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.

An ion source having an electrically isolated extraction plate is disclosed. By isolating the extraction plate, a different voltage can be applied to the extraction plate than to the body of the arc chamber. By applying a more positive voltage to the extraction plate, more efficient ion source operation with higher plasma density can be achieved. In this mode the plasma potential is increased, and the electrostatic sheath reduces losses of electrons to the chamber walls. By applying a more negative voltage, an ion rich sheath adjacent to the extraction aperture can be created. In this mode, conditioning and cleaning of the extraction plate is achieved via ion bombardment. Further, in certain embodiments, the voltage applied to the extraction plate can be pulsed to allow ion extraction and cleaning to occur simultaneously.

An ion source having an electrically isolated extraction plate is disclosed. By isolating the extraction plate, a different voltage can be applied to the extraction plate than to the body of the arc chamber. By applying a more positive voltage to the extraction plate, more efficient ion source operation with higher plasma density can be achieved. In this mode the plasma potential is increased, and the electrostatic sheath reduces losses of electrons to the chamber walls. By applying a more negative voltage, an ion rich sheath adjacent to the extraction aperture can be created. In this mode, conditioning and cleaning of the extraction plate is achieved via ion bombardment. Further, in certain embodiments, the voltage applied to the extraction plate can be pulsed to allow ion extraction and cleaning to occur simultaneously.

An ion beam profiling system include a beam profiling element, an ion sensitive element electrically isolated from the beam profiling element, an ion source configured to emit an ion beam at the beam profiling element and the ion sensitive element, and a current measuring device coupled to the ion sensitive element. The beam profiling element includes a plate of material having two parallel major surfaces, a first slit aperture extending through the plate of material and having a first longitudinal length extending in a direction parallel to the two parallel major surfaces, and a second slit aperture extending through the plate of material and having a second longitudinal length extending in a direction parallel to the two parallel major surfaces, wherein the first longitudinal length of the first slit aperture is perpendicular to the second longitudinal length of the second slit aperture.

A radio frequency (RF) system includes a RF power source configured to power a load with an RF signal; an RF pipe including an inner conductor and an outer conductor connected to ground coupling the RF power source to the load; and a current sensor aligned to a central axis of the RF pipe carrying the RF signal. A sensor casing is disposed around the RF pipe, where the sensor casing includes a conductive material connected to the outer conductor of the RF pipe. A gallery is disposed within the sensor casing and outside the outer conductor of the RF pipe, where the current sensor is disposed in the gallery. A slit in the outer conductor of the RF pipe exposes the current sensor to a magnetic field due to the current of the RF signal in the inner conductor of the RF pipe.

A device may include an electron source, a detector, and a deflector. The electron source may be directed toward a sample area. The detector may receive an electron signal or an electron-induced signal. A deflector may be positioned between the electron source and the sample. The deflector may modulate an intensity of the electron source directed to the sample area according to an electron dose waveform having a continuously variable temporal profile.

The present invention relates to a method for measuring a sample with a microscope, the method comprising the steps of: measuring a tilt of the sample, correcting an orientation of the sample based on the tilt, and scanning the sample.

The present invention relates to a method for measuring a sample with a microscope, the method comprising the steps of: measuring a tilt of the sample, correcting an orientation of the sample based on the tilt, and scanning the sample.

A particle beam system comprises a particle beam column, a detection system and a controller. The particle beam column is configured to generate a particle beam and to direct it onto a sample, as a result of which charged particles are emitted by the sample. The detection system detects charged particles and comprises: an electrode, which can accelerate the charged particles; a potential source, which applies an adjustable electrical potential to the electrode; a scintillator; and a light detector, which outputs a detection signal. The controller controls the potential source and is configured to change the potential on the basis of the detection signal such that the scintillator operates outside its saturation and such that the light detector operates outside its saturation.

A particle beam system comprises a particle beam column, a detection system and a controller. The particle beam column is configured to generate a particle beam and to direct it onto a sample, as a result of which charged particles are emitted by the sample. The detection system detects charged particles and comprises: an electrode, which can accelerate the charged particles; a potential source, which applies an adjustable electrical potential to the electrode; a scintillator; and a light detector, which outputs a detection signal. The controller controls the potential source and is configured to change the potential on the basis of the detection signal such that the scintillator operates outside its saturation and such that the light detector operates outside its saturation.