each sample exhibited uniaxial
magnetic anisotropy, the measurement was conducted with a pickup coil set in the center
of the sample in the direction of the magnetic easy axis. The result is shown in Fig.
13. As seen in Fig. 13, in each sample of the invention, the magnetic device had a
satisfactory square hysteresis loop and the magnetization changed abruptly at -1 Oe
and +0.6 Oe to provide discontinuous jumps in magnetization.
Comparative Example 1
[0097] An amorphous thin film having the composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed on a PET (polyethylene terephthalate)
film using the same apparatus and under the same conditions as in Example 1, except
that no spacer copper wires were not interposed between the substrate and the mask
member (i.e., the substrate was in contact with the mask member). Circular thin films
were formed each having a diameter of 15 mm equal to the diameter of the openings
in the mask member. These thin films had a substantially uniform thickness. Magnetic
device samples were cut out from the circular thin films and their magnetic characteristics
were measured using the same method as in Example 1. The result is shown in Fig. 14.
As seen from Fig. 14, the magnetic device samples made of the thin films having a
uniform thickness did not produce the desired square hysteresis loop under the influence
of a strong demagnetizing field. In addition, the change in magnetization was continuous,
and no discontinuous jumps in magnetization were observed.
Example 2
[0098] A 100-µm thick PET (polyethylene terephthalate) film was set as a substrate on a
roll-to-roll apparatus of the same type as used in Example 1. Two stainless steel
bars each having a diameter of 4 mm were spaced apart by 20 mm and set as masks just
beneath the can, with the smallest clearance from the substrate adjusted to 0.1 mm.
[0099] Then, by continuously taking up the substrate, an amorphous thin film having the
composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed in a thickness of 0.5 µm on the substrate
using a DC magnetron sputtering apparatus of the same type as used in Example 1. Two
bands of a film having a smaller thickness were observed on the substrate at a spacing
of about 20 mm in the direction of travel of the substrate, and the change in the
film thickness was continuous.
[0100] The thickness profile of the thin film was evaluated by the following procedure.
A water-soluble ink was preliminarily printed in a pattern of 1 mm × 50 mm on the
substrate PET film. The length of the ink pattern and that of the mask were oriented
in a vertical direction. After film formation, the water-soluble ink and the overlying
thin film were washed away with water. Thus, a level difference was established between
the area retaining the thin film and the area from which it was removed, and the difference
was measured with a surface profile measuring system Dektak 300 of Dektak Co., Ltd.
As a result, the film thickness was found to be 0.6 µm in the central area between
the traces of the two masks (which corresponded to the central area of the magnetic
device). The thickness profile in the neighborhood of each mask was measured by scanning
at 0.5-mm intervals. The result is shown in Fig. 15. As seen from Fig. 15, the thickness
of the thin film deposited on the substrate varied continuously on account of the
masks, and the thickness was smallest at an area corresponding to the center of either
mask (about 63% of the thickness at the areas not covered by the mask). Thus, by providing
the above masking structure, areas having a smaller thickness than at the center of
the magnetic device were formed, and the film thickness continuously varied to provide
a gradient.
[0101] For the measurement of magnetic characteristics, a PET film not having a printed
pattern of a water-soluble ink was used as a substrate, and a thin film was formed
thereon under the same conditions described above. From the substrate having the thin
film formed thereon, rectangular samples measuring about 28 mm long by 10 mm wide
were cut out such that the area having the smaller thickness would occur at either,
to thereby obtain magnetic device samples of the invention.
[0102] The magnetic characteristics of these samples were measured by the same method as
employed in Example 1. Since each magnetic device sample exhibited uniaxial magnetic
anisotropy in the longitudinal direction, the measurements were conducted along the
magnetic easy axis. The result is shown in Fig. 16. As seen from Fig. 16, the magnetic
device samples of the invention each had a satisfactory square hysteresis loop, and
the magnetization changed abruptly at -1 Oe and +1.1 Oe to provide discontinuous jumps
in magnetization.
Comparative Example 2
[0103] An amorphous thin film having the composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed on a PET film using the same apparatus
and under the same conditions as in Example 2, except that a mask member was not set
below the can. As a result, a thin film was uniformly deposited on the substrate with
no thickness gradient. From this substrate, rectangular samples measuring 28 mm long
by 10 mm wide as in Example 2 were cut out such that the length of each sample was
oriented parallel to the width of the substrate. The magnetic characteristics of the
cut out samples were measured by the same method as used in Example 2. The result
is shown in Fig. 17. As seen from Fig. 17, the magnetic device samples made of thin
films having a uniform thickness did not produce the desired square hysteresis loop,
but rather produced a largely skewed loop under the influence of a strong demagnetizing
field. In addition, the change in magnetisation was continuous, and discontinuous
jumps in magnetization were not obtained.
