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Description
of Inframat Magnetic Nanocomposite Research
1.
Introduction
Inductive components are extensively used in high frequency
(> 1 MHz) electronic devices from radar, satellite, telecommunication
systems to home radio stereos. Conventional inductive components
use metallic alloys and ferrites as core materials. The major
problem for metallic materials is their low resistivity (~10-6
W-cm). Since it is impossible to dramatically increase their
resistivity, metallic materials were excluded in high frequency
applications and ferrites have been the only choice for five
decades since World War II. Although efforts have been made
extensively to improve the performance of the ferrites, very
limited progress was obtained. Magnetic materials have been
a key impediment for the miniaturization of electronic equipment.
To overcome the difficulties
of both metallic alloys and ferrites, InframatÒ Corporation
(“IMC”) is developing metal/ceramic nanocomposites
for the next generation of high frequency magnetic applications.
Nanocomposite processing has provided a new approach for fabricating
soft magnetic materials. In a magnetic/ceramic nanocomposite,
the resistivity can be drastically increased, leading to significantly
reduced eddy current loss. In addition, the exchange coupling
between neighboring magnetic nanoparticles can overcome the
anisotropy and demagnetizing effect, resulting in much better
soft magnetic properties than conventional bulk form materials.
IMC has developed
innovative processes to facilitate microstructure of exchange
coupled magnetic nanocomposite that retains nanograin size in
the bulk-consolidated phase. This result is the first compelling
evidence demonstrates in metal/insulator magnetic nanocomposites.
This development has been done under contracts from NSF, NASA,
DARPA, Airforce, and the US NAVY. Specifically IMC has demonstrated
· Chemical
synthesis of Ni-Fe/SiO2, Co/SiO2, Fe-Co/SiO2, Fe/nickel-ferrite,
Ni-Zn-ferrite/SiO2, Fe-Ni/ polymer, and Co/polymer magnetic
nanocomposites
· Consolidate these magnetic nanocomposite powders into
exchange coupled (>90% theoretical density) bulk components
via vacuum hot press consolidation
· Consolidate these magnetic nanocomposite powders into
exchange coupled (>90% theoretical density) bulk components
via tape casting process
· Performance evaluation of the exchange coupled magnetic
nanocomposite components
2.
Commercialization Strategy
IMC is seeking corporate partner to prosecute the exciting opportunity
to extend the lab results and implement in actual device as
a part of an aggressive commercialization strategy.
3.
Technology Development
IMC’s technology for the synthesis and processing of metal/insulator
magnetic nanocomposite is a radical departure from the conventional
metallic and ferrite materials. A schematic of IMC’s magnetic
nanocomposite technology is illustrated in Fig. 1, which includes
powder synthesis (insulated coated magnetic nanoparticles),
consolidation of the powder into exchange coupled cores. A completely
new phenomenon has been observed when reducing the particle
size and the separation between neighboring particles into a
nanometer scale in composite matters. For example, it has been
found that a Co- or Fe-based nanocomposite can possess a permeability
much higher than that obtainable from the bulk Co or Fe metal.
This large enhancement in permeability is due to the exchange
coupling effect. The exchange interaction which leads to magnetic
ordering within a grain also extends out to neighboring environments
within a characteristic distance, the so-called exchange length
lex. Thus, neighboring grains separated by distances shorter
than lex can be magnetically coupled by exchange interaction.
For a traditional powder material of large particle sizes, exchange
coupling effect is negligibly small in determining magnetic
properties. However, when the particle size plus the separation
between particles is reduced to approximately lex, intergrain
exchange coupling plays a dominant role and the material will
possess a variety of properties different from the bulk size
material. One important effect is the cancellation of the magnetic
anisotropy of individual nanoparticles: when the particle-particle
separation is significantly less than lex, the intergrain exchange
interaction makes all the neighboring particles coupled. This
coupling averages out the magnetic anisotropy of individual
nanoparticles. As a consequence, the permeability of an exchange-coupled
nanocomposite can be even much higher than the permeability
of its bulk counterpart.
