MODIFIED NI-ZN FERRITES FOR RADIOFREQUENCY APPLICATIONS

Abstract

Embodiments disclosed herein relate to using cobalt (Co) to fine tune the magnetic properties, such as permeability and magnetic loss, of nickel-zinc ferrites to improve the material performance in electronic applications. The method comprises replacing nickel (Ni) with sufficient Co+2 such that the relaxation peak associated with the Co+2 substitution and the relaxation peak associated with the nickel to zinc (Ni/Zn) ratio are into near coincidence. When the relaxation peaks overlap, the material permeability can be substantially maximized and magnetic loss substantially minimized. The resulting materials are useful and provide superior performance particularly for devices operating at the 13.56 MHz ISM band.

Description

INCORPORATION BY REFERENCE TO ANY PRIORITY APPLICATIONS

Any and all applications for which a foreign or domestic priority claim is identified in the Application Data Sheet of the present application are hereby incorporated by reference under 37 CFR 1.57.

BACKGROUND OF THE INVENTION

Field of the Invention

Embodiments of the invention relate to compositions and materials useful in electronic applications, and in particular, in radio frequency (RF) electronics.

Description of the Related Art

Various crystalline materials with magnetic properties have been used as components in electronic devices such as cellular phones, biomedical devices, and RFID sensors. It is often desirable to modify the composition of these materials to improve their performance characteristics. For example, doping or ion substitution in a lattice site can be used to tune certain magnetic properties of the material to improve device performance at radio frequency ranges. However, different ions introduce different changes in material property that often result in performance trade-offs. Thus, there is a continuing need to fine tune the composition of crystalline materials to optimize their magnetic properties, particularly for RF applications.

SUMMARY

The compositions, materials, methods of preparation, devices, and systems of this disclosure each have several aspects, no single one of which is solely responsible for its desirable attributes. Without limiting the scope of this invention, its more prominent features will now be discussed briefly.

Any terms not directly defined herein shall be understood to have all of the meanings commonly associated with them as understood within the art. Certain terms are discussed below, or elsewhere in the specification, to provide additional guidance to the practitioner in describing the compositions, methods, systems, and the like of various embodiments, and how to make or use them. It will be appreciated that the same thing may be said in more than one way. Consequently, alternative language and synonyms may be used for any one or more of the terms discussed herein. No significance is to be placed upon whether or not a term is elaborated or discussed herein. Some synonyms or substitutable methods, materials and the like are provided. Recital of one or a few synonyms or equivalents does not exclude use of other synonyms or equivalents, unless it is explicitly stated. Use of examples in the specification, including examples of terms, is for illustrative purposes only and does not limit the scope and meaning of the embodiments herein.

Embodiments disclosed herein relate to using cobalt (Co) to fine tune the magnetic properties, such as permeability and magnetic loss, of nickel-zinc ferrites to improve the material performance in electronic applications. In one embodiment, the method comprises replacing nickel (Ni) with sufficient Co⁺² such that the relaxation peak associated with the Co⁺² substitution and the relaxation peak associated with the nickel to zinc (Ni/Zn) ratio are into near coincidence. Advantageously, when the relaxation peaks overlap, the material permeability can be substantially maximized and magnetic loss substantially minimized. The resulting materials are useful and provide superior performance particularly for devices operating at the 13.56 MHz ISM band. In one embodiment, permeability in excess of 100 is achieved with a Q factor of the same order at 13.56 MHz. In another embodiment, the method comprises doping NiZn spinels with Co⁺² to produce a series of NiZn plus Co materials with reducing Zn, which covers up to about 200 MHz with permeability in excess of 10 and favorable Q factor. The method of using Co to fine tune NiZn compositions are preferably achieved through advanced process control using high resolution X-ray fluorescence.

In a preferred embodiment, the material composition is represented by the formula Ni_1-x-yZn_xCo_yFe₂O₄ which can be formed by doping Ni_(i-x)Zn_xFe₂O₄ with Co⁺². In certain implementations, x=0.2 to 0.6, and 0≤y<0.2. Embodiments of the material composition can have the spinel crystal structure and can be single phase. The material compositions can be used in a wide variety of applications including but not limited to antennas with high material content such as those useful for cellular phones, biomedical devices, and RFID sensors.