Example 3
[0104] From the substrate prepared in Example 2, rectangular magnetic device samples measuring
about 38 mm long by 10 mm wide were cut out such that areas having a smaller thickness
were located 5 mm from either end. The magnetic characteristics of these samples were
measured by the same method as used in Example 1. Since each magnetic device sample
exhibited uniaxial magnetic anisotropy in the longitudinal direction, the measurements
were conducted along the magnetic easy axis. The result is shown in Fig. 18. As seen
from Fig. 18, the magnetic device samples of the invention each had a satisfactory
square hysteresis loop, and the magnetization changed abruptly at ±0.4 Oe to provide
discontinuous jumps in magnetization.
Example 4
[0105] A 100-µm thick polyethylene terephthalate (PET) film was set as a substrate on a
roll-to-roll apparatus, and stainless steel sheets measuring 10 mm wide by 30 cm long
which were bent to the curvature of the can were set as mask members just beneath
the can. The two stainless steel sheets as mask members were spaced apart by 20 mm.
The lengthwise direction of each mask member formed an angle of 5° with the direction
of travel of the substrate.
[0106] By continuously taking up the substrate on the setup described above, an amorphous
thin metallic film having the composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed in a thickness of 0.5 µm on the substrate
using a DC magnetron sputtering apparatus. Two bands of a film having a smaller thickness
were observed on the substrate at a spacing of about 17 mm in the direction of travel
of the substrate, and the change in film thickness was continuous.
[0107] From the thus prepared substrate, rectangular samples measuring 25 mm long on the
longer side (across the width of the substrate) by 10 mm wide were cut out such that
the area having the smaller thickness was located at either end. The cut-out samples
were magnetic devices. The magnetic characteristics of these devices were measured
with an ac B-H tracer (AC, BH-100 K of Riken Denshi Co., Ltd.) at 60 Hz. The result
is shown in Fig. 19.
[0108] As seen from Fig. 19, the magnetic device samples manufactured by the process of
the invention had a satisfactory square hysteresis loop, and the magnetization changed
abruptly at -0.7 Oe and +0.9 Oe to provide discontinuous jumps in magnetization.
Comparative Example 3
[0109] An amorphous metallic thin film having the composition Co
51Fe
26Si
10B
13 (the subscripts represent atomic %) was formed on a polyethylene terephthalate (PET)
film using the same apparatus and under the same conditions as in Example 4, except
that the length of the mask members was adjusted parallel to the direction of travel
of the substrate (i.e., the angle between the lengthwise direction of the mask members
and the direction of travel of the substrate was zero degrees). Because of this parallel
alignment, the region of the substrate which was shaded by the mask members did not
vary with time. The substrate having a thin film thus formed thereon was characterized
as having two bands of film-free areas that were spaced apart by about 20 mm in the
direction of travel of the substrate, and the change in film thickness at the boundary
was clearly visible.
[0110] From the thus prepared substrate, rectangular samples measuring 25 mm long on the
longer side (across the width of the substrate) by 10 mm wide were cut out such that
a film-free area was located at either end. The cut-out samples were magnetic devices.
The magnetic characteristics of these devices were measured as in Example 1, and the
result is shown in Fig. 20.
[0111] As seen from Fig. 20, the magnetic device samples manufactured without varying over
time the region of the substrate shaded by the mask members had hysteresis characteristics
exhibiting a lower degree of squareness as compared to the samples of Fig. 19.
[0112] While the invention has been described in detail and with reference to specific embodiments
thereof, it will be apparent to one skilled in the art that various changes and modifications
can be made therein without departing from the spirit and scope thereof.
1. A magnetic device comprising a soft magnetic thin film formed on a substrate, including
a central area and a second area having a film thickness that is smaller than that
of the central area, and wherein said magnetic device has a magnetic hysteresis loop
which exhibits a discontinuous magnetization reversal.
2. The magnetic device as claimed in claim 1, wherein the soft magnetic thin film of
said second area has a film thickness gradient.
3. The magnetic device as claimed in claim 1, wherein the film thickness in areas other
than said central area is smaller than that of said central area.
4. The magnetic device as claimed in claim 1 having a circular shape, and including a
central area of uniform film thickness and a peripheral area having a film thickness
that is smaller than that of the central area and which progressively decreases toward
the periphery of the magnetic device.
5. The magnetic device as claimed in claim 4, wherein the film thickness at said peripheral
area progressively decreases over a distance of about 1 to 20 mm and becomes almost
zero at the periphery.
6. The magnetic device as claimed in claim 1 having a rectangular shape, and including
a central area of uniform film thickness and an area at opposite ends thereof having
a film thickness that is smaller than that of the central area and which progressively
decreases toward an edge of the device.
