Semiconductor system with waveguide assembly capable of controlling RF signal impedance by applied electromagnetic radiation - Patents.com

Abstract

A waveguide assembly integrated with a semiconductor wafer is provided. The waveguide assembly includes a waveguide channel defined by an inner wall of the wafer lined with a metal layer and having at least one port for transmitting an RF signal into and out of the waveguide channel. The waveguide assembly also includes a semiconductor barrier 5 member disposed within the waveguide channel. The waveguide assembly may be fabricated using etching and deposition processes for semiconductor devices. In use, selectively varying either the frequency or the power level or both of the electromagnetic radiation applied to the barrier member changes the electrical conductance of the barrier member, thereby changing the electrical impedance of the barrier member to the transmission of an RF signal 10 through the waveguide channel. The waveguide assembly may be used for switching, attenuating, routing, filtering, and transforming RF signals.

Description

[Technical field]

[0001] The present invention relates to a waveguide assembly in a semiconductor wafer, its fabrication using microfabrication processes, and a method for controlling the waveguide assembly by applied electromagnetic radiation to change the impedance to an RF signal transmitted within the waveguide assembly for purposes such as switching, attenuating, routing, filtering, and transforming the RF signal. [Background technology]

[0002] Radio frequency (RF) switches are fundamental building blocks of modern transceiver systems, enabling a variety of functionalities including signal routing, redundancy switching, band selection, and phase shifting. In particular, waveguide switches are typically chosen for millimeter-wave (mm-wave) to submillimeter-wave applications due to their low insertion loss and high power handling [1].

[0003] Several technologies for waveguide switching elements have been developed, including electromechanical rotor and pin diode switches [Refs. 2 and 19], as well as RF MEMS and microfluidic-based switches as reported in the literature [Refs. 3–5 and 20–21]. However, most of these approaches use conventional metal-machined waveguides and are therefore large, heavy, and difficult to integrate with planar microwave technologies and on-chip.

[0004] Silicon (Si) microfabrication techniques offer advantages including high precision with micrometer tolerances, high performance up to and beyond the sub-millimeter wave band, and integration with planarization techniques [References 10 and 22].

[0005] Integrated waveguide switches using RF MEMS have been proposed (see Ref. 4), but issues of self-actuation, reliability, and stiction limit their use for high-power applications. Optical control of microwave and millimeter-wave signals through the optical generation of solid-state plasmas in semiconductors has shown promise as a high-performance switching and phase-shifting technique [Refs. 6-7]. Not only are the bias networks of the light sources isolated from the RF signals, but the plasma elements themselves offer advantages including high-power handling and linearity [Ref. 23], fast switching times [Ref. 24], and low insertion loss [Ref. 25]. Applications in the literature include switches, variable attenuators, and tunable phase shifters [Refs. 7-9].

[0006] The prior art discloses waveguide devices and related switches. U.S. Patent No. 5,393,363 (Baril et al., March 26, 1985) discloses an electromagnetic switch formed from a rectangular waveguide having dimensions capable of propagating millimeter waves and including the step of providing a so-called ridge space of a given volume in which a bar of semiconductor material having a high breakdown voltage and low thermal resistance is disposed, the volume of which is equal to the volume of the ridge space.

[0007] US Patent No. 5,399,233 (Rosen et al., March 24, 1992) discloses a waveguide having walls defining an opening. An optically transmissive opening in one wall allows light from an optical illumination source, such as a laser diode array, to illuminate the opening in which is located a semiconductor slab positioned to be illuminated. When the array illuminates the slab, the propagation characteristics (phase velocity and attenuation constant) of the waveguide are changed. Thus, continuous wave signals passing through the waveguide are attenuated and phase shifted.

[0008] U.S. Patent No. 5,333,939 (Bacon et al., May 31, 1994) discloses an RF switch circuit including a waveguide transmission line having a wall with a cavity disposed therein aligned with a centerline of the waveguide transmission line, and means for presenting a substantially short circuit impedance characteristic between the cavity and the waveguide transmission line to RF signals propagating along the waveguide transmission line.

[0009] US Patent No. 5,399,323 (James, Dec. 8, 1998) discloses a microwave device incorporating a photosensitive baffle that can be selectively illuminated to change the electronic properties of the baffle from transmissive to reflective of microwave energy. The baffle functions as a gate, tuning element, reflector, etc.

[0010] Patent document 5 (Boutayeb, Jan. 12, 2017) discloses a substrate-integrated waveguide switch and a method of operating a substrate-integrated waveguide switch. The system includes a dielectric substrate and a switch supported by the dielectric substrate, the switch including at least one first transmission path, at least one first switching element in each of the at least one first transmission path, a second transmission path, and at least one second switching element in the second transmission path.

[0011] There remains a need in the art for switches for RF signals at millimeter wave frequencies in micromachined waveguide channels, methods for fabricating such switches, and methods for switching RF signals in semiconductor devices. [Prior art documents] [Patent documents]

[0012] [Patent Document 1] U.S. Pat. No. 4,507,632 [Patent Document 2] U.S. Patent No. 5,099,214 [Patent Document 3] U.S. Patent No. 5,317,293 [Patent Document 4] U.S. Patent No. 5,847,672 [Patent Document 5] US Patent Application Publication No. 2017 / 0012335 Summary of the Invention

[0013] In one aspect, the invention includes a system for impeding radio frequency (RF) signals, the system including a waveguide assembly integrated with a semiconductor wafer, the system including: (a) a waveguide channel defined by an inner wall of the wafer lined with a metal layer, the waveguide channel including at least one port for transmitting an RF signal into and out of the waveguide channel, and (b) at least one semiconductor barrier member disposed within the waveguide channel, the at least one semiconductor barrier member configured to change an electrical impedance of the barrier member to transmission of the RF signal through the waveguide channel by changing a waveguide electrical conductance of the barrier member in response to applied electromagnetic radiation.

[0014] In an embodiment of the system, the waveguide channel has a substantially rectangular prism shape or a substantially cylindrical shape. In an embodiment of the system, the waveguide channel includes a first waveguide channel portion and a second waveguide channel portion, and a channel height of the first waveguide channel portion is greater than a channel height of the second waveguide channel portion such that an electrical impedance of the first waveguide channel portion is greater than an electrical impedance of the second waveguide channel portion.

[0015] In an embodiment of the system, the waveguide channel includes a third waveguide-through channel portion, a fourth waveguide-through channel portion, and a fifth waveguide-through channel portion, the third waveguide-through channel portion being disposed between the fourth and fifth waveguide-through channel portions, a lateral channel width of the third waveguide-through channel portion being less than the lateral channel widths of the fourth and fifth waveguide-through channel portions, and at least one barrier member being disposed within the third waveguide-through channel portion.

[0016] In an embodiment of the system, at least one output port of the waveguide channel comprises a single port. In an embodiment of the system, the at least one port of the waveguide channel includes an input port, a first output port, and a second output port disposed away from the first output port, the waveguide channel defines a first path from the input port to the first output port, the waveguide channel defines a second path from the input port to the second output port, separate from the first path, and the at least one barrier member includes a first barrier member disposed in the first path and a second barrier member disposed in the second path. The waveguide assembly may further include a tuning stub disposed between the first path and the second path.

[0017] In an embodiment of the system, the at least one port of the waveguide channel includes an input port and an output port, the waveguide channel defines a first path from the input port to the output port and a shorting stub path extending from the first path, and the at least one barrier member is disposed in the stub path. The at least one barrier member may include a plurality of barrier members disposed in the stub path. The plurality of barrier members may be disposed in aligned rows along a length of the stub path.

[0018] In an embodiment of the system, the metal layer comprises gold, nickel, aluminum, chromium, tungsten, platinum, or silver. In embodiments of the system, the barrier member comprises silicon, germanium, gallium arsenide, gallium nitride, silicon germanium, silicon carbide, indium phosphide, or gallium phosphide.

[0019] In an embodiment of the system, the interior walls defining the waveguide channel and the barrier member comprise the same semiconductor material or different semiconductor materials. In an embodiment of the system, the barrier member extends from a metal layer lining the inner wall of the wafer to the window.

[0020] In an embodiment of the system, the barrier members are in the form of posts extending laterally in a direction perpendicular to the plane defined by the wafer. The posts may have a generally circular cross-sectional shape. In an embodiment of the system, the at least one barrier member includes a plurality of barrier members arranged in a row or array.

[0021] In an embodiment of the system, the waveguide assembly further includes a window including an electromagnetic radiation (ER) transparent semiconductor layer terminating the barrier member to allow excitation of the barrier member by applied electromagnetic radiation emitted from an external source to the wafer. The ER transparent semiconductor layer may include silicon nitride, silicon dioxide, indium tin oxide, or a transparent metal mesh membrane integrated into the semiconductor support. The window may have a dimension less than 1 / 12 of the wavelength (λ) of the RF signal transmitted through the waveguide. In an embodiment of the use, the RF signal has a frequency of about 1 GHz to 300 GHz, or a wavelength of about 1 mm to about 300 mm. Thus, in an embodiment, the window may have a dimension (e.g., diameter) of about 0.083 mm to about 25 mm, more specifically about 0.45 mm or less. The window may be recessed from the outer surface of the surrounding wafer.

[0022] In an embodiment of the system, the system further includes an electromagnetic radiation (ER) emitter for emitting the applied electromagnetic radiation. The ER emitter may include a light emitting diode (LED), a laser diode, or a Vertical Cavity Surface Emitting Laser (VCSEL). The ER emitter may be configured to emit electromagnetic radiation in the UV spectrum, the visible spectrum, or the infrared spectrum. The system may further include an optical fiber for optically coupling the electromagnetic radiation emitted by the ER emitter to the barrier member. The system may further include a control means including a microcontroller, a switch, or a variable resistor operably connected to the electromagnetic radiation ER emitter and configured to selectively control either or both of the frequency or power level of the electromagnetic radiation emitted by the ER emitter.

[0023] In embodiments of the system, the waveguide channel may be a space free of semiconductor material, except for the semiconductor material of the barrier members, between metal layers lining the interior walls defining the waveguide channel, or may include semiconductor material, except for the semiconductor material of the barrier members.

