This disclosure relates to an integrated circuit package that includes a phononic band gap structure in the package.
individual discrete components are typically fabricated on a silicon wafer before being cut into separate semiconductor the and assembled in a package. The package provides protection against impact and corrosion, holds the contact pins or leads which are used to connect from external circuits to the device, and dissipates heat produced in the device.
Wire bonds may be used to make electrical connections between an integrated circuit and the leads of the package with fine wires connected from the package leads and bonded to conductive pads on the semiconductor die. The leads external to the package may be soldered to a printed circuit board. Modern surface mount devices eliminate the need for drilled holes through circuit boards and have short metal leads or pads on the package that can be secured by reflow soldering.
Many devices are encapsulated with an epoxy plastic that provides adequate protection of the semiconductor devices and mechanical strength to support the leads and handling of the package. Some integrated circuits have no-lead packages such as quad-flat no-leads (QFN) and dual-flat no-leads (DFN) devices that physically and electrically couple it circuits to printed circuit boards. Flat no-lead devices, also known as micro leadframe (MLF) and small outline no-leads (SON) devices, are based on a surface-mount technology that connects integrated circuits to the surfaces of printed circuit boards without through-holes in the printed circuit boards. Perimeter lands on the package provide electrical coupling to the printed circuit board.
Particular embodiments in accordance with the disclosure will now be described, by way of example only, and with reference to the accompanying drawings:
Other features of the present embodiments will be apparent from the accompanying drawings and from the detailed description that follows.
Specific embodiments of the disclosure will now be described in detail with reference to the accompanying figures. Like elements in the various figures are denoted by like reference numerals for consistency. In the following detailed description of embodiments of the disclosure, numerous specific details are set forth in order to provide a more thorough understanding of the disclosure. However, it will be apparent to one of ordinary skill in the art that the disclosure may be practiced without these specific details. In other instances, well-known features have not been described in detail to avoid unnecessarily complicating the description.
The epoxy encapsulant for semiconductor chips/packages has typically served the primary purpose of providing environmental and mechanical protection for the integrated circuit (IC). Previously, in order for an additional package function to be added, it must be added before or after the encapsulation step. Performing additional packaging steps may increase cost and limit functionality on the processes that can be performed. A method for encapsulating an IC will now be disclosed in which a structure to perform an additional package function may be created during the process of encapsulation.
In physics, a phonon is a collective excitation in a periodic, elastic arrangement of atoms or molecules in condensed matter, like solids and some liquids. Often designated a quasiparticle, it represents an excited state in the quantum mechanical quantization of the modes of vibrations of elastic structures of interacting particles. Viewing a phonon as a particle, a quantum of vibration, it can be said that a phonon carries energy just like a molecule.
Additive manufacturing has enabled the deposition of patterned materials in a rapid and cost efficient manner. By utilizing additive manufacturing, control structures may be integrated directly into the encapsulation material of an IC. As will be disclosed herein, high frequency phononic devices, such as an ultrasound generator and/or receiver device may be provided in the encapsulation of an IC package through the implementation of multi-material phononic bandgap (PBG) structures within the encapsulation.
A phononic emitter device 110 may be fabricated on IC die 102 using known or later developed processing techniques. Phononic device 110 may be fabricated using a piezoelectric material, for example. Phononic device 110 may be designed to emit ultrasonic sound waves in the form of phonons.
Ultrasound is sound waves with frequencies higher than the upper audible limit of human hearing. Ultrasound devices may operate with frequencies from 20 kHz up to several gigahertz. Ultrasound is used in many different fields. For example, ultrasonic devices may be used to detect objects and measure distances. Ultrasound imaging or sonography is often used in medicine. In the nondestructive testing of products and structures, ultrasound is used to detect invisible flaws. Industrially, ultrasound may be used for cleaning, mixing, and to accelerate chemical processes.
A phonon detector device 111 may be formed on IC die 102 using known or later developed processing techniques. Phonon detector device 111 may be fabricated using a piezoelectric material, for example. Phonon detector 111 may be designed to produce an electrical signal in response to detecting ultrasound phonons, for example. For another application, phonon detector may 111 may be designed to detect high frequency vibration and shock waves, for example. In some embodiments, phonon detector 111 may be a microelectromechanical system (MEMS) vibration sensor device. In other embodiments, phonon devices 110, 111 may be various forms of microphones, speakers, emitters, detectors, etc.
