Flexible ceramic waveguides for terahertz applications and use as on-board interconnects
11105976 · 2021-08-31
Assignee
Inventors
- Lars Martin Otfried Brusberg (Corning, NY, US)
- Alan Frank Evans (Beaver Dams, NY, US)
- Michael John Yadlowsky (Sunnyvale, CA, US)
Cpc classification
H01P3/16
ELECTRICITY
H05K1/0243
ELECTRICITY
H05K2201/09063
ELECTRICITY
H05K1/0274
ELECTRICITY
G02B6/1225
PHYSICS
H05K1/024
ELECTRICITY
H04B3/52
ELECTRICITY
G02B6/1228
PHYSICS
H05K2201/10121
ELECTRICITY
International classification
H01P3/16
ELECTRICITY
Abstract
A terahertz (THz) waveguide and method for production allows for THz waveguides to be used in or on a printed circuit board (PCB) such that the propagation of THz waves require less power, result in less signal loss due to radiation or dispersion, and propagate more efficiently. Additionally, the position and/or geometry of a waveguide, as well as any additional antenna or coupling element, may be adjusted on or in the PCB such that the electromagnetic field of the waveguide may more efficiently couple with the electromagnetic field of the PCB.
Claims
1. An electronic assembly, comprising: a printed circuit board (PCB) assembly comprising first and second ends and at least one PCB layer wherein the at least one PCB layer comprises at least one conductive element, an integrated circuit (IC) operably disposed on the top surface of the PCB assembly by I/O pads, the IC having at least one IC device, at least one coupling element; a ceramic dielectric terahertz (THz) waveguide for guiding signals having a THz frequency in the range from about 0.1 THz to about 10 THz comprising a ceramic core comprising an alumina ribbon wherein the alumina ribbon has a dielectric constant (Dk.sub.1) and a cladding surrounding the ceramic core, wherein the cladding has a dielectric constant (Dk.sub.2) such that Dk.sub.2<Dk.sub.1, and a major surface and an access aperture wherein the major surface is disposed between the first end and second end, and the ceramic dielectric waveguide is mounted to the top surface of at least one PCB layer, the ceramic dielectric terahertz (THz) waveguide comprising a first-end section with an end face accessible through the access aperture.
2. The electronic assembly according to claim 1, wherein the PCB comprises multiple ceramic dielectric THz waveguides.
3. The electronic assembly according to claim 1, wherein the ceramic dielectric terahertz (THz) waveguide is fully or partially embedded within the printed circuit board (PCB) assembly.
4. The electronic assembly according to claim 1, the ceramic dielectric terahertz (THz) waveguide is disposed between at least two PCB layers.
5. The electronic assembly according to claim 1, further comprising a cavity for a source or transceiver component and a cavity for a detector or transceiver component on opposite terminal ends of the ceramic dielectric terahertz (THz) waveguide.
6. The electronic assembly according to claim 5, wherein the source component is a transmitter.
7. The electronic assembly according to claim 5, wherein the detector component is a receiver.
8. The electronic assembly according to claim 5, further comprising a strut, wherein the strut consists of an alumina ribbon, and wherein a strut is at the terminal ends of the ceramic dielectric terahertz (THz) waveguide.
9. The electronic assembly according to claim 5, further comprising at least one strut, wherein the strut is transverse to the ceramic dielectric terahertz (THz) waveguide.
10. The electronic assembly according to claim 1, wherein the ceramic core is surrounded on two parallel sides by at least one cutout.
11. The electronic assembly according to claim 10, wherein the at least one cutout is empty.
12. The electronic assembly according to claim 10, wherein the at least one cutout has a bending angle of at least 10 degrees.
13. The electronic assembly according to claim 10, wherein the at least one cutout progressively tapers along the propagation direction.
14. The electronic assembly according to claim 10, wherein the at least one cutout is filled with a dielectric material having a dielectric constant lower than the dielectric constant that of the ceramic core.
15. The electronic assembly according to claim 14, wherein the dielectric material is polymer, glass, or silicon dioxide.
16. The electronic assembly according to claim 15, wherein the polymer is selected from the group consisting of polytetrafluoroethylene (PTFE), SU-8, fluoropolymers, and polystyrene, polyimide (Kapton or Cirlex), parylene-N, high-density polyethylene (HDPE), polypropylene (PP) and polyethylene cyclic olefin copolymer (Topas), polybenzoxazole (PBO), benzocylobutene (BCB), and liquid crystal polymers.