In some embodiments, an antenna designed to operate at the 13.56 MHz ISM band comprising nickel zinc ferrite doped with Co⁺² is provided. Preferably, the relaxation peak associated with the Co⁺² substitution and the relaxation peak associated with the Ni/Zn ratio are in near coincidence. In one implementation, the nickel zinc ferrite doped with Co⁺² can be represented by the formula Ni_1-x-yZn_xCo_yFe₂O₄, where x=0.2 to 0.6, and 0≤y<0.2. In some other embodiments, an RFID sensor designed to operate at the 13.56 MHz ISM band comprising nickel zinc ferrite doped with Co⁺² is provided. Preferably, the relaxation peak associated with the Co⁺² substitution and the relaxation peak associated with the Ni/Zn ratio are in near coincidence. In one implementation, the nickel zinc ferrite doped with Co⁺² can be represented by the formula Ni_1-x-yZn_xCo_yFe₂O₄, where x=0.2 to 0.6, and 0≤y<0.2.

Some embodiments include methods of replacing at least some of the nickel (Ni) with sufficient Cobalt (Co²⁺) in nickel-zinc ferrites. In one embodiment, the method comprises blending NiO, Fe₂O₃, CoO_x, MnO_x, ZnO, and CuO_x to form a mixture having a pre-determined ratio of Ni to Zn and a pre-determined Co concentration. The formula for this series of materials is preferably Ni_1-w-x-y-zZn_wCo_xMn_yCu_zFe₂O₄. The method further comprises drying the material, followed by calcining, milling, and spray drying the material. The method further comprises forming the part and then sintering the part. The part can be an antenna such as those useful for cellular phones, biomedical devices, and RFID sensors.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates the variations in permeability (μ) of a nickel-zinc system at various levels of Ni and Zn content;

FIG. 2 shows a listing of FIGS. 2A-2L which illustrates a series of cobalt spectra showing the shift in frequency (x axis) of the first peak (lowest frequency) as well as complex permeability (y axis);

FIG. 3 illustrates that two relaxation peaks are observed in the magnetic permeability spectra of the material between 100 kHz and 1 GHz;

FIG. 4 illustrates a method of tuning the magnetic properties of a Ni—Zn ferrite system according to one embodiment of the present disclosure;

FIG. 5 illustrates a method of manufacturing a cobalt doped nickel-zinc ferrite composition according to one embodiment of the present disclosure; and

FIG. 6 shows that in some embodiments, a wireless device can incorporate a material composition as described herein.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

Disclosed herein are methods for fine tuning the magnetic properties of nickel zinc ferrites to improve the material performance in various electronic applications. Also disclosed herein are modified nickel zinc ferrite materials that are particularly suitable for use in various electronic devices operating at the 13.56 MHz ISM band. The modified nickel zinc ferrite material prepared according to embodiments described in the disclosure exhibits favorable magnetic properties such as increasing permeability and reducing magnetic loss.

Aspects and embodiments of the present invention are directed to improved materials for use in electronic devices. For example, these materials may be used to form an RF antenna for implantable medical devices, such as glucose sensors. These materials may also be used for other purposes, such as to form antennas for non-implantable devices, or other components of implantable or non-implantable devices. Advantageously, the materials have a combination of superior magnetic permeability and magnetic loss tangent at or about the 13.56 MHz industrial, medical and scientific band. In various embodiments, the materials are formed by fine tuning the permeability and magnetic loss of NiZn spinels with cobalt. As described in greater detail below, by bringing the relaxation peak associated with the Co²⁺ substitution and that associated with the Ni/Zn ratio into near coincidence, the permeability can be maximized and the magnetic loss minimized, such that permeability in excess of 100 can be achieved with Qs of the same order at 13.56MHz. The same technique can be used to produce a series of NiZn plus Co materials with reducing Zn covering up to 200 MHz with permeability in excess of 10 and good Q.

Ni—Zn Systems

Nickel-zinc ferrites can be represented by the general formula Ni_xZn_1-xFe₂O₄ and are useful in electromagnetic applications that require high permeability. FIG. 1 illustrates the variations in permeability (μ) of a nickel-zinc ferrite system at various levels of Ni and Zn content. For example, the permeability decreases with decreasing zinc content at about 13.56 MHz. Variation of permeability suggests that low magnetic loss (high magnetic Q) material can be derived from the Ni—Zn system with low or zero zinc content in applications where the permeability is not so important. However, for certain RFID tags and sensors, the Ni—Zn system does not provide the optimum performance because either the permeability is too low for compositions with favorable Q, or that the Q is too low for compositions with high permeability.

