The present invention generally relates to the construction of embedded electronic components, and in particular, to such components as they apply to signal processing.
Conventional digital communications utilize the intensity of a signal pulse to encode a binary bit of information, using a full or high amplitude pulse to convey the 1 bit of information and a low or no amplitude pulse to signal the 0 bit datum, or vice versa. Wireless communications operate under the constraints of finite bandwidth and multiple sources of signal interference that can cause high bit error rate levels in data streams using simple digital codes. Spread-spectrum signaling protocols have been developed to address these issues in a manner that provide meaningful data rates and higher signal integrity. These protocols utilize phase shift keying (PSK) or quadrature amplitude modulation techniques to shape the transmitted pulse into a symbol that encodes a series of consecutive data bits into a single pulse.
These symbol modulation techniques affect the shape of the pulse through the signal roll-off parameter, α, which can take on values ranging between 1≦α≦0. As shown in
Conventional receivers will use sensors to register the pulse's time domain signature and dedicate processor functions to perform inverse Fast Fourier Transforms (IFFF) or inverse Discrete Fast Fourier Transforms that mathematically compute pulse's power spectral density. The use of mathematical methods to de-convolve a symbol's power spectral density adds component cost to the receiver, consumes additional power from any available power budget, and occupies valuable real estate when packaged on a mobile wireless platform.
This is particularly so in wireless communications systems based on orthogonal frequency division multiplexing (OFDM). OFDM techniques, including, but not limited to, WiMAX systems, are multi-carrier modulation methods developed to boost data rates reliably. Boosting data rates on a single carrier by shortening symbol time lengths is often more susceptible to increased bit error rates. OFDM methods use a plurality of carriers (often referred to as “sub-carriers”) operating at a lower data rate. This allows the composite data of all sub-carriers to be communicated at a combined rate that is comparable to the data rate of a single carrier with the same channel bandwidth using the same basic modulation at a higher data rate. The principal advantages to using longer symbol duration times is a net reduction in error rate by reduced susceptibility to errors from inter-symbol interference caused by multi-path time dispersion. Furthermore, inter-symbol interference is not as problematic when frequency-selective fading is distributed only over a few of the sub-carriers and the fading depth over the majority of sub-carriers is not great enough to generate significant bit errors.
Passive resistor, capacitor, and inductor components, collectively referred to as passive components, are used to form the filtering stages that comprise these devices. At present, most passive components are assembled on the surface of a printed circuit board and generally comprise 80% of all the components used in a fully populated circuit board and account for 50% of the real estate occupied on the circuit board's major surface. Small form factor is a general requirement for mobile wireless systems. Therefore, methods that reduce a circuit's footprint by transferring the passive components from the circuit board's surface to one or more interior layers are desirable. This practice, more commonly known as embedded passive technology, is also useful in larger scale high-speed circuits, such as servers and telecommunications switches, which require a large number of electrically terminated transmission lines. Although embedded passive technologies have been under development since the early 1980's, very few approaches have been successful in meeting optimal performance tolerances. The inability to rework (exchange) an out-of-tolerance passive component after it has been embedded into the circuit board requires tolerances of ±1% of targeted performance for these components, since the failure of a single component causes the entire board value to be lost. Additionally, it is desirable for embedded passives to maintain their targeted performance tolerances over all anticipated operating temperatures to facilitate design and ensure circuit reliability. Operating temperatures typically range from −40° C. to +125° C. Most of the prior art on embedded passive technologies relies on thin film technologies that comprise a layer of material with uniform dielectric properties. Resistive metal thin films have demonstrated the greatest ability to achieve thermally stable performance with tolerances within ±1%.
As shown in
Thin film techniques are also used to fabricate embedded capacitors. Demand for embedded capacitors has been driven largely by a need to suppress power noise in high-speed CMOS semiconductor circuits, wherein simultaneous flipping of switching devices draws a large surge current that is supplied by the power plane embedded in the circuit board to which the semiconductor device is attached. Power noise is generated in the circuit when inadequate charge is available from within the power plane to supply the surge current. Decoupling capacitors are used to suppress power noise in high-speed circuits.
U.S. Pat. No. 5,154,973 to Imagawa, et al., disclose a dielectric lens antenna that includes high-κ dielectric ceramic compositions prepared from powders with a mean particle size ranging between 1 and 50 micron that are mixed with an organic thermoplastic material. U.S. Pat. No. 5,892,489 to Kanba et al., disclose a chip antenna incorporating high-κ oxide ceramics formed from powders having a mean particle size of 10 microns. U.S. patent No. to K-D Koo, et al., disclose a chip antenna which comprises helically wound conductors formed by printing planar trace structures on dielectric sheets and assembling those sheets to form said chip antenna. U.S. Pat. No. 6,028,568 to K. Asakura, et al., disclose a chip antenna containing at least one folded antenna formed by printing conductor on a plurality of dielectric layers, wherein at least one dielectric layer is a magnetic material, and fusing said dielectric layers into a solid structure. U.S. Pat. No. 6,222,489 B1 to T. Tsuru, et al., disclose a chip antenna containing monopole or dipole antenna prepared by printing conductor traces on a plurality of dielectric layers, wherein each individual layer has uniform composition providing said individual layer with either a relative permittivity of ∈R=1-130 or relative permeability of μR 1-7, and said plurality of layers is fused into a single component. U.S. Pat. No. 6,650,303 B2 to H. J. Kim, et al., disclose a chip antenna comprising a plurality of dielectric sheets, wherein each sheet has uniform composition throughout the sheet, and conductor leads that are configured to form a helical antenna. U.S. Pat. Nos. 6,680,700 B2 and 6,683,576 B2 to A. Hilgers disclose a chip antenna that comprises a core ceramic substrate having uniform dielectric properties and conducting metal traces on its periphery that is surface mounted to a circuit board. U.S. Ser. No. 6,025,811 to Canora et al. disclose a directional antenna with a closely-coupled director embedded or mounted on a circuit wherein the director element is a conductive element that has a rectangular cross-sectional profile. U.S. Ser. No. 10/265,351 filed by T. T. Kodas et al. disclose inkjet techniques to form conductive electronic materials from a colloidal suspension of nanoparticles in a low viscosity solvent. U.S. Ser. No. 10/286,363 filed by Koda et al. disclose direct-write (syringe-based) methods to form inorganic resistors and capacitors from a flowable high-viscosity precursor solution consisting of combination of molecular precursors and inorganic powders. U.S. Pat. Nos. 6,036,899 and 5,882,722 disclose methods and formulations to apply metallization layers using nano-particle pastes.
U.S. Pat. No. 6,027,826 to de Rochemont, et al., disclose articles and methods to form oxide ceramic on metal substrates to form laminate, filament and wire metal-ceramic composite structures using metalorganic (molecular) precursor solutions and liquid aerosol spray techniques. U.S. Pat. Nos. 6,323,549 and 6,742,249 to de Rochemont, et al., disclose articles that comprise, and methods to construct, an interconnect structure that electrically contacts a semiconductor chip to a larger system using at least on discrete wire that is embedded in silica ceramic, as well as methods to embed passive components within said interconnect structure using metalorganic (molecular) precursor solutions and liquid aerosol spray techniques. U.S. Pat. Nos. 5,707,715 and 6,143,432 to de Rochemont, et al., disclose articles and methods to relieve thermally-induced mechanical stress in metal-ceramic circuit boards and metal-ceramic and ceramic-ceramic composite structures prepared from a solution of metalorganic (molecular) precursors, and further discloses the incorporation of secondary phase particles (powders) in said solution of said solution of metalorganic (molecular) precursors. The contents of each of these references are incorporated herein by reference as if laid out in their entirety. U.S. Ser. No. 11/243,422 discloses articles and methods to impart frequency selectivity and thermal stability to a miniaturized antenna element, and the construction of simplified RF front-end architectures in a single ceramic module.
One embodiment of the present invention provides an electrical component, comprising a ceramic element located on or in a dielectric substrate between and in contact with a pair of electrical conductors, wherein the ceramic element includes one or more metal oxides having fluctuations in metal-oxide compositional uniformity less than or equal to 1.5 mol % throughout the ceramic element.
The metal oxides may substantially consist of particles having a substantially uniform grain size. The grain size is measured along a major axis of each particle, and it is less than 1.5 times and greater than 0.5 times an average grain size contained in the ceramic element. The grain size is determined by controlling heat treatment during fabrication.