Some embodiments may include only phononic emitter device 110 or phononic detector device 111, while other embodiments may include both devices or multiple devices. In either case, additional signal processing circuitry may be included on IC die 102 and coupled to phononic devices 110, 111. The signal processing circuitry may be designed to receive digital data from a local storage or an external system and convert it to analog electrical signals that are then converted to ultrasonic waves 112 by phononic emitter device 110 and thereby launched into encapsulant material 120. The ultrasonic waves may travel through encapsulant material 120 and emerge from the surface of IC 100 where they may be directed to a test subject located nearby, for example.
Similarly, ultrasound waves 113 may be received from an external source and travel through encapsulation material 120 and be converted to electrical signals by detector 111 and then be provided to the signal processing circuitry for processing, storage, and/or communicating to another system, for example.
As will be described in more detail below a PBG structure within encapsulation material 120 may be used to guide ultrasound waves 112, 113 into and/or out of encapsulant material 120 by confining the ultrasound waves to a designated phononic channel region 115, for example. Phononic channel region 115 may also be referred to herein as a “bandpass channel” since it allows phonons within a selected band to pass through.
In this example, a solid encapsulant material 120 surrounds and encapsulates IC die 102. A portion of the encapsulation, material may in a matrix of interstitial nodes such as indicated at 121 that may be filled with a material that is different from encapsulation material 120. In this example, nodes 121 are arranged in a three dimensional array of spherical nodes that are in turn separated by a lattice of encapsulation material 123. Encapsulation material 123 may be the same or different as solid encapsulation material 120. The structure formed by the matrix of nodes 121 and lattice 123 will be referred to herein as a “phononic bandgap structure.”
Solid encapsulant material 120 is typically an epoxy based material that provides mechanical protection and seals IC die 102 from environmental gases and liquids.
In this example, lattice 123 may be in contact at various places on the top or side surfaces of IC die 102. As mentioned above, lattice 123 may be formed from the same material as solid encapsulation material 120, or it may be formed using a different material by using an additive manufacturing process. The array of nodes 121 may be formed with one or more different materials. For example, some of the nodes 121 may be filled with a first material and some of the nodes 121 may be filled with different types of material. There may be a number (N) of different materials that are used to fill N different sets of nodes within encapsulation material 123. Node material may be a polymer or other material that has different intrinsic material properties from the lattice material 123.
For example, node material 121 may be air, some other gas, or even a vacuum in some embodiments. In other embodiments, node material 121 may be soft or rubbery. In another embodiment, certain nodes 121 may be filled with a hard material, while other nodes 121 are filled with a soft material, for example. The hardness or softness of each material may be referred to as the “acoustic impedance” of the material.
In the example of
In some embodiments, die attachment 125 may be a thin layer of adhesive material. In other embodiments, die attachment 125 may include a portion 126 that is a phononic bandgap structure. As will be explained in more detail below, this may allow shielding a portion of the IC die 102 from acoustic noise that is transferred to thermal pad 104 from a substrate to which IC 100 is attached while still allow heat energy to propagate from IC die 102 to thermal pad 104, for example.
A phononic crystal is an artificially manufactured structure, or material, with periodic constitutive or geometric properties that are designed to influence the characteristics of mechanical wave propagation. When engineering these crystals, it is possible to isolate these waves within a certain frequency range. Conversely it may be more helpful to consider these waves as particles and rely on the wave-particle duality throughout the explanation. For this reason, any reference to propagation henceforth may refer to either wave movement or particle movement through the substrate. Propagation within this selected frequency range, referred to as the band gap, is attenuated by a mechanism of interferences within the periodic system. Such behavior is similar to that of a more widely known nanostructure that is used in semiconductor applications, a photonic crystal. The general properties and characteristics of phononic structures are known, for example, see; “Fundamental Properties of Phononic Crystal,” Yan Pennec and Bahram Djarari-Rouhani, Chapter 2 of “Phononic, Crystals, Fundamentals and Applications” 2015, which is incorporated by reference herein.
Phononic crystals are formed by a periodic repetition of inclusions in a matrix. The elastic properties, shape, and arrangement of the scatterers may strongly modify the propagation of the acoustic/elastic waves in the structure. The phononic band structure and dispersion curves can then be tailored with appropriate choices of materials, crystal lattices, and topology of inclusions.
