Abstract: With evacuation of interior of a vacuum chamber halted and with gas supply into the vacuum chamber halted, in a state that a mixed gas of helium gas and diborane gas is sealed in the vacuum chamber, a plasma is generated in a vacuum vessel and simultaneously a high-frequency power is supplied to a sample electrode. By the high-frequency power supplied to the sample electrode, boron is introduced to a proximity to the substrate surface.

Abstract: An object is to provide a semiconductor device in which uniform properties are intended and high yields are provided. Process steps are provided in which variations are adjusted in doping and annealing process steps that are subsequent process steps so as to cancel in-plane variations in a substrate caused by dry etching to finally as well provide excellent in-plane consistency in a substrate.

Abstract: A top plate, disposed on an upper portion of a vacuum container so as to face a substrate-placing area of a sample electrode, is provided with an impurity-containing film that contains an impurity, and is formed on a top plate peripheral edge portion area that is a face exposable to a plasma generated in the vacuum container, and is located on a peripheral edge of a top plate center portion area that faces the center portion of the substrate-placing area.

Abstract: An amount of leakage of a substrate-cooling gas into a vacuum container is measured by using a flow-rate measuring device so that the flow rate of a diluting gas that is the same as the substrate-cooling gas is controlled by a control device or a plasma doping time is prolonged, in accordance with the amount of leakage.

Abstract: A fin-shaped semiconductor region is formed on a substrate, and then the substrate is placed in a chamber. Then, an ignition gas is introduced into a chamber to thereby turn the ignition gas into a plasma, and then a process gas containing an impurity is introduced into the chamber to thereby turn the process gas into a plasma. Then, a bias voltage is applied to the substrate so as to dope the semiconductor region with the impurity after confirming attenuation of an amount of the ignition gas remaining in the chamber.

Abstract: A semiconductor region having an upper surface and a side surface is formed on a substrate. A first impurity region is formed in an upper portion of the semiconductor region. A second impurity region is formed in a side portion of the semiconductor region. The resistivity of the second impurity region is substantially equal to or smaller than that of the first impurity region.

Abstract: An impurity region is formed in a surface of a substrate by exposing the substrate to a plasma generated from a gas containing an impurity in a vacuum chamber. In this process, a plasma doping condition is set with respect to a dose of the impurity to be introduced into the substrate so that a first one of doses in a central portion and in a peripheral portion of the substrate is greater than a second one of the doses during an initial period of doping, with the second dose becoming greater than the first dose thereafter.

Abstract: A semiconductor device includes: a fin-type semiconductor region (13) formed on a substrate (11); a gate insulating film (14) formed so as to cover an upper surface and both side surfaces of a predetermined portion of the fin-type semiconductor region (13); a gate electrode (15) formed on the gate insulating film (14); and an impurity region (17) formed on both sides of the gate electrode (15) in the fin-type semiconductor region (13). An impurity blocking portion (15a) for blocking the introduction of impurities is provided adjacent both sides of the gate electrode (15) over an upper surface of the fin-type semiconductor region (13).

Abstract: A method of forming an impurity-introduced layer is disclosed. The method includes at least a step of forming a resist pattern on a principal face of a solid substrate such as a silicon substrate (S27); a step of introducing impurity into the solid substrate through plasma-doping in ion mode (S23), a step of removing a resist (S28), a step of cleaning metal contamination and particles attached to a surface of the solid substrate (S25a); a step of anneal (S26). The step of removing a resist (S28) irradiates the resist with oxygen-plasma or brings mixed solution of sulfuric acid and hydrogen peroxide water, or mixed solution of NH4OH, H2O2 and H2O into contact with the resist. The step of cleaning (S25a) brings mixed solution of sulfuric acid and hydrogen peroxide water, or mixed solution of NH4OH, H2O2 and H2O into contact with the principal face of the solid substrate.

Abstract: A plasma of a gas containing an impurity is produced through a discharge in a vacuum chamber, and a plurality of substrates are successively doped with the impurity by using the plasma, wherein a plasma doping condition of a subject substrate is adjusted based on an accumulated discharge time until the subject substrate is placed in the vacuum chamber.

Abstract: A method for introducing impurities includes a step for forming an amorphous layer at a surface of a semiconductor substrate, and a step for forming a shallow impurity-introducing layer at the semiconductor substrate which has been made amorphous, and an apparatus used therefore. Particularly, the step for forming the amorphous layer is a step for irradiating plasma to the surface of the semiconductor substrate, and the step for forming the shallow impurity-introducing layer is a step for introducing impurities into the surface which has been made amorphous.