The ceramic element an electrical characteristic determined by which specific metal oxides are included. The electrical characteristic is effected by controlling average grain size using heat treatment during fabrication. The electrical characteristic of the ceramic element exhibits a substantially constant value which varies ≦1% over an operating temperature range of 40° C. to 120° C.
The ceramic element may be fabricated by causing simultaneous decomposition of metalorganic precursors. The simultaneous decomposition may be achieved by using rapid thermal annealing on deposited the metalorganic precursors. The ceramic element may be fabricated by depositing carboxylate salt precursors prior to the simultaneous decomposition. The precursors may be deposited as a wax compound. Radiant energy may be applied to the deposited precursors to cause the simultaneous decomposition.
The metal oxides may have a rutile, pyrochlore, perovskite, body-centered cubic, rhombic dodecahedron, rhombic trapezohedron crystalline phase, or mixtures thereof, that includes amounts of one or more of copper oxide (CuO), nickel oxide (NiO), ruthenium oxide (RuO2), iridium oxide (IrO2), rhodium oxide (Rh2O3), osmium oxide (OsO2), antimony oxide (Sb2O3), titanium oxide (TiO2), zirconium oxide (ZrO), hafnium oxide (HfO), tantalum oxide (Ta2O5), niobium oxide (Nb2O5), iron oxide (Fe2O3), and silicon oxide (SiO4).
The ceramic element may include a resistive metal oxide material having an intrinsic sheet resistivity greater than 25 μΩ-cm. The ceramic element may also include a conductive metal oxide and further wherein the electrical component is a resistor. The metal oxides may have a rutile, pyrochlore, or perovskite crystalline phase that includes amounts of one or more of copper oxide (CuO), nickel oxide (NiO), ruthenium oxide (RuO2), iridium oxide (IrO2), rhodium oxide (Rh2O3), osmium oxide (OsO2), antimony oxide (Sb2O3), and indium-tin oxide. The metal oxides may be from the group consisting of: bismuth oxide (Bi2O3), lanthanum oxide (La2O3), cerium oxide (Ce2O3), lead oxide (PbO) and neodymium oxide (Nd2O3). The metal oxides may include alkaline earth metal oxides drawn from the group consisting of magnesium oxide (MgO), calcium oxide (CaO), strontium oxide (SrO), barium oxide (BaO), scandium oxide (Sc2O3), titanium oxide, (Ti2O3), vanadium oxide (V2O3), chromium oxide (Cr2O3), manganese oxide (Mn2O3), and iron oxide (Fe2O3). The metal oxides may substantially consist of particles having a substantially uniform grain size. The ceramic element may have a resistivity or resistance value which varies ≦5% over an operating temperature range of −40° C. to 125° C. The ceramic element may have a resistivity or resistance value which varies ≦1% over an operating temperature range of −40° C. to 125° C. The ceramic element can have a resistance value anywhere between 10 ohms and 50 mega-ohms. The ceramic element can have a resistance value anywhere between 1 ohm and 500 mega-ohms.
The electrical component may be a capacitor with the pair of electrical conductors forming opposing electrodes and the ceramic element forming a dielectric thereof. The one or more metal oxides may substantially consist of particles having a substantially uniform grain size.
The capacitor can have a capacitance value anywhere between 0.01 pF to 900 μF. Each of the pair of electrical conductors may include a separate enlarged area having an opposed orientation to each other with the ceramic element located there between. The electrical conductors and the ceramic element may form a sheet capacitor having a capacitance>20 nF/inch2.
The pair of electrical conductors may be in the form of circuit board traces and create a multiplicity of closely spaced, interdigitated fingers for the opposing electrodes. The ceramic element may be located in a meandering gap formed between the interdigitated fingers, and the meandering gap may maintains a substantially constant spacing and even in curved or corner areas of the meandering gap.
The ceramic element may have a dielectric constant value which varies ≦5% over an operating temperature range of 40° C. to 120° C. The metal oxides may substantially consist of particles having a substantially uniform grain size which averages less than 70 nanometers. The ceramic element may have a dielectric constant value which varies ≦1% over an operating temperature range of 40° C. to 120° C. The metal oxides may substantially consist of particles having a substantially uniform grain size which averages less than 50 nanometers.
The ceramic element may have high permittivity, and the one or more metal oxides may have perovskite crystal structures and will generally have the chemical formula M(1)M(2)O3, with metals from group M(1) and M(2) included in 1:1 molar ratios. Each group M(1), M(2) may include a plurality of metals with the combined molarity for each group being the same. The two metals, M(1a), M(1b), may be selected from group M(1) and two other metals may selected from group M(2), and the one or more metal oxides have the chemical formula M(1a)(1-x)M(1b)(x)M(2a)(1-y) M(2b)(y)O3. The metal oxides of group M(1) may include: alkaline earth metal oxides selected from magnesium oxide (MgO), calcium oxide (CaO), strontium oxide (SrO), and barium oxide (BaO); alkali metal oxides selected from lithium oxide (Li2O), sodium oxide (Na2O), potassium oxide (K2O), and rubidium oxide (Rb2O); and heavy-metal oxides selected from the group including lanthanum oxide (La2O3), cerium oxide (Ce2O3), lead oxide (PbO) and neodymium oxide (Nd2O3). The metal oxides of group M(2) may include titanium oxide (TiO2), zirconium oxide (ZrO), hafnium oxide (HfO), tantalum oxide (Ta2O5), and niobium oxide (Nb2O5).
The pair of electrical conductors may be connected by one or more additional electrical conductors, which encircle the ceramic element to form an inductor. The inductor may exhibits an inductance anywhere over the range of 0.1 pH to 500 nH. The inductor may maintains its inductance value within ±1% over an operating temperature range of 40° C. to 120° C. The metal oxides may have a body-centered cubic crystalline phase, that includes iron oxide (Fe2O3) and amounts of one or more of: cobalt monoxide (CoO), nickel oxide (NiO), zinc oxide (ZnO), manganese oxide (MnO), copper oxide (CuO), vanadium oxide (VO), magnesium oxide (MgO) and lithium oxide (Li2O) The electrical component of claim 42, wherein one metal oxide of the one or more metal oxides is silicon oxide (SiO4) and the ceramic element adopts a rhombic dodecahedron or rhombic trapezohedron crystalline phase, and the other metal oxides include amounts of one or more of: aluminum oxide (Al2O3), iron oxide (Fe2O3), chromium oxide (Cr2O3), vanadium oxide (V2O3), zirconium oxide (ZrO2), titanium oxide (TiO2), silicon oxide (SiO2), yttrium oxide (Y2O3), cobalt oxide (CO3O4), gadolinium oxide (Gd2O3) neodymium oxide (Nd2O3) and holmium oxide (Ho2O3).
The additional electrical conductors may form a coil around the ceramic element. The additional electrical conductors may include a multiplicity of additional conductors, including one or more second electrical conductors formed as circuit board traces and located beneath the ceramic element. Each of the one or more second electrical conductors may be elongated and have contact pads located at opposing ends thereof, wherein the multiplicity of additional conductors includes a plurality of electrical contact posts located on the contact pads and adjacent the ceramic element. The multiplicity of additional conductors may include one or more wire bonds located over the ceramic element and connecting the electrical conductor posts.
The ceramic element may include a plurality of ceramic elements embedded in the dielectric substrate and operatively interconnected. The plurality of ceramic elements may include first and second ceramic elements which each form a different type of passive component. The first and second ceramic elements may form a capacitor and an inductor, respectively. The plurality of ceramic elements may form an electronic filter.
The electrical component may further comprise an integrated circuit mounted on the dielectric substrate and operatively connected to one of the pair of electrical conductors. The ceramic element may include a plurality of ceramic elements embedded in the dielectric substrate, and further wherein the plurality of ceramic elements form an electronic filter. The electrical component may further comprise an antenna element operatively connected to the electronic filter.
The dielectric substrate may be one of a plurality of layers in a multilayer circuit board. One or more of the electrical conductors may include a contact pad, and further comprise an electrical conductor post positioned on the contact pad for providing electrical connection through the dielectric substrate to an adjacent layer in the circuit board. One or more other layers in the multilayer circuit board may include embedded electrical components. The electrical component may further comprise an integrated circuit mounted on one layer of the multilayer circuit board, and operatively connected to one of the pair of electrical conductors.