The propagation of acoustic waves in a phononic crystal may be governed by the Bloch or Floquet theorem from which one can derive the band structure in the corresponding Brillouin zone. The periodicity of the structures that defines the Brillouin zone may be in one (1D), two (2D), or three dimensions (3D).
The general mechanism for the opening of a band gap is based on the destructive interference of the scattered waves by the inclusions. This necessitates a high contrast between the elastic properties of the materials. In periodic structures, this is called the Bragg mechanism and the first band clap generally occurs at a frequency which is about a fraction of c/a, where “c” is a typical velocity of sound, and “a” is the period of the structure.
Phononic bandgap structures may be designed and modeled using simulation software available from various vendors. For example, physics-based systems may be modeled and simulated using COMSOL Multiphysics® simulation software from COMSOL®. “Multiphysics” and “COMSOL” are registered trademarks of COMSOL AB.
The x-axis of
The width and the frequency range covered by a phononic bandgap depends on the periodic spacing of the nodes 233, which may be represented by lattice constant “a” as indicated at 336 in
The phononic wavelength (λ) can be determined using expression (1), where the velocity (v) in materials is typically on the order of 103-105 m/s and ν is the frequency of the phonon.
lambda (λ)=v/ν (1)
For ultrasonic signals in the Mhz/Ghz frequency range, for example, the corresponding wavelengths in encapsulant material 120 may be in the range of several microns. The opening of phononic band gaps requires two main conditions. The first one is to have a large physical contrast, such as density and speed of propagation of the wave movements, between the nodes and the lattice. The second condition is to present a sufficient filling factor of the nodes in the lattice unit cell. The forbidden band gap occurs in a frequency domain given by the ratio of an effective propagation velocity in the composite material to the value of the lattice parameter of the periodic array of nodes. Referring to
The node spacing 454-556 in this example may be selected to be approximately 10 μm, for example. Phononic channel 451 may be formed by not having any nodes within the region 451. In this manner, acoustic energy wave movement in the form of phonons 452 that fall within the bandgap frequency range of PBG structure 450 that enter region 451 may blocked from penetrating into PBG structure 450. Thus, region 451 may be formed by omitting nodes within this region.
The size 453 of phononic channel 451 may vary based on the application. In some embodiments, the width 453 of phononic channel 451 may be just a few times the lattice constant, as illustrated here. In other embodiments, the width 453 may be arbitrarily large.
Each individual leadframe may include a thermal pad, such as thermal pads 104. Thermal pad 104 may also be referred to as a “die attach pad,” Each individual lead frame also includes a set of contacts that surround the thermal pad, such as contacts 105. A sacrificial strip of metal connects all of the contacts together and provides mechanical support until a sawing process removes it. An IC die may be attached to each thermal pad during a packaging process. Wire bonding may then be performed to connect bond pads on each IC chip to respective contacts on the lead frame. The entire lead frame strip 700 may then be covered with a layer of mold compound using an additive process as described in more detail below to encapsulate the ICs. Lead frame strip 700 may then be singulated into individual packaged ICs by cutting along cut lines 728, 729.
In this example, a vat photopolymerization process may be used in which leadframe strip and the ICs attached to it, such as IC die 102, are lowered into a vat of liquid photo polymer resin. A light source, such as a laser or projector, may then expose selected regions of the liquid photopolymer resin to initiate polymerization that converts exposed areas of the liquid resin to a solid. In this manner, layers of encapsulant material 120 may be formed in selected shapes. For example, encapsulant material that forms lattice 123 may be the same or different as the solid enscapsulant material 120. Nodes 121 may be formed with a selected lattice spacing.
The leadframe strip may be submerged in different vats at different times in order to allow different materials to form the nodes 121 within lattice 123.
The nearly complete formation of phononic channel 115 may be seen in
Additional layers of resin may be exposed and hardened to form the final outside encapsulation layer illustrated in
In another embodiment, other additive manufacturing processes may be used to form encapsulation material 120. For example, a powdered bed diffusion process may be used in which a powdered material is selectively consolidated by melting it together using a heat source such as a laser or electron beam.
In another embodiment, a material jetting process may be used in which droplets of material are deposited layer by layer to produce an acoustic directing encapsulation structure as described herein. However, bond wires 106 may require extra care to avoid disrupting the droplet streams.
