Abstract: A layer of amorphous Ge is formed on a substrate using electron-beam evaporation. The evaporation is performed at room temperature. The layer of amorphous Ge has a thickness of at least 50 nm and a purity of at least 90% Ge. The substrate is complementary metal-oxide-semiconductor (CMOS) compatible and is transparent at Long-Wave Infrared (LWIR) wavelengths. The layer of amorphous Ge can be used as a waveguide in chemical sensing and data communication applications. The amorphous Ge waveguide has a transmission loss in the LWIR of 11 dB/cm or less at 8 ?m.

Abstract: Disclosed is a method of facilitating straining of a semiconductor element (331) for semiconductor fabrication. In a described embodiment, the method comprises: providing a base layer (320) with the semiconductor element (331) arranged on a first base portion (321) of the base layer (320), the semiconductor element (331) being subjected to a strain relating to a characteristic of the first base portion (321); and adjusting the characteristic of the first base portion (321) to facilitate straining of the semiconductor element (331).

Abstract: A layer of amorphous Ge is formed on a substrate using electron-beam evaporation. The evaporation is performed at room temperature. The layer of amorphous Ge has a thickness of at least 50 nm and a purity of at least 90% Ge. The substrate is complementary metal-oxide-semiconductor (CMOS) compatible and is transparent at Long-Wave Infrared (LWIR) wavelengths. The layer of amorphous Ge can be used as a waveguide in chemical sensing and data communication applications. The amorphous Ge waveguide has a transmission loss in the LWIR of 11 dB/cm or less at 8 ?m.

Abstract: A layer of amorphous Ge is formed on a substrate using electron-beam evaporation. The evaporation is performed at room temperature. The layer of amorphous Ge has a thickness of at least 50 nm and a purity of at least 90% Ge. The substrate is complementary metal-oxide-semiconductor (CMOS) compatible and is transparent at Long-Wave Infrared (LWIR) wavelengths. The layer of amorphous Ge can be used as a waveguide in chemical sensing and data communication applications. The amorphous Ge waveguide has a transmission loss in the LWIR of 11 dB/cm or less at 8 ?m.

Abstract: Optical interconnects can offer higher bandwidth, lower power, lower cost, and higher latency than electrical interconnects alone. The optical interconnect system enables both optical and electrical interconnection, leverages existing fabrication processes to facilitate package-level integration, and delivers high alignment tolerance and low coupling losses. The optical interconnect system provides connections between a photonics integrated chip (PIC) and a chip carrier and between the chip carrier and external circuitry. The system provides a single flip chip interconnection between external circuitry and a chip carrier using a ball grid array (BGA) infrastructure. The system uses graded index (GRIN) lenses and cross-taper waveguide couplers to optically couple components, delivers coupling losses of less than 0.5 dB with an alignment tolerance of ±1 ?m, and accommodates a 2.5× higher bandwidth density.

Abstract: Optical interconnects can offer higher bandwidth, lower power, lower cost, and higher latency than electrical interconnects alone. The optical interconnect system enables both optical and electrical interconnection, leverages existing fabrication processes to facilitate package-level integration, and delivers high alignment tolerance and low coupling losses. The optical interconnect system provides connections between a photonics integrated chip (PIC) and a chip carrier and between the chip carrier and external circuitry. The system provides a single flip chip interconnection between external circuitry and a chip carrier using a ball grid array (BGA) infrastructure. The system uses graded index (GRIN) lenses and cross-taper waveguide couplers to optically couple components, delivers coupling losses of less than 0.5 dB with an alignment tolerance of ±1 ?m, and accommodates a 2.5× higher bandwidth density.

Abstract: An integrated optical modulator array useful for modulating light at different wavelengths in the same optical band includes multiple GeSi waveguides on a substrate. Each GeSi waveguide has a different width and is coupled to electrodes to form an electro-absorption modulator. A stressor material, such as SiN, disposed between the GeSi waveguides in the optical modulators applies a strain to the GeSi waveguides. Because each GeSi waveguide has a different width, it experiences a different strain. This difference can be a difference in magnitude, type (homogeneous v. inhomogeneous, compressive v. tensile), or both. The different strains shift the bandgaps of the Ge in the GeSi waveguides by different amounts, shifting the optical absorption edges for the GeSi waveguides by different amounts. Put differently, the stressor layer strains each GeSi modulator differently, causing each GeSi modulator to operate at a different wavelength.

