An ion implanter includes an implantation processing chamber in which an implantation process of irradiating a wafer with an ion beam is performed, a first Faraday cup disposed inside the implantation processing chamber to measure a beam current of the ion beam during a preparation process performed before the implantation process, a second Faraday cup disposed inside the implantation processing chamber to measure a beam current of the ion beam during a calibration process for calibrating a beam current measurement value of the first Faraday cup, and a blockade member for blocking the ion beam directed toward the second Faraday cup, the blockade member being configured so that the ion beam is not incident into the second Faraday cup during the implantation process and the preparation process, and the ion beam is incident into the second Faraday cup during the calibration process.

An ion collector includes a plurality of segments and a plurality of integrators. The plurality of segments are physically separated from one another and spaced around a substrate support. Each of the segments includes a conductive element that is designed to conduct a current based on ions received from a plasma. Each of the plurality of integrators is coupled to a corresponding conductive element. Each of the plurality of integrators is designed to determine an ion distribution for a corresponding conductive element based, at least in part, on the current conducted at the corresponding conductive element. An example benefit of this embodiment includes the ability to determine how uniform the ion distribution is across a wafer being processed by the plasma.

The invention provides a bias voltage to the component (such as the Faraday cup) for reducing the generation of particles, such as the implanted ions and/or the combination of the implanted ions and the material of the component, and preventing particles peeling away the component. The strength of the biased voltage should not significantly affect the implantation of ions into the wafer and should significantly prevent the emission of radiation and/or electrons away the biased component. How to provide and adjust the biased voltage is not limited, both the extra voltage source and the amended Pre-Amplifier are acceptable. Moreover, due to the electric field generated by the Faraday cup is modified by the biased voltage, the ion beam divergence close to the Faraday cup may be reduced such that the potential difference between the ion beam measured by the profiler and received by the Faraday cup may be minimized.

A Fast Faraday Cup includes a group of electrodes including a grounded electrode having a through hole and a collector electrode configured with a blind hole that functions a collector hole. The electrodes are configured to allow a beam (e.g., a non-relativistic beam) to fall onto the grounded electrode so that the through hole cuts a beamlet that flies into the collector hole and facilitates measurement of the longitudinal distribution of particle charge density in the beam. The diameters, depths, spacing and alignment of the collector hole and the through hole are controllable to enable the Fast Faraday day cup to operate with a fast response time (e.g., fine time resolution) and capture secondary particles.

An ion collector includes a plurality of segments and a plurality of integrators. The plurality of segments are physically separated from one another and spaced around a substrate support. Each of the segments includes a conductive element that is designed to conduct a current based on ions received from a plasma. Each of the plurality of integrators is coupled to a corresponding conductive element. Each of the plurality of integrators is designed to determine an ion distribution for a corresponding conductive element based, at least in part, on the current conducted at the corresponding conductive element. An example benefit of this embodiment includes the ability to determine how uniform the ion distribution is across a wafer being processed by the plasma.

A system and method for optimizing a ribbon ion beam in a beam line implantation system is disclosed. The system includes a calibration sensor disposed in the beam line after the mass analyzer. The calibration sensor is able to measure both the total current of the ribbon ion beam, as well as provide information about its vertical position. Information from the calibration sensor can then be utilized by a controller to adjust various parameters to improve the density as well as the vertical position. In some embodiments, the calibration sensor may include a plurality of Faraday sensors, where, both the total current and the vertical position of the ion beam can be determined. Furthermore, the focus of the ion beam can be estimated based on the distribution of the current in the height direction.

An angle measurement device includes: a slit through which an ion beam is incident, and a width direction of which is orthogonal to a beam traveling direction of the ion beam toward a wafer; and a plurality of electrode bodies which are provided at positions away from the slit in the beam traveling direction, and each of which includes a beam measurement surface that is a region which is exposed to the ion beam having passed through the slit. The plurality of electrode bodies are disposed such that the beam measurement surfaces of the electrode bodies are arranged in order in the width direction of the slit and the beam measurement surfaces adjacent to each other in the width direction of the slit deviate from each other in the beam traveling direction.

A beam adjustment method includes: installing, on an irradiation surface to which an electron beam is radiated, a detection part having a Faraday cup catching electrical charges of the electron beam, and installing, on a side of an electron gun further than the detection part, a shielding plate having opening holes through which the electron beam is passable. The method includes causing, upon performing beam diameter measurement processing, the electron beam to pass through the opening holes, and radiating the electron beam to the Faraday cup. In addition, the method includes radiating, upon performing normal processing, the electron beam to the shielding plate.

An ion implanter includes a beam scanner that performs a scanning with an ion beam in a scanning direction perpendicular to a traveling direction of the ion beam, and a beam profiler that is disposed downstream of the beam scanner and measures a beam current distribution of the ion beam when the scanning by the beam scanner is performed. The beam profiler includes an aperture array that includes a first aperture and a second aperture, a cup electrode array that is disposed to be fixed with respect to the aperture array, the cup electrode array including a first cup electrode and a second cup electrode, and a plurality of magnets.

An device for measuring electron beam comprises a Faraday cup comprising an opening; a porous carbon material layer located on a surface of the Faraday cup and suspended at the opening; and an electricity meter electrically connected to the porous carbon material layer. A length of a suspended portion of the porous carbon material layer is greater than or equal to a maximum diameter of an electron beam to be measured. A diameter or a width of the porous carbon material layer is smaller than a minimum diameter of a cross section of the electron beam to be measured. The porous carbon material layer comprises a plurality of carbon material particles, and a plurality of micro gaps exist between the plurality of carbon material particles. A method for measuring an electron beam using the device for measuring electron beam is also provided.