A electronic blackbody cavity is provided. The electronic blackbody cavity comprises an inner surface; a chamber surrounded by the inner surface; an opening configured to make an electron beam enter the chamber; and a porous carbon material layer located on the inner surface. The porous carbon material layer consists of a plurality of carbon material particles and a plurality of micro gaps. The plurality of micro gaps are defined by the plurality of carbon material particles. A secondary electron detection device using the electronic blackbody cavity is also provided.

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.

Provided herein are approaches for optimizing a full horizontal scanned beam distance of an accelerator beam. In one approach, a method may include positioning a first Faraday cup along a first side of an intended beam-scan area, positioning a second Faraday cup along a second side of the intended beam-scan area, scanning an ion beam along the first and second sides of the intended beam-scan area, measuring a first beam current of the ion beam at the first Faraday cup and measuring a second beam current of the ion beam at the second Faraday cup, and determining an optimal scan distance of the ion beam across the intended beam-scan area based on the first beam current and the second beam current.

A electronic blackbody cavity is provided. The electronic blackbody cavity comprises an inner surface; a chamber surrounded by the inner surface; an opening configured to make an electron beam enter the chamber; and a porous carbon material layer located on the inner surface. The porous carbon material layer consists of a plurality of carbon material particles and a plurality of micro gaps. The plurality of micro gaps are defined by the plurality of carbon material particles. A secondary electron detection device using the electronic blackbody cavity is also provided.

There is provided a charged particle beam system having a computer system for controlling an acceleration voltage of a charged particle beam emitted from a charged particle source, the system including: a first diaphragm group having first and second diaphragms which are diaphragms that act on the charged particle beam and have different thicknesses; and a first diaphragm switching mechanism for switching the diaphragm in the first diaphragm group, in which the computer system controls the first diaphragm switching mechanism so as to switch from the first diaphragm to the second diaphragm according to an increase or decrease of the acceleration voltage.

A system and method that is capable of measuring the incident angle of an ion beam, especially an ion beam comprising heavier ions, is disclosed. In one embodiment, X-rays, rather than ions, are used to determine the channeling direction. In another embodiment, the workpiece is constructed, at least in part, of a material having a high molecular weight such that heaver ion beams can be measured. Further, in another embodiment, the parameters of the ion beam are measured across an entirety of the beam, allowing components of the ion implantation system to be further tuned to create a more uniform beam.

A system and method that is capable of measuring the incident angle of an ion beam, especially an ion beam comprising heavier ions, is disclosed. In one embodiment, X-rays, rather than ions, are used to determine the channeling direction. In another embodiment, the workpiece is constructed, at least in part, of a material having a high molecular weight such that heaver ion beams can be measured. Further, in another embodiment, the parameters of the ion beam are measured across an entirety of the beam, allowing components of the ion implantation system to be further tuned to create a more uniform beam.

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 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.