The dielectric substrate may be formed around the ceramic element. One or more of the electrical conductors and the ceramic element may be first formed on a base substrate. The base substrate may be removed before combining the dielectric substrate with other dielectric substrates to form a multilayer circuit board. One or more additional electrical components may be formed on top of the dielectric substrate at the level of a second layer of the multilayer circuit board, wherein a second dielectric layer is formed around the one or more additional electrical components to form the multilayer circuit board.
In another embodiment of the present invention, a method of fabricating an electrical component, comprises the steps of forming a ceramic element between and in contact with a pair of electrical conductors on a substrate including depositing a mixture of metalorganic precursors and causing simultaneous decomposition of the metal oxide precursors to form the ceramic element including one or more metal oxides.
The simultaneous decomposition may be achieved by using rapid thermal annealing of deposited metalorganic precursors. The ceramic element may be fabricated by depositing carboxylate salt precursors prior to the simultaneous decomposition. The precursors may be deposited as a wax compound. Radiant energy may be applied to the deposited precursors to cause the simultaneous decomposition. The metal oxides may have a rutile, pyrochlore, or perovskite crystalline phase that includes amounts of one or more of copper oxide (CuO), nickel oxide (NiO), ruthenium oxide (RuO2), iridium oxide (IrO2), rhodium oxide (Rh2O3), osmium oxide (OsO2), and antimony oxide (Sb2O3). The metal oxides are formed having fluctuations in metal-oxide compositional uniformity less than or equal to 1.5 mol % throughout the ceramic element. The metal oxides may substantially consist of particles having a substantially uniform grain size. The grain size is measured along a major axis of each particle, and further wherein the grain sizes are less than 1.5 times and greater than 0.5 times an average grain size contained in the ceramic element. The grain size is determined by controlling heat treatment during fabrication.
Yet another embodiment of the invention provides an antenna, comprising: a folded antenna element having a maximum dimension D; and a meta-material dielectric body embedding the folded antenna element a distance S from an exterior surface of the meta-material dielectric body; wherein the meta-material dielectric body comprises a dielectric host have a relative permittivity ∈R≦10 and one or more dielectric inclusions having relative permittivity ∈R>10; the distance S is greater than the protrusion length d of the folded antenna element's reactive near-field region, wherein the reactive near-field protrusion length d is defined as d=0.62√(D3/λ), and λ is the wavelength of an electromagnetic excitation emitted or received by the folded antenna element.
The dielectric host may be an organic dielectric. The organic dielectric may include FR4, Rogers Duroid or PFTE Teflon dielectric. The organic dielectric host may have a loss tangent tan δ≦10−3. The dielectric host may be an inorganic dielectric. The inorganic dielectric host may be a silica or alumina dielectric. The inorganic dielectric host may have a loss tangent tan δ≦10−3. The inorganic dielectric host may have a value for relative permittivity ∈R that is stable over operating temperatures between −150° C. and +250° C.
A further embodiment of the present invention provides an antenna, comprising: a folded antenna element having a maximum dimension D; and a meta-material dielectric body embedding the folded antenna element a distance S from a dielectric inclusion contained within the meta-material dielectric body; wherein the meta-material dielectric body comprises a dielectric host have a relative permittivity ∈R≦10 and one or more dielectric inclusions having relative permittivity ∈R>10; the distance S is greater than the protrusion length d of the folded antenna element's reactive near-field region, wherein the reactive near-field protrusion length d is defined as d=0.62√(D3/λ), and λ is the wavelength of an electromagnetic excitation emitted or received by the folded antenna element.
The present invention describes various embodiments that allow frequency-selective antennas to be configured as a spread-spectrum receiver and use high-k inclusions and closely coupled directors in a manner that imparts radiative gain.
For a better understanding of the present invention, together with other and further aspects thereof, reference is made to the following description taken in conjunction with the accompanying figures of the drawing, wherein:
FIGS. 12A1, 12A2, 12B depict an alternative method to apply a plurality of ceramic compositions in selective locations on a substrate surface by printing LCD electroceramic using solid wax precursors;
The following terms are used herein in the sense of their stated meanings.
The term circuit board is hereinafter defined to mean a passive circuit comprising a single dielectric layer or a plurality of stacked dielectric layers on which conductive traces have been printed or applied that is used to route electrical or electronic signals between one or more semiconductor devices, passive components, and power sources within a larger electronic system. For the purpose of this invention, circuit board may be understood to mean a back plane, a mother board, or a daughter card.
The term “interconnect” is hereinafter defined to mean passive circuit comprising a single dielectric layer or a plurality of stacked dielectric layers on which conductive traces have been printed or applied that is used to route electrical or electronic signals between one or more semiconductors, passive components, power sources, and a circuit board within a larger electronic system. For the purpose of this invention, interconnect is understood to mean a smaller wiring structure that is inserted between one or more semiconductor devices and a circuit board, such that the combination of the interconnect and the one or semiconductor devices functions as a module, or a subsystem module.
The term “electroceramic” is hereinafter defined to mean a ceramic composition that comprises two or more metal oxide components, wherein said metal oxide components have been selected to produce a specific electrical or dielectric response or physical property, such as, dielectric constant (principally defined by the materials relative permittivity (∈R), relative permeability (μR), and loss tangent (tan δ)) or electrical resistivity, etc.
The term “ferroelectric” is used to define a state of spontaneous polarization generated by the collective displacement of ions within the lattice of certain ionic crystals that produces a state of internal electrical polarization without the application of an external electric field. Ferroelectric materials are characterized by a transition-temperature, known as the Curie transition-temperature, below which the ionic crystal displays paraelectric behavior.
The term “paraelectric” is used to define a condition in which a material does not possess internal electrical polarization in the absence of electrical fields.
The acronym “LCD” is hereinafter defined to refer to liquid chemical deposition. Liquid chemical deposition is hereinafter defined to mean the method whereby low-volatility metalorganic salt solutions containing metal oxide precursors to a desired ceramic composition, preferably carboxylate salt precursors, are used to deposit a desired oxide composition by means of a liquid aerosol spray on a substrate heated to temperatures between 250° C. and 500° C., preferably 325° C. and 430° C., or by means of a wax-based inkjet system on substrates held at temperatures below 350° C., preferably below 250° C.
The term “metalorganic precursor” is hereinafter understood to describe an organic molecule to which a specific metal atom has been attached to a carbon atom through an intermediate oxygen bond.
The term “organometallic precursor” is hereinafter understood to describe an organic molecule to which a desired metal atom has been attached directly to a carbon atom.
The term “meta-material dielectric” is hereinafter understood to describe a dielectric body that comprises a lower permittivity, non-magnetic host dielectric that contains at least one higher permittivity or high permeability (μR≠1) dielectric inclusion within its body, wherein the inclusion has physical dimension that is small (≦λ/4, preferably ≦λ/8) compared to the wavelength of an electromagnetic excitation propagating through or incident upon the meta-material dielectric body.
The term “nano-particle conductive pastes” is hereinafter understood to describe a flowable precursor that consists of fine metal particles, with particle dimensions ranging from 10 nm to 100 nm, and additional chemical additives that can be used to screen print or inkjet high quality metallization layers with low conversion temperatures in the range or 100° C. to 350° C.
The term “rapid thermal annealing” is hereinafter understood to describe a heating process wherein a combination of resistive heat and focused radiation are applied to material layers deposited on the surface of substrate in such a way that cause said deposited material layers to be heated to internal temperatures sufficient to initiate crystallization processes in said deposited materials for a short duration of time, but leaves said substrate largely unaffected by the rapid thermal annealing process even if said substrate is susceptible to change in material phase at internal temperatures significantly lower than those used to crystallize said deposited materials. Focused radiation normally is understood to mean an absorptive wavelength of infrared, visible, or ultraviolet light delivered using a laser, a pulsed laser, or one or more lamps. Focused radiation may also include microwave radiation. Controlled gas atmospheres may also need to be used during a rapid thermal annealing process.
The term “passive component” is hereinafter understood to describe an elemental resistor, capacitor, or inductor.
The term “standard operating temperatures” is hereinafter understood to mean temperatures in the range of −40° C. to +125° C.
Applicant hereby incorporates by reference herein the contents of co-pending U.S. patent application Ser. No. 11/243,422, filed Oct. 3, 2005, entitled CERAMIC ANTENNA MODULE AND METHODS OF MANUFACTURE THEREOF.