The Effect of Cobalt Doping

FIG. 2 shows a listing of FIGS. 2A-2L which illustrates a series of cobalt spectra showing the shift in frequency (x axis) of the first peak (lowest frequency) as well as complex permeability (y axis). The effect of cobalt on frequency begins to stall out at about 0.025 cobalt because the magnetocrystalline anisotropy eventually passes through a minimum, just as the complex permeability flattens out, then falls again. As shown in FIGS. 2A-2L, the cobalt driven first peak eventually merges with the second peak as the Co⁺² concentration increases.

FIG. 3 shows that two relaxation peaks are observed in the magnetic permeability spectra of the material between 100 kHz and 1GHz. Without being bound to a particular theory, it is believed that the lower frequency peak corresponds to magnetic domain wall rotation and the higher frequency peak corresponds to magnetic domain wall bulging. It is also believed that the cobalt oxide may push the lower frequency relaxation peak associated with the magnetic loss to higher frequency values by reducing the magnetocrystalline anisotropy of the spinel material. These higher frequency values are, in some embodiments, higher than 13.56 MHz, which is a frequency often used in RFID tags and RF medical sensor applications. It is also believed that manganese may serve to prevent the iron from reducing from Fe³⁺ to Fe²⁺ state and therefore improves the dielectric loss of the material across the spectrum, and copper may serve as a sintering aid allowing the firing temperatures to be reduced, thus preventing Zn volatilization from the surface of a part formed from the material. Both the relaxation peaks referred to above may be adjusted to provide high permeability low-loss materials throughout a range of between about 1 MHz and about 200 MHz.

Without wishing to be bound by theory, it is believed that the second peak is determined by the Ni/Zn ratio and is therefore static for a fixed ratio. The Co²⁺ is lost as a distinguishing peak in the spectrum at higher Co²⁺ concentration. It is also believed that the first peak may be dominated by domain movement, and the second peak may be dominated by rotation and that the peaks can be merged at some Co²⁺ doping levels for a given Ni/Zn ratio, and that only the domain movement peak is strongly susceptible to Co²⁺.

Based on the inventors' theory that domain rotation is driven by the Ni/Zn ratio and is responsible for a characteristic peak frequency, and that wall movement (bulging via magnetorestriction) is driven by the Co²⁺ concentration which creates a second, independent characteristic peak, a combination of Co²⁺ and Ni/Zn can be selected to merge at a given frequency such that the slope of the absorption curve is a given frequency distance way to minimize magnetic losses. The optimum peak position can be selected depending on the desired permeability and loss. For some applications, the optimum peak position is about 100 MHz to give low losses but high permeability at 13.56 MHz.

Modified Ni—Zn Systems

Certain embodiments of the present disclosure provide a modified nickel-zinc ferrite material. The base nickel-zinc ferrite material preferably has a composition that is represented by the formula Ni_0.5Zn_0.5Fe₂O₄. The material has an iron deficiency of between 0.02 and 0.10 formula units, a cobalt content of between 0 and 0.05 formula units (substituting for Ni), and manganese (substituting for Fe) and copper (substituting for Ni) contents of between 0 and 0.03 formula units. Embodiments of the material can have a spinel crystal structure and can be single phase.

In some implementations, the modified Ni—Zn ferrite material can have a composition represented by the formula Ni_1-w-x-y-zZn_wCo_xMn_yCu_zFe₂O₄ where w ranges from 0.2 to 0.6, and x, y, and z each range from 0 to 0.2, and a ranges from 0 to 0.2. In a preferred implementation, w=0.4725, x=0.0225, y=0.02, z=0, and a=0.08, which can result in a material that displays particularly desirable magnetic properties at 13.56 MHz. In another preferred implementation, w=0.4, x=0.0275, y=0.01, z=0, and a=0.08, which can result in a material that displays particularly desirable magnetic properties at 27 MHz.

Table 1 below illustrates the effects of embodiments of Co substitution in a fully dense 5000 Gauss Ni_1-x-yZn_xCo_yFe₂O₄ Spinel on Spectra.