In another embodiment, bond wires are not initially bonded to contacts 105 and bond pads 843. In this example, a material jetting process may be used in which droplets of material are deposited layer by layer to produce a phononic bandgap structure as described herein. As part of the material jetting process, a conductive material may be deposited to form the bond wires between contacts 105 and bond pads 843. In some embodiments, a sintering process may be done by heating the encapsulated leadframe 700 assembly to further solidify the bond wires. The leadframe strip 700 may then be sawed or otherwise separated into individual encapsulated IC packages.
In another embodiment, IC die 102 is not initially attached to thermal pad 104 of a leadframe that may be part of a leadframe strip similar to leadframe strip 700 shown in
In another embodiment, the phononic bandgap structure may be fabricated using a lattice material that includes filler particles in place of the explicitly formed nodes as described above, such as nodes 121. In this case, the filler particles are selected to have a size and material composition that will influence the characteristics of mechanical wave propagation, as described above. The filler material may be a polymer or other material that has different intrinsic material properties from the lattice material, in a similar manner as the difference between nodes 121 and lattice material 123. In some embodiments, the filler material may be hard, while in other embodiments the filler material may be soft or rubbery.
In another embodiment, multiple phononic bandgaps may be formed by using two or more types of fillers. For example, a portion of the filler material may be a hard material, while another portion of the filler material may be a soft material. In some embodiments, different size filler particle may be used in different regions or in a same region to form multiple bandgaps. In some embodiments, a different number of filler particles per unit volume may be used in different regions to form different bandgaps.
In this case, the filler dispersion will not be perfectly crystalline, but there will be a statistical mean separation of the filler particle that may lend itself to a bandgap based on the statistical mean separation distance of the filler particles.
An additive manufacturing process may be used to encapsulate an IC die using two or more different polymers, such as one with filler particles and one without filler particles to form the PBG structures as described herein or other configurations of PBG structures.
Alternatively, a selective molding process may be used in which one area of the encapsulation is molded with first polymer having either no filler particles or a first configuration of filler particles (size, material, number of particles per unit volume, etc.) and other areas are molded with a polymer having a different filler particle configuration to form a PBG structure as described herein or other configurations of PBG structures.
In other embodiments, a relatively small phononic bandgap structure may be fabricated during the encapsulation process to provide phononic guidance in a limited area of the encapsulation material.
QFN package 1000 includes a set of contacts 1005 arrayed around the perimeter of the package on the bottom side. Thermal pad 1004 has an exposed surface on the bottom side of QFN 1000. An integrated circuit die (not shown) is mounted to the other side of thermal pad 1004. The entire assembly is encapsulated in an encapsulation material 1010 using an additive manufacturing process as described herein to form a phononic directing phononic bandgap structure. While a QFN is illustrated in
In another embodiment, a layer of phononic guiding material that includes a phononic bandgap structure may be first formed on the thermal pad of the leadframe, as indicated at 1104. The encapsulation material may be formed into a lattice with periodically spaced nodes that are filled with a different type of material to form a phononic bandgap structure. As described above in more detail, an additive manufacturing process may be used to create the lattice and fill the nodes in the lattice.
An IC die may then be attached to the layer of phononic guiding encapsulation material, as indicated at 1106.
In either case, the IC die may then be completely encapsulated by an additive process to form a phononic guiding structure within the encapsulation material as indicated at 1108. A first portion of the encapsulation material may be solid and a second portion of the encapsulation material may include nodes filled with a second material to form a phononic bandgap structure. As described above in more detail, an additive manufacturing process may be used to create a lattice and fill the periodically spaced nodes in the lattice with a different type of material, or with several different types of material in different locations.
In another embodiment, the encapsulation process indicated at box 1108 may be done using a selective molding process in which one area of the encapsulation is molded with first polymer having either no filler particles or a first configuration of filler particles (size, material, number of particles per unit volume, etc.) and other areas are molded with a polymer having a different filler particle configuration to form a PBG structure as described herein or other configurations of PBG structures.