Abstract: In a method for electrically doping a semiconducting material, a layer of germanium is formed having a germanium layer thickness, while in situ incorporating phosphorus dopant atoms at a concentration of at least about 5×1018 cm?3 through the thickness of the germanium layer during formation of the germanium layer. Additional phosphorus dopant atoms are ex situ incorporated through the thickness of the germanium layer, after formation of the germanium layer, to produce through the germanium layer thickness a total phosphorus dopant concentration of at least about 2×1019 cm?3.

Abstract: A layer of amorphous Ge is formed on a substrate using electron-beam evaporation. The evaporation is performed at room temperature. The layer of amorphous Ge has a thickness of at least 50 nm and a purity of at least 90% Ge. The substrate is complementary metal-oxide-semiconductor (CMOS) compatible and is transparent at Long-Wave Infrared (LWIR) wavelengths. The layer of amorphous Ge can be used as a waveguide in chemical sensing and data communication applications. The amorphous Ge waveguide has a transmission loss in the LWIR of 11 dB/cm or less at 8 ?m.

Abstract: An integrated optical modulator array useful for modulating light at different wavelengths in the same optical band includes multiple GeSi waveguides on a substrate. Each GeSi waveguide has a different width and is coupled to electrodes to form an electro-absorption modulator. A stressor material, such as SiN, disposed between the GeSi waveguides in the optical modulators applies a strain to the GeSi waveguides. Because each GeSi waveguide has a different width, it experiences a different strain. This difference can be a difference in magnitude, type (homogeneous v. inhomogeneous, compressive v. tensile), or both. The different strains shift the bandgaps of the Ge in the GeSi waveguides by different amounts, shifting the optical absorption edges for the GeSi waveguides by different amounts. Put differently, the stressor layer strains each GeSi modulator differently, causing each GeSi modulator to operate at a different wavelength.

Abstract: Disclosed is a method of facilitating straining of a semiconductor element (331) for semiconductor fabrication. In a described embodiment, the method comprises: providing a base layer (320) with the semiconductor element (331) arranged on a first base portion (321) of the base layer (320), the semiconductor element (331) being subjected to a strain relating to a characteristic of the first base portion (321); and adjusting the characteristic of the first base portion (321) to facilitate straining of the semiconductor element (331).

Abstract: A method of manufacturing a germanium-on-insulator substrate is disclosed, comprising: (i) doping a first portion of a germanium layer with a first dopant to form a first electrode, the germanium layer arranged with a first semiconductor substrate; (ii) forming at least one layer of dielectric material adjacent to the first electrode to obtain a combined substrate; (iii) bonding a second semiconductor substrate to the layer of dielectric material and removing the first semiconductor substrate from the combined substrate to expose a second portion of the germanium layer with misfit dislocations; (iv) removing the second portion of the germanium layer to enable removal of the misfit dislocations and to expose a third portion of the germanium layer; and (v) doping the third portion of the germanium layer with a second dopant to form a second electrode. The electrodes are separated from each other by the germanium layer, and the first dopant is different to the second dopant.

Abstract: A method of forming an integrated circuit is disclosed. The method includes: (i) forming at least a pair of optoelectronic devices from at least a first wafer material arranged on a semiconductor substrate, the first wafer material different to silicon; (ii) etching the first wafer material to form a first recess to be filled with a second material; (iii) processing the second material to form a waveguide for coupling the pair of optoelectronic devices to define an optical interconnect; and (iv) bonding at least one partially processed CMOS device layer having at least one transistor to the second semiconductor substrate to form the integrated circuit, the partially processed CMOS device layer arranged adjacent to the optical interconnect. An integrated circuit is also disclosed.

