Abstract: A method to compensate for drift while controlling a charged particle beam (CPB) system having at least one charged particle beam controllable in position. Sources of drift include mechanical variations in the stage supporting the sample, beam deflection shifts, and environmental impacts, such as temperature. The method includes positioning a sample supported by a stage in the CPB system, monitoring a reference fiducial on a surface of the sample from a start time to an end time, determining a drift compensation to compensate for a drift that causes an unintended change in the position of a first charged particle beam relative to the sample by a known amount over a period of time based on a change in the position of the reference fiducial between the start time and the end time, and adjusting positions of the first charged particle beam by applying the determined drift compensation during an operation of the CPB system.

Abstract: A method for attaching a prepared sample to a carrier in a focused ion beam chamber. The method includes reducing a temperature within the chamber to substantially below room temperature followed by moving the prepared sample adjacent to a substrate carrier surface. The temperature can be lowered sufficiently to establish a cryogenic condition in the chamber. Attachment of the prepared sample to the substrate carrier is done by controlling the focused ion beam to raster a target area of the surface in the absence of a gas deposition precursor, to sputter material onto the base of the sample and the substrate carrier surface, thereby binding the prepared sample to the substrate carrier.

Abstract: A carrier grid with integrated gas delivery system for use in a charged particle beam system (CPB). The carrier grid has a body with an internal reservoir for storing a gas. A post extends from the body with an end for supporting a sample to be operated upon, and an outlet tip extends from the end of the post. A channel extends from the reservoir, through the post and ends in the outlet tip, where the outlet tip seals the stored gas in the body. Cutting the outlet tip near its base, with a focused ion beam (FIB) by example, will open the channel to the CPB chamber, allowing the prestored gas within the reservoir to escape. A FIB or electron beam directed at the junction of the sample positioned near the post will cause deposition and subsequent attachment of the sample to the post in presence of the gas.

Abstract: A method to compensate for drift while controlling a charged particle beam (CPB) system having at least one charged particle beam controllable in position. Sources of drift include mechanical variations in the stage supporting the sample, beam deflection shifts, and environmental impacts, such as temperature. The method includes positioning a sample supported by a stage in the CPB system, monitoring a reference fiducial on a surface of the sample from a start time to an end time, determining a drift compensation to compensate for a drift that causes an unintended change in the position of a first charged particle beam relative to the sample by a known amount over a period of time based on a change in the position of the reference fiducial between the start time and the end time, and adjusting positions of the first charged particle beam by applying the determined drift compensation during an operation of the CPB system.

Abstract: A carrier grid with integrated gas delivery system for use in a charged particle beam system (CPB). The carrier grid has a body with an internal reservoir for storing a gas. A post extends from the body with an end for supporting a sample to be operated upon, and an outlet tip extends from the end of the post. A channel extends from the reservoir, through the post and ends in the outlet tip, where the outlet tip seals the stored gas in the body. Cutting the outlet tip near its base, with a focused ion beam (FIB) by example, will open the channel to the CPB chamber, allowing the prestored gas within the reservoir to escape. A FIB or electron beam directed at the junction of the sample positioned near the post will cause deposition and subsequent attachment of the sample to the post in presence of the gas.

Abstract: Linear fiducials including notches or chevrons with known angles relative to each other are formed such that each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: A novel method for cross-section sample preparation has a sample oriented normal to an SEM/GFIS or other imaging column via a stage