Fig. 1. Schematics
representation of Inframat’s magnetic nanocomposite technology
Powder synthesis:
IMC’s chemical synthesis route for metal/insulator nanocomposite
magnetic materials provides a unique opportunity to modify the
magnetic as well as electrical properties of the complex material
in a rather large scale. For example, a nanocomposite consisting
of a magnetic phase and an insulating phase such that the magnetic
particles are embedded in the insulating matrix, the material
now has essentially no overall electric conductivity. In addition,
since the magnetic particle is in a nanometer size, the eddy
current produced within the particle is also negligibly small.
Therefore, conductivity of the magnetic constituent is no longer
a factor in the material selection consideration and metallic
materials can be used as magnetic phase.
IMC developed a nanocomposite
technique suitable for massive production of bulk-size magnetic
nanocomposite manufacturing. The synthesis procedures include
(1) preparation of aqueous precursor solutions, (2) atomization
of the precursor solutions to form a nanoparticle colloidal
suspensions with maximal nucleation and minimal growth, (3)
refluxing of the colloidal solution under controlled pH and
time to form the desired microstructure and phases, washing
and filtration, and low temperature calcination
IMC’s aqueous
solution reaction technique is intrinsically low cost and scaleable
to volume production. Utilizing the technique, we have successfully
fabricated Co/SiO2 and Fe-Ni/SiO2 nanocomposite soft magnetic
materials, which possess higher initial permeability and higher
cut-off frequency than the conventional micrometer sized ferrites.
Nanocomposite consolidation:
IMC’s current core consolidation steps include (1) preparation
of ready-to-press powders, (2) consolidation of the ready-to-press
powder into a green compact, (3) toroidal sample fabrication,
and (4) low temperature annealing.
The consolidation
of high density nanocomposite materials is a critical step towards
development of an optimal soft magnetic material. An isolated
nanocomposite particle possesses very high anisotropy due to
its large surface anisotropy and demagnetizing effect. For nanocomposite
materials, the soft magnetic properties come from the intergrain
interaction, mostly due to the exchange coupling of the neighboring
magnetic nanoparticles. The intergrain interaction tends to
average the anisotropy of each individual particle, resulting
in much reduced anisotropy and, consequently, higher permeability.
A critical parameter, the exchange coupling length, is the distance
within which the magnetic moments of the two particles can be
coupled. For Co and Fe, the exchange length is estimated to
be ~35 nm. Thus, the particles have to be consolidated to achieve
separation of the neighboring particles that are less than the
exchange length.
Thick film fabrication:
IMC is developing a coating formulation (or paste) that can
be screen printed for thick film magnetic circuit board applications.
Here, polymer coated magnetic colloidal nanoparticles are prepared
in organic or aqueous solvents. Suitable surfactants are added
to the solutions to assess potential benefits for achieving
optimal homogeneity of dispersed magnetic nanoparticles. After
screen printing, the materials are then cured to form high packing-density
thick film.
IMC is currently
exploiting a sputtering technique for the fabrication of both
thin and thick film magnetic nanocomposite materials. In the
case of a thin film, multilayered structure of magnetic/nonmagnetic
layers will be resulted. The thickness of the layer is limited
to be < 100 nm. The resultant multiplayer thin is suitable
for GMR devices.
In the case of thick
film, granular magnetic particles are uniformly coated with
a thin layer of insulating nonmagnetic phase. The thickness
of the film can be up to 50 mm. The resultant thick film will
be suitable for high frequency power converters (e.g., >30
MHz), and microwave (>1 GHz) and millimeter wave (>15
GHz) radar applications.
Tape Casting consolidation:
IMC’s tape casting approach seems to be a very effective
way to process large volume magnetic nanocomposite components
for high quality device applications. Unlike conventional tape
casting techniques, IMC’s technique involves the addition
of chemical precursors to the slurry composition to promote
low temperature sintering so that high density with minimal
grain growth had resulted in the sintered components.