[0024] In another aspect, the invention includes a method for varying impedance to transmission of radio frequency (RF) signals through a waveguide channel defined within a semiconductor wafer, the method including the steps of: (a) providing at least one semiconductor barrier member disposed within the waveguide channel; and (b) selectively varying either a frequency or a power level, or both, of electromagnetic radiation applied to the at least one barrier member to change an electrical conductance of the barrier member, thereby varying the impedance of the at least one barrier member to transmission of the RF signal through the waveguide channel.

[0025] In an embodiment of the method, the RF signal has a frequency in the range of about 1 GHz to about 300 GHz, and more specifically, the RF signal has a frequency in the range of about 26.5 GHz to about 40 GHz. a It may be in the band.

[0026] In an embodiment of the method, varying either the energy level or the power level or both of the electromagnetic radiation applied by the ER emitter to the at least one barrier member results in an insertion loss of at least 20 dB between the input port and the output port.

[0027] In an embodiment of the method, selectively varying the power level of the electromagnetic radiation applied by the ER emitter includes varying the intensity of the emitted electromagnetic radiation between a null power level and a non-null power level.

[0028] In an embodiment of the method, selectively varying a power level of the electromagnetic radiation applied by the ER emitter includes varying a power level of the emitted electromagnetic radiation between a first non-null power level and a second non-null power level different from the first non-null power level.

[0029] In an embodiment of the method, the at least one barrier member includes a first barrier member and a second barrier member, and selectively varying either a frequency or a power level or both of the electromagnetic radiation applied to the at least one barrier member by the ER emitter includes selectively varying either a frequency or a power level or both of the electromagnetic radiation applied to the first barrier member independently of selectively varying either or both of the electromagnetic radiation applied to the second barrier member.

[0030] In embodiments of the method, the electromagnetic radiation applied by the ER emitter is in the UV spectrum, the visible spectrum, or the infrared spectrum. In another aspect, the invention includes a method of manufacturing a waveguide assembly for impeding radio frequency (RF) signals, the waveguide assembly being integrated with a semiconductor wafer, the method comprising the steps of: (a) providing a first portion of the wafer and a separate second portion of the wafer; (b) etching an inner surface of the first portion of the wafer to define (i) walls of a waveguide channel including at least one port for transmitting an RF signal into or out of the waveguide channel, and (ii) a semiconductor barrier member disposed within the waveguide channel; (c) depositing a first metal layer on an inner surface of the first portion of the wafer to line walls of the waveguide channels; (d) optionally etching the deposited first metal layer to expose barrier members to the waveguide channels; (e) optionally depositing a second metal layer on an inner surface of the second portion of the wafer to provide a metallized inner surface on the second portion of the wafer; and (f) bonding the first metal layer deposited on the inner surface of the first portion of the wafer to the metallized inner surface of the second portion of the wafer.

[0031] In the drawings, like elements may be assigned like reference numbers. The drawings are not necessarily to scale, emphasis instead being placed on the principles of the invention. Moreover, each illustrated embodiment is only one of many possible configurations that utilize the underlying concepts of the invention. [Brief description of the drawings]

[0032] [Figure 1A] 1 shows a schematic cross-section through the thickness of a semiconductor wafer including an embodiment of the inventive waveguide assembly including barrier members in the form of Si posts and having electromagnetic radiation (ER) emitters. [Figure 1B] FIG. 1B shows a schematic isometric view of the waveguide channel and barrier member of FIG. [Figure 1C] 1B shows a cross-sectional view of the waveguide channel and barrier member of FIG. 1A taken along line A'-A' of FIG. [Figure 2A] 1B is a chart showing the results of an HFSS™ analysis of the barrier member of FIG. 1A when in the on state (ie, no electromagnetic radiation is applied to the barrier member). [Figure 2B] 1C is a chart showing the results of an HFSS™ analysis of the barrier member of FIG. 1B when in an off state (i.e., electromagnetic radiation is applied to the barrier member) and the optical power of the irradiated electromagnetic radiation is increased. [Figure 3A] 1 shows a π-design layout of an embodiment of the underside of the upper wafer of a waveguide assembly of the present invention, including barrier members in the form of Si posts and a π-shaped matching network, all dimensions shown in μm. [Figure 3B] 3B illustrates a pi-design layout of the top wafer embodiment of FIG. 3A when flipped over for bonding onto a bottom wafer embodiment of the inventive waveguide assembly. [Figure 4] 4 illustrates a process flow for an embodiment of a method of the present invention for fabricating a waveguide assembly of the present invention. [Figure 5A]1 is a photograph of one embodiment of the underside of the top wafer of a waveguide assembly of the present invention highlighting the switch region, CPW-waveguide transition, and back-to-back waveguide. [Figure 5B] 1 is a photograph of an embodiment of the top surface of the bottom wafer of a waveguide assembly of the present invention highlighting the CPW-waveguide transition and the coplanar waveguide. [Figure 5C] 5B is a photograph of an embodiment of a waveguide assembly of the present invention formed by bonding the top wafer shown in Figure 5A with the bottom wafer shown in Figure 5B. All dimensions are in μm. [Figure 5D] Measurement of the waveguide assembly of FIG. 5C as a device-under-test (DUT) using two FormFactor |Z| probes with four optical fibers inserted into four holes etched into the backside of the top wafer, located above each barrier member (Si post). [Figure 6] 5C and its back-to-back waveguide configuration (see inset (a) of FIG. 6). The conductivity of copper for the HFSS™ simulation was 2.3×107 S / m, determined by measuring with a four-point probe after the wafer bonding step. [Figure 7] 5C is a chart showing the measured off-state isolation (|S21|) of the waveguide assembly of FIG. 5C as the optical fiber output power increases. The values ​​shown are the power at the output of each individual fiber for a 2×2 array of barrier elements (Si posts) as shown in FIG. 5A. [Figure 8A] 1 shows an isometric view of the layout of another embodiment of the waveguide assembly of the present invention with the top layer removed to show the internal structure that can be used as a T-matched solid-state plasma waveguide switch. [Figure 8B] 8B shows an equivalent circuit diagram for the waveguide assembly of FIG. 8A. [Figure 9A]FIG. 1 shows an isometric view of the layout of another embodiment of the waveguide assembly of the present invention with the top layer removed to reveal the internal structure that can be used as a π-aligned solid-state plasma waveguide switch. [Figure 9B] 9B shows an equivalent circuit diagram for the waveguide assembly of FIG. 9A. [Figure 10] 1 shows a top view of an embodiment of a layout of a waveguide assembly of the present invention that can be used as a single-pole N-throw solid-state plasma waveguide switch. [Figure 11A] 1 illustrates an isometric view of an embodiment of a layout of a waveguide assembly of the present invention that can be used as an evanescent mode bandpass filter waveguide switch. [Figure 11B] 11B shows an equivalent circuit diagram of an evanescent mode waveguide channel of the waveguide assembly of FIG. 11A. [Figure 11C] 11B shows an equivalent circuit diagram of the barrier member of the waveguide assembly of FIG. 11A when the barrier member is in a dark (capacitive) state. [Figure 11D] 11B shows an equivalent circuit diagram for the waveguide assembly of FIG. 11A when the barrier member is in a dark (capacitive) state within the evanescent mode waveguide channel. [Figure 12A] 1 illustrates an isometric view of another embodiment of a layout of a waveguide assembly of the present invention that can be used as an N-pole evanescent mode bandpass filter waveguide switch. [Figure 12B] 12B shows an equivalent circuit diagram of the waveguide assembly of FIG. 12A. [Figure 13A] 1 illustrates an isometric view of an embodiment of a layout of a waveguide assembly of the present invention that can be used as an optically tunable and reconfigurable solid-state plasma waveguide cavity resonator. [Figure 13B] 13B shows a top view of the waveguide assembly of FIG. 13A. [Figure 14] 1 illustrates an isometric view of another embodiment of a layout of a waveguide assembly of the present invention that can be used as an optically tunable and reconfigurable solid-state plasma waveguide cavity resonator. [Figure 15]1 shows a top view of an embodiment of a layout of a waveguide assembly of the present invention that can be used as an impedance matching network or phase shifter for an optically tunable solid-state plasma waveguide. [Figure 16] FIG. 1 shows a top view of another embodiment of a waveguide assembly of the present invention, which can be used as an impedance matching network or phase shifter for optically tunable solid-state plasma waveguide. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0033] definition The invention relates to a waveguide assembly in a semiconductor wafer, its fabrication using microfabrication processes, and a method for controlling the waveguide assembly by applied electromagnetic radiation to change the impedance to a radio frequency (RF) signal transmitted within the waveguide assembly for purposes such as switching, routing, filtering, and conversion of RF signals. Any term or expression not expressly defined herein shall have its generally accepted definition as understood by one of ordinary skill in the art.

[0034] Waveguide assembly. FIG 1A shows a schematic cross-section through the thickness of a semiconductor wafer (10) including one embodiment of a waveguide assembly of the present invention. In FIGS 1A-1C, a set of mutually orthogonal axes (XYZ) are provided for spatial reference. The waveguide assembly integrated with the wafer (10) includes a waveguide channel (20), a semiconductor barrier member (30), and a window (40). The wafer (10) and an electromagnetic radiation (ER) emitter (100) form the system of the present invention.

[0035] Semiconductor wafer. The wafer (10) is made of a semiconductor material. In the embodiment shown in FIG. 1A, the wafer (10) is made of a semiconductor material, which may be, from top to bottom, silicon nitride, silicon oxide (SiO), substantially pure silicon (Si), which may or may not contain dopants, or a combination of the above. <100> ), and borosilicate glass. In other embodiments, the wafer (10) may include different semiconductor material(s) that may be disposed in a single layer or in different layers.

[0036] Waveguide channel. The waveguide channel (20) is the interior portion of the wafer (10) that allows for the transmission of RF signals, and is defined by the interior walls of the wafer (10) that are lined with a metal layer (22).

