摘要:
A method for modifying the chemistry or microstructure of silicon-based technology via an annealing process is provided. The method includes depositing a reactive material layer within a selected proximity to an interconnect, igniting the reactive material layer, and annealing the interconnect via heat transferred from the ignited reactive material layer. The method can also be implemented in connection with a silicide/silicon interface as well as a zone of silicon-based technology.
摘要:
A method for modifying the chemistry or microstructure of silicon-based technology via an annealing process is provided. The method includes depositing a reactive material layer within a selected proximity to an interconnect, igniting the reactive material layer, and annealing the interconnect via heat transferred from the ignited reactive material layer. The method can also be implemented in connection with a silicide/silicon interface as well as a zone of silicon-based technology.
摘要:
A system for determining an amount of radiation includes a dosimeter configured to receive the amount of radiation, the dosimeter comprising a circuit having a resonant frequency, such that the resonant frequency of the circuit changes according to the amount of radiation received by the dosimeter, the dosimeter further configured to absorb RF energy at the resonant frequency of the circuit; a radio frequency (RF) transmitter configured to transmit the RF energy at the resonant frequency to the dosimeter; and a receiver configured to determine the resonant frequency of the dosimeter based on the absorbed RF energy, wherein the amount of radiation is determined based on the resonant frequency.
摘要:
A system for determining an amount of radiation includes a dosimeter configured to receive the amount of radiation, the dosimeter comprising a circuit having a resonant frequency, such that the resonant frequency of the circuit changes according to the amount of radiation received by the dosimeter, the dosimeter further configured to absorb RF energy at the resonant frequency of the circuit; a radio frequency (RF) transmitter configured to transmit the RF energy at the resonant frequency to the dosimeter; and a receiver configured to determine the resonant frequency of the dosimeter based on the absorbed RF energy, wherein the amount of radiation is determined based on the resonant frequency.
摘要:
A semiconductor structure in which the contact resistance in the contact opening is reduced as well as a method of forming the same are provided. This is achieved in the present invention by replacing conventional contact metallurgy, such as tungsten, or a metal silicide, such as Ni silicide or Cu silicide, with a metal germanide-containing contact material. The term “metal germanide-containing” is used in the present application to denote a pure metal germanide (i.e., MGe alloy) or a metal germanide that includes Si (i.e., MSiGe alloy).
摘要:
A semiconductor structure in which the contact resistance in the contact opening is reduced as well as a method of forming the same are provided. This is achieved in the present invention by replacing conventional contact metallurgy, such as tungsten, or a metal silicide, such as Ni silicide or Cu silicide, with a metal germanide-containing contact material. The term “metal germanide-containing” is used in the present application to denote a pure metal germanide (i.e., MGe alloy) or a metal germanide that includes Si (i.e., MSiGe alloy).
摘要:
A semiconductor structure in which the contact resistance in the contact opening is reduced as well as a method of forming the same are provided. This is achieved in the present invention by replacing conventional contact metallurgy, such as tungsten, or a metal silicide, such as Ni silicide or Cu silicide, with a metal germanide-containing contact material. The term “metal germanide-containing” is used in the present application to denote a pure metal germanide (i.e., MGe alloy) or a metal germanide that includes Si (i.e., MSiGe alloy).
摘要:
A semiconductor structure in which the contact resistance in the contact opening is reduced as well as a method of forming the same are provided. This is achieved in the present invention by replacing conventional contact metallurgy, such as tungsten, or a metal silicide, such as Ni silicide or Cu silicide, with a metal germanide-containing contact material. The term “metal germanide-containing” is used in the present application to denote a pure metal germanide (i.e., MGe alloy) or a metal germanide that includes Si (i.e., MSiGe alloy).
摘要:
A computer program product, comprising a computer readable storage device having a computer readable program code stored therein, said program code including an algorithm adapted to be executed by a computer to implement a method. First, design information of a design structure is provided including a back-end-of-line layer of an integrated circuit which includes N interconnect layers, wherein N is a positive integer. Next, each interconnect layer is divided into multiple pixels. Next, a first path of a traveling particle in a first interconnect layer of the N interconnect layers is determined. Next, M path pixels of the multiple pixels of the first interconnect layer on the first path of the traveling particle are identified, wherein M is a positive integer. Next, a first loss energy lost by the traveling particle due to its completely passing through a first pixel of the M path pixels is determined.
摘要:
A method of determining a stopping power of a design structure with respect to a traveling particle. The method includes (i) providing design information of the design structure comprising a back-end-of-line layer which includes N interconnect layers, N being a positive integer, (ii) dividing each interconnect layer of the N interconnect layers into multiple pixels, and (iii) determining a first path of the traveling particle in a first interconnect layer of the N interconnect layers, (iv) identifying M path pixels of the multiple pixels of the first interconnect layer on the first path of the traveling particle, M being a positive integer, and (v) determining a first loss energy lost by the traveling particle due to its completely passing through a first pixel of the M path pixels.