Abstract: There is provided a method of introducing impurity capable of efficiently realizing a shallow impurity introduction. The impurity introducing method includes a first step of making a surface of a semiconductor layer to be amorphous by reacting plasma composed of particles which are electrically inactive in the semiconductor layer to a surface of a solid base body including the semiconductor layer, and a second step of introducing impurity to the surface of the solid base body. After performing the first step, by performing the second step, an amorphous layer with fine pores is formed on the surface of the solid base body including the semiconductor layer, and impurity are introduced in the amorphous layer to form an impurity introducing layer.

Abstract: A plasma doping method that can control a dose precisely is realized. In-plane uniformity of the dose is improved. It has been found that, if a bias is applied by irradiating B2H6/He plasma onto a silicon substrate, there is a time at which a dose of boron is made substantially uniform, and the saturation time is comparatively long and ease to stably use, compared with a time at which repeatability of an apparatus control can be secured. The invention has been finalized focusing on the result. That is, if plasma irradiation starts, a dose is initially increased, but a time at which the dose is made substantially uniform without depending on a time variation is continued. In addition, if the time is further increased, the dose is decreased. The dose can be accurately controlled through a process window of the time at which the dose is made substantially uniform without depending on the time variation.

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 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: It is an object to prevent functions expected originally from being unexhibited when impurities to be introduced into a solid sample are mixed with each other, and to implement plasma doping with high precision. In order to distinguish impurities which may be mixed from impurities which should not be mixed, first of all, an impurity introducing mechanism of a core is first distinguished. In order to avoid a mixture of the impurities in very small amounts, a mechanism for delivering a semiconductor substrate to be treated and a mechanism for removing a resin material to be formed on the semiconductor substrate are used exclusively.

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: 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: To provide an impurity introducing method which can repeatedly carry out such a process that plasma irradiation for realization of amorphous and plasma doping were combined, in such a situation that steps are simple and through-put is high, without destroying an apparatus. At the time of switching over plasmas which are used in plasma irradiation for realization of amorphous and plasma doping, electric discharge is stopped, and an initial condition of a matching point of a high frequency power supply and a peripheral circuit is reset so as to adapt to plasma which is used in each step, or at the time of switching, a load, which is applied to the high frequency power supply etc., is reduced by increasing pressure and decreasing a bias voltage.

Abstract: An object of this invention is to provide a method for making a junction which is simple in the process, high in the throughput, and can make a shallow junction with high accuracy. After the suitable state of a substrate surface adapted to the wavelength of an electromagnetic wave to be applied has been formed, the electromagnetic wave is applied to electrically activate impurities so that the excited energy is effectively absorbed within the impurity thin film, thereby effectively making a shallow junction.

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 liquid phase etching method which comprises spraying a chemically reactive liquid, with a specific speed, to a solid article, an aggregate of solid articles or a gelatinous material to be treated; and a liquid etching apparatus having a mechanism for holding a processing object to be treated and a nozzle structure for spraying a chemically reactive liquid to the processing object to be treated which is held by the mechanism. The method and apparatus allow the significant improvement of the etching rate while maintaining the accuracy of etching.

Abstract: An ion-implanting apparatus and method can dynamically control a beam current value with time and does not change energy. This ion-implanting apparatus controls a dynamic change in beam current value with time by giving feedback on the beam current value measured with a beam current measuring device.

Abstract: A plasma doping method, even though a plasma doping treatment is repeated, can make a dose from a film to a silicon substrate uniform for each time. The method includes preparing a vacuum chamber having a film containing an impurity formed on an inner wall thereof such that, when the film is attacked by ions in plasma, the amount of an impurity to be doped into the surface of a sample by sputtering is not changed even though the plasma containing the impurity ions is repeatedly generated in the vacuum chamber; placing the sample on the sample electrode; and irradiating the plasma containing the impurity ions so as to implant the impurity ions into the sample, and doping the impurity into the sample by sputtering from the film containing the impurity fixed to the inner wall of the vacuum chamber.

Abstract: A plasma doping method that can control a dose precisely is realized. In-plane uniformity of the dose is improved. It has been found that, if a bias is applied by irradiating B2H6/He plasma onto a silicon substrate, there is a time at which a dose of boron is made substantially uniform, and the saturation time is comparatively long and ease to stably use, compared with a time at which repeatability of an apparatus control can be secured. The invention has been finalized focusing on the result. That is, if plasma irradiation starts, a dose is initially increased, but a time at which the dose is made substantially uniform without depending on a time variation is continued. In addition, if the time is further increased, the dose is decreased. The dose can be accurately controlled through a process window of the time at which the dose is made substantially uniform without depending on the time variation.

Abstract: A plasma doping method, even though a plasma doping treatment is repeated, can make a dose from a film to a silicon substrate uniform for each time. The method includes preparing a vacuum chamber having a film containing an impurity formed on an inner wall thereof such that, when the film is attacked by ions in plasma, the amount of an impurity to be doped into the surface of a sample by sputtering is not changed even though the plasma containing the impurity ions is repeatedly generated in the vacuum chamber; placing the sample on the sample electrode; and irradiating the plasma containing the impurity ions so as to implant the impurity ions into the sample, and doping the impurity into the sample by sputtering from the film containing the impurity fixed to the inner wall of the vacuum chamber.

Abstract: The invention provides a method of doping impurities that includes a step of doping impurities in a solid base substance by using a plasma doping method, a step of forming a light antireflection layer that functions to reduce light reflection on the surface of the solid base substance, and a step of performing annealing by light radiation. According to the method, it is possible to reduce the reflectance of light radiated during annealing, to efficiently apply energy an impurity doped layer, to improve activation efficiency, to prevent diffusion, and to reduce sheet resistance of the impurity doped layer.

Abstract: The present invention provides a beam measuring device which can measure a beam current value with high accuracy in a non-destructive manner and, at the same time, can measure a position of a beam. A measuring device includes a magnetic shielding part for shielding an outer magnetic field, and a plurality of magnetic field sensors which are arranged in a shielding space which is formed by the magnetic shielding part, wherein the magnetic field sensor includes a plurality of magnetic field collection mechanisms which collect magnetic fields which the beam current to be measured generates, and the magnetic field collection mechanism is a cylindrical structural body which has at least a surface thereof formed of a superconductive body and includes a bridge portion which has only a portion thereof formed of a superconductive body on an outer peripheral portion thereof, and a magnetic field which the beam current to be measured generates is measured by the magnetic field sensors.

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: Disclosed is a charge neutralizing device which is capable of being applied to a substrate 13 having a large area and in which electrons having low energy of 5 eV or less, and preferably 2 eV, are supplied so that charge due to ion implantation and damage by the electrons are avoided with respect to a cusp device. The charge neutralizing device includes a microwave generating unit, a plasma generating unit that generates electron plasma using a microwave generated from the microwave generating unit, and a contact unit that brings the electron plasma generated from the plasma generating unit into contact with a beam plasma region including an ion beam.

Abstract: A beam current sensor is composed of a cylindrical super-conductive body having a bridge unit formed on the outer diameter side wherein a beam passes through the inner diameter side. The sensor improves efficiency of creating a magnetic field from a current and can measure a beam current as 1 nA. The bridge unit includes a first coil unit formed so as to have an eddy shape wound counterclockwise from the outer diameter side toward the inner diameter side; a second coil unit formed so as to have an eddy shape wound clockwise from the outer diameter side toward the inner diameter side; and a connection portion for connecting the center position of the inner diameter side of the first coil unit with the center position of the inner diameter side of the second coil.