CERAMIC ANTENNA MODULE AND METHODS OF MANUFACTURE THEREOF

• US 20090011922A1
• Filed: 07/21/2008
• Published: 01/08/2009
• Est. Priority Date: 10/01/2004
• Status: Active Grant

• Current Assignee: L. Pierre De Rochemont
• Original Assignee: L. Pierre De Rochemont
• Inventors: de Rochemont, L. Pierre
• Granted Patent: US 8,178,457 B2
• Time in Patent Office: Days
• US Class Current: 501/137
• CPC Class Codes: H01L 2223/6677 for antenna, e.g. antenna included within housing of semiconductor device antennas per se H01Q
• CPC Class Codes: H01L 2924/00 Indexing scheme for arrangements or methods for connecting or disconnecting semiconductor or solid-state bodies as covered by H01L24/00
• CPC Class Codes: H01L 2924/0002 Not covered by any one of groups H01L24/00, H01L24/00 and H01L2224/00
• CPC Class Codes: H01Q 1/362 for broadside radiating helical antennas
• CPC Class Codes: H01Q 1/38 formed by a conductive layer on an insulating support patch antennas H01Q9/0407; microstrip dipole antennas H01Q9/065; microstrip slot antennas H01Q13/106; transmission line microstrip antennas H01Q13/206; manufacturing reflecting surfaces using insulating material for supporting the reflecting surface H01Q15/142
• CPC Class Codes: H01Q 15/0046 Theoretical analysis and design methods of such selective devices
• CPC Class Codes: H01Q 15/006 Selective devices having photonic band gap materials or materials of which the material properties are frequency dependent, e.g. perforated substrates, high-impedance surfaces
• CPC Class Codes: H01Q 15/0086 said selective devices having materials with a synthesized negative refractive index, e.g. metamaterials or left-handed materials
• CPC Class Codes: H01Q 21/0025 Modular arrays
• CPC Class Codes: H01Q 5/307 Individual or coupled radiating elements, each element being fed in an unspecified way
• CPC Class Codes: H01Q 7/00 Loop antennas with a substantially uniform current distribution around the loop and having a directional radiation pattern in a plane perpendicular to the plane of the loop
• CPC Class Codes: H01Q 9/0407 Substantially flat resonant element parallel to ground plane, e.g. patch antenna dipole H01Q9/285; monopole H01Q9/40
• CPC Class Codes: H01Q 9/16 with feed intermediate between the extremities of the antenna, e.g. centre-fed dipole H01Q9/44 takes precedence

Abstract

Circuit modules and methods of construction thereof that contain composite meta-material dielectric bodies that have high effective values of real permittivity but which minimize reflective losses, through the use of host dielectric (organic or ceramic), materials having relative permittivities substantially less than ceramic dielectric inclusions embedded therein. The composite meta-material bodies permit reductions in physical lengths of electrically conducting elements such as antenna element(s) without adversely impacting radiation efficiency. The meta-material structure may additionally provide frequency band filtering functions that would normally be provided by other components typically found in an RF front-end.

Claims

1-167. -167. (canceled)

168. A meta-material dielectric body, comprising:

a composite dielectric body including a host material having a loss tangent that is ≦

3×

10<sup>−

3</sup>, and at least one dielectric inclusion embedded in the host material such that the composite dielectric body has an effective relative permittivity ≧

4.

169. The meta-material dielectric body of claim 168, wherein:

the dielectric inclusions have a maximum nominal grain size ≦

50 nanometers; and

the composite dielectric body has an effective permittivity that changes as a function of temperature ≦

5×

10<sup>−

2</sup>°

C.<sup>−

1</sup>.

170. The meta-material dielectric body of claim 168, wherein:

the dielectric inclusions each have a maximum nominal grain size ≦

35 nanometers; and

the composite dielectric body has an effective permittivity that changes as a function of temperature ≦

8×

10<sup>−

3</sup>°

C.<sup>−

1</sup>.

171. The meta-material dielectric body of claim 168, wherein the host material is composed of a material selected from the group consisting of amorphous silica and titania.

