Magnetic nanofiber composite materials and devices using same
09620839 ยท 2017-04-11
Assignee
Inventors
Cpc classification
B33Y10/00
PERFORMING OPERATIONS; TRANSPORTING
D01D5/0092
TEXTILES; PAPER
B33Y30/00
PERFORMING OPERATIONS; TRANSPORTING
B82Y30/00
PERFORMING OPERATIONS; TRANSPORTING
International classification
Abstract
A nonreciprocal device is described. It includes a housing, a waveguide layer and at least one layer of magnetic nanofiber composite. The magnetic nanofiber composite layer is made up of a polymer base layer, a dielectric matrix comprising magnetic nanofibers. The nanofibers have a high aspect ratio and wherein said dielectric matrix is embedded in the polymer base layer.
Claims
1. A tunable nonreciprocal device comprising: a housing; a waveguide layer; and at least one layer of magnetic nanofiber composite wherein said magnetic nanofiber composite layer comprises: a polymer base layer; a dielectric matrix comprising coated magnetic nanofibers; wherein said nanofibers have an aspect ratio of at least 100 to 1 length to width and wherein said dielectric matrix is embedded in the polymer base layer.
2. The device of claim 1 wherein said dielectric matrix further comprises nanoparticles.
3. The device of claim 1 wherein said nanofibers are flexible.
4. The device of claim 1 wherein said dielectric matrix comprises a self-biased magnetic material.
5. The device of claim 1 further comprising high dielectric constant nanoparticles dispersed within the dielectric matrix.
6. The device of claim 5 wherein said high dielectric constant nanoparticles are dispersed in the dielectric matrix between the nanofibers wherein the nanofibers are substantially parallel.
7. The device of claim 1 wherein each of said coated nanofibers comprising the dielectric matrix in turn comprises a shell and a magnetic core.
8. The device of claim 7 wherein said shell comprises an insulating coating comprises a sputtered layer of aluminum oxide.
9. The device of claim 7 wherein said coated nanofibers are insulated from direct contact with each other.
10. A tunable microwave circulator comprising: a housing; a waveguide layer; and at least one layer of magnetic nanofiber composite wherein said magnetic nanofiber composite layer comprises: a polymer base layer; a dielectric matrix comprising coated magnetic nanofibers; wherein said nanofibers have an aspect ratio of at least 100 to 1 length to width and wherein said dielectric matrix is embedded in the polymer base layer.
11. The circulator of claim 10 wherein said circulator comprises a microstripline device.
12. The circulator of claim 10 wherein said circulator comprises a stripline device having two layers of magnetic nanofiber composite.
13. The circulator of claim 10 wherein said dielectric matrix further comprises nanoparticles.
14. The circulator of claim 10 wherein said circulator excludes a permanent bias magnet and a ferrite magnetic core.
15. The circulator of claim 10 wherein said nanofibers comprising the dielectric matrix comprise a shell and a magnetic core and wherein said shell acts as an insulator.
16. The circulator of claim 15 wherein said shell comprises an insulating coating comprises a sputtered layer of aluminum oxide.
17. The circulator of claim 15 wherein said coated nanofibers are insulated from direct contact with each other.
18. A tunable nonreciprocal device consisting of: a housing; a waveguide layer defining several ports; and one layer of magnetic nanofiber composite wherein said magnetic nanofiber composite layer comprises: a polymer base layer; a dielectric matrix comprising coated magnetic nanofibers; wherein said nanofibers have an aspect ratio of at least 100 to 1 length to width and wherein said dielectric matrix is embedded in the polymer base layer.
19. The device of claim 18 wherein said nanofibers comprising said magnetic nanofiber composite layer are substantially parallel to one another within said nanofiber composite layer.
Description
BRIEF DESCRIPTION OF DRAWING
(1) The invention together with the above and other objects and advantages will be best understood from the following detailed description of the preferred embodiment of the invention shown in the accompanying drawings, wherein:
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DETAILED DESCRIPTION OF THE INVENTION
(10) The foregoing summary, as well as the following detailed description of certain embodiments of the present invention, will be better understood when read in conjunction with the appended drawings.
(11) To the extent that the figures illustrate diagrams of the functional blocks of various embodiments, the functional blocks are not necessarily indicative of the division between hardware circuitry. Thus, for example, one or more of the functional blocks (e.g. processors or memories) may be implemented in a single piece of hardware (e.g. a general purpose signal processor or a block of random access memory, hard disk or the like). Similarly, the programs may be stand-alone programs, may be incorporated as subroutines in an operating system, may be functions in an installed software package, and the like. It should be understood that the various embodiments are not limited to the arrangements and instrumentality shown in the drawings.