		2nd		Initial
Cobalt	1st Frequency	Frequency	3rd Frequency	Permeability
Substitution (y)	(MHz)	(MHz)	(MHz)	at 1 MHz
0.00	16	merged	merged	170
0.005	40	merged	merged	92
0.01	50	70	150	68
0.0125	60	80	200	62
0.015	60	80	250	50
0.0175	60	85	250	55
0.02	70	100	250	45
0.0225	70	110	230	51
0.025	80	110	230	52
0.0275	100	120	230	54
0.03	100	130	230	50

Methods of Manufacturing Modified Ni—Zn Material

FIG. 4 illustrates a method of tuning the magnetic properties of a Ni—Zn ferrite system according to one embodiment of the present disclosure. The method begins with identifying a desired operational frequency in Step 100, followed by adjusting the nickel to zinc ratio in Step 110. Preferably, the Ni/Zn ratio is adjusted to provide a relaxation absorption peak at a desired frequency above a desired low magnetic loss frequency. The method further comprises adjusting the cobalt content in Step 120. Preferably, the cobalt content is adjusted to a level where the cobalt dominated relaxation peak merges into the low frequency end of the Ni/Zn ratio peak. The method can be followed by forming a part with the identified Ni/Zn ratio and Co concentration in Step 130. In some applications, it would be desirable to use excess cobalt because excess cobalt would likely reduce the magnetic permeability without increasing the magnetic loss. A desirable amount of cobalt can be determined by identifying an amount of cobalt that produces a relaxation absorption peak at a frequency that cannot be resolved from the Ni/Zn ratio peak by eye in an impedance analysis trace on the low frequency side. For example, if one were interested in an RF application at 27 MHz, a material could be synthesized with the composition Ni_0.5725Co_0.0275Zn_0.4Fe₂O₄, which has a permeability of 54 and a magnetic Q greater than 100, wherein the magnetic Q is the ratio of the real permeability to the imaginary permeability at a specified frequency.

FIG. 5 illustrates a method of manufacturing a cobalt doped nickel-zinc ferrite composition according to one embodiment of the present disclosure. The method begins with Step 200 in which the raw oxides nickel oxide (NiO), iron oxide (Fe₂O₃), zinc oxide (ZnO), copper oxide (CuO, CuO₂, Cu₂O, and/or Cu₂O₃), cobalt oxide (CoO, Co₂O₃, and/or Co₃O₄), and manganese oxide (MnO, Mn₂O₃, Mn₂O₇, Mn₃O₄, MnO₂, and/or MnO₃), are blended by a shear mixing method such as a Cowles mixer or by vibratory mill blending. Step 210 indicates drying the material. The method further includes Step 220 in which the material is calcined at a temperature in the range of 900° C.-1,200° C. to react the components of the material and form the spinel phase, followed by Step 230 in which the material is milled to a particle size between 1 to 10 microns, and spray dried with added binder in Step 240. In some implementations, the method further comprises Step 250 in which the material is formed into a part by isostatic or hard die pressing and Step 260 in which the part is sintered to a temperature in the range of 1,100° C.-1400° C. in air or in oxygen.

Device and System Incorporating Modified Ni—Zn Material

The material compositions made in accordance with embodiments described herein can be used in a wide variety of applications including but not limited to antennas with high material content such as those useful for cellular phones, biomedical devices, and RFID sensors. FIG. 6 shows that in some embodiments, a wireless device 600 can incorporate a material composition as described herein. Such a device 600 can include a module 602, a battery 604, an interface 606, and an antenna 608. The antenna 608 can be configured to facilitate transmission and reception of RF signals, preferably in the 13.56 MHz range. The antenna 608 comprises a cobalt doped nickel zinc ferrite configured in such a manner that the cobalt content is adjusted to a level where the cobalt dominated relaxation peak merges into the low frequency end of the Ni/Zn ratio peak. In one implementation, at least a portion of the antenna 608 has a composition that can be represented by the formula Ni_1-x-yZn_xCo_yFe₂O₄, where x=0.2 to 0.6, and 0≤y<0.2. In another implementation, at least a portion of the antenna 608 has a composition that can be represented by the formula Ni_1-w-x-y-zZn_wCo_xMn_yCu_zFe_2-aO_4-x where 0.2≤w≤0.6; 0≤x≤0.2; 0≤y≤0.2; 0≤z≤0.2; and 0≤a≤0.2.