As discussed above in more detail, various types of IC packages may be formed in this manner. For example, a quad-flat no-leads (QFN) package is illustrated in
Phononic device 1240 may be fabricated on a substrate 1241 which in this example is silicon with a passivation layer 1242, 1244 of silicon oxide. Substrate 1241 may be a thin layer of silicon that acts as a vibrating membrane in response to piezoelectric layer 1246. Another layer 1243 of silicon may be formed adjacent passivation layer 1242. A cavity 1248 may be formed in layer 1243 to allow piezoelectric layer 1246 and membrane layer 1241 to vibrate. Cavity 1248 may be formed in layer 1243 by back etching using passivation layer 1242 as an etch stop, for example.
Phononic device 1240 is merely an example of a phononic device that may be used in an encapsulated IC, as illustrated in
MCM module 1300 may be encapsulated as described above in more detail to form a PBG structure using nodes or particles 1321 that are dispersed in encapsulant material 1323. A bandpass region 1315 may be formed is described above in more detail by leaving out nodes or particles 1321 in the band as region. As discussed above, an additive manufacturing process may be used to form nodes 1321 in a periodic matrix. Alternatively, a selective molding process may be used with encapsulation material having a selected density of filler particles to form a PBG structure and an encapsulation material with no filler particles to form band as region 1315, for example. Cavity region 1248 and region 1249 above phononic device 1240 may be left clear encapsulant to allow for vibration of the device membrane 1241, as shown in
Phononic device 1240 may be configured to receive an analog signal from the signal processing circuitry on IC die 1362 and convert it into a stream of phonons 1350 that may then be guided through bandpass region 1315 by the PBG structure formed by nodes/particles 1321 and emitted from the surface of MCM 1300.
Alternatively, phononic device 1240 may be configured to receive a stream of phonons 1350 that may be impinging on a surface of MCM 1300 and then be guided through bandpass region 1315 by the PBG structure formed by nodes/particles 1321. Phononic device 1240 may generate an analog signal in response to the received phonons and pass the analog signal to the processing circuitry on IC die 1362 for further processing and storage.
In another embodiment, there may be two or more phononic devices such as device 1240 included within a single MCM.
While the disclosure has been described with reference to illustrative embodiments, this description is not intended to be construed in a limiting sense. Various other embodiments of the disclosure will be apparent to persons skilled in the art upon reference to this description. For example, in some embodiments, the lattice material may be relatively soft and the node material may be relatively hard. In other embodiments, the lattice material may be relatively soft and the node material may be relatively hard. In some embodiments, the node material may be air, another gas, or a vacuum, for example.
In some embodiments, a portion of the nodes may be formed with one kind of material, while another portion of the nodes may be formed with a different material. Several different types of material may be used to form different sets of nodes within the phononic bandgap structure to thereby tailor the performance of the phononic ban gap structure.
In some embodiments a portion of the nodes may be formed with one lattice constant, while another portion of the nodes may be formed with a different lattice constant. Several different lattice constants may be used to form different sets of nodes within the phononic bandgap structure to thereby tailor the performance of the phononic bandgap structure.
In some embodiments, the PBG structure may be symmetric in 3D, while in other embodiments the PBG structure may be asymmetric with different lattice spacing in different directions.
In some embodiments, the PBG structure may have a bandgap that is effective in all directions, while in other embodiments the PBG structure may have a bandgap in one direction but not in another direction, for example.
While a phononic guiding channel, such as channel 115 as shown in
As described above, a phononic channel may be formed through a PBG structure by simply omitting the interstitial nodes within the channel to thereby form a bandpass channel. In another embodiment, a bandpass channel may be formed by superimposing several different PBG structures having different bandgaps, for example.
Another example may demonstrate packages that are entirely encased in mold compound, such as a DIP (dual inline package). In this case there is not a thermal pad that is in contact with the board. The only direct electrical contact with the board is through the pin legs.
Certain terms are used throughout the description and the claims to refer to particular system components. As one skilled in the art will appreciate, components in digital systems may be referred to by different names and/or may be combined in ways not shown herein without departing from the described functionality. This document does not intend to distinguish between components that differ in name but not function. In the following discussion and in the claims, the terms “including” and “comprising” are used in an open-ended fashion, and thus should be interpreted to mean “including, but not limited to . . . .” Also, the term “couple” and derivatives thereof are intended to mean an indirect, direct, optical, and/or wireless electrical connection. Thus if a first device couples to a second device, that connection may be through a direct electrical connection, through an indirect electrical connection via other devices and connections, through an optical electrical connection, and/or through a wireless electrical connection.