7. The magnetic device as claimed in claim 6, wherein the film thickness at said opposite
ends progressively decreases over a distance of about 1 to 20 mm and becomes almost
zero at the edge.
8. The magnetic device as claimed in claim 1 having a rectangular shape, and including
a central area of uniform thickness and an area offset from an end thereof having
a film thickness that is smaller than that of the central area.
9. The magnetic device as claimed in claim 8, having an area at an end of said magnetic
device having a film thickness that is the same as that of the central area.
10. The magnetic device as claimed in claim 8, wherein the film thickness at the offset
area changes over a length of about 0.1 to 5 mm such that the smallest thickness of
said offset area ranges from about 10% to about 80% that of the central area.
11. A process for producing a magnetic device comprising a soft magnetic thin film formed
on a substrate, including a central area and a second area having a film thickness
that is smaller than that of the central area, and wherein said magnetic device has
a magnetic hysteresis loop which exhibits a discontinuous magnetization reversal,
comprising the steps of:
positioning a mask member having an opening over said substrate with sufficient clearance
so as not to contact the substrate, and
depositing a soft magnetic thin film through the opening of said mask member and onto
said substrate.
12. The process as claimed in claim 11, wherein the soft magnetic thin film of said second
area has a film thickness gradient, and which process further comprises the step of
controlling the film thickness gradient by adjusting the distance between the mask
member and the substrate.
13. The process as claimed in claim 11, wherein the distance between the mask member and
the substrate is about 0.1 to 5 mm.
14. A process for producing a magnetic device comprising a soft magnetic thin film of
a given shape formed on a substrate, including a central area and a second area having
a film thickness that is smaller than that of the central area, and wherein said magnetic
device has a magnetic hysteresis loop which exhibits a discontinuous magnetization
reversal, comprising the steps of:
winding a substrate on a cylindrical can,
winding a mask member having an opening corresponding to the shape of said thin film
onto said substrate via a spacer so as not to contact the substrate, and
depositing a soft magnetic film through the opening of said mask member and onto said
substrate.
15. The process as claimed in claim 14, wherein said spacer comprises a plurality of metal
wires having a diameter of about 0.5 to about 5 mm.
16. A process for producing a magnetic device comprising a soft magnetic thin film of
a given shape formed on a substrate, including a central area and a second area having
a film thickness that is smaller than that of the central area, and wherein said magnetic
device has a magnetic hysteresis loop which exhibits a discontinuous magnetization
reversal, comprising the steps of:
winding a substrate on a cylindrical can,
positioning a mask member having an opening corresponding to the shape of said thin
film over said substrate with sufficient clearance so as not to contact said substrate,
and
depositing a soft magnetic film through the opening of said mask member and onto said
wound substrate.
17. An apparatus for producing a magnetic device comprising a soft magnetic thin film
of a given shape formed on a substrate, including a central area and a second area
having a film thickness that is smaller than that of the central area, and wherein
said magnetic device has a magnetic hysteresis loop which exhibits a discontinuous
magnetization reversal, which comprises:
means for superposing, in the following order, (1) a substrate, (2) a spacer and (3)
a mask member having an opening corresponding to the shape of said thin film around
a cylindrical can in such manner that the mask member does not contact the substrate,
means for depositing a soft magnetic thin film through the opening of said mask member
and onto said substrate, and
means for winding the superposed substrate, spacer and mask member.
18. An apparatus for producing a magnetic device comprising a soft magnetic thin film
of a given shape formed on a wound substrate, including a central area and a second
area having a film thickness that is smaller than that of the central area, and wherein
said magnetic device has a magnetic hysteresis loop which exhibits a discontinuous
magnetization reversal, which comprises:
means for winding a substrate on a cylindrical can,
means for positioning a mask member having an opening corresponding to the shape of
said thin film over said substrate with sufficient clearance so as not to contact
said substrate, and
means for depositing a soft magnetic film through the opening of said mask member
and onto said wound substrate.
19. A process for producing a magnetic device comprising a thin film formed on a substrate,
including a central area and a second area having a film thickness that is smaller
than that of the central area, comprising the steps of:
positioning a mask member between said substrate and a thin film deposition source,
to thereby selectively block deposition from said deposition source, and
depositing a thin film onto said substrate while moving said mask member and said
substrate relative to each other, to thereby, vary the area blocked by said mask member
over time and form said second area having a reduced film thickness.
20. The process as claimed in claim 19, wherein said thin film deposition source comprises
an evaporation source or a sputtering cathode.
21. The process as claimed in claim 19, wherein said mask member comprises a plurality
of rods having a lengthwise axis, and which process comprises positioning the lengthwise
axes of said rods at an angle relative to the direction of movement of said substrate.
22. The process as claimed in claim 19, wherein said mask member has a nonlinear shape.