[0037] In the embodiment shown in Figures 1A-1C, the waveguide channel (20) is a cavity that is devoid of semiconductor material and filled with air between the metal layers (22). However, in other embodiments, the waveguide channel (20) may include semiconductor material between the metal layers (22). In one embodiment, the semiconductor material between the metal layers (22) may be the same as the semiconductor material that forms the barrier members (30), but may not completely fill the space between the metal layers (22) such that the barrier members (30) are structurally distinct features disposed in the space between the metal layers (22). In such an embodiment, the waveguide channel (20) and the barrier members (30) may be formed using bulk microfabrication methods. In another embodiment, such as a substrate-integrated waveguide channel (20), the semiconductor material that forms the waveguide channel (20) between the metal layers (22) may be compositionally different from the semiconductor material that forms the barrier members (30). In such embodiments, the barrier member (30) may be inserted, grown, or deposited within the waveguide channel (20) after fabrication of the waveguide channel (20). Thus, when not optically stimulated, the dielectric constant of the semiconductor material forming the barrier member (30) may or may not be matched to the dielectric constant of the semiconductor material forming the waveguide channel (20), as may be required by a particular application.

[0038] In this embodiment, the metal layer (22) is a mixture of titanium and copper (Ti / Cu). In other embodiments, other metallic materials may be used, non-limiting examples of which include gold, nickel, aluminum, chromium, tungsten, platinum, and silver, among others, and mixtures thereof.

[0039] The waveguide channel (20) has at least one port for transmitting an RF signal into or out of the waveguide channel (20). In some embodiments, the waveguide channel (20) has at least two ports extending from an input port to an output port for transmission of an RF signal. In FIG. 1A, for example, the waveguide channel (20) extends longitudinally in a direction perpendicular to the plane of the drawing such that the input and output ports (such as labeled port 1 and port 2 in FIG. 1B and FIG. 1C) are spaced apart in a direction perpendicular to the plane of the drawing. In use, transmission of an RF signal from the input port to the output port is guided along the waveguide channel (20) by the impedance of the metal wall (22). In FIG. 1B, an RF signal (21) is shown entering the waveguide channel (20) from one of the ports (labeled port 1), while another RF signal (23) is shown entering the other port (labeled port 2). It will be understood that with respect to RF signal (21), port 1 is considered to be the input port while port 2 is considered to be the output port, and with respect to RF signal (23), port 2 is considered to be the input port while port 1 is considered to be the output port.

[0040] In other embodiments, the waveguide communication channel (20) may have only one port that functions as both an input port through which an RF signal enters the waveguide communication channel (20) and an output port through which an RF signal exits the waveguide communication channel (20). Non-limiting examples of such single-port waveguide communication channels (20) are shown in the cavity resonators of Figures 13A, 13B, and 14. Another example of such a single-port waveguide communication channel is the embodiment of a reflective phase shifter (see Example 9 described below), which in an alternative embodiment (not shown) may be implemented by a single-port waveguide communication channel (20). In yet other embodiments, the at least one port may include three or more ports, such as the three-port waveguide communication channel (20) shown in Figure 10.

[0041] 1A and 1B, the cavity of the waveguide channel (20) has the shape of a rectangular prism. In one embodiment, the lateral width (W) of the waveguide channel (20) is determined based on the desired operating bandwidth, i.e., TE, for a particular application. 1、0 It is selected according to the single mode bandwidth. (Note that in FIGS. 1A and 1B, the lateral width is the dimension parallel to the plane of the wafer (10) and perpendicular to the direction of transmission of the RF signals (21, 23) between the ports of the waveguide channel.) In other embodiments, the cavity of the waveguide channel (20) can have other shapes and dimensions.

[0042] Semiconductor barrier members. A semiconductor barrier member 30 is integral with the wafer 10. The barrier member 30 is disposed within the waveguide channel 20 (e.g., between an input port and an output port of the waveguide channel 20) such that the barrier member 30 impedes the transmission of an RF signal from the input port to the output port of the waveguide channel 20.

[0043] In the embodiment of FIG. 1A, the barrier member (30) is made of substantially pure silicon (Si), selected for its high resistivity and long carrier lifetime. <100> In other embodiments, the barrier member 30 may comprise another semiconductor material.

[0044] As will be appreciated by those skilled in the art, the electrical conductance of a semiconductor material increases with the energy level, i.e., photon frequency, of the electromagnetic radiation (ER) applied to the semiconductor material. The energy level of the applied electromagnetic radiation must be greater than the semiconductor band gap energy level in order to generate electron-hole pairs and increase the electrical conductance of the semiconductor material. As will be further appreciated by those skilled in the art, semiconductor materials also increase in electrical conductance with increasing intensity, i.e., power level, of the electromagnetic radiation applied to the semiconductor material (when the electromagnetic radiation frequency has an energy level above the semiconductor band gap energy). This is because increasing the power level increases the number of electron-hole pairs that are generated for a given energy level of the applied ER. Non-limiting examples of semiconductor materials suitable for forming the barrier member (30), as well as their band gap energies and corresponding wavelengths in parentheses, include the following: Silicon, Si (1.12 eV = 1107 nm), Germanium, Ge (0.661 eV = 1876 nm), Gallium Arsenide, GaAs (1.424 eV = 870.7 nm), Gallium Nitride, GaN (3.28 eV = 378 nm), Silicon Germanium, SeGe (0.66-1.86 eV = 665.6-1879 nm), Silicon Carbide, SiC (2.36-6 eV = 206.6-525.4 nm), Indium Phosphide, InP (1.344 eV = 922.5 nm), Gallium Phosphide, GaP (2.26 eV = 548.6 nm), and other silicon-based semiconductor materials. Others may also be selected, each with their own particular set of attributes. For example, one skilled in the art will appreciate that the electrical conductance of silicon can be increased by application of ER in the visible spectrum (wavelengths of about 400 to about 700 nm) as well as in the infrared spectrum (wavelengths of about 700 nm to about 1 mm). In contrast, gallium nitride has a band gap energy that is in the UV spectrum (wavelengths of about 10 nm to about 400 nm), and its electrical conductance can be increased by application of ER in the UV spectrum.

[0045] In the embodiment of Figure 1A, the barrier members (30) are in the form of substantially cylindrical posts that extend transversely (i.e., perpendicularly) to the planar direction defined by the wafer (10). In the embodiment of Figure 1A, the barrier members (30) extend from the metal layer (22) lining the inner wall of the wafer (10) to the window (40). In other embodiments, the barrier members (30) may have different forms, so long as the barrier members (30) provide an obstruction to the waveguide channel (20).

[0046] In the embodiment of FIGS. 1A and 1B, the barrier member (30) is preferably configured with a TE in order to maximize the isolation effect in the off state when the barrier member (30) is used as a switch, as described below. 1、0 The barrier member (30) is positioned approximately at the lateral center of the waveguide channel (20) across its width (W) (i.e., perpendicular to the direction of transmission of the RF signal from the input port to the output port), where the peak electric field of the mode is located. In other embodiments, the barrier member (30) can be at different locations within the waveguide channel (20). For example, the barrier member (30) can be offset from the lateral center of the waveguide channel (20) to optimize the amount of off-state isolation and on-state insertion loss for a particular design application.

[0047] The barrier member (30) may be monolithically constructed within the same material as the waveguide channel (20) and thus be completely integrated, or may be constructed from a separate material and subsequently assembled to the waveguide channel (20).

[0048] The barrier member (30) is customizable with respect to its position, size, and shape within the waveguide channel (20) for different design purposes, such as to improve impedance matching, to match the shape of the light source to improve efficiency, or to account for skin depth.

[0049] window. The window (40) is disposed on the outer surface of the wafer (10) and terminates the barrier member (30). In FIG. 1A, the wafer (10) is shown as being separate. In other embodiments, the wafer (10) may be integrated with an additional upper wafer (not shown) attached to a top surface of the wafer (10) or an additional lower wafer (not shown) attached to a bottom surface of the wafer (10) to form a stack of wafers for integrated circuit (IC) chips. In such embodiments, the top or bottom surface of the wafer (10) may still be considered the "outer surface" of the wafer (10), even though they do not form a terminating layer of the stack of wafers.

[0050] The window (40) includes an electromagnetic radiation (ER) transparent semiconductor layer terminating the barrier member (30), which allows electromagnetic radiation to be applied to the barrier member (30) by an ER emitter (100) external to the wafer. Thus, as used herein, "electromagnetic radiation transparent" or "ER transparent" refers to a semiconductor material that allows electromagnetic radiation in any portion of the electromagnetic spectrum, whether in the UV spectrum, the visible spectrum, or the infrared spectrum, i.e., having a wavelength between about 10 nm and about 1 mm, to be transmitted through the semiconductor material. In embodiments, the ER transparent semiconductor material may be optically transparent. As used herein, "optically transparent" refers to a semiconductor material that allows electromagnetic radiation in the visible spectrum (i.e., the portion of the electromagnetic spectrum having a wavelength between about 400 and about 700 nm) to be transmitted through the semiconductor material. In the embodiment of FIG. 1A, the optically transparent semiconductor material of the window (40) is silicon nitride, which may be advantageous for its anti-reflective (AR) properties. In other embodiments, the optically transparent semiconductor material of window (40) can be another material that not only provides AR properties at optical frequencies, non-limiting embodiments of which include indium tin oxide (ITO) or an optically transparent metal mesh film integrated into a semiconductor support, but also provides conductive properties to RF signals. In yet another embodiment, the ER transparent semiconductor of window (40) can include a grown or deposited layer of silicon dioxide, which would also have AR properties.

[0051] If the area of ​​the window (40) is sufficiently small and has a dimension (e.g., diameter) that is generally less than 1 / 12 (<λ / 12) of the wavelength (λ) of the RF signal transmitted through the waveguide, the window (40) is expected to have a negligible effect on the performance of the waveguide assembly. In an embodiment of the invention, the RF signal has a frequency of about 1 GHz to 300 GHz, or a wavelength of about 1 mm to about 300 mm. Thus, in an embodiment, the window dimension (e.g., diameter) may be about 0.083 mm to about 25 mm, or more specifically about 0.45 mm or less. However, it will be understood that these wavelengths assume that the RF signal travels through air as a dielectric in the waveguide. If instead the RF signal is transmitted through a semiconductor material with a higher dielectric constant in the waveguide, the wavelength will be reduced by a factor that is the inverse of the square root of the dielectric constant, which would therefore affect the preferred dimensions of the window (40).

