An electrical device includes a counterdoped heterojunction selected from a group consisting of a pn junction or a p-i-n junction. The counterdoped junction includes a first semiconductor doped with one or more n-type primary dopant species and a second semiconductor doped with one or more p-type primary dopant species. The device also includes a first counterdoped component selected from a group consisting of the first semiconductor and the second semiconductor. The first counterdoped component is counterdoped with one or more counterdopant species that have a polarity opposite to the polarity of the primary dopant included in the first counterdoped component. Additionally, a level of the n-type primary dopant, p-type primary dopant, and the one or more counterdopant is selected to the counterdoped heterojunction provides amplification by a phonon assisted mechanism and the amplification has an onset voltage less than 1 V.

The production process according to the invention consists of a nanometric scale transformation of the crystalline silicon in a hybrid arrangement buried within the crystal lattice of a silicon wafer, to improve the efficiency of the conversion of light into electricity, by means of hot electrons. All the parameters, procedures and steps involved in manufacturing giant photoconversion cells have been tested and validated separately, by producing twenty series of test devices.

An example of the technology consists of manufacturing a conventional crystalline silicon photovoltaic cell with a single collection junction and completing the device thus obtained by an amorphizing ion implantation followed by a post-implantation thermal treatment.

The modulation of the crystal, specific to the giant photoconversion, is then carried out on a nanometric scale in a controlled manner to obtain SEGTONs and SEG-MATTER which are active both optically and electronically, together with the primary conversion of the host converter.

A photovoltaic device and method include a substrate coupled to an emitter side structure on a first side of the substrate and a back side structure on a side opposite the first side of the substrate. The emitter side structure or the back side structure include layers alternating between wide band gap layers and narrow band gap layers to provide a multilayer contact with an effectively increased band offset with the substrate and/or an effectively higher doping level over a single material contact. An emitter contact is coupled to the emitter side structure on a light collecting end portion of the device. A back contact is coupled to the back side structure opposite the light collecting end portion.

A solar cell comprising a bulk germanium silicon growth substrate; a diffused photoactive junction in the germanium silicon substrate; and a sequence of subcells grown over the substrate, with the first grown subcell either being lattice matched or lattice mis-matched to the growth substrate.

An optoelectronic semiconductor component is disclosed. In an embodiment an optoelectronic semiconductor component includes a front side, a first diode and a second diode arranged downstream of one another in a direction away from the front side and electrically connected in series such that the first diode is located closer to the front side than the second diode and an electrical tunnel contact between the first and the second diodes, wherein the second diode comprises a diode layer of Si.sub.nGe.sub.1-n, where 0n1, wherein the first diode comprises a first partial layer of SiGeC, a second partial layer of SiGe and a third partial layer of SiGeC, and wherein the partial layers follow one another directly in the direction away from the front side according to their numbering such that the first and third partial layers are of (Si.sub.yGe.sub.1-y).sub.1-xC.sub.x, whereas 0.05x0.5 or 0.25x0.75, and whereas 0y1, and the second partial layer is of SizGe1-z, whereas 0z1.

An electrical device includes a counterdoped heterojunction selected from a group consisting of a pn junction or a p-i-n junction. The counterdoped junction includes a first semiconductor doped with one or more n-type primary dopant species and a second semiconductor doped with one or more p-type primary dopant species. The device also includes a first counterdoped component selected from a group consisting of the first semiconductor and the second semiconductor. The first counterdoped component is counterdoped with one or more counterdopant species that have a polarity opposite to the polarity of the primary dopant included in the first counterdoped component. Additionally, a level of the n-type primary dopant, p-type primary dopant, and the one or more counterdopant is selected to the counterdoped heterojunction provides amplification by a phonon assisted mechanism and the amplification has an onset voltage less than 1 V.

A semiconductor device comprises a plurality of quantum structures comprising predominantly germanium. The plurality of quantum structures are formed on a first semiconductor layer structure. The quantum structures of the plurality of quantum structures have a lateral dimension of less than 15 nm and an area density of at least 810.sup.11 quantum structures per cm.sup.2. The plurality of quantum structures are configured to emit light with a light emission maximum at a wavelength of between 2 m and 10 m or to absorb light with a light absorption maximum at a wavelength of between 2 m and 10 m.

A photo-detecting apparatus includes a semiconductor substrate. A first germanium-based light absorption material is supported by the semiconductor substrate and configured to absorb a first optical signal having a first wavelength greater than 800 nm. A first metal line is electrically coupled to a first region of the first germanium-based light absorption material. A second metal line is electrically coupled to a second region of the first germanium-based light absorption material. The first region is un-doped or doped with a first type of dopants. The second region is doped with a second type of dopants. The first metal line is configured to control an amount of a first type of photo-generated carriers generated inside the first germanium-based light absorption material to be collected by the second region.

A method for making a CMOS image sensor may include forming a superlattice on a semiconductor substrate having a first conductivity type, with the superlattice including a plurality of stacked groups of layers. Each group of layers may include a plurality of stacked base semiconductor monolayers defining a base semiconductor portion, and a non-semiconductor monolayer(s) constrained within a crystal lattice of adjacent base semiconductor portions. The method may further include forming a plurality of laterally adjacent photodiodes on the superlattice. Each photodiode may include a semiconductor layer on the superlattice and having a first conductivity type dopant and with a lower dopant concentration than the semiconductor substrate, a retrograde well extending downward into the semiconductor layer and having a second conductivity type, a first well around a periphery of the retrograde well having the first conductivity type, and a second well within the retrograde well having the first conductivity type.

A CMOS image sensor may include a semiconductor substrate having a first conductivity type, and a plurality of laterally adjacent photodiodes formed in the substrate. Each photodiode may include a retrograde well extending downward into the substrate from a surface thereof and having a second conductivity type, a first well around a periphery of the retrograde well having the second conductivity type, and a second well within the retrograde well having the first conductivity type. Each photodiode may further include first and second superlattices respectively overlying each of the first and second wells. Each of the first and second superlattices may include a plurality of stacked groups of layers, with each group of layers including a plurality of stacked base semiconductor monolayers defining a base semiconductor portion, and at least one non-semiconductor monolayer constrained within a crystal lattice of adjacent base semiconductor portions.