Methods and devices that provide a means to determine the power spectral density of transmitted symbols using passive, rather than computational methods, have value in reducing the power consumption and cost of a transceiver component used in mobile wireless systems. Furthermore, methods and devices that reduce the form factor of such simplified receivers are also desirable in mobile wireless systems. Precisely tuned passive circuitry with tuning parameters that remain stable with operational temperature, and which is not affected by the surrounding electromagnetic environment, plays an important role in providing the above benefits. Factors that make these circuits susceptible to de-tuning are related primarily to materials selection, the manufacturing methods used to process the selected materials and the design of the dielectric medium that envelopes one or more antennas contained within the module. In general, the tuning of an antenna is affected by dielectric materials that are located within the antenna's near-field radiation pattern. As discussed below, the antenna's near field pattern extends a distance, dnear field, away from the antenna element that is a function of the antenna's maximum dimension and its radiation wavelength. Near-fields often extend beyond the perimeter of the handheld device, which causes the antenna's tuning to change by the dielectric loads that are applied when the device is handled or brought close to the users' head. As discussed below, a specific objective of the present invention is to provide one or more antennas embedded within a dielectric medium that has been engineered to contain all or most of the antenna's reactive near-field within the device. This reduces external influences on the near-field and, in turn, stabilizes the antenna's electromagnetic tuning. Another specific objective is to provide circuits and manufacturing methods with the ability to integrate passive components and dielectric materials having a wide range of performance values on a single circuit layer, wherein said performance values have tolerances and thermal stability that is ≦±1% of the targeted value. This is achieved using liquid chemical deposition (LCD), alternatively referred to as spray-pyrolyzed metalorganic decomposition (SP-MOD) in de Rochemont et al., provides the means to achieve this need.
LCD uses liquid solution to mix one or more metalorganic salt precursors to one or more desired metal oxides at the molecular level. Low volatility metalorganic salts are preferred precursor compounds, specifically carboxylate salt compounds, and, in particular, carboxylate salt compounds having rank (number of carbon atoms) greater than 5. Carboxylate salt compounds with rank 5 or more are predisposed to decompose rather than evaporate at elevated temperatures. This allows a wide variety of precursor compounds to be intimately mixed at the molecular-level in solution, atomized into an aerosol spray and deposited on a substrate that is heated to temperatures elevated above the decomposition temperatures of said precursor compounds. Each species of metalorganic precursor will have a unique decomposition temperature, ranging roughly between 250° C. and 350° C. The molecular-level precursor subdivision achieved in the solution is replicated in the sprayed deposit when the substrate is heated to temperatures that initiate the simultaneous decomposition of all metalorganic species. LCD methods provide a means to achieve a very high degree of chemical uniformity in deposited materials and, more specifically, provide a means to prepare very precisely controlled materials formulations irrespective of the deposited materials' chemical complexity (number of distinct metal oxide components). LCD methods have demonstrated an ability to produce chemically uniform materials with control over metal stoichiometry that has a statistical variance ≦±1.5 mol %. Fluctuations in electroceramic composition that are less than 1.5 mol % have a negligible affect on dielectric performance when the electroceramic is processed into a state of controlled and uniform microstructure. The initial physical state of dielectric materials prepared using LCD methods is that of a solid solution/or glass, which has no discernible crystalline microstructure or grain/particle-size. Microstructure is now understood to have a very strong influence on the dielectric constant and physical properties of electroceramics. A uniform microstructure is a key characteristic of properly annealed LCD ceramics. Unlike powder processed ceramics, which provide a distribution of grain/particle sizes around a certain average where 20%-30% of the grains/particles will have diameters>1.5× the average grain/particle size, a properly annealed LCD 100% of the grains will have particle diameters that are ≦1.5× and ≧0.5× the average grain size, preferably 100% of the grains will have particle diameters that are ≦1.25× and ≧0.75× the average grain size. Proper annealing conditions include temperatures and redox atmospheres that are dependent upon specific ceramic compositions.
In the case of high permittivity electroceramics, smaller grain sizes suppress the formation of critical domains that initiate cooperative interactions responsible for the paraelectric to ferroelectric phase transition. A BST electroceramic parallel plate capacitor, where total capacitance C is derived as:
C=A∈o∈R/d (1)
Where A is the plate area, ∈o is the permittivity constant for free-space (∈o=8.854×10−12 F/m), and ∈R is the relative permittivity constant of the material, will have thermally unstable performance values when the ceramic contains grains have particle dimensions that are greater than 50-70 nm. Stable electrical performance (≦±1% of targeted performance values over designated operating temperatures) cannot be achieved in electroceramic capacitors formed from powder preparations due to their inability to control ceramic microstructure with the requisite precision. Although, recent advances in nano-powder technology claim fine powder preparations ranging from 10 nm to 80 nm, powder preparations do not permit uniform control over particle diameter. Particle diameter is typically defined as the length of the particle's major axis. In general, a given powder preparation will consist of a distribution of particle sizes with an average diameter, wherein 20%-30% of the distribution by volume will include particle diameters that are >1.5× larger than the distributions' average. Although the relationship between grain size (particle diameter) and value of dielectric performance is not linear, however, the curves for 202 and 204 in
LCD electroceramics deposits initially form as a solid solution without any discernible grains. Subsequent heat or laser treatments can be used to supply energy to the electroceramic to nucleate specific microstructure states. The rate of grain growth within the ceramic is dependent upon the precise chemical composition at a nucleation site. LCD controls ceramic composition very precisely (≦±1.5%) throughout the deposit to assure uniform grain growth when energy in sufficient quantities is supplied to initiate nucleation. Thus a specific embodiment of the invention is its ability to fabricate capacitors using high permittivity ceramic electroceramics (∈R≧50), generally known to exhibit ferroelectric behavior, that are provided stable temperature performance through uniform microstructure with grain sizes<70 nm, preferably <50 nm. In a further embodiment of the present invention, said capacitors are embedded within a circuit board or interconnect structure.
Reference is now made to
The reacted solutions are then assayed to determine a precise molar concentration 208A, 208B, . . . , 208N. Inductively-coupled plasma atomic emission spectroscopy (ICP-AES) is the preferred assay method. The assayed solutions are then titrated and thoroughly blended to form a mixed solution 210 that contains a molar stoichiometry known to produce the desired stoichiometry after spray deposition when a multi-component electroceramic is desired. The mixed precursor solution is then filtered once more after blending the plurality of precursors. Solution stoichiometry will differ from the deposit stoichiometry and depend very strongly on specific characteristics of the deposition system. The precursor solution may have to be enriched with certain metal cation concentrations that might be prone to higher loss rates during the deposition process; however, metal cation loss rates are extremely predictable when all process parameters are tightly controlled. Solutions prepared with high rank carboxylate solutions are capable of dissolving high molar concentrations of carboxylic acid salts. Metal densities in solution are more conveniently expressed in terms of their percentage weight of equivalent oxides (wt % equiv. oxide), which allows a quick calculation to determine how much solid oxide material will be created from a given quantity of solution. For instance, 100 gms of a solution that has an 10% wt % equiv. oxide, will produce 10 gms of metal oxide material after the entire quantity of material has been deposited. In general, it is advisable to prepare solutions to have wt % equiv. oxide ranging from 0.001% to 25%, preferably 0.1% to 20%. Dilute solutions (0.001% to 1% wt % equiv. oxide, are preferred when making thin film materials (<1 micron thickness) using liquid aerosol spray deposition. More concentrated solutions, 1% to 25% wt % equiv. oxide, are preferred when fabricating precursor waxes, thick films (1 micron≦deposit thickness<1 mm), or bulk materials (thickness≧1 mm). The prepared solution may then be deposited on a substrate heated to temperatures between 200° C. and 500° C., preferably 250° C. and 430° C., using a liquid aerosol spray 212 for curtain coating processes, or for blanket coating processes when it is intended to completely cover the substrate surface area. The deposition is then followed by a bake out step 213 at temperatures ranging between 300° C. and 600° C., preferably 350° C. and 450° C., to remove any residual organic material remaining in the deposit after the deposition process. Controlled gas atmospheres comprising dry air, an inert gas, such as nitrogen, helium, argon, or others, with or without partial pressure redox gases, such as oxygen, or mixtures of carbon monoxide and carbon dioxide may also be applied during the bake out process to accelerate the removal or residual organic compounds. The bake out step 213 may also comprise a rapid thermal annealing step. Most often, the deposited material remains as a solid solution with no visible crystallization after the bake out step 213. It is usually desirable to render the deposited material into an advanced state of crystallization with a precisely controlled microstructure therefore an optional annealing step 214, preferably a rapid thermal annealing step, is applied. Focused pulsed laser light, using a wavelength that is absorbed by the medium, is a preferred process to be used in the rapid thermal annealing step because it allows a very high degree of control over the energy/power delivered to the deposit during the optional annealing step 214. It is advantageous to use the pulsed laser light annealing in conjunction with other thermal controls described above.