(12) As used herein, an element or step recited in the singular and proceeded with the word a or an should be understood as not excluding plural said elements or steps, unless such exclusion is explicitly stated. Furthermore, references to one embodiment of the present invention are not intended to be interpreted as excluding the existence of additional embodiments that also incorporate the recited features. Moreover, unless explicitly stated to the contrary, embodiments comprising or having an element or a plurality of elements having a particular property may include additional such elements not having that property.
(13) Turning to the figures, as shown in
(14) The nonreciprocal device depicted is a circulator 10. The circulator 10 is formed from a magnetic nanofiber composite layer 12 and a waveguide 20. The waveguide 20 is superimposed on the magnetic nanofiber composite layer 12. The circulator 10 is a non-reciprocal device, with a clockwise configuration shown by the embodiment in
(15) As shown in the cross section view 22 of the circulator 10, the circulator 10 comprises the magnetic nanofiber composite layer 12 and the waveguide 20. As shown in the cross-section view 22, the magnetic nanofiber composite layer 12 substantially surrounds the waveguide 20.
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(17) The details of the magnetic nanofiber composite 32 are shown in
(18) Embedded within the polymer 40 forming the composite 32 is a dielectric matrix 44. A first component of the matrix are high-dielectric constant (HDC) nanoparticles 42. The density of the nanoparticles controls the permittivity. In one embodiment, substrates having different permittivity values are assembled into one final construct. The inclusion of the HDC nanoparticles 42 results in a larger effective dielectric constant for the composite being achieved.
(19) The dielectric matrix 44 further includes magnetic fibers 50 dispersed within the matrix 44. Each fiber includes a magnetic core 46 and a dielectric/piezoelectric shell 48. High quality ultrathin magnetic nanofibers are produced by a proprietary scalable electrospinning technology, described in applicant's own earlier patent application Ser. No. 14/803,339, the contents of which are incorporated by reference.
(20) Nanofibers are pre-treated by an in-house developed ALD coating to control magnetic and electrical loss at RF. Moreover, such MNC is made free-standing, and can be integrated with RF circuits at room temperature through film casting or nano-printing directly, which allows compact circulator design such as stripline structure shown in
(21) The details of the nanofibers 50 and the matrix 44 are described below.
(22) As can be appreciated from
(23) The high shape anisotropy (nanofiber 50 length to width ratio >100) introduces a very strong self-bias field that eliminates the need for the external magnets, which would also overcome the de-magnetization when operating at RF frequency. By engineering the morphology and orientation of the nanofibers in the MNC, the instant invention achieves desired magnetic properties without the constraint of material crystallinity that could negatively impact device performance and limit integration process options. The very small diameter of nanofibers (<50 nm diameter) with precision insulation coating by atomic layer deposition (ALD) allows the use of ferromagnetic materials such as FeCo which introduces a very high saturated magnetization (Ms) without increasing magnetic/electrical loss. The dielectric constant () can be readily engineered by doping a small amount (<10%) of ultra-high E material such as Ba(Sr,Ti)O.sub.3 nanoparticles 42 into the composite.
(24) As shown in
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(26) Nanofiber Details
(27) As shown in
(28) As shown in
(29) In one embodiment, the nanofibers have a width w of 30 nm and a length l of 3000 nm to 30,000 nm or lengths of 3 to 30 pm.
(30) The demagnetizing effect of a finite sized magnetic particle also affects its apparent permeability .sub.app, the actual permeability a device can use. High aspect ratio shapes (long rods and thin films) can achieve the full permeability in their magnetic easy axis, while spherical shaped magnets only have a .sub.app up to 3, even if the intrinsic p is very high, see
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(32) High shape anisotropy also enhances f.sub.r, according to the equation:
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where N.sub.x, N.sub.y, N.sub.z, are the demagnetization factor along x, y, z, direction respectively, H.sub.eff is the effective external bias field and is the gyromagnetic ratio.
(34) Compared with other systems such as mechanically deformed metallic flakes, nanofibers have fundamental advantage such as higher shape anisotropy, lower eddy current loss and lower stress/defect in magnetic crystals. Magnetic nanofibers with high shape anisotropy maintain high saturation magnetization similar to their bulk counter parts and high permeability in their easy axis.
(35) In one embodiment, FeCo magnetic nanofibers are used inasmuch as Fe.sub.2Co's specific composition have some of the highest available saturation magnetization values and are oxidation resistantf.sub.r may be tuned by the fiber composition and fiber dimension (Snoek's law, f.sub.rM.sub.s). A trade-off between permeability and f.sub.r and p could be made as desired by varying f.sub.r. For eddy current loss, as long as the dimension of the magnetic entities in the direction perpendicular to the AC magnetic field direction are smaller than the skin depth, the loss tangent due to eddy current is estimated to be <10.sup.3. Nanofiber diameter is <30 nm, more than one order smaller than the skin depth.