While certain embodiments of the inventions have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the disclosure. Indeed, the novel compositions, methods and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the compositions, methods and systems described herein may be made without departing from the spirit of the disclosure. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the disclosure.

Claims

1. (canceled)

2. A fine-tuned nickel-zinc ferrite material comprising: a base nickel-zinc ferrite material doped with cobalt (CO2+) to adjust a nickel to zinc ratio of the base nickel-zinc ferrite material thereby providing a Ni/Zn relaxation absorption peak at a desired frequency above a desired low magnetic loss frequency, the cobalt being doped into the base nickel-zinc ferrite material to a level where a cobalt dominated relaxation peak merges into a low frequency end of the Ni/Zn relaxation absorption peak, the fine-tuned nickel-zinc ferrite material being represented by the formula Ni1-x-yZnxCoyFe2O4, x being between 0.2 and 0.6, and y being between 0 and 0.2

3. The fine-tuned nickel-zinc ferrite material of claim 2 wherein the fine-tuned nickel-zinc ferrite material has a composition Ni0.5725Co0.0275Zn0.4Fe2O4.

4. The fine-tuned nickel-zinc ferrite material of claim 2 wherein the base nickel-zinc ferrite material has a composition Ni0.5Zn0.5Fe2O4.

5. The fine-tuned nickel-zinc ferrite material of claim 2 wherein the fine-tuned nickel-zinc ferrite material has a permeability in excess of 100.

6. The fine-tuned nickel-zinc ferrite material of claim 2 wherein the desired frequency is about 100 MHz.

7. A radiofrequency component comprising: a base nickel-zinc ferrite material doped with cobalt (CO2+) to adjust a nickel to zinc ratio of the base nickel-zinc ferrite material thereby providing a Ni/Zn relaxation absorption peak at a desired frequency above a desired low magnetic loss frequency, the cobalt being doped into the base nickel-zinc ferrite material to a level where a cobalt dominated relaxation peak merges into a low frequency end of the Ni/Zn relaxation absorption peak, the fine-tuned nickel-zinc ferrite material being represented by the formula Ni1-x-yZnxCoyFe2O4, x being between 0.2 and 0.6, and y being between 0 and 0.2

8. The radiofrequency component of claim 7 wherein the fine-tuned nickel-zinc ferrite material has a composition Ni0.5725Co0.0275Zn0.4Fe2O4.

9. The radiofrequency component of claim 7 wherein the base nickel-zinc ferrite material has a composition Ni0.5Zn0.5Fe2O4.

10. The radiofrequency component of claim 7 wherein the fine-tuned nickel-zinc ferrite material has a permeability in excess of 100.

11. The radiofrequency component of claim 7 wherein the desired frequency is about 100 MHz.

12. The radiofrequency component of claim 7 wherein the component is included in an antenna.

13. The radiofrequency component of claim 12 wherein the antenna is configured to facilitate transmission and reception of radiofrequency signals in the 13.56 MHz range.

14. The radiofrequency component of claim 7 wherein the component is included in a battery.

15. The radiofrequency component of claim 7 wherein the component is included in a glucose sensor.

16. A method of fine tuning nickel-zinc ferrite material into a fine-tuned nickel-zinc ferrite material, said method comprising: adjusting a nickel to zinc ratio of a base nickel-ferrite material to provide a Ni/Zn relaxation absorption peak at a desired frequency above a desired low magnetic loss frequency; anddoping the material with cobalt (CO2+) to a level where a cobalt dominated relaxation peak merges into a low frequency end of the Ni/Zn relaxation absorption peak, the material being represented by the formula Ni1-x-yZnxCoyFe2O4, x being between 0.2 and 0.6, and y being between 0 and 0.2.

17. The method of claim 16 wherein the fine-tuned nickel-zinc ferrite material has a composition Ni0.5725Co0.0275Zn0.4Fe2O4.

18. The method of claim 16 wherein the base nickel-zinc ferrite material has a composition Ni0.5Zn0.5Fe2O4.

19. The method of claim 16 wherein the fine-tuned nickel-zinc ferrite material has a permeability in excess of 100.

20. The method of claim 16 wherein the desired frequency is about 100 MHz.

21. The method of claim 16 further comprising calcining the fine-tuned nickel-zinc ferrite material at a temperature range of 1100° C.-1400° C.