A low cost technique to disperse a variety of ceramic compositions useful as passive components in selective locations over a single sheet or layer is preferred. A low cost technique to disperse a variety of ceramic compositions in selective locations over a single sheet or layer at room temperature or temperatures below 250° C. is also preferred. As a solution process, LCD technology is amenable to direct-write processing, which allows multiple material compositions to be applied locally on a single layer. While inkjet deposition systems would be a likely choice for this objective, a solid-solution deposit is preferred to realize the microstructure controls that achieve the best tolerances. As noted above, the solid-solution is formed when all liquid precursors are decomposed simultaneously. A multi-component precursor solution applied to the substrate at low temperature that is subsequently ramped through all precursor decomposition temperatures would initiate the sequential decomposition of multiple precursors. Sequential decomposition favors all the individual metal oxides to segregate from the solution as nano-nucleates that remain dispersed throughout the deposited material, which is disadvantageous to microstructure control. Applying the solutions to a substrate heated to temperatures sufficient to initiate the simultaneous decomposition of all metalorganic precursors preserves the molecular-level mixing achieved in the liquid solution. The boiling solvent and decomposition products generated with the simultaneous decomposition produces a “steam” of waste products to emanate from the deposit. This is disadvantageous to inkjet deposition systems as the steaming waste products will contaminate the printing heads. As shown in
Another specific embodiment of the invention includes methods to locate a plurality of ceramic compositions at selective locations on the substrate surface at lower deposition temperatures. In this instance, the solvent is completely removed from mixed solution 210 using a solvent extraction step 215 (
FIGS. 12A1, 12A2, 12B make reference to an alternative wax printing technique wherein a plurality of wax precursor compositions 240A, 240B, 240C, 240D, etc. are applied to the surface of a tape 242 to form a precursor ribbon 244 with an alternating pattern of wax precursor compositions. One or more precursor ribbons 244 can then be feed off of a spool through a printing head 246 (
The simultaneous decomposition of liquid aerosols at a substrate's surface generates a free-radical chemistry that causes the depositing metal oxides to bond aggressively to metal and dielectric surfaces. The decomposition cycle of the wax-based precursor does not share the same level of aggressive free-radical bonding between the metal oxide deposit and the substrate. These deposits show a preference for bonding to oxide surfaces over clean metallic surfaces. In this instance, a thin oxide layer 256 can be applied to the surface of a metallic electrode 258, to which wax precursors 254 will be applied to form an electroceramic. In order to better achieve performance tolerances and thermal stability≦±5%, preferably ≦±1%, it is preferable to avoid the sequential decomposition of wax precursors that may cause agglomerations of single species oxides that disrupt fine microstructure controls. To maximize decomposition rates of the solid precursor wax deposits 254 an ultraviolet-assisted (UV-assisted) pyrolysis step 217 (
Reference is now made to
The intrinsic resistivity of the resistive electroceramic 264 is dependent upon electroceramic chemical composition and microstructure. Elemental resistors are characterized as having intrinsic sheet resistivity greater than 25 μΩ-cm. As mentioned above, LCD resistive electroceramic will exhibit the properties of an amorphous phase solid-state solution immediately after the bake-out step 213 (
A specific embodiment is shown in
Resistive electroceramic compositions are usually classified in terms of their crystal structure and typically contain the following metal oxides as a primary component: copper oxide (CuO), nickel oxide (NiO), ruthenium oxide (RuO2), iridium oxide (IrO2), rhodium oxide (Rh2O3), osmium oxide (OsO2), and antimony oxide (Sb2O3). This group of primary metal oxides comprises the group of preferred electroceramic compositions. These single component resistive electroceramics adopt a rutile crystal structure, with the exception of antimony oxide (Sb2O3) and rhodium oxide (Rh2O3), which have a trigonal crystal structures, and copper oxide (CuO) and nickel oxide (NiO), which have a cubic close-packed crystal structure. Intrinsic resistivity of the primary metal oxides with rutile crystal structures can be altered when the rutile primary oxides are combined together and with one or more transition-metal oxides and/or heavy-metal oxides in amounts that crystallize into a pyrochlore crystal structure. Intrinsic resistivity of the primary metal oxides with rutile crystal structures can also be altered when the rutile primary oxides are combined together and with one or more alkaline earth metal oxides and heavy-metal oxides in amounts that crystallize into a perovskite crystal structure. The compositional chemistry of these crystal structures generally adopt the following formulas:
M(1)M(2)2O7(pyrochlore) (2a)
M(3)M(2)O3(perovskite). (2b)
Where M(1) represents one or more trivalent transition-metal oxides and/or one or more trivalent heavy-metal oxides, M(2) represents one or more of the primary metal oxides with rutile crystal structure cited above, and M(3) represents one or more alkaline earth metal oxides. Preferred trivalent transition-metal oxides are from the group consisting of: scandium oxide (Sc2O3), titanium oxide, (Ti2O3), vanadium oxide (V2O3), chromium oxide (Cr2O3), manganese oxide (Mn2O3), iron oxide (Fe2O3). Preferred heavy-metal oxides are drawn from the group consisting of bismuth oxide (Bi2O3), lanthanum oxide (La2O3), cerium oxide (Ce2O3), lead oxide (PbO) and neodymium oxide (Nd2O3). Preferred alkaline earth metal oxides are drawn from the group consisting of magnesium oxide (MgO), calcium oxide (CaO), strontium oxide (SrO), and barium oxide (BaO). Indium-tin oxide (ITO) and antimony-tin oxide are preferred electroceramic compositions when there is a need to have an optically transparent conductor or resistive element, for instance in optical display applications.
As shown in
As will be described below, a specific need of the invention requires electroceramic resistors having a wide range of resistance values, allowing the user to select precise resistance values from 1Ω to 500 mega-Ω, preferably resistance values selected from 10Ω to 50 mega-Ω. A further need requires these electroceramic resistor need to have thermal stability and performance tolerances≦±5%, preferably ≦±1%, and to be integrated into at least one layer of a circuit board or interconnect that is in electrical communication with a semiconductor chip or another passive circuit element, including an antenna. The wide range of resistance values are derived by selectively depositing appropriate electroceramic compositions or appropriate electroceramic compositions blended with a small amount of strongly insulating oxides and controlling the microstructure of the electroceramic composition to have grain size ranging from 0 nm to 10 microns, preferably ranging from 0 nm to 2 microns.
Reference is now made to
Once all resistor elements are fabricated within desired tolerances, an insulating dielectric layer 298, a metallization layer 300, and vertical interconnects (vias) 301 that maintain electrical communications between the metallization layer 300 and the pad and trace electrode network 295 are then applied to the structure as shown in
The embedded resistor layer structure 302 can then be combined with one or more additional signal routing layers 304A, 304B into a stacked multilayer structure 305 as shown in
Reference is now made to
A further need of the invention includes distributed sheet capacitance or decoupling capacitors that have COG-type behavior. COG-type behavior refers to a capacitance value that changes≦±250 ppm/° C. Therefore, a COG-type capacitor will hold its performance value within 4.1% of its target over temperatures ranging from 40° C. to 125° C. As noted above, decoupling capacitors have value in suppressing power noise. Reference is now made to
As noted above, a thermally stable capacitance value is a specific objective.
High permittivity electroceramics preferred under this invention have perovskite crystal structures and will generally have the following chemical formula.
M(1)M(2)O3 (3a)
Where metals from group M(1) and M(2) exist in 1:1 molar ratios. It is possible for a plurality of metals to be represented within each group; however, the combined molarity for each group must remain the same. For instance, if two metals, M(1a), M(1b), are selected from group M(1) and two other metals are selected from group M(2), the chemical formula (3) is modified as:
M(1a)(1-x)M(1b)(x)M(2a)(1-y)M(2b)(y)O3. (3b)
Group M(1) metal oxides preferred for use in high permittivity electroceramics include: alkaline earth metal oxides selected from the group consisting of magnesium oxide (MgO), calcium oxide (CaO), strontium oxide (SrO), and barium oxide (BaO); alkali metal oxides selected from the group including lithium oxide (Li2O), sodium oxide (Na2O), potassium oxide (K2O), and rubidium oxide (Rb2O); and heavy-metal oxides selected from the group including lanthanum oxide (La2O3), cerium oxide (Ce2O3), lead oxide (PbO) and neodymium oxide (Nd2O3). Group M(2) metal oxides preferred for use in high permittivity electroceramics include: titanium oxide (TiO2), zirconium oxide (ZrO), hafnium oxide (HfO), tantalum oxide (Ta2O5), and niobium oxide (Nb2O5).