[0052] In the embodiment of Figure 1A, the window (40) is recessed from the remainder of the outer surface of the wafer (10). The recess effectively forms a receptacle (18) or hole that receives a fiber optic cable (16) (as shown in Figure 5D) that optically couples the electromagnetic radiation emitted by the ER emitter (100) to the window (40).

[0053] Electromagnetic radiation (ER) emitter. The electromagnetic radiation (ER) emitter (100) is any device that emits electromagnetic radiation with energy greater than the band gap of the semiconductor material of the barrier member (30) to be excited. The particular wavelength of emitted ER to be selected will depend on the particular semiconductor material selected to form the barrier member (30). For example, if the semiconductor material of the barrier member is silicon (with a band gap wavelength of about 1100 nm), the ER emitter can be a laser that emits ER radiation at a wavelength of about 915 nm in the infrared spectrum. In embodiments, the ER emitter emits electromagnetic radiation in the UV spectrum (with wavelengths of about 10 nm to about 400 nm), the visible spectrum (with wavelengths of about 400 to about 700 nm), or the infrared spectrum (with wavelengths of about 700 nm to about 1 mm). Non-limiting examples of ER emitters (100) include light emitting diodes (LEDs), laser diodes that can emit ER in the visible or infrared spectrum, or vertical cavity surface emitting lasers (VCSELs).

[0054] In embodiments in which the ER emitter (100) is an LED, the LED may be integral with the wafer (10) by fabrication using microfabrication processes for semiconductor devices. In other embodiments, the ER emitter (100) may be formed separately and attached to the wafer (10). In yet other embodiments, the ER emitter (100) may be physically separate from the wafer (10) but optically coupled to the window (40) such as by a fiber optic cable (16) (see FIG. 5D).

[0055] In an embodiment, the ER emitter (100) is operatively connected to a control means (102) for selectively controlling one or both of the energy level or power of the electromagnetic radiation energy applied by the ER emitter (100) to the barrier member (30), thereby allowing selective control of the impedance effect of the barrier member (30) on the transmission of an RF signal through the waveguide channel (30), as described below. Suitable control means (102) are known to those skilled in the art, and non-limiting examples include, among others, a microcontroller, a variable resistor for controlling the power supplied to the ER emitter (100), a switch for selectively controlling one of multiple ER emitting elements of the ER emitter (100), a color tunable LED, and a tunable laser having a wavelength that can be changed in a controlled manner. In embodiments in which the waveguide assembly includes multiple barrier members (30), the control means may be configured to selectively vary the energy level (i.e., frequency) and / or intensity (i.e., power level) of the electromagnetic radiation applied to one of the barrier members (30) independently of the frequency and / or power level of the electromagnetic radiation applied to another one of the barrier members (30). For example, each barrier member (30) may be associated with a different one of the multiple ER emitters (100), which can be controlled with respect to energy level and / or power independently of the other ER emitters (100). Additionally, the control means may control the ER emitters (100) to be pulsed (e.g., to emit electromagnetic radiation intermittently) to improve thermal management of the wafer (10) as well as the ER emitters (100).

[0056] Use and principle of operation of barrier elements. In general, the energy level and / or power level of the electromagnetic radiation applied to the barrier member (30) by the ER emitter (100) may be selectively varied by the control means (102) to control the electromagnetic excitation of the barrier member (30) for the purpose of changing the electrical conductance of the barrier member (30) and thus changing the impedance of the barrier member (30) to the transmission of RF signals in the waveguide channel (20). This may be done for exemplary uses of the waveguide assembly such as switching, attenuating, routing, filtering, and transforming RF signals in the waveguide channel (30). The present invention is not limited by the frequency of the RF signal. In a non-limiting embodiment, the RF signal is within the millimeter wave band (about 1 GHz to about 300 GHz), more specifically, within the K a The frequency band may be within the range of about 26.5 GHz to about 40 GHz.

[0057] Figures 1B and 1C show the waveguide (20) and barrier member (30) (Si post) of the waveguide assembly of Figure 1A. Other parts of the wafer (10) shown in Figure 1A are omitted to illustrate the working principle of the waveguide assembly.

[0058] The attenuating effect of the barrier member (30) on the transmission of RF signals through the waveguide channel (20) can be controlled by the energy level (frequency) and / or power level of the electromagnetic radiation energy applied to the barrier member (30) by the electromagnetic radiation source (100). For ease of explanation, the following discussion describes the effect using the cases when the ER emitter (100) is "off" (e.g., not emitting electromagnetic radiation) and when it is "on" (i.e., emitting electromagnetic radiation). Intermediate effects can be produced by varying the intensity (power level) of the electromagnetic radiation emitted from the ER emitter (100) between different non-null energy levels and / or powers. Thus, if the energy level and / or power of the electromagnetic radiation emitted by the ER emitter (100) can be selectively controlled using the control means (102), the attenuating effect of the barrier member (30) on the transmission of RF signals in the waveguide channel (20) can be selectively, and possibly continuously, adjusted.

[0059] When the ER emitter (100) is "off," the barrier member (30) is in an insulating state compared to when the ER emitter (100) is "on." Stated another way, when the ER emitter (100) is "on," the barrier member (30) is in a conductive state compared to when the ER emitter (100) is "off." When the barrier member (30) is in an insulating state, the barrier member (30) allows microwave and millimeter-wave RF signals to pass from the input port to the output port of the waveguide channel (20) with low insertion loss. Thus, the barrier member (30) may be considered to be in an "on state." Conversely, when the barrier member (30) is in a conductive state, the barrier member (30) behaves like a shorting shunt within the waveguide channel (20) and reflects the incoming microwave and millimeter-wave RF signals, thus providing a relatively high isolation for the transmission of RF signals from the input port to the output port of the waveguide channel (20). Thus, the barrier member 30 may be considered to be in the "off state."

[0060] Specifically, as shown in FIG. 1C, photons emitted from the ER emitter (100) that pass through the window (40) are incident on the barrier member (30) and are absorbed by the barrier member (30). If the photons have sufficient energy (e.g., the energy is greater than the band gap of Si, hν>E g ≈1.12 eV), this will generate free carriers in the barrier member 30, which will change the barrier member 30 from a capacitive load to a conductive load, allowing the transmission or reflection of millimeter waves in the waveguide channel 20.

[0061] To relate the incident optical power at the top of the barrier member (30) to the photogenerated free carrier concentration, and hence to the bulk DC conductivity within the barrier member (30), the continuity and charge neutrality equations for the creation and recombination of electrons and holes in semiconductors are used [Ref. 11]. At steady state, when the spatial distribution of free carriers is constant, the continuity equation can be written as:

[0062] D eff ▽ 2 nn / τ eff +g=0 (1) where n is the total number of free carriers, D eff is the effective diffusion coefficient, τ eff is the effective carrier lifetime and g is the generation rate

[12] . As shown in FIG. 1C, when the optical excitation is perpendicular to the surface of the barrier member 30, the generation rate is

[0063]

number

[0064] Assuming a one-dimensional case with exponential decay in the direction, g can be expressed as g(y) = αP opt (1-R)λ opt e -αy / hc (2) where α is the absorption coefficient and R is the optical excitation wavelength λ opt Reflectivity of Si atopt is λ opt where h is the Planck constant and c is the free space velocity of light

[12] . opt Solving for the total carrier concentration, n, as a function of , the resulting bulk DC conductivity of the semiconductor can be calculated as:

[0065] σ DC =qμ eff n (3) Here, μ eff is the effective mobility of both electrons and holes, and q is the fundamental unit charge

[11] . To reduce the lateral diffusion of free carriers, the barrier member (30) is D =√(D eff τ eff ) which helps confine the free carriers within the region of the barrier member (30), justifying the 1D theoretical approach [Ref. 12].

[0066] The effect of increasing the conductivity of the barrier member (30) (Si post) shown in Figures 1B and 1C was simulated using HFSS™ (High Frequency Structure Simulator Software, available from Ansys, Inc., Canonsburg, Pennsylvania, USA). In Figure 2A, the on-state scattering parameters are shown without optical excitation, i.e., the semiconductor barrier member (30) is in a dark state where no light source is shining or incident on the surface. The barrier member (30) behaves as a shunt dielectric or capacitive load. Electromagnetic waves can pass through the waveguide channel (20).

[0067] In the particular embodiment shown in FIG. 2B, as the optical power incident on the top of the barrier member (30) is increased, the amount of off-state isolation increases, reaching a maximum at a conductivity of 350-400 S / m. Further increases in conductivity improve the total loss of the system. In other designs or embodiments, the amount of isolation achieved can be increased, decreased, or the same. When electromagnetic radiation is applied to the semiconductor barrier member (30) that is above the band gap energy of the semiconductor material, the barrier member (30) behaves as a conductor.

[0068] Thus, electromagnetic waves are mostly absorbed or reflected by the barrier member (30) depending on the amount of applied optical energy related to the realized value of electrical conductivity in the barrier member (30). By exciting the barrier member (30) with electromagnetic radiation of the correct photon energy (specific to the choice of semiconductor), a solid-state plasma can be formed, changing the electrical properties of the barrier member (30) from dielectric to conductive depending on the amount of applied electromagnetic radiation energy. As used herein, "solid-state plasma" refers to a solid-state substance with mobile charged particles. By carefully selecting the arrangement and design of the barrier member (30) or barrier members (30), the electric and magnetic fields in the waveguide channel (20) can be perturbed in customized and highly flexible ways, enabling a wide variety of tunable and reconfigurable transfer functions in single-port, double-port, or multi-port configurations. Advantages of the microwave and millimeter wave waveguide assemblies using solid-state plasmas described herein include high power handling, high linearity, fast switching speeds, low insertion loss, and virtually unlimited lifetime, all within a highly integrated form factor that can be combined with other planar or non-planar circuits and systems. Additionally, the DC bias network of the electromagnetic radiation control system (i.e., the ER emitter (100)) is isolated from the RF signal path, eliminating unwanted transients due to control voltage switching appearing at the input or output of the waveguide assembly, improving performance.