(36) Another embodiment uses ferrite nanofibers. Ferrites have higher electrical resistivity than ferromagnetic metals. They can be used where the material's loss requirement is critical. M.sub.s is usually smaller than ferromagnetic metal, resulting in a moderate p value and low FMR frequency. In one embodiment, spinel ferrite is the chosen material. In another embodiment, more complicated hexagonal ferrite nanofibers such as Z-phase cobalt ferrite, which has higher FMR frequency, is used.
(37) Turning to,
(38) An alternative embodiment 110 is depicted in
(39) A further alternative embodiment 120 is depicted in
(40) While the embodiments shown in
(41) Insulation Layer
(42) As shown, for example, in
(43) In one embodiment, the insulation layer 112 is added to individual fibers by a process of atomic layer deposition (ALD). The resulting layer can be as thin as only about one nanometer thick, and thickness can be precisely adjusted to optimize magneto-electric effect and balance the magnetic/dielectric properties The insulation layer 112 comprises piezoelectric materials and an electric field is used to adjust the functioning parameters of the substrate. In one embodiment, additional piezoelectric elements are suspended in the dielectric layer 114. As such, the insulation layer composition is used to not only prevent conductive paths from forming, but also to adjust the antenna in the field of use. In embodiments where the orientation of the nanofibers 116 is controlled, such as an embodiment where the orientation is controlled through extrusion or 3-dimensional printing, the insulation layer 112 is omitted as damaging conductive paths will not be allowed to form. Other than providing for electric insulation, the layer 114 provides for tune-ability of the substrate by coupling magnetic and electric fields.
(44) Final Composite
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(46) The key for this aspect is to eliminate the need for bulky and heavy external magnets, through a self-biased, magnet free operation. The MNC possesses a very high shape anisotropy, which in turn generates a very strong self-bias field of 0.050.5T as required by device performance parameters. In turn the MNC acts as a natural solution for such a self-biased operation.
(47) Two key parameters that determine the dimension of a magnetic material based (including both ferrite in prior art devices and MNC in the instant device) circulator are the Ms and . In the instant invention MNC offers a much higher Ms and compared with ferrite. The high Ms of up to 2.2 Tesla comes from ferromagnetic nanofiber material, compared to ferrites with Ms of <0.2 Tesla. Using the current approach, phase 1 circulator dimension specifications can readily be met, based on current MNC without tuning of the dielectric constant. However, the dielectric constant of the magnetic nanofiber is readily tunable, by doping extremely high dielectric constant (6001500) material such as Ba(Sr, Ti)O.sub.3, Pb(Zr, Ti)O.sub.3, SrTi O.sub.3 into the composite (see nanoparticles 42 in
(48) For all magnetic material based circulator, both insertion loss and isolation performances are closely correlated to the FMR line-width of the magnetic material. In the instant invention, given the source material and the manufacturing process, the system results in MNC homogeneity and alignment. In one embodiment, the instant invention employs film casting under the external magnetic field, which shows a >90% alignment of the nanofibers, and has demonstrated a narrow FMR line width of the MNC material that leads to low insertion loss.
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(50) Although exemplary implementations of the invention have been depicted and described in detail herein, it will be apparent to those skilled in the relevant art that various modifications, additions, substitutions, and the like can be made without departing from the spirit of the invention and these are therefore considered to be within the scope of the invention as defined in the following claims.
(51) It is to be understood that the above description is intended to be illustrative, and not restrictive. For example, the above-described embodiments (and/or aspects thereof) may be used in combination with each other. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from its scope. While the dimensions and types of materials described herein are intended to define the parameters of the invention, they are by no means limiting, but are instead exemplary embodiments. Many other embodiments will be apparent to those of skill in the art upon reviewing the above description. The scope of the invention should, therefore, be determined with reference to the appended claims, along with the full scope of equivalents to which such claims are entitled. In the appended claims, the terms including and in which are used as the plain-English equivalents of the terms comprising and wherein. Moreover, in the following claims, the terms first, second, and third, are used merely as labels, and are not intended to impose numerical requirements on their objects. Further, the limitations of the following claims are not written in means-plus-function format and are not intended to be interpreted based on 35 U.S.C. 112, sixth paragraph, unless and until such claim limitations expressly use the phrase means for followed by a statement of function void of further structure.