Reference is now made to
Reference is now made to
Reference is now made to
L=N2μoμRA/l (4)
Where N is the number of turns in the coil, μo=4π×10−7 H/m, μR is the relative permittivity of the electroceramic 426, A is the cross-sectional area of a single turn in the coil, and l is the length of the coil. The resistance, dimensional uniformity, and surface roughness of the metal conductor used to fabricate the coil, and the precision placement of the all conducting elements are key tolerance parameters, which is why wire bonding methods are preferred. Stud bumping and stitch bonding equipment having a bond placement accuracy<±5 μm, preferably ≦±3.5 μm, a height accuracy of <±10 μm, preferably ≦±3 μm, and a minimum pitch of 60 μm, preferably 50 μm, such as that provided by the AT Premier (in AccuBump mode), K&S, Willow Grove, Pa., are recommended process tools. Laser trimming the selectively deposited electroceramic 426 is recommended to maintain accurate control over dimensional tolerances.
Controlling the permeability of the inductor coil electroceramic 426 to a value≦±5%, preferably ≦±1%, is another specific embodiment of the invention. It is another specific embodiment of the invention to produce elemental ceramic inductor coils providing inductance in the range of 0.01 pH to 500 nH with performance values≦±5%, preferably ≦±1% of the targeted value. Electroceramic permeability is primarily a function of electroceramic composition, grain size, and is usually dependent upon frequency and temperature. Preferred electroceramic compositions for use in a ceramic inductor coil include ferrites and garnets. Ferrites adopt body-centered cubic crystal structure and have the following chemical formula:
M1Fe2O4 (5a)
Where Fe is iron oxide and M1 represents one or more select metal oxides having a total molar concentration that is half the iron oxide molar concentration. Group M1 metal oxides preferred for use in high permeability ferrite electroceramics include: cobalt monoxide (CoO), nickel oxide (NiO), zinc oxide (ZnO), manganese oxide (MnO), copper oxide (CuO), vanadium oxide (VO), magnesium oxide (MgO) and lithium oxide (Li2O). Garnets adopt either rhombic dodecahedron or trapezohedron crystal structures, or a combination of the two, and have the following chemical formula:
A3B2(SiO4)3 (5b)
Where group A metal oxides have equal molar concentration to silicon oxide and group B metal oxides have molar concentration that is ⅔ the molar concentration of silicon oxide. Group A metal oxides preferred for use in high permeability garnet electroceramics include: calcium oxide (CaO), magnesium oxide (MgO), iron oxide (FeO), and manganese oxide (MnO). Group B metal oxides preferred for use in high permeability garnet electroceramics include: aluminum oxide (Al2O3), iron oxide (Fe2O3), chromium oxide (Cr2O3), vanadium oxide (V2O3), zirconium oxide (ZrO2), titanium oxide (TiO2), silicon oxide (SiO2), yttrium oxide (Y2O3), cobalt oxide (CO3O4), gadolinium oxide (Gd2O3) neodymium oxide (Nd2O3) and holmium oxide (Ho2O3). Ceramic inductor coils 432 (
Reference is now made to
Reference is now made to
Reference is now made to
Reference is now made to
The methods and embodiments described above provide a means to produce thermally stable filtering circuits that comprise circuit LCR elements with tolerances≦±5%, preferably ≦±1%, that can be used to control a circuit's reactive impedance Z with a tolerance of ≦±5%, preferably ≦±1%. Wireless circuits include an antenna as a principle circuit element. The tuning (impedance) of an antenna element is affected by dielectric materials that are positioned within the antenna's reactive near-field region. Making reference to
d=0.62√(D3/λ) (6)
Where λ is the wavelength of the electromagnetic emissions radiated by the antenna element 490. A handset device that contains an antenna element surrounded by low permittivity dielectric materials has a reactive near-field region that protrudes beyond the handset's packaging and is therefore influenced by dielectric loads in the immediate vicinity of the handset, such as the users' hands and heads, or the layout or the mobile device's packaging. These loads are likely to shift dramatically during use, which is undesirable to maintaining stable impedance in the antenna circuit element. Furthermore, making even minor changes to the design of the handset package requires a re-design of its RF front-end circuitry if the same antenna is to be re-used in the renovated handset package. Therefore, it is desirable to provide a platform-independent antenna module that has a tuning (impedance) that is not affected by changes in the dielectric loads surrounding the antenna module. A specific embodiment of the invention produces a platform-independent antenna module that produces a reactive near field that is contained within the body of the antenna module and, therefore, not affected by changes in the dielectric loads that surround it.
Reference is now made to
λEff=c/(f√μR∈R) (7a)
=λfreespace/√{square root over (μr∈R)} (7b)
Where c is the speed of light in a vacuum (c=2.9979×108 n/sec2), f is the frequency of the electromagnetic excitation, and μR and ∈R are the relative permeability and relative permittivity of the dielectric medium, respectively, and λfreespace is the wavelength of electromagnetic excitation in a vacuum. Therefore, an electromagnetic excitation propagating through a non-magnetic medium (μR=1) will have an effective wavelength λEff equal to λfreespace/4 and λfreespace/10 when the dielectric medium has relative permittivity ∈R=16 and ∈R=100, respectively. Therefore, the resonant length lres of a folded dipole or a folded monopole antenna, which is generally given by lres≈λ/2, and lresλ/4, respectively, is decreased proportionally, thereby allowing the maximum physical dimension of the folded antenna element 492 to be reduced to the point that its reactive near field protrudes a distance d 502 that is contained within a distance S 503 separating the folded antenna element 492 from an exterior surface of the meta-material dielectric body 494. In this embodiment, the reactive near field will remain unaffected by changes in dielectric loading beyond the physical dimensions 504 of the antenna module 506. High permittivity dielectric media generally have unstable thermal properties and high loss that can adversely affect frequency tuning and signaling performance. Therefore, it is another preferred embodiment of the invention to fabricate the antenna module 506 using selectively deposited dielectric inclusions 498 having thermal stability tolerances for relative permittivity ∈R and relative permeability μR that are ≦±5%, preferably ≦±1% of targeted values. High-loss materials located within an antenna's reactive near field region will affect the antenna's signal modulation in a manner that limits phase modulation roll-off rates, which, in turn, limits the number of wireless symbols that can be transmitted by the antenna. Thus, it is desirable to engineer the folded antenna element 492 and the meta-material dielectric body 494 such that the at least one high permittivity dielectric inclusion 496 is located a distance 508 away from the folded antenna element 492 that is greater than the distance d 510 to which the reactive near field protrudes In this special embodiment the reactive near field is contained within a low loss host dielectric 512 having a loss tangent tan δ≦10−3, preferably an ultra-low loss dielectric host having a loss tangent tan δ≦2×10−4. Amorphous silica is a preferred ultra-low loss dielectric medium because it has stable dielectric properties over temperatures ranging from −150° C. to +250° C. and a loss tangent tan δ=2×10−5. Organic dielectric media suitable for use as an ultra-low loss dielectric host 512 include PFTE Teflon and Rogers Duroid dielectric. This special embodiment also provides a platform-independent antenna module since the reactive near field protrudes a distance d 510 that remains within the antenna module's solid state dimensions 514.
The art described above instructs methods and embodiments that provide wireless circuit elements (embedded passive components and platform-independent antenna modules) that maintain precise impedance tuning in the presence of electromagnetic and thermal disturbances. These embodiments are combined into a further embodiment that establishes the passive spread-spectrum receiver. Making reference to
B=[XL±√(RL/Zo)×√(RL2+XL2−ZoRL)]/(RL2+XL2) (8a)
And, the reactive series load jX 536 is determined by:
X=(1/B)+(XLZo/RL)−(Zo/BRL) (8a)
L-section matching 530 (
B=±√[(RL(Zo−RL)]−XL (8c)
And, the reactive series load jX 536 is determined by:
X=(1/B)+(XLZo/RL)−(Zo/BRL) (8d)
It is not a requirement for all impedance tuning within the printed circuit board or interconnect structure 520 to be managed using L-section matching methods as circuit tuning can also be realized using transmission-line stubs. However, the high tolerance controls, small size, and wide range of performance values enabled by the invention provide convenient means to integrate precise bandwidth filters, such as quarter-wave transformers, binomial multi-section transformers, and Chebyshev multi-section matching transformers into the spread-spectrum receiver. These filtering devices are well known to practitioners skilled in the art of microwave circuit, reference is made to Microwave Engineering, 3rd Edition, David M. Pozar, John Wiley & Sons, Hoboken, N.J. © 2005 (ISBN: 0-471-44878-8) for a complete description on impedance tuning parameters for these devices.