Nanocomposite
properties: A typical TEM bright field image for IMC’s
synthetic n-Co/SiO2 is shown in Fig. 2. It reveals that the
nanocomposite is a two-phase material, where the Co magnetic
nanoparticles are coated with a thin film of silica. The Co
phase has an average particle size of ~30 nm. Selected area
electron and x-ray diffraction experiments indicated that the
Co particles are fcc nanocrystals, where the matrix silica phase
is amorphous.
High frequency
applications require magnetic materials with large m¢ and
large Q, while keeping m¢¢ minimal. The currently used
ferrites, including spinel ferrites ((Ni,Zn)2Fe4) and hexagonal
ferrites (Co2Z, where Z = Ba3Me2Fe24O41), have a m¢ value
< 15, and the cutoff frequencies (the frequency at which Q
£ 1) are less than 500 MHz. Fig.
3 shows a schematic representation the frequency dependence
of m¢ and m¢¢ for the nanocomposite in comparison
with conventional magnetic materials. Compared with conventional
magnetic materials, IMC’s magnetic nanocomposite shows
a flat frequency response, with minimal core loss agains all
frequency, while conventional magnetic materials exhibited high
losses at elevated frequencies. General speaking, the advantage
of magnetic nanocomposite include, (1) reduction in total core
power losses, (2) the high flux capabilities at elevated temperatures
that the nanocomposite cores are expected to support, thereby
enabling manufacture of smaller power devices, and (3) broadband
devices. IMC's breakthrough technology in nanostructured magnetic
components will be extremely attractive to reduce the cost and
size of the current magnetic components.
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4.
Background and Applications
There has been a great deal of interest in recent years in artificially
engineered nanomaterials with novel physical properties. Among
the researches, perhaps the effort in magnetic nanostructures
attained the biggest rewards to date. These achievements imply
a brilliant prospective of nanomagnetics.
4.1.
What makes nano-magnetics so unique?
Spin memory: For conventional materials with dimensions much
longer than the spin diffusion length of electron, which is
in a scale of 10 nm, an electron flips its spin direction up
and down many times in the path, thus the effect of spin direction
on material’s resistivity is time-averaged out. However,
when reducing the dimension of the building block unit of a
material to the same scale, the spin of electron remains unchanged
when passing through the unit. In this case, the electron current
is characterized not only by its charge current, but also by
its spin current. In macroscopic world, the electron spin plays
as a concept, its existence can only be felt indirectly except
in some special fundamental experiments. In nano-world, electron
spin becomes a real thing. It can be seen directly; it can be
engineered and utilized. Nano-magnetics is quickly bringing
electron spin explicitly into ordinary people’s daily
life.
Spin-dependent
transport characteristics: Taking electric resistivity as an
example. For transition metal magnetic materials, the s-d scattering
is the major contribution to electrical resistivity of these
materials, and the scattering is very much dependent on the
relative orientation between the electron spin moment and the
3d atomic moment. When electrons travel in a magnetic metal,
the resistivity for the electrons with spins parallel to the
magnetization of the metal is different from that for the electrons
with spins antiparallel to the magnetization. For conventional
materials with dimensions much longer than the spin diffusion
length, the effect of spin orientation on the resistivity is
time-averaged out in its long distance journey. However, when
the dimension of the material is comparable to the spin diffusion
length, the spin-dependent resistivity behavior is well pronounced.
In this case, the resistivity is subjected to a large change
when the magnetic state of the material is varied by an applied
magnetic field. It is so called giant magnetoresistive (GMR)
effect as it was found that such magnetoresistive effect in
nanomagnetic materials is of 10 times larger in magnitude than
in macroscopic materials. Based on the similar mechanism, other
transport effect also subjected to giant variations.
Exchange
coupling: The quantum mechanics rooted exchange interaction
exists not only within the building block unit of a magnetic
material (which leads to the magnetic ordering of the atomic
moments within the entity), but also extend to neighboring units.