[0069] The off-state isolation provided by the barrier member (30) can be improved using one or more of the following methods. First, the size of the barrier member (30) can be increased, but at the expense of on-state insertion loss due to increased shunt capacitive loading. This increased shunt capacitive loading can be matched using techniques including T-matched and pi-matched switch networks to significantly improve on-state insertion loss. Second, the shape of the barrier member (30) can be configured in a specific way to improve off-state isolation. Third, additional barrier members (30) can be added to improve off-state isolation, keeping in mind the need to compensate for the increased on-state capacitive loading due to the pi-matched region.

[0070] As mentioned above, a T-match or π-match network can be used to match the shunt capacitive load of the on-state semiconductor barrier member (30) to improve insertion loss and return loss over a reasonable bandwidth. Details of the design of T-match and π-match networks are given in Reference 13 and their application in the present invention is described in the Examples below.

[0071] Fabrication of the Waveguide Assembly. The waveguide assembly is fabricated using microfabrication processes for semiconductor devices. In one embodiment, a method for manufacturing a waveguide assembly integrated with a semiconductor wafer (10) includes the following steps. For illustrative purposes, reference is made to FIG. 4, which is further described in the Examples below.

[0072] Initially, the method includes providing a first portion of the wafer 10 and a separate second portion of the wafer 10. In the example of Figure 4, the first portion of the wafer 10 is represented by the top wafer and the second portion of the wafer 10 is represented by the bottom wafer.

[0073] Next, the method includes etching an outer surface of the first portion of the wafer 10 to define a receptacle for the window 40. In the example of Figure 4, this step is shown as (step c).

[0074] Next, the method includes depositing a layer of optically transparent semiconductor material for the window 40. In the example of Figure 4, this step is shown as (step d). Next, the method includes etching an inner surface of the first portion of the wafer (10). The etching is performed to define walls of a waveguide channel (20) extending from an input port to an output port for an RF signal. Etching is also performed on an outer surface of the first portion of the wafer (10) to define a waveguide switch including a semiconductor barrier member (30) extending from a window (40) including an optically transparent semiconductor layer into the waveguide channel (20) between the input port and the output port of the waveguide channel (20). In the example of FIG. 4, this step is shown as (steps 1f, 1h, 1i).

[0075] Next, the method includes depositing a first metal layer on the inner surface of the first portion of the wafer 10 to line the walls of the waveguide channels 20. In the example of Figure 4, this step is shown as (Step 1j).

[0076] Next, the method includes etching the deposited first metal layer to expose the barrier member 30 to the waveguide channel 20. In the example of Figure 4, this step is shown as (Step 1l).

[0077] Next, the method includes depositing a second metal layer on the inner surface of the second portion of the wafer 10 to provide a metallized inner surface of the second portion of the wafer 10. In the example of Figure 4, this step is shown as (Step 2a).

[0078] Finally, the method includes bonding the first metal layer deposited on the inner surface of the first portion of the wafer 10 to the metallized inner surface of the second portion of the wafer 10. In the example of Figure 4, this step is shown as (Step 3). EXAMPLES

[0079] The following examples illustrate certain aspects of exemplary embodiments of the waveguide assembly, its fabrication, and its use as a waveguide switch, a waveguide variable attenuator, an evanescent mode bandpass filter waveguide switch, a tunable waveguide cavity resonator, an impedance matching network, and a distributed phase shifter. Further embodiments and uses are possible without departing from the scope of the claims.

[0080] Example 1 - Waveguide assembly layout. In Figures 3A and 3B, a layout for the microfabrication of the waveguide assembly is shown. All dimensions are in μm. The layout was chosen to operate in the Ka band with a total waveguide width of 7.112 mm (WR28). After a series of optimization studies using HFSS to achieve an isolation of over 20 dB, a 2x2 array of barrier members (30) (Si posts), each 400 μm in diameter, is placed in the waveguide channel (20) defined by the copper-containing metal layer (22). In other embodiments, more or fewer barrier members (30) can be added to the design to modify the performance of the waveguide assembly. In this embodiment, the circular cross-section of the barrier members (30) is chosen to match the circular cross-section of the optical fiber (16) (see Figure 5D) used to optically couple the ER emitter (100) to the window (40). This helps to ensure that the most photons from the output of the optical fiber (16) are captured by the barrier members (30). To ensure that the barrier members (30) (Si posts) become completely conductive upon photoexcitation, a diffusion length L D A height of 200 μm is chosen to fit within the 100 μm space defined by the 1000 μm spacing. This in turn determines the height of the waveguide channel (20) for this particular design. Furthermore, a π-switch configuration is chosen to improve matching due to the capacitive loading effect of the barrier members (30) (Si posts) in the on-state [Reference 13].

[0081] A high impedance section between the rows of barrier members (30) (Si posts) is created by providing slots 24 (labelled π-match) with a longitudinal length of 550 μm and a depth of 220 μm, thereby increasing the depth of the waveguide channel in this region.

[0082] As shown in Figure 3B, the top portion (12) of the wafer (10) is then flipped over and bonded to the bottom portion (14) of the wafer (10). Four optical fibers (16) inserted into receivers (18) (holes) etched into the backside of the top wafer directly above the barrier members (30) (Si posts) provide optical coupling of the ER emitters (100) for exciting the barrier members (30).

[0083] Example 2 - Process flow for fabrication of a waveguide assembly. Figure 4 shows the fabrication process of a waveguide assembly according to the layout shown in Figures 3A and 3B. Si micromachining using deep reactive-ion etching (DRIE) is chosen for its ability to achieve both small and large features with high precision [Reference 10]. The process begins with a 675 μm thick high resistivity intrinsic Si wafer having a 1.2 μm thermal oxide grown (step 1a) and patterned on both sides for top and backside DRIE masks (step 1b). Next, a receiving portion (18) for the optical fiber (16) is etched on the backside using DRIE (step 1c) and plasma-enhanced chemical vapor deposition (PECVD) nitride is deposited as an anti-reflective coating for the window (40) (step 1d). Next, AZ1529™ (MicroChemicals GmbH, Ulm, Germany) photoresist is patterned on top of the top oxide (step 1e) to achieve two different top etch depths, and high impedance pi-shaped alignment slots (24) are etched (step 1f). The resist is stripped (step 1g) and the main waveguide channels (20) are etched (step 1h). The top oxide mask is stripped (step 1i) to improve the electrical connection of the barrier members 30 (Si posts). The top waveguide channels are metallized (step 1j) by deposition of a sputtered 100 / 1000 nm Ti / Cu layer, and the metal from the sidewalls of the barrier members (30) (Si posts) is removed by patterning AZ1529™ photoresist (step 1k) and wet chemical etching (step 1l). Negative photoresist or image-reversed photoresist can be used instead of the positive photoresist AZ1529™ to pattern the sidewalls of the barrier members (30) (Si posts). Individual samples are then diced (step 1m).

[0084] Figure 5A is a photograph of the top wafer piece fabricated according to (steps 1a-1m) of the process flow in Figure 4, prior to the bonding step. Figure 5A shows the switch region including the waveguide channel (20) and four barrier members (30) (Si posts), as well as the back-to-back waveguide structure for switching loss extraction.

[0085] In this embodiment, a 1.1 mm thick borosilicate glass wafer was selected as the bottom carrier wafer. A 40 / 1000 nm Ti / Cu layer was patterned using MicroChem LOR 5B™ (MicroChem Corp., Newton, Massachusetts, USA) lift-off resist and AZ1512™ (MicroChemicals GmbH, Ulm, Germany) bilayer lift-off process, and individual samples were diced (step 2a).

[0086] Figure 5B is a photograph of the bottom wafer piece fabricated according to (step 2a) of the process flow of Figure 4 prior to the bonding step. Figures 5A and 5B show the coplanar waveguide-to-waveguide (CPW-waveguide) transition (32) region. The coplanar waveguide transition region houses the coplanar waveguide (31), an electrical planar transmission line that can be fabricated using printed circuit board technology and configured to carry microwave frequency signals.

[0087] Figure 5C is a photograph of the fabricated waveguide assembly after bonding the top and bottom wafer pieces according to the bonding step (step 3a) of Figure 4 using Cu-Cu thermocompression bonding, and shows the final dimensions of the waveguide assembly, including the location of the receiving portion (18) (hole) for the optical fiber (16) and the transition portion.

[0088] In summary, in this embodiment, the barrier members (30) (Si posts) are patterned into the waveguide channels (20) using deep reactive ion etching. The waveguide channels (20) are metallized using physical vapor deposition, and the metal coating on the barrier members (30) is removed using photolithography. A portion of the wafer (10) is bonded to another metallized carrier portion of the wafer (10) using thermocompression bonding to form a waveguide assembly in the wafer (10). The selection of silicon microfabrication process using deep reactive ion etching allows low-cost, high-precision fabrication with customizable designs of the waveguide channels (10) and barrier members (30) (Si posts) according to application needs, along with direct integration with other integrated circuits or systems. In other embodiments, other semiconductor microfabrication processes are also applicable, including anisotropic etching using potassium hydroxide (KOH) or tetramethyl ammonium hydroxide (TMAH). See also Reference 15 for other methods of anisotropic etching of silicon structures that may be applied to the method of the present invention.

[0089] Example 3 - Solid-state plasma switch or variable attenuator. Figure 5D is a photograph of a test setup of the waveguide communication assembly shown in Figure 5C to characterize the effect of a waveguide communication switch on the transmission of an RF signal in the CPW-waveguide communication region shown in Figure 5C. Figure 5D shows a wafer (10) with the waveguide communication assembly integrated as a device under test (DUT).

[0090] 5D shows a measurement probe (50) in which four optical fibers (16) are inserted into receptacles (18) (holes) located directly above the barrier member (30) (Si post). The ER emitter (not shown) is located at a wavelength λ 1 within the range of high quantum efficiency for Si. opt =915nm(hν opt =1.36 eV) [Reference 14].