As shown in
Reference is now made to
Although the invention has been described with respect to various embodiments, it should be realized this invention is also capable of a wide variety of further and other embodiments within the spirit and scope of the appended claims.
Applicant claims priority of U.S. Provisional Patent Application No. 60/695,485, filed Jun. 30, 2005 and entitled SPREAD SPECTRUM RECEIVER AND METHOD OF MANUFACTURE, the contents of which are hereby incorporated herein.
Number | Name | Date | Kind |
---|---|---|---|
2283925 | Harvey | May 1942 | A |
2886529 | Louis | May 1959 | A |
3574114 | Monforte | Apr 1971 | A |
3614554 | Shield et al. | Oct 1971 | A |
3983077 | Fuller et al. | Sep 1976 | A |
4400683 | Eda et al. | Aug 1983 | A |
4455545 | Shelly | Jun 1984 | A |
4523170 | Huth, III | Jun 1985 | A |
4646038 | Wanat | Feb 1987 | A |
4759120 | Bernstein | Jul 1988 | A |
4859492 | Rogers, Jr. et al. | Aug 1989 | A |
4967201 | Rich, III | Oct 1990 | A |
5084749 | Losee et al. | Jan 1992 | A |
5154973 | Imagawa et al. | Oct 1992 | A |
5198824 | Poradish | Mar 1993 | A |
5217754 | Santiago-Aviles et al. | Jun 1993 | A |
5219377 | Poradish | Jun 1993 | A |
5272485 | Mason et al. | Dec 1993 | A |
5403797 | Ohtani et al. | Apr 1995 | A |
5427988 | Sengupta et al. | Jun 1995 | A |
5456945 | McMillan et al. | Oct 1995 | A |
5513382 | Agahi-Kesheh et al. | Apr 1996 | A |
5535445 | Gunton | Jul 1996 | A |
5540772 | McMillan et al. | Jul 1996 | A |
5543773 | Evans et al. | Aug 1996 | A |
5584053 | Kommrusch et al. | Dec 1996 | A |
5614252 | McMillan et al. | Mar 1997 | A |
5625365 | Tom et al. | Apr 1997 | A |
5635433 | Sengupta | Jun 1997 | A |
5707459 | Itoyama et al. | Jan 1998 | A |
5707715 | deRochemont et al. | Jan 1998 | A |
5747870 | Pedder | May 1998 | A |
5759923 | McMillan et al. | Jun 1998 | A |
5764189 | Lohninger | Jun 1998 | A |
5771567 | Pierce et al. | Jun 1998 | A |
5854608 | Leisten | Dec 1998 | A |
5859621 | Leisten | Jan 1999 | A |
5888583 | McMillan et al. | Mar 1999 | A |
5889459 | Hattori et al. | Mar 1999 | A |
5892489 | Kanba et al. | Apr 1999 | A |
5903421 | Furutani et al. | May 1999 | A |
5933121 | Rainhart et al. | Aug 1999 | A |
5945963 | Leisten | Aug 1999 | A |
6023251 | Koo et al. | Feb 2000 | A |
6027826 | deRochemont et al. | Feb 2000 | A |
6028568 | Asakura et al. | Feb 2000 | A |
6031445 | Marty et al. | Feb 2000 | A |
6040805 | Huynh et al. | Mar 2000 | A |
6046707 | Gaughan et al. | Apr 2000 | A |
6052040 | Hino | Apr 2000 | A |
6111544 | Dakeya et al. | Aug 2000 | A |
6143432 | deRochemont et al. | Nov 2000 | A |
6154176 | Fathy et al. | Nov 2000 | A |
6176004 | Rainhart et al. | Jan 2001 | B1 |
6181297 | Leisten | Jan 2001 | B1 |
6188368 | Koriyama et al. | Feb 2001 | B1 |
6195049 | Kim et al. | Feb 2001 | B1 |
6208843 | Huang et al. | Mar 2001 | B1 |
6222489 | Tsuru et al. | Apr 2001 | B1 |
6266020 | Chang | Jul 2001 | B1 |
6271803 | Watanabe et al. | Aug 2001 | B1 |
6300894 | Lynch et al. | Oct 2001 | B1 |
6320547 | Fathy et al. | Nov 2001 | B1 |
6323549 | deRochemont et al. | Nov 2001 | B1 |
6492949 | Breglia et al. | Dec 2002 | B1 |
6496149 | Birnbaum et al. | Dec 2002 | B1 |
6501415 | Viana et al. | Dec 2002 | B1 |
6552693 | Leisten | Apr 2003 | B1 |
6559735 | Hoang et al. | May 2003 | B1 |
6583699 | Yokoyama | Jun 2003 | B2 |
6611419 | Chakravorty | Aug 2003 | B1 |
6620750 | Kim et al. | Sep 2003 | B2 |
6639556 | Baba | Oct 2003 | B2 |
6642908 | Pleva et al. | Nov 2003 | B2 |
6650303 | Kim et al. | Nov 2003 | B2 |
6670497 | Tashino et al. | Dec 2003 | B2 |
6680700 | Hilgers | Jan 2004 | B2 |
6683576 | Achim | Jan 2004 | B2 |
6686406 | Tomomatsu et al. | Feb 2004 | B2 |
6690336 | Leisten et al. | Feb 2004 | B1 |
6697605 | Atokawa et al. | Feb 2004 | B1 |
6737364 | Black et al. | May 2004 | B2 |
6742249 | deRochemont et al. | Jun 2004 | B2 |
6743744 | Kim et al. | Jun 2004 | B1 |
6762237 | Glatkowski et al. | Jul 2004 | B2 |
6791496 | Killen et al. | Sep 2004 | B1 |
6864848 | Sievenpiper | Mar 2005 | B2 |
6906674 | McKinzie, III et al. | Jun 2005 | B2 |
6919119 | Kalkan et al. | Jul 2005 | B2 |
7047637 | deRochemont et al. | May 2006 | B2 |
7405698 | deRochemont | Jul 2008 | B2 |
7763917 | deRochemont | Jul 2010 | B2 |
20010023779 | Sugaya et al. | Sep 2001 | A1 |
20010027119 | Furutani et al. | Oct 2001 | A1 |
20010048969 | Constantino et al. | Dec 2001 | A1 |
20020039667 | Takaya et al. | Apr 2002 | A1 |
20020047768 | Duffy | Apr 2002 | A1 |
20020092472 | Hayashi et al. | Jul 2002 | A1 |
20020190818 | Endou et al. | Dec 2002 | A1 |
20030002045 | Nemat-Nasser et al. | Jan 2003 | A1 |
20030034124 | Sugaya et al. | Feb 2003 | A1 |
20030073565 | Ellis et al. | Apr 2003 | A1 |
20030107455 | Imanaka et al. | Jun 2003 | A1 |
20030111714 | Bates et al. | Jun 2003 | A1 |
20030122647 | Ou | Jul 2003 | A1 |
20030148024 | Kodas et al. | Aug 2003 | A1 |
20030161959 | Kodas et al. | Aug 2003 | A1 |
20030170436 | Sumi et al. | Sep 2003 | A1 |
20030221621 | Pokharna et al. | Dec 2003 | A1 |
20040000964 | Killen et al. | Jan 2004 | A1 |
20040000966 | Killen et al. | Jan 2004 | A1 |
20040000970 | Killen et al. | Jan 2004 | A1 |
20040000972 | Killen et al. | Jan 2004 | A1 |
20040000975 | Killen et al. | Jan 2004 | A1 |
20040000976 | Killen et al. | Jan 2004 | A1 |
20040001024 | Killen et al. | Jan 2004 | A1 |
20040001026 | Killen et al. | Jan 2004 | A1 |
20040001027 | Killen et al. | Jan 2004 | A1 |
20040001028 | Killen et al. | Jan 2004 | A1 |
20040012081 | Kwon | Jan 2004 | A1 |
20040033654 | Yamagata | Feb 2004 | A1 |
20040070915 | Nagai et al. | Apr 2004 | A1 |
20040084080 | Sager et al. | May 2004 | A1 |
20040092236 | Irie et al. | May 2004 | A1 |
20040113738 | Ahn et al. | Jun 2004 | A1 |
20040118448 | Scher et al. | Jun 2004 | A1 |
20040189528 | Killen et al. | Sep 2004 | A1 |
20050036269 | Ma et al. | Feb 2005 | A1 |
20050051870 | Yamazaki et al. | Mar 2005 | A1 |
20060125681 | Smith et al. | Jun 2006 | A1 |
20070139976 | deRochemont | Jun 2007 | A1 |
20090011922 | deRochemont | Jan 2009 | A1 |
20110021007 | deRochemont | Jan 2011 | A1 |