17. The electronic assembly according to claim 10, wherein the at least one cutout comprises an array of holes.
18. The electronic assembly according to claim 17, wherein the array of holes creates a electronic bandgap cladding layer.
19. The electronic assembly according to claim 17, wherein the holes are uniform in shape, size, and/or linear placement.
20. The electronic assembly according to claim 17, wherein the holes vary in size along the propagation direction.
Description
BRIEF DESCRIPTION OF SEVERAL VIEWS OF THE DRAWINGS
(1) These as well as other features of the present invention will become more apparent upon reference to the drawings wherein:
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(15) The foregoing summary, as well as the following detailed description of certain features of the present application, will be better understood when read in conjunction with the appended drawings. For the purposes of illustration, certain features are shown in the drawings. It should be understood, however, that the claims are not limited to the arrangements shown in the attached drawings.
DETAILED DESCRIPTION
(16) Referring generally to the figures, aspects of the present disclosure relate to the use of a ceramic dielectric waveguide to couple an electrical transmission line signal with that of a printed circuit board. Advantageously, the shape and position of the ceramic dielectric waveguide with respect to the printed circuit board adjusts how the electromagnetic field of the waveguide couples with that of the conductive structures within the printed circuit board, creating opportunities to make propagation of THz waves more efficient and less lossy. Also advantageously, the potential addition coupling elements such as antenna elements creates more opportunities for the same. Some potential shapes and positions of the ceramic dielectric waveguide, along with the potential addition of antenna or coupling elements, will be discussed in the following sections. The aspects described herein are for the purposes of illustration and should not be considered limiting.
Waveguide Creation
(17) The present disclosure relates to waveguides configured to transmit electromagnetic waves within the THz range that include a ceramic core and an optional dielectric material cladding. Amongst other factors, propagation of an electromagnetic wave is influenced by the size and shape of the waveguide. In some aspects, a ceramic core with smaller cross-sectional dimensions may be more suitable for transmitting waves in the THz range than a core with larger cross-sectional dimensions. The ceramic core may have a cross-sectional dimension in the range of about 10 microns to about 500 microns (μm), preferably about 20 μm. The cross sectional dimension is not limited to rectangular cross-sectional shapes but may be applied interchangeably to circular, elliptical, or other cross-sectional shapes.
(18) The ceramic core may be comprised of any suitable ceramic material and may be rectangular or ribbon-shaped. Electromagnetic waves propagate within the confines of the walls of a waveguide, with the walls acting as boundaries. Therefore, some cross-sectional shapes may be more suitable for transmitting waves in the THz range than other cross-sectional shapes.
(19) In some aspects, the THz waveguide may have a long form factor. In these aspect, the THz waveguide 10 may have a length 12 of about 3 centimeters (cm) or greater. A longer form factor may be more suitable for transmitting waves in the THz range than a shorter form factor. Similarly, a longer form factor may be more suitable for transmitting waves over a longer distance than a shorter form factor that transmits waves over a shorter distance.
(20) In other aspects, the THz waveguide may also be thin. For example, it may have a rectangular cross-section of a THz waveguide having a width and a height. In this aspect, the ceramic core may have a width or height in the range of about 20 μm to about 500 μm, preferably about 20 μm. A ceramic core with a smaller width and/or height may be more suitable for transmitting waves in the THz range than a ceramic core with a larger width and/or height. Similarly, a ceramic core with a smaller width and/or height may be more suitable for THz applications requiring smaller waveguides, e.g. inter-chip interconnects or chip-to-chip communication.
(21) In some aspects, the THz waveguides may transmit signals in the frequency range of about 0.1 THz to about 10 THz with a ceramic core comprised of alumina. In other aspects, an alumina core may be comprised of ultra-high purity alumina with a purity level of about 99% or higher, about 99.5% or higher, about 99.75% or higher, about 99.9%, about 99.95% or higher, about 99.96% or higher, or about 99.99% or higher. In yet a further aspect, the alumina has a purity of about 99.96% or higher. In these aspects, an alumina core with a high purity level enables greater dielectric performance than an alumina core with lower purity level. In one aspect, the core may have a Dk in the range of 10-1000 and a dissipation factor (“Df”) in the range of less than 1×10.sup.−3, preferably a Dk=10 and a Df<=1×10.sup.−4, respectively. In view of the present aspects, a waveguide comprised of a high purity alumina core can effectively transmit signals within the THz range while still having low transmission loss.