Although method steps may be presented and described herein in a sequential fashion, one or more of the steps shown and described may be omitted, repeated, performed concurrently, and/or performed in a different order than the order shown in the figures and/or described herein. Accordingly, embodiments of the disclosure should not be considered limited to the specific ordering of steps shown in the figures and/or described herein.
It is therefore contemplated that the appended claims will cover any such modifications of the embodiments as fall within the true scope and spirit of the disclosure.
Number | Name | Date | Kind |
---|---|---|---|
3868759 | Hartleroad et al. | Mar 1975 | A |
3868764 | Hartleroad et al. | Mar 1975 | A |
4974590 | Saito | Dec 1990 | A |
4999587 | Evans | Mar 1991 | A |
5355577 | Cohn | Oct 1994 | A |
5500912 | Alonas et al. | Mar 1996 | A |
5528074 | Goto et al. | Jun 1996 | A |
5834320 | Huddleston et al. | Nov 1998 | A |
6664615 | Bayan et al. | Dec 2003 | B1 |
6967347 | Estes et al. | Nov 2005 | B2 |
6979105 | Leysath | Dec 2005 | B2 |
7228016 | Beausoleil | Jun 2007 | B2 |
7305161 | Zhou | Dec 2007 | B2 |
7733198 | Olsson | Jun 2010 | B1 |
8031012 | Hasegawa | Oct 2011 | B2 |
8054145 | Mohammadi | Nov 2011 | B2 |
8094023 | El-Kady et al. | Jan 2012 | B1 |
8138868 | Arnold | Mar 2012 | B2 |
8143637 | Kanatake | Mar 2012 | B2 |
8587182 | Reiche | Nov 2013 | B2 |
9018074 | Zhang et al. | Apr 2015 | B2 |
9070703 | Haroun et al. | Jun 2015 | B2 |
9123737 | Haroun et al. | Sep 2015 | B2 |
9343426 | Parvarandeh | May 2016 | B1 |
9373878 | Schuppener et al. | Jun 2016 | B2 |
9450563 | Gorisse | Sep 2016 | B2 |
9583811 | Seler et al. | Feb 2017 | B2 |
9647329 | Herbsommer et al. | May 2017 | B2 |
9651718 | Chen | May 2017 | B2 |
10062583 | Costa | Aug 2018 | B2 |
10139564 | Homeijer et al. | Nov 2018 | B1 |
20050224956 | Kao et al. | Oct 2005 | A1 |
20060038168 | Estes et al. | Feb 2006 | A1 |
20060054780 | Garrood et al. | Mar 2006 | A1 |
20070108545 | Chua et al. | May 2007 | A1 |
20080112665 | Beausoleil et al. | May 2008 | A1 |
20080218299 | Arnold | Sep 2008 | A1 |
20090288852 | Hirokawa et al. | Nov 2009 | A1 |
20100019247 | Joichi et al. | Jan 2010 | A1 |
20110001233 | Iwase et al. | Jan 2011 | A1 |
20110089815 | Yeh et al. | Apr 2011 | A1 |
20110103632 | Leclair | May 2011 | A1 |
20110133597 | Pavlov et al. | Jun 2011 | A1 |
20110221057 | Lin et al. | Sep 2011 | A1 |
20120043628 | Martin | Feb 2012 | A1 |
20120098611 | Sinha et al. | Apr 2012 | A1 |
20120154168 | Duncan et al. | Jun 2012 | A1 |
20130038174 | Kim | Feb 2013 | A1 |
20130228796 | Mieczkowski | Sep 2013 | A1 |
20140287703 | Herbsommer et al. | Sep 2014 | A1 |
20140326902 | Tahan et al. | Nov 2014 | A1 |
20150237423 | Bahr et al. | Aug 2015 | A1 |
20150295305 | Herbsommer et al. | Oct 2015 | A1 |
20160028367 | Shealy | Jan 2016 | A1 |
20160276311 | Meyer et al. | Sep 2016 | A1 |
20160327977 | Tang et al. | Nov 2016 | A1 |
20170084519 | Speight et al. | Mar 2017 | A1 |
20170108655 | Zarbock et al. | Apr 2017 | A1 |
20170186793 | Ockenfuss | Jun 2017 | A1 |
20170253476 | Shibuya et al. | Sep 2017 | A1 |
20170276870 | Snyman | Sep 2017 | A1 |
20170288123 | Hatano et al. | Oct 2017 | A1 |