20110049394 | deRochemont | Mar 2011 | A1 |
20110248900 | deRochemont | Oct 2011 | A1 |
Number | Date | Country |
---|---|---|
0939451 | Jan 1999 | EP |
1376759 | Feb 2004 | EP |
Entry |
---|
Joshi et al., “Processing and Characterization of Pure and Doped Ba0.6Sr0.4TiO3 Thin Films for Tunable Microwave Applications” Mat. Res. Soc. Symp. Proc., vol. 656E, 2001, pp. DD4.9.1-DD4.9.6. |
Tsunemine et al., “Pt/BaxSr(1-x)TiO3/Pt Capacitor Technology for 0.15 micron Embedded Dynamic Random Access Memory”, Japanese Journal of Applied Physics, vol. 43, No. 5A, 2004, pp. 2457-2461. |
Cheng et al., “Preparation and Characterization of (Ba.Sr)TiO3 thin films using interdigital electrodes”, Microelectronic Engineering, vol. 66, (2003), pp. 872-879. |
Viviani et al., “Positive Temperature Coefficient of Electrical Resistivity below 150k of Barium Strontium Titanate”, Journal of the American Ceramic Society, vol. 87, 2004, pp. 756-758. |
Pontes et al., “Study of the dielectric and ferroelectric properties of chemically processed BaxSr1-xTiO3 thin films”, Thin Solid Films, vol. 386, No. 1, 2001, pp. 91-98. |
International Search Report, date of mailing Feb. 5, 2007, international Application No. PCT/US06/25650, International Filing Date Jun. 30, 2006, L. Pierre DeRochemont, applicant. |
Andrenko, A.S. et al. EM Analysis of PBG Substrate Microstrip Circuits for Integrated Transmitter Front End. MMET 2000 Proceedings, 295-297. |
Bardi, I. et al. Plane Wave Scattering From Frequency-Selective Surfaces by the Finite-Element Method. IEEE Transactions on Magnetics 38(2) Mar. 2002, 641-644. |
Chappell, W. et al. Composite Metamaterial Systems for Two-Dimensional Periodic Structures. © 2002 IEEE, 384-387. |
Cheng, Y.L. et al. Preparation and Characterization of (Ba.Sr)TiO3 thin films using interdigital electrodes. Microelectronic Engineering vol. 66 (2003), 872-879. |
Clavijo, S. et al. Design Methodology for Sievenpiper High-Impedance Surfaces: An Artificial Magnetic Conductor for Positive Gain Electrically Small Antennas. IEEE Transactions on Antennas and Propagation 51(10), Oct. 2003, 2678-2690. |
Diaz, R. et al. Magnetic Loading of Artificial Magnetic Conductors for Bandwidth Enhancement. © 2003 IEEE, 431-434. |
Hansen, R.C. Effects of a High-Impedance Screen on a Dipole Antenna. IEEE Antennas and Wireless Propagation Letters vol. 1 (2002), 46-49. |
Joshi, P.C. et al. Processing and Characterization of Pure and Doped Ba0.6Sr 0.4TiO3 thin films for tunable microwave applications. Mat. Res. Soc. Symp. Proc. vol. 656E (2001), DD4.9.1-DD4.9.6. |
Kern, D.J. et al. Active Negative Impedance Loaded EBG Structures for the Realization of Ultra-Wideband Artificial Magnetic Conductors. © 2003 IEEE, 427-430. |
Kern, D.J. et al. The Synthesis of Metamaterial Ferrites for RF Applications Using •Electromagnetic Bandgap Structures. © 2003 IEEE, 497-500. |
Kern, D.J. et al. Ultra-thin Electromagnetic Bandgap Absorbers Synthesized via Genetic Algorithms. © 2003 IEEE, 1119-1122. |
Khun, R. et al., Characterization of Novel Mono- and Bifacially Active Semi-Transparent Crystalline Silicon Solar Cells, IEEE Transactions on Electron Devices, 46(10), Oct. 1999, 2013-2017. |
Kretly, L.C. et al. The Influence of the Height Variation on the Frequency Bandgap in an AMC Artificial Magnetic Conductor for Wireless Applications: an EM Experimental Design Approach. Proceedings SBMO/IEEE MTT-S IMOC 2003, 219-223. |
Lee, Y. et al. Investigation of Electromagnetic Bandgap (EBG) Structures for Antenna Pattern Control. © 2003 IEEE, 1115-1118. |
McKinzie III, W.E. et al. Mitigation of Multipath Through the Use of an Artificial Magnetic Conductor for Precision CPS Surveying Antennas. © 2002 IEEE, 640-643. |
McKinzie, W. et al. A Multi-Band Artificial Magnetic Conductor Comprised of Multiple FSS Layers. © 2003 IEEE, 423-426. |
Monorchio, A. et al. Synthesis of Artificial Magnetic Conductors by Using Multilayered Frequency Selective Surfaces. IEEE Antennas and Wireless Propagation Letters vol. 1 (2002), 196-199. |
Mosallaei, H. et al. Periodic Bandgap and Effective Dielectric Materials in Electromagnetics: Characterization and Applications in Nanocavities and Waveguides. IEEE Transactions on Antennas and Propagation 51(3). Mar. 2003, 549-563. |
Pontes, F.M. et al. Study of the dielectric and ferroelectric properties of chemically processed BaxSrl-xTiO3 thin films. Thin Solid Films, vol. 386, No. 1 (2001), 91-98. |
Rogers, S. et al. AMCs Comprised of Interdigital Capacitor FSS Layers Enable Lower Cost Applications. © 2003 IEEE, 411-414. |
Rogers, S. et al. An AMC-Based 802.11a/b Antenna for Laptop Computers. © 2003 IEEE, 10-13. |
Sievenpiper, D.F. et al. Two-Dimensional Beam Steering Using an Electrically Tunable Impedance Surface. IEEE Transactions on Antennas and Propagation 51(10), Oct. 2003, 2713-2722. |
Sun, J. et al. Efficiency of Various Photonic Bandgap (PBG) Structures. 3rd Int'l. Conf. on Microwave and Millimeter Wave Technology Proceedings 2002, 1055-1058. |
Tsunemine, Y. et al. Pt/BaxSr(1-x)TiO3/Pt Capacitor Technology for 0.15 micron Embedded Dynamic Random Access Memory. Jap. J. Appl. Phys. vol. 43 No. 5A (2004), 2457-2461. |
Viviani, M. et al. Positive Temperature Coefficient of Electrical Resistivity below 150k of Barium Strontium Titanate. J. Amer. Ceram. Soc. vol. 87 (2004) 756-758. |
Weily, A.R. et al. Antennas Based on 2-D and 3-D Electromagnetic Bandgap Materials. © 2003 IEEE, 847-850. |
Yang, H-Y. D. et al. Surface Waves of Printed Antennas on Planar Artificial Periodic Dielectric Structures. IEEE Transactions on Antennas and Propagation 49(3). Mar. 2001, pp. 444-450. |
Zhang, Y. et al. Planar Artificial Magnetic Conductors and Patch Antennas. IEEE Transactions on Antennas and Propagation 51(10). Oct. 2003, pp. 2704-2712. |
Ziroff, A. et al. A Novel Approach for LTCC Packaging Using a PBG Structure for Shielding and Package Mode Suppression. 33rd European Microwave Conference—Munich 2003, 419-422. |
Number | Date | Country | |
---|---|---|---|
20070003781 A1 | Jan 2007 | US |
Number | Date | Country | |
---|---|---|---|
60695485 | Jun 2005 | US |