172. The meta-material dielectric body of claim 168, wherein:

the host material is composed of an organic material selected from the group consisting of Roger Duroid, GTEK and Teflon (PFTE) organic polymers; and

the dielectric inclusions have a maximum nominal grain size ≦

50 nanometers.

173. The meta-material dielectric body of claim 168, wherein the host material is composed of an admixture of amorphous silica (α

-SiO₂) and either titania (TiO₂) or alumina (Al₂O₃) and has a corresponding chemical composition Si_1-xY_xO₂, where 0≦

x≦

1 and Y is Ti or Al.

174. The meta-material dielectric body of claim 168, wherein the host material is comprised of a ceramic dielectric material having a ∈

_R between about 60 and about 100.

175. The meta-material dielectric body of claim 168, wherein the dielectric inclusions are selected from the group consisting of inclusions having relative a permittivity ∈

_R≧

10 and inclusions having a relative permeability μ

_R≠

1.

176. The meta-material dielectric body of claim 168, wherein the inclusions are composed of one or more ceramic materials having a ∈

_R between about 200 and about 2000.

177. The meta-material dielectric body of claim 168, wherein the dielectric inclusions are composed of a multi-component dielectric materials are selected from the group consisting of barium-strontium titanate ceramic (Ba_XSr_1-XTiO₃), barium-strontium zirconate-titanate (Ba_XSr_1-XZr_YTi_1-YO₃), and lead-lanthanum zirconate-titanate (Pb_XLa_1-XZr_YTi_1-YO₃), where 0≦

x≦

1 and 0≦

Y≦

1.

178. The meta-material dielectric body of claim 168, wherein the inclusions are composed of materials containing a single metal oxide component and at least one valence state.

179. The meta-material dielectric body of claim 168, wherein the dielectric inclusions are composed of a material selected from the group consisting of ferrites, ferroelectric oxide ceramics, and titania.

180. The meta-material dielectric body of claim 168, wherein the dielectric inclusions are periodically arrayed with a period of between about 5% and about 15% of a wavelength of an electromagnetic wave so as to produce a broad stop band of frequencies above and below the frequency of said electromagnetic wave over which the transmission of electromagnetic frequencies are suppressed by at least 3 dB.

181. The meta-material body of claim 180, further comprising an inclusion-free zone in the host material within which propagation of a narrow band of electromagnetic frequencies above and below the frequency of the electromagnetic wave is permitted while electromagnetic waves outside of the narrow band but within the stop band is suppressed by at least 3 dB.

182. The meta-material dielectric body of claim 180, wherein the ratio of the relative permittivity of the dielectric inclusions to the relative permittivity of the host material is from about 10 to about 50.

183. The meta-material dielectric body of claim 168, wherein the dielectric inclusions are periodically arrayed in the host material and each has a cross-sectional area nominally defined by a major axis a and minor axis b, where a has a length between about 2.5% and 7.5% of a wavelength λ

_c, and b has a length between about 1% and 50% of a, wavelength λ

_c corresponding to an electromagnetic wave having a frequency centered within a stop band of frequencies within the propagation of electromagnetic waves outside will be substantially suppressed.

184. The meta-material dielectric body of claim 168, wherein:

the dielectric inclusions are periodically arrayed and composed of titania modified with between 0.1 and 5 mol % of at least one additive selected from the group consisting of magnesium oxide (MgO), calcium oxide (CaO), strontium oxide (SrO), barium oxide (BaO), zirconium oxide (ZrO₂), hafnium oxide (HfO₂), lanthanum oxide (La₂O₃), neodymium oxide (Nd₂O₃), tantalum pentoxide (Ta₂O₅), niobium oxide (NbO, NbO₂, or Nb₂O₅), tungsten oxide (WO₂, WO₃) and lead oxide (PbO); and

the ratio of the relative permittivity of the dielectric inclusions to that of the host materials is between about 25 and about 40.

185-231. -231. (canceled)

232. A method of forming a meta-material dielectric body, comprising the step of embedding in a host material having a loss tangent that is ≦

3×

10<sup>−

3</sup> at least one dielectric inclusion so as to obtain a composite dielectric body having an effective relative permittivity ≧

4.