20170292884 | Ching, Jr. | Oct 2017 | A1 |
20190128735 | Cook et al. | May 2019 | A1 |
Number | Date | Country |
---|---|---|
1780469 | Oct 1995 | RU |
2006101577 | Sep 2006 | WO |
2017111892 | Jun 2017 | WO |
Entry |
---|
International Search Report for PCT/US2018/049166 dated Dec. 13, 2018. |
International Search Report for PCT/US2018/049135 dated Dec. 13, 2018. |
Benjamin Stassen Cook and Daniel Lee Revier, “Thermal Management in Integrated Circuit Using Phononic Bandgap Structure”, U.S. Appl. No. 15/92,580, filed Oct. 24, 2017, pp. 1-33. |
Benjamin Stassen Cook and Daniel Lee Revier, “Electromagnetic Interference Shield within Integrated Circuit Encapsulation Using Photonic Bandgap Structure”, U.S. Appl. No. 15/799,757, filed Oct. 31, 2017, pp. 1-38. |
Benjamin Stassen Cook and Daniel Lee Revier, “integrated Circuit with Dielectric Waveguide Connector Using Photonic Bandgap Structure”, U.S. Appl. No. 15/800,042, filed Oct. 31, 2017, pp. 1-42. |
Benjamin Stassen Cook and Daniel Lee Revier, “Galvanic Signal Path Isolation in an Encapsulated Package Using a Photonic Structure”, U.S. Appl. No. 15/799,740, filed Oct. 31, 2017, pp. 1-38. |
Benjamin Stassen Cook and Daniel Lee Revier, “Spectrometry in Integrated Circuit Using a Photonic Bandgap Structure”, U.S. Appl. No. 15/800,009, filed Oct. 31, 2017, pp. 1-41. |
International Search Report for PCT/US2018/058478 dated Feb. 14, 2019. |
Mohammadi, et al. Complete phononic bandgaps and bandgap maps in two-dimensional silicon phononic crystal plates; Electronics Letters Aug. 2, 2017, vol. 43 No. 16. 2 pages. |
International Search Report for PCT/US2018/058481 dated Feb. 7, 2019. |
International Search Report for PCT/US2018/058487 dated Feb. 7, 2019. |
International Search Report for PCT/US2018/057358 dated Feb. 7, 2019. |
International Search Report for PCT/US2018/057351 dated Feb. 7, 2019. |
Optical Sensor-On-Chip ICs Simplify Handheld Spectrometer Design, available at https://www.digikey.com/en/articles/techzone/2017/jun/optical-sensor-on-chip-ics-simplify-handheld-spectrometer-design, Digi-Key Electronics, Jun. 28, 2017, pp. 1-6. |
Hideo Kosaka et al, “Self-Collimating Phenomena in Photonic Crystals”, Applied Physics Letters, vol. 74, No. 9, Mar. 1, 1999, pp. 1212-1214. |
“Phonon”, Wikipedia, available at https://en.wikipedia.org/wiki/Phonon on Aug. 2, 2017, pp. 1-9. |
Yan Pennec and Bahram Djafari-Rouhani, “Fundamental Properties of Phononic Crystal”, Chapter 2 in “Phononic Crystals”, 2016, pp. 23-50. |
Daniel Frederic Sievenpiper, “High-Impedance Electromagnetic Surfaces”, 1999, University of California, pp. 1-162. |
“7 Families of Additive Manufacturing”, According to ASTM F2792 Standards, Hybrid Manufacturing Technologies, pp. 1-2. |
“Standard Terminology for Additive Manufacturing Technologies”, ASTM International, F2792-12a,Sep. 9, 2013, pp. 1-3. |
Nagi Elabbasi, “Modeling Phononic Band Gap Materials and Structures”, Comsol Blog, Feb. 10, 2016, pp. 1-7. |
Dr. Qin Hu, “Multiphoton Lithograpy Based 3D Micro/Nano Printing”, EPSRC Centre for Innovative Manufacturing in Additive Manufacturing, pp. 1-30. |
International Search Report for PCT/US2018/058494 dated Feb. 21, 2019. |
Number | Date | Country | |
---|---|---|---|
20190123711 A1 | Apr 2019 | US |