(22) In other aspects, the alumina ceramic core may have a Dk of ε.sub.r, surrounded by air. A high dielectric constant can enable single mode operation in a wide frequency window. Waveguide propagation modes depend on the operating wavelength and polarization, along with the shape and size of the waveguide. For the rectangular waveguide shown in
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(24) For single mode operation in both the x and y directions, V.sub.x=π, and V.sub.y=π. The cutoff frequency for single mode operation can be determined by the following equations:
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(26) Depending on the form factor of the waveguide and its dielectric properties, a waveguide can permit single mode operation at a high cut-off frequency. Single mode operation can be achieved if the waveguide dimensions width (w) and height (h) satisfy the above equations. For material with a high dielectric constant, the waveguide dimensions can be reduced for single mode operation. Small waveguide dimensions increase the waveguide density for waveguide arrays used in interconnects and improve the mechanical flexibility. For a suitably dimensioned alumina ceramic ribbon waveguide having low-loss and a high dielectric constant, the waveguide can exhibit an attenuation coefficient of less than 10 dB/cm.
(27) A THz waveguide needs to have both low transmission loss in the THz frequency and a wide range of mechanical properties that allow for operation in a variety of environmental conditions. In one aspect, the ceramic core comprises alumina and may have a grain size of at least about 0.5 μm. A ceramic core that comprises alumina with a smaller grain size can be denser and may exhibit more flexibility than a ceramic core with a larger grain size. In some aspects, ceramic core that comprises alumina with a grain size of at least about 0.5 μm may have variable flexibility, e.g. a bending radius of about 17 mm for a form factor with a thickness in the range from about 10 μm to about 200 μm. In view of the present aspects, a waveguide comprised of a ceramic core that comprises alumina can effectively transmit signals within the THz range while still having low transmission loss and improved flexibility.
(28) Conventional waveguides that exhibit flexibility may still fracture or shatter when exposed to a variety environmental conditions. Therefore, a THz waveguide that has greater mechanical strength but remains flexible, pliable, or supple, may be more suitable for terahertz applications. As discussed above, a ceramic core that comprises alumina with a smaller grain size can be denser and may exhibit more flexibility, and mechanical strength, than a ceramic core that comprises alumina with a larger grain size. In some aspects, a ceramic core that comprises alumina with a grain size of at least about 0.5 μm may have a mechanical strength of at least 700 MPa when undergoing a 2pt flexural bending strength test. In view of the present aspects, a waveguide comprised of a ceramic core that comprises alumina can effectively transmit signals within the THz range while still having low transmission loss and improved strength.
(29) In other aspects, the ceramic core material is not limited to alumina; core material may also include, for example, silica (Dk˜4), mullite (Dk˜6), magnesium titinate (Dk˜15-20), zirconium tin titinate (Dk˜37), titânia (Dk˜100), or barium titinate (Dk>1000). Other core materials are contemplated that similarly transmit signals in the frequency range of 0.1 THz to 10 THz but provide for a high Dk.
(30) In some aspects, a THz waveguide may have a cladding disposed around a ceramic core that comprises alumina. A cladding serves as a protective gliding material for a ceramic core thereby enabling propagation in the THz range with low transmission loss. In addition, a cladding may inhibit any potential interactions between a propagating wave and the surrounding environment.
(31) A cladding can be disposed around a ceramic. In some aspects, it may be preferable for cladding to have a lower dielectric constant than the dielectric constant of core. In other aspects, it may be preferable for cladding to have a Df less than 1×10.sup.−3. As a result, cladding may assist in confining an electromagnetic wave inside the ceramic core structure so that it limits how much the fields spread out, and losses resulting from this effect are eliminated. It is advantageous for cladding to have a similar loss tangent in the THz range as the ceramic core (though it can be somewhat higher because the total loss is less sensitive to the cladding), as well as a low dielectric constant so to minimize transmission loss and the size of the structure formed as part of the waveguide. In some aspects, cladding may have a dielectric constant within the range of 10-1000.
(32) Cladding 25 can be made of air, glass, silicon dioxide (silica glass), or polymers. In aspects where cladding 25 is made of a polymer, polymers may include, for example, SU-8, polytetrafluoroethylene (Teflon), or other fluoropolymers that have low loss properties in the frequency range of 100 GHz-1000 GHz. Other suitable materials for the cladding 18 may be any combination thereof.