[0091] FIG. 6 plots the measured and simulated scattering parameters when the waveguide assembly is in the "on state", i.e., when the barrier member (30) is not receiving any applied electromagnetic radiation. At 35 GHz, the measured insertion loss is 2.86 dB and the return loss is greater than 20 dB from 29.2 GHz to 41.6 GHz, both including the CPW-waveguide transition. To extract the transition loss, a back-to-back waveguide as shown in FIG. 5A was also measured and its scattering parameters are shown in the inset (a) of FIG. 6. Along with the measured back-to-back insertion loss of 2.34 dB at 35 GHz, the extracted loss of the switch itself is 0.52 dB, while the net effect of the switch element over the entire band from 30 GHz to 40 GHz is less than 0.88 dB.

[0092] FIG. 7 shows the measured isolation (|S 21 3, the measured isolation is 20 dB for an optical power of 50.1 mW, while the measured isolation is 25 dB for an optical power of 166.7 mW. This is a remarkable isolation for this frequency range and clearly demonstrates the feasibility of the waveguide assembly for millimeter-wave switch applications. These results are consistent with the operating principle described above: as the energy level of electromagnetic radiation applied to the barrier members (30) increases, their conductance increases. This increases the effectiveness of the barrier members (30) in reflecting the incoming microwave and millimeter-wave signals, thus providing higher isolation from the input port to the output port of the waveguide channel (20).

[0093] Figure 7 shows that as the optical power is increased, there is a saturation point where further increases in optical power no longer result in significant changes in isolation. Using equations (1)-(3) (above), the average DC bulk conductivity for 25 dB isolation is approximately 281 S / m. Increasing the optical power will further improve the total loss in the system by increasing the conductivity of the posts.

[0094] The result is that within the waveguide channel 20 of the semiconductor wafer 10, a The barrier member 30 has been demonstrated for use as a waveguide switch for RF signals in the band. The measured off-state isolation was greater than 20 dB over the entire band from 30 to 40 GHz. The measured extracted on-state insertion loss was 0.52 dB at 35 GHz. The waveguide switch is useful for switching millimeter wave signals in semiconductor microfabricated waveguides for communication or radar systems requiring high performance and high power handling.

[0095] The semiconductor barrier member (30) in the waveguide channel can be designed to adjust the optical power incident on the barrier member (30) so that the input impedance of the barrier member (30) matches the characteristic impedance of the waveguide channel (20). Thus, electromagnetic energy incident on the semiconductor barrier member (30) can be completely absorbed by the barrier member (30) in the off state, and only a very limited amount of power can be reflected or transmitted. Absorptive switches are useful in applications where high reflected power can damage upstream RF components or equipment.

[0096] Furthermore, by adjusting the amount of optical power incident on the semiconductor barrier member (30), a variable amount of off-state isolation can be achieved. Thus, a variable attenuator can be designed using the barrier member (30). Attenuators can be used in applications where the microwave or millimeter wave signal level needs to be controlled, i.e., where high signal levels need to be reduced to protect downstream components or equipment. Variable attenuators are extremely useful in applications where the signal level needs to be continuously changed, where the signal level needs to be continuously leveled, or even where the signal level needs to be changed only once infrequently, but where it is much cheaper not to replace the entire component, i.e., in the case of fixed attenuators.

[0097] Example 4 - T-matched solid-state plasma waveguide switch. Referring to FIG. 8A, a T-shaped matching circuit of the present invention can be constructed by inserting high impedance waveguide sections before and after the semiconductor barrier member (30). The high impedance section in the waveguide channel (20) can be realized by increasing the height of the waveguide wall in the desired section. It is known that the characteristic impedance of the waveguide channel (20) is proportional to the channel height [see Reference 16]. As known to those skilled in the art, "T-shaped matching" refers to an electric circuit used to match the impedance between two points, usually a source and a load, in which inductors and capacitors can be arranged in the shape of the letter "T" in the corresponding schematic diagram as shown in FIG. 8B.

[0098] The T-match helps improve the insertion loss and return loss for large shunt capacitive loads in the on-state of the solid-plasma barrier member 30 without substantially increasing the overall size of the barrier members 30 in the waveguide assembly or the number of barrier members 30. However, with a T-match, there exists a maximum shunt capacitive load that can be matched by a reasonable high impedance section.

[0099] Example 5 - Pi-matched solid-state plasma waveguide switch. As mentioned above, FIG. 3A shows a design layout of a waveguide assembly in which a high impedance pi-shaped matching section is placed between four barrier members (30) (silicon posts).

[0100] FIG. 9A shows another pi-matching circuit constructed by inserting a high impedance waveguide section between two barrier members (30) that act as a shunt capacitive load. To maximize the amount of off-state isolation, the impedance of the pi-matching should be matched to the characteristic impedance of the waveguide channel (20) with a length of about λ / 4. To reduce the length of the pi-matching section and the overall size of the waveguide assembly, the impedance of the pi-matching section can be increased by increasing the height of the lower wall of the waveguide channel (20) in the pi-matching section. This design will result in a smaller form factor of the switch, at the expense of a slightly reduced off-state isolation. Furthermore, compared to a T-matching circuit, for a given shunt capacitive load, the pi-matching circuit always has a solution. The pi-matching switch provides a wide on-state bandwidth with low insertion loss, and high off-state isolation. As known to those skilled in the art, a "π match" or "pi match" refers to an electrical circuit used to match impedance between two points, usually a source and a load, in which the inductors and capacitors may be arranged in the shape of the letter "π" in a corresponding schematic diagram such as that shown in FIG. 9B.

[0101] Example 6 - Single-pole n-throw solid-state plasma waveguide switch. Referring to FIG. 10, a single-pole N-throw solid-state plasma waveguide switch can be designed using the co-feed structure (see reference 17 for details) along with the proposed semiconductor barrier member (30). In FIG. 10, the co-feed structure splits the incident wave from port 1 into two separate paths toward ports 2 and 3 of the waveguide channel (20). Equal or unequal power division can be designed. A tuning stub (60) located between the two branches at ports 2 and 3 can be added to improve matching and bandwidth. In an embodiment, the tuning stub (60) can be patterned and coated with metal in the same way that the waveguide channel (20) sidewalls are coated with metal layer (22), or the tuning slab (60) can be a semiconductor barrier stimulated with electromagnetic radiation for tunable matching. A semiconductor barrier member (30) is placed in each path to enable switching of signals through each path. The placement and design of the semiconductor barrier members (30) can be optimized for on-state return loss and insertion loss, along with off-state isolation, according to the implementations previously described. Additional paths (arms or branches) or multiple corporate feed structures with semiconductor barrier members (30) can be utilized to increase the number of output ports from 2 (as shown in FIG. 10) to allowing N ports.

[0102] Example 7 - Evanescent mode bandpass filter waveguide switch. To significantly improve off-state isolation and increase DC power efficiency, an evanescent mode waveguide switch implementation can be utilized [see References 18 and 19].

[0103] Referring to FIG. 11A, the basic TE 1、0 A narrow waveguide section (26) of the waveguide channel (20) operating below the cutoff frequency of the mode (i.e. operating in an evanescent mode) is 1、0 It is inserted between two waveguide portions (28) of a waveguide channel (20) that operates above the cutoff frequency of the mode (ie, operates within the normal waveguide single mode region).

[0104] As shown in FIG. 11B, a waveguide operating below cutoff can be modeled as either a T-shaped section or a π-shaped section equivalent circuit with an inductive load. Furthermore, a semiconductor barrier member (30) in a waveguide channel (20) operating in a dark state (i.e., without electromagnetic radiation excitation) can be modeled as a capacitor in a shunt, as shown in FIG. 11C. By inserting a semiconductor barrier member (30) inside an evanescent mode waveguide section (26) as shown in FIG. 11A, its shunt capacitance is coupled in parallel with the shunt inductance shown in FIG. 11B to form a resonator element, as shown in the equivalent diagram of FIG. 11D. A series inductance can provide coupling between the resonators. Thus, a filtering transfer function can be formed between two standard waveguide sections (28). By adding multiple semiconductor barrier members (30), a multi-pole filter can be constructed as shown in FIG. 12A, with the equivalent circuit shown in FIG. 12B.

[0105] By exciting the semiconductor barrier member 30 with electromagnetic radiation, a solid-state plasma is formed, causing the barrier member 30 to become conductive and the waveguide to change from a filter to a switch, blocking the transmission of electromagnetic waves. Because the lateral width of the waveguide portion 26 is reduced, the amount of isolation provided by the barrier member 30 is increased compared to a barrier member 30 of the same size in a larger main waveguide portion 28, because the barrier member 30 blocks more of the incident electromagnetic wave. Additionally, the high attenuation of evanescent modes in the narrow waveguide portion 26 also improves the amount of isolation achieved by the switch.

[0106] The advantages of solid-state plasma switching elements over PIN diodes are simple integration, decoupled DC bias network, higher power handling, and lower insertion loss.

[0107] Example 8 - Optically tunable and reconfigurable solid-state plasma waveguide resonator. In this example, inside the (either rectangular or cylindrical) waveguide channel (20) cavity, a semiconductor barrier member (30) can be utilized in which a solid-state plasma is excited by electromagnetic radiation to tune the resonant frequency of the cavity, to tune the input / output coupling from the cavity, or to tune the inter-resonator coupling between two cavities, i.e., for a bandpass filter response.

[0108] As an example of an embodiment, referring to FIGS. 13A and 13B, a semiconductor barrier member (30) is placed in a cylindrical waveguide channel (20) cavity. Here, the barrier member (30) is positioned in the center of the cavity to maximize tunability. However, the selection of the location of the barrier member (30) can be changed based on design requirements to optimize the amount of coupling to the resonant electric or magnetic field located inside the cavity. With the semiconductor barrier member (30) in a dark state (i.e., in the absence of electromagnetic radiation excitation), the cavity will be inductively loaded by the barrier member (30) and its fundamental resonant mode will be at a specific frequency. When the semiconductor barrier member (30) is excited by electromagnetic radiation to generate a solid-state plasma inside, the electric or magnetic field in the waveguide channel (20) cavity will reorient based on the new boundary condition introduced by the conductive barrier member (30) at that time, and the fundamental resonant frequency will shift. Thus, tuning of the waveguide cavity resonant frequency can be achieved.