Abstract: A method for introducing impurities includes a step for forming an amorphous layer at a surface of a semiconductor substrate, and a step for forming a shallow impurity-introducing layer at the semiconductor substrate which has been made amorphous, and an apparatus used therefore. Particularly, the step for forming the amorphous layer is a step for irradiating plasma to the surface of the semiconductor substrate, and the step for forming the shallow impurity-introducing layer is a step for introducing impurities into the surface which has been made amorphous.

Abstract: A subject of the present invention is to realize an impurity doping not to bring about a rise of a substrate temperature. Another subject of the present invention is to measure optically physical properties of a lattice defect generated by the impurity doping step to control such that subsequent steps are optimized. An impurity doping method, includes a step of doping an impurity into a surface of a solid state base body, a step of measuring an optical characteristic of an area into which the impurity is doped, a step of selecting annealing conditions based on a measurement result to meet the optical characteristic of the area into which the impurity is doped, and a step of annealing the area into which the impurity is doped, based on the selected annealing conditions.

Abstract: A method for introducing impurities includes a step for forming an amorphous layer at a surface of a semiconductor substrate, and a step for forming a shallow impurity-introducing layer at the semiconductor substrate which has been made amorphous, and an apparatus used therefore. Particularly, the step for forming the amorphous layer is a step for irradiating plasma to the surface of the semiconductor substrate, and the step for forming the shallow impurity-introducing layer is a step for introducing impurities into the surface which has been made amorphous.

Abstract: It is intended to provide a plasma doping method and apparatus which are superior in the controllability of the concentration of an impurity that is introduced into a surface layer of a sample. A prescribed gas is introduced into a vacuum container 1 from a gas supply apparatus 2 while being exhausted by a turbomolecular pump 3 as an exhaust apparatus. The pressure in the vacuum container 1 is kept at a prescribed value by a pressure regulating valve 4. High-frequency electric power of 13.56 MHz is supplied from a high-frequency power source 5 to a coil 8 disposed close to a dielectric window 7 which is opposed to a sample electrode 6, whereby induction-coupled plasma is generated in the vacuum container 1. A high-frequency power source 10 for supplying high-frequency electric power to the sample electrode 6 is provided. Every time a prescribed number of samples have been processed, a dummy sample is subjected to plasma doping and then to heating.

Abstract: A subject of the present invention is to realize an impurity doping not to bring about a rise of a substrate temperature. Another subject of the present invention is to measure optically physical properties of a lattice defect generated by the impurity doping step to control such that subsequent steps are optimized. An impurity doping method, includes a step of doping an impurity into a surface of a solid state base body, a step of measuring an optical characteristic of an area into which the impurity is doped, a step of selecting annealing conditions based on a measurement result to meet the optical characteristic of the area into which the impurity is doped, and a step of annealing the area into which the impurity is doped, based on the selected annealing conditions.

Abstract: A method for introducing impurities includes a step for forming an amorphous layer at a surface of a semiconductor substrate, and a step for forming a shallow impurity-introducing layer at the semiconductor substrate which has been made amorphous, and an apparatus used therefore. Particularly, the step for forming the amorphous layer is a step for irradiating plasma to the surface of the semiconductor substrate, and the step for forming the shallow impurity-introducing layer is a step for introducing impurities into the surface which has been made amorphous.

Abstract: A plasma of a gas containing an impurity is produced through a discharge in a vacuum chamber, and a plurality of substrates are successively doped with the impurity by using the plasma, wherein a plasma doping condition of a subject substrate is adjusted based on an accumulated discharge time until the subject substrate is placed in the vacuum chamber.

Abstract: An impurity region having a box-shaped impurity profile is formed. An impurity introducing method includes a step of introducing a desired impurity into a surface of a solid base body, and a step of radiating plasma to a surface of the solid base body after the impurity introducing step thus forming an impurity profile having an approximately box-shape.

Abstract: A method is provided for controlling a dose amount of dopant to be doped into an object to be processed in plasma doping. According to the method, the doping control is formed of the following processes: determining the temperature of the object, the amount of ions having dopant in plasma that collide with the object, and types of gases in plasma during doping; calculating a dose amount by neutral gas according to the temperature of the object, and a dose amount by ions from the determined amount of ions containing dopant that collide with the object; and carrying out doping so that the sum of the dose amount by neutral gas and the dose amount by ions equal to a predetermined dose amount.