(33) As discussed above,
(34) In some aspects, it may be preferable for the first planar 27 layer of the cladding to have a lower dielectric constant than the dielectric constant of ceramic core. In other aspects, it may be preferable for the second 28 planar layer of the cladding to have a lower dielectric constant than the dielectric constant of the ceramic core. In other aspects, it may be preferable for both the first 27 and second 28 planar layers of the cladding to have lower dielectric constants than the dielectric constant of the ceramic core. As a result, the first 27 and second 28 planar layers of the cladding may assist in confining an electromagnetic wave inside the ceramic core structure so that it does not spread out, and losses resulting from this effect are eliminated. It is advantageous for the first and second planar layers of the cladding to have a similar loss tangent in the THz range as the ceramic core, as well as a low Dk so to minimize transmission loss and the size of the structure formed as part of the waveguide.
(35) In yet another aspect, it may be preferable for the first planar 27 layer of the cladding to have a Df less than 1×10.sup.−3. In other aspects, it may be preferable for the second 28 planar layer of the cladding to have a Df less than 1×10.sup.−3. In other aspects, it may be preferable for both the first 27 and second 28 planar layers of the cladding to have a Df less than 1×10.sup.−3. As a result, the first 27 and second 28 planar layers of the cladding may assist in confining an electromagnetic wave inside the ceramic core structure so that it does not spread out, and losses resulting from this effect are eliminated. It is advantageous for the first and second planar layers of the cladding to have a similar loss tangent in the THz range as the core, as well as a low DF so to minimize transmission loss and the size of the structure formed as part of the waveguide.
(36) The first and second planar layers of the cladding can be made of air, glass, silicon dioxide (silica glass), or polymers. In aspects where the first and second planar layers of the cladding are made of a polymer, polymers may include, for example, SU-8, polytetrafluoroethylene (Teflon), or other fluoropolymers that have low loss properties in the frequency range of 100 GHz-1000 GHz. Other suitable materials for the cladding 18 may be glass, air, polymer and any combination thereof.
(37) In aspects where a cladding is disposed around a ceramic core, the waveguide may become stiff, inflexible, or fragile. In addition, disposing a cladding around a ceramic core may increase the overall size of the waveguide. Therefore, the thickness of a cladding may influence the flexibility, durability, and size of a waveguide. In one aspect, the cladding comprises a thickness 31 in the range from 0.1 mm to 10 mm. In another aspect, the first and second planar layers of a cladding comprises a thickness in the range of 0.1 mm to 10 mm. Because of the thickness of a cladding, a THz waveguide may remain flexible with the added benefit of reducing the overall size of the waveguide structure.
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(39) A cutout 42 may be filled with air, forming a cladding layer between each waveguide 14. Cladding material can be composed of two materials of differing dielectric constants acting as an effective index material such that they retain their distinct composition in local regions upon combination, the size of these distinct regions being much less than the THz operating wavelength, and on average the dielectric constant of the cladding material is lower than the dielectric constant of the THz waveguide 14. An example of cladding material could be a fluoropolymer where it is made porous with air bubbles to lower the dielectric constant and the pore size is much less than the THz operating wavelength. Another example of cladding material could be silica soot deposited as a cladding. Pore size as deposited is small enough that silica soot need not be consolidated. Localized heating and consolidation can be done to create transitions in the THz waveguide effective index that can be useful for mode field conversion. Alternatively, any or all cutouts 42 may also be filled with a dielectric material, for example a polymer, having a lower dielectric constant than a THz waveguide 14. Each cutout 42 shown runs in a straight line, but it is also contemplated within the scope of the present invention that it may contain a bend, for example a cutout curved by somewhere between 0-90 degrees (see
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Wire Bonds
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Planar Ceramic Dielectric Waveguide
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(46) Also embedded within the ceramic dielectric waveguide 16 may be a ceramic support structure 18 (see
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(51) In the present disclosure, use of the singular includes the plural except where specifically indicated.
(52) The present described technology is now described in such full, clear, concise, and exact terms as to enable any person skilled in the art to which it pertains to practice the same. It is to be understood that the foregoing described preferred aspects of the technology and that modification may be made therein without departing from the spirit of scope of the invention as set forth in the appended claims. The scope of the following claims is to be accorded the broadest interpretation to encompass all such modifications and equivalent structures and functions. Therefore, it is intended that the application not be limited to the particular aspects disclosed, but that the application will include all aspects falling within the scope of the appended claims.