The later is called exchange coupling. For the currently used
(conventional) magnetic materials, their building block unit,
grain, is in micron scale; the exchange coupling is negligibly
small compared with the macroscopic thermodynamic interactions
within each grain. Thus their macroscopic properties are determined
by macroscopic thermodynamic rules within each grain. When reducing
the scale of the entity to a few nanometers or so, the exchange
coupling is comparable or even greater than the thermodynamic
interactions; the grains will be exchange coupled to each other.
In this case, the individual grains losses their classical characteristics,
and new magnetic structures and new magnetic properties can
be created. The rules governing magnetic properties are different
4.2.
What does (or will) small-size bring to magnetics?
Spin electronics: The name of spin electronics (also called
spintronics or magnetoelectronics) was appeared first in 1995.
Taking electron spin as information carrier, spin electronics
engineers attaining net spin current, transporting and detecting
spin signal, integrating spin signal with electron charge signal
and the related physics. The major advantages of spin electronics
devices are (i) high sensitivity, (ii) miniaturization, (iii)
high operation speed, and (iv) low power consumption. As to
the prospective of spin electronics, if recalling what photonics
has played in science and technology when electron is combined
with photon, one would expect the same, if not more, from spin
electronics when electron charge is combined with electron spin.
Revolution
in magnetism: For conventional materials, grain is the elementary
unit; the ferromagnetism is determined by the domain and domain
wall structure in the grain. In nanostructured magnetic materials,
the grain is just like a point with giant moment. The ferromagnetism
is governed by the intergrain exchange interaction. Thus the
magnetic structure, static and dynamic magnetic behavior of
nanomagnetic systems are different from those for conventional
magnetic materials. With the creation of nanomagnetic systems,
magnetism is now heading for a new generation.
Novel magnetic materials with better magnetic properties and
new functionalities: In less than 15 years, a lot of nanostructured
magnetic materials and devices have been developed or in progress.
Following are some examples.
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(1).
Spin electronics materials and devices, including (i) GMR
read head devices, (ii) magnetic random-access-memory devices,
(iii) nanostructures for sensors, and other low dimensional
nanostructures such as multilayers, nanowires
(2). Magnetic recording media, such as granular thin films
and arrays
(3). Function materials, including (i) nanocrystalline soft
magnetic alloys (such as Fe-Cu-Nb-Si-B), (ii) nanocomposite
high frequency soft magntic thin films (such as Fe-Co-Zr-O),
(iii) exchange coupled hard magnetic materials (such as
Nd2Fe14B/Fe3B). |
In summary,
nanomagnetic materials drive one more physical quantity, electron
spin, to the front stage as a major player; they change major
interaction in the material; they brings extra degrees of freedom
to the magnetic materials science. Magnetics is experiencing
a revolutionary progress. Recognized such enormous opportunities,
Inframat Corporation is moving ahead to catch the strength.
4.3.
Inframat’s Vision in Magnetic Nanocomposites
Nanocomposite soft magnetic materials: The electronics industry
is directed towards high frequency of operation, which in turn
requires bulk sized high frequency soft magnetic materials.
Conventionally used ferrites possess poor magnetic properties
at elevated frequencies. According to IMC’s metal/insulator
nanocomposite design, the metal nanograins are insulated by
insulating layers, thus the resistivity of the system will be
dramatically increased, leading to a significantly reduced eddy
current loss, while the exchange coupling between neighboring
magnetic nanoparticles can overcome the anisotropy and demagnetizing
effect, resulting in much better soft magnetic properties than
conventional ferrites. This design provides more degree of freedom
(phase constituents, their ratio and grain size) to tailor magnetic
as well as electric properties. We have been studying several
metal/insulator systems to meet various requirements.
Planar magnetic
devices: The Development of high quality nanostructured soft
magnetic materials make it possible to miniaturize magnetic
devices and integrate them in circuit board. We pan to develop
thin film technique to fabricate high frequency metal/insulator
nanocomposite films and devices for DC-to-DC applications.
Magnetic
sensors: In addition to computer related areas, spin electronic
devices have an enormous potential in sensor technology. The
high sensitivity, low power consumption, small size and large
tolerance of spin electronics devices make them ideal for sensor.
We plan to explore spin valve based GMR sensors for a variety
of applications.
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