[0109] As another example of the embodiment, referring to FIG. 14, the semiconductor barrier members (30) inserted inside the waveguide channel (20) can be used as reconfigurable sidewalls of the waveguide cavity resonator. As shown in FIG. 14, a rectangular waveguide channel (20) cavity has four semiconductor barrier members (30) arranged to electrically form new sidewalls of the waveguide channel (20) when excited by electromagnetic radiation to form a solid-state plasma, thus changing the resonant length of the waveguide channel (20) cavity and its fundamental resonant frequency. A different shape of the waveguide channel (20) cavity, i.e., a cylindrical waveguide cavity, can also be applied to this embodiment. Furthermore, the size, number, and shape of the semiconductor barrier members (30) can be optimized for a specific design application.

[0110] Example 9 - Optically tuned solid-state plasma waveguide impedance matching network and phase shifter. In FIG. 15, the waveguide channel (20) includes a short-circuited waveguide stub path (29) that extends away from the primary path (27) from port 1 to port 2. The stub path (29) can be used to tune the input and output impedance of the waveguide channel (20) portion, thus creating a tunable or reconfigurable impedance matching network. For example, in FIG. 15, by placing a semiconductor barrier member (30) at the input to the H-plane short-circuited waveguide stub path (29), the input impedance of the stub path (29) can be reconfigured, thus changing the input / output impedance looking into the waveguide ports 1 and 2. Additional stub paths (29) (not shown) can be added to create double-stub, triple-stub, or multi-stub impedance matching networks.

[0111] Referring to FIG. 16, multiple semiconductor barrier members (30) can be positioned at different lengths along the shorted waveguide stub path (29), thereby reconfiguring the amount of input impedance seeing into the waveguide stub path (29) and allowing for additional tuning states.

[0112] A distributed waveguide phase shifter can be designed by utilizing multiple reconfigurable solid-state plasma short-circuit waveguide stub paths (29) loaded on the waveguide section. Electromagnetic excitation of the semiconductor barrier members (30) in each waveguide stub path (29) will shift the amount of phase of the transmission coefficient between port 1 and port 2 to some extent as designed, as shown in FIG. 15. By switching different stubs (29) on or off, an increasing or decreasing amount of phase change can be produced. Furthermore, the amount of phase change introduced by a single stub (29) can be tuned by using multiple semiconductor barrier members (30), as shown in FIG. 16.

[0113] Using the solid-state plasma switching elements of the present invention, other types of waveguide phase shifter topologies can be realized, including reflective phase shifters and switched-line phase shifters. interpretation.

[0114] Corresponding structures, materials, acts, and equivalents of all means or step and functional elements recited in the claims appended hereto are intended to include any structure, materials, acts for performing the function in combination with other elements that are specifically claimed.

[0115] References herein to "one embodiment," "an embodiment," and the like indicate that the described embodiment may include a particular aspect, feature, structure, or characteristic, but not all embodiments necessarily include that aspect, feature, structure, or characteristic. Moreover, such phrases may, but do not necessarily, refer to the same embodiment as mentioned elsewhere in this specification. Moreover, when a particular aspect, feature, structure, or characteristic is described in connection with an embodiment, it is within the knowledge of one of ordinary skill in the art to use or combine such module, aspect, feature, structure, or characteristic in other embodiments, whether or not explicitly described. In other words, any module, element, or function can be combined with any other element or function of different embodiments, unless there is an obvious or inherent incompatibility or is specifically excluded.

[0116] Further, it should be noted that the claims may be drafted to exclude optional elements. Thus, this statement is intended to serve as a predicate for the use of exclusive terms such as "solely," "only," and the like in connection with the recitation of claim elements or the use of a "negative" limitation. The terms "preferably," "preferred," "preferred," "optionally," "may," and similar terms are used to indicate that a stated item, condition, or step is an optional (but not required) feature of the invention.

[0117] The singular forms "a," "an," and "the" include plural references unless the context clearly dictates otherwise. The term "and / or" means any one of the items, any combination of the items, or the items as a whole with which the term is associated. The phrase "one or more" is readily understood by those of ordinary skill in the art, especially when read in the context of its usage.

[0118] The term "about" may refer to a variation of ±5%, ±10%, ±20%, or ±25% of the specified value. For example, "about 50" percent may have a variation of 45-55 percent in some embodiments. With respect to integer ranges, the term "about" may include one or two integers greater than and / or less than the recited integer at each end of the range. Unless otherwise indicated herein, the term "about" is intended to include values ​​and ranges near the recited range that are equivalent in terms of the functionality of the composition or embodiment.

[0119] As will be understood by those skilled in the art, for any and all purposes, particularly in terms of providing a written description, all ranges recited herein also encompass any and all possible subranges and combinations of those subranges, as well as the individual values, particularly integer values, that make up the range. A recited range includes each specific value, integer, fractional, or identical value within the range. Any range described can be readily recognized as being capable of dividing the same range into at least equal halves, thirds, quarters, fifths, tenths, etc. As a non-limiting example, each range described herein above can be readily divided into a lower third, middle third, upper third, etc.

[0120] Additionally, as will be appreciated by those of skill in the art, language such as "up to," "at least," "greater than," "less than," "more than," "or more than," and the like, is inclusive of all recited numbers, and such terms refer to ranges that can be subsequently divided into subranges, as discussed above. Similarly, any ratio recited herein includes all sub-ratios falling within the broader ratio.

[0121] References The following publications are referenced herein as indicated by the following reference numbers: 1. U. Shah et al., “A 500-750 GHz RF MEMS waveguide switch”, IEEE Trans. Terahertz Sci. Technol, vol. 7, no. 3, pp. 326-334, May 2017. 2. “QuinStar Technology Inc.”, [Online], [Searched on February 1, 2021], Internet <URL:https: / / quinstar.com / shop / control-products-ferrite / waveguide-pin-switches-single-33 double-throw / waveguide-pin-switches-double-throw-qss-qsd / > 3. D. Psychogiou et al., “Millimeter- wave phase shifter based on waveguide-mounted RF-MEMS”, Microw. Opt. Technol. Lett., vol. 55, no. 3, pp. 465-468, Mar. 2013. 4. N. Vahabisani and M. Daneshmand, “Monolithic millimeter-wave MEMS waveguide switch”, IEEE Trans. Microw. Theory Tech., vol. 63, no. 2, pp. 340- 351, Feb. 2015. 5. C. H. Chen and D. Peroulis, “RF design, power handling, and hot switching of waveguide water-based absorptive switches”, IEEE Trans. Microw. Theory Tech., vol. 57, no. 1, pp. 2038-2046, Aug. 2009. 6.C. Gamlath, D. Benton, and M. Cryan,“Microwave properties of an inhomogeneous optically illuminated plasma in a microstrip gap”,IEEE Trans. Microw. Theory Tech., vol. 63, no. 2, pp. 374-383, Feb. 2015. 7.C. H. Lee, P. S. Mak, and A. P. Defonzo,“Optical Control of Millimeter-Wave Propagation in Dielectric Waveguides”,IEEE J. Quantum Electron., vol. 16, no. 3, pp. 277-288, 1980. 8.A. W. Pang, C. D. Gamlath, and M. J. Cryan,“An optically controlled coplanar waveguide millimeter- wave switch”,IEEE Microw. Wirel. Components Lett., vol. 28, no. 8, pp. 669-671, 2018. 9. J. Ren, Z. Jiang, P. Fay, J. L. Hesler, C. Y. E. Tong, and L. Liu,“High-performance WR-4.3 optically controlled variable attenuator with 60-dB range”,IEEE Microw. Wirel. Components Lett., vol. 28, no. 6, pp. 512-514, Jun. 2018. 10. A. Krivovitca, U. Shah, O. Glubokov, and J. Oberhammer, “Micromachined silicon-core substrate-integrated waveguides at 220-330 GHz”, IEEE Trans. Microw. Theory Tech., vol. PP, pp. 1-9, 2020. 11.DA Neamen, Semiconductor Physics and Devices: Basic Principles, 4th ed. New York: McGraw-Hill, 2012. 12. A. Kannegulla, MI Bin Shams, L. Liu, and L.-J. Cheng, “Photo-induced spatial modulation of THz waves: opportunities and limitations”, Opt. Express, vol. 23, no. 25, pp. 32098-32112, Dec. 2015. 13.GM Rebeiz, RF MEMS Theory, Design, and Technology. Hoboken, NJ: John Wiley & Sons, Inc., 2003. 14, SM Sze, Semiconductor Devices: Physics and Technology, 2nd ed. New York: John Wiley & Sons, Inc., 2002. 15. U.S. Patent No. 6,531,068, entitled “Method of anisotropic etching of silicon”, issued March 11, 2003, by Laermer et al. 16.PA Rizzi, Microwave Engineering: Passive Circuits. Englewood Cliffs, NJ: Prentice Hall, 1998. 17.S. H. Shehab, N. C. Karmakar, and J. Walker,“Substrate-integrated- waveguide power dividers”,IEEE Antennas Propag. Mag., vol. 62, no. 4, pp. 27-38, Aug. 2020. 18.G. F. Craven and C. K. Mok,“The design of evanescent mode waveguide bandpass filters for a prescribed insertion loss characteristic”,IEEE Trans. Microw. Theory Tech., vol. 19, no. 3, pp. 295-308, Mar. 1971. 19.T. Sickel, P. Meyer, and P. W. Van Der Walt,“An in situ tunable diode mounting topology for high-power X-band waveguide switches”,IEEE Trans. Microw. Theory Tech., vol. 55, no. 2, pp. 281-285, 2007. 20.Z. Baghchehsaraei and J. Oberhammer,“Parameter analysis of millimeter-wave waveguide switch based on a MEMS-reconfigurable surface”,IEEE Transactions on Microwave Theory and Techniques, vol. 61, no. 12, pp. 4396-4406, Dec 2013. 21.L. Pelliccia, F. Cacciamani, P. Farinelli, and R. Sorrentino,“High-Q tunable waveguide filters using ohmic RF MEMS switches”,IEEE Transactions on Microwave Theory and Techniques, vol. 63, no. 10, pp.3381-3390, Oct 2015. 22.J. Campion, Y. Li, H. Zirath, J. Oberhammer, A. Hassona, Z. S. He, B. Beuerle, A. Gomez-Torrent, U. Shah, S. Vecchiattini, R. Lindman, and T. S. Dahl,“Toward industrial exploitation of THz frequencies: integration of SiGe MMICs in silicon- micromachined waveguide systems”,IEEE Transactions on Terahertz Science and Technology, vol. 9, no. 6, pp. 624-636, Nov 2019. 23.A. W. Pang, S. Bensmida, and M. J. Cryan,“Nonlinearity and Power Handling Characterization of an Optically Reconfigurable Microwave Switch”,in IEEE MTT-S International Microwave Symposium Digest, Philadelphia, PA, Jun 2018, pp. 420-422. 24.E. K. Kowalczuk, C. J. Panagamuwa, and R. D. Seager,“Design and operation influences regarding rise and fall time of a photoconductive microwave switch”,in Loughborough Antennas and Propagation Conference, LAPC, Loughborough, UK, Nov 2013, pp. 149-154. 25.A. Fisher, Z. Missen, T. Jones, and D. Peroulis,“A fiber-free DC-7GHz W integrated semiconductor plasma switch”,in IEEE International Microwave Symposium, IMS, Atlanta, GA, Jun 2021, pp. 1-4.