Abstract: A method of manufacturing a germanium-on-insulator substrate is disclosed, comprising: (i) doping a first portion of a germanium layer with a first dopant to form a first electrode, the germanium layer arranged with a first semiconductor substrate; (ii) forming at least one layer of dielectric material adjacent to the first electrode to obtain a combined substrate; (iii) bonding a second semiconductor substrate to the layer of dielectric material and removing the first semiconductor substrate from the combined substrate to expose a second portion of the germanium layer with misfit dislocations; (iv) removing the second portion of the germanium layer to enable removal of the misfit dislocations and to expose a third portion of the germanium layer; and (v) doping the third portion of the germanium layer with a second dopant to form a second electrode. The electrodes are separated from each other by the germanium layer, and the first dopant is different to the second dopant.

Abstract: In a method for electrically doping a semiconducting material, a layer of germanium is formed having a germanium layer thickness, while in situ incorporating phosphorus dopant atoms at a concentration of at least about 5×1018 cm?3 through the thickness of the germanium layer during formation of the germanium layer. Additional phosphorus dopant atoms are ex situ incorporated through the thickness of the germanium layer, after formation of the germanium layer, to produce through the germanium layer thickness a total phosphorus dopant concentration of at least about 2×1019 cm?3.

Abstract: A method of forming an integrated circuit is disclosed. The method includes: (i) forming at least a pair of optoelectronic devices from at least a first wafer material arranged on a semiconductor substrate, the first wafer material different to silicon; (ii) etching the first wafer material to form a first recess to be filled with a second material; (iii) processing the second material to form a waveguide for coupling the pair of optoelectronic devices to define an optical interconnect; and (iv) bonding at least one partially processed CMOS device layer having at least one transistor to the second semiconductor substrate to form the integrated circuit, the partially processed CMOS device layer arranged adjacent to the optical interconnect. An integrated circuit is also disclosed.

Abstract: A device includes a substrate, a pedestal extending from the substrate, and a ring resonator disposed on the pedestal above the substrate. The ring resonator has a resonance wavelength greater than 1.5 ?m and includes at least one of silicon and chalcogenide glass. The device can be used as a ring resonator sensor or a light source. The ring resonator is substantially transparent to mid-infrared radiation to reduce optical losses. The pedestal has a narrower width compared to the ring resonator to generate improved interaction between evanescent fields of light in the ring resonator and analytes nearby the ring resonator, thereby increasing sensing sensitivity. In addition, fabrication of the device is compatible with complementary metal-oxide-semiconductor (CMOS) processes and hence is amenable to large scale manufacturing.

Abstract: A method (100) of forming an integrated circuit is disclosed. The method comprises: (i) forming at least a pair of optoelectronic devices from at least a first wafer material arranged on a semiconductor substrate, the first wafer material different to silicon; (ii) etching the first wafer material to form a first recess to be filled with a second material; (iii) processing (104) the second material to form a waveguide for coupling the pair of optoelectronic devices to define an optical interconnect; and (iv) bonding (106) at least one partially processed CMOS device layer having at least one transistor to the second semiconductor substrate to form the integrated circuit, the partially processed CMOS device layer arranged adjacent to the optical interconnect. An integrated circuit is also disclosed.

Abstract: A germanium metal-semiconductor-metal (MSM) photodetector is fabricated by growing crystalline germanium from an amorphous silicon seed, supported by an amorphous substrate, at a temperature of about 450° C. In this fabrication, crystalline Ge is grown via selective deposition in geometrically confined channels, where amorphous silicon is disposed as the growth seed. Ge growth extends from the growth seed along the channels to a lithographically defined trench. The Ge emerging out of the channels includes crystalline grains that coalesce to fill the trench, forming a Ge strip that can be used as the active area of a photodetector. One or more Schottky contacts can be formed by a thin tunneling layer (e.g., Al2O3) deposited on the Ge strip and metal contracts formed on the tunneling layer.

Abstract: A device includes a substrate, a pedestal extending from the substrate, and a ring resonator disposed on the pedestal above the substrate. The ring resonator has a resonance wavelength greater than 1.5 ?m and includes at least one of silicon and chalcogenide glass. The device can be used as a ring resonator sensor or a light source. The ring resonator is substantially transparent to mid-infrared radiation to reduce optical losses. The pedestal has a narrower width compared to the ring resonator to generate improved interaction between evanescent fields of light in the ring resonator and analytes nearby the ring resonator, thereby increasing sensing sensitivity. In addition, fabrication of the device is compatible with complementary metal-oxide-semiconductor (CMOS) processes and hence is amenable to large scale manufacturing.