Claims

1. 1. A system for intercepting radio frequency (RF) signals, the system including a waveguide assembly integrated with a semiconductor wafer; (a) a waveguide channel defined by an inner wall of a wafer lined with a metal layer, the waveguide channel including at least one port for transmitting an RF signal into and out of the waveguide channel; (b) at least one semiconductor barrier member disposed within the waveguide channel, the at least one semiconductor barrier member changing a waveguide electrical conductance of the barrier member in response to applied electromagnetic radiation, thereby changing an electrical impedance of the barrier member to transmission of RF signals through the waveguide channel; A system including:

2. The system of claim 1 , wherein the waveguide channel has a substantially rectangular prism shape.

3. The system of claim 1 , wherein the waveguide channel has a substantially cylindrical shape.

4. 4. The system of claim 1, wherein the waveguide channel comprises a first waveguide channel portion and a second waveguide channel portion, the channel height of the first waveguide channel portion being greater than the channel height of the second waveguide channel portion such that an electrical impedance of the first waveguide channel portion is greater than an electrical impedance of the second waveguide channel portion.

5. 4. The system of claim 1, wherein the waveguide channel includes a third waveguide channel portion, a fourth waveguide channel portion, and a fifth waveguide channel portion, the third waveguide channel portion being disposed between the fourth waveguide channel portion and the fifth waveguide channel portion, a lateral channel width of the third waveguide channel portion being less than lateral channel widths of the fourth and fifth waveguide channel portions, and at least one barrier member being disposed within the third waveguide channel portion.

6. 4. The system of claim 1, wherein at least one output port of the waveguide channel comprises a single port.

7. A system according to any one of claims 1 to 3, comprising: (a) the at least one port of the waveguide channel includes an input port, a first output port, and a second output port spaced apart from the first output port; (b) the waveguide channel defines a first path from the input port to the first output port; (c) the waveguide channel defines a second path from the input port to the second output port, the second path being separate from the first path; (d) the at least one barrier member comprises a first barrier member disposed in the first passage and a second barrier member disposed in the second passage. A system including:

8. The system of claim 7 , wherein the waveguide assembly further comprises a tuning stub disposed between the first path and the second path.

9. A system according to any one of claims 1 to 3, comprising: (a) the at least one port of the waveguide channel includes an input port and an output port; (b) the waveguide channel defines a first path from the input port to the output port and a short stub path extending from the first path; (c) the at least one barrier member is disposed within a stub path.

10. The system of claim 9 , wherein the at least one barrier member comprises a plurality of barrier members disposed within the stub path.

11. The system of claim 10 , wherein the at least one barrier member comprises a plurality of barrier members arranged in a row aligned along a length of the stub path.

12. The system of claim 1 , wherein the metal layer comprises gold, nickel, aluminum, chromium, tungsten, platinum, or silver.

13. 4. The system of claim 1, wherein the barrier member comprises silicon, germanium, gallium arsenide, gallium nitride, silicon germanium, silicon carbide, indium phosphide, or gallium phosphide.

14. The system of claim 1 , wherein the inner walls defining the waveguide channel and the barrier member comprise the same semiconductor material.

15. The system of claim 1 , wherein the inner walls defining the waveguide channel and the barrier member comprise different semiconductor materials.

16. The system of claim 1 , wherein the barrier member extends from a metal layer lining the inner wall of the wafer to the window.

17. The system of claim 1 , wherein the barrier members are in the form of posts extending perpendicular to a plane defined by the wafer.

18. The system of claim 17 , wherein the post has a substantially circular cross-sectional shape.

19. The system of claim 1 , wherein the at least one barrier member comprises a plurality of barrier members arranged in a row or array.

20. 4. The system of claim 1, wherein the waveguide assembly further comprises a window comprising an electromagnetic radiation (ER) transparent semiconductor layer terminating the barrier member to allow excitation of the barrier member by applied electromagnetic radiation emitted from an external source to the wafer.

21. 21. The system of claim 20, wherein the ER transparent semiconductor layer comprises silicon nitride, silicon dioxide, indium tin oxide, or a transparent metal mesh membrane embedded in a semiconductor substrate.

22. 21. The system of claim 20, wherein the window has a diameter of about 0.083 mm to about 0.450 mm and / or has a diameter less than 1 / 12 of the wavelength (λ) of the applied electromagnetic radiation.

23. 21. The system of claim 20, wherein the window is recessed from a peripheral outer surface of the wafer.

24. 4. The system of claim 1, further comprising an electromagnetic radiation (ER) emitter for emitting the applied electromagnetic radiation.

25. 25. The system of claim 24, wherein the ER emitter comprises a light emitting diode (LED), a laser diode, or a vertical cavity surface emitting laser (VCSEL).

26. 25. The system of claim 24, wherein the ER emitter is configured to emit electromagnetic radiation in the UV spectrum, the visible spectrum, or the infrared spectrum.

27. 25. The system of any one of claims 24, further comprising an optical fiber for optically coupling electromagnetic radiation emitted by the ER emitter to the barrier member.

28. 4. The system according to any one of claims 1 to 3, further comprising control means comprising a microcontroller, a switch or a variable resistor operably connected to the electromagnetic radiation ER emitter and configured to selectively control either a frequency or a power level or both of the electromagnetic radiation emitted by the ER emitter.

29. 30. The system of claim 28, wherein the control means is configured to vary a frequency of electromagnetic radiation emitted by the ER emitter.

30. 30. The system of claim 28, wherein the control means is configured to vary a power level of electromagnetic radiation emitted by the ER emitter.

31. 4. The system of claim 1, wherein the waveguide channel is a space between the metal layers lining the inner walls defining the waveguide channel that is free of semiconductor material, except for the semiconductor material of the barrier member.

32. 4. The system of claim 1, wherein the waveguide channel includes semiconductor material between the metal layers lining inner walls defining the waveguide channel, the semiconductor material being exclusive of the barrier member semiconductor material.

33. 1. A method for varying impedance to transmission of a radio frequency (RF) signal through a waveguide channel defined within a semiconductor wafer, the method comprising: (a) providing at least one semiconductor barrier member disposed within the waveguide channel; (b) selectively varying either a frequency or a power level, or both, of electromagnetic radiation applied to the at least one barrier member to change an electrical conductance of the barrier member, thereby varying an impedance of the at least one barrier member to transmission of the RF signal through the waveguide channel; The method includes:

34. 34. The method of claim 33, wherein the RF signal has a frequency in the range of about 1 GHz to about 300 GHz.

35. 35. The method of claim 34, wherein the RF signal is in the Ka band having a frequency ranging from about 26.5 GHz to about 40 GHz.

36. 36. The method of any one of claims 33 to 35, wherein varying either an energy level or a power level or both of the electromagnetic radiation applied by the ER emitter to the at least one barrier member results in an insertion loss of at least 20 dB between the input port and the output port.

37. 36. The method of any one of claims 33 to 35, wherein selectively varying a power level of electromagnetic radiation applied by the ER emitter comprises varying an intensity of emitted electromagnetic radiation between a null power level and a non-null power level.

38. 36. The method of any one of claims 33 to 35, wherein selectively varying a power level of the electromagnetic radiation applied by the ER emitter comprises varying a power level of the emitted electromagnetic radiation between a first non-null power level and a second non-null power level different from the first non-null power level.

39. 36. The method of any one of claims 33 to 35, (a) the at least one obstacle member includes a first obstacle member and a second obstacle member; (b) selectively varying either a frequency or a power level, or both, of the electromagnetic radiation applied by the ER emitter to the at least one barrier member selectively varying either a frequency or a power level, or both, of the electromagnetic radiation applied to the first barrier member independently of selectively varying either a frequency or a power level, or both, of the electromagnetic radiation applied to the second barrier member. The method includes:

40. 36. The method of any one of claims 33 to 35, wherein the electromagnetic radiation applied by the ER emitter is in the UV spectrum, the visible spectrum, or the infrared spectrum.

41. 1. A method of manufacturing a waveguide assembly for blocking radio frequency (RF) signals, the waveguide assembly being integrated with a semiconductor wafer, the method comprising: (a) providing a first portion of the wafer and a separate second portion of the wafer; (b) etching an interior surface of the first portion of the wafer, (i) a wall of a waveguide channel including at least one port for transmitting said RF signal into and out of said waveguide channel; (ii) a semiconductor barrier member disposed within the waveguide channel; and etching to define (c) depositing the first metal layer on the interior surface of the first portion of the wafer to lining the walls of the waveguide channel; (d) bonding the first metal layer deposited on the inner surface of the first portion of the wafer to a metallized inner surface of the second portion of the wafer; The method includes:

42. 42. The method of claim 41 further comprising, after step (c) and before step (d), etching the deposited first metal layer to expose the obstruction member to the waveguide channel.

43. 43. The method of claim 41 or 42, further comprising, after step (a) and before step (d), depositing the second metal layer on the inner surface of the second portion of the wafer to provide a metallized inner surface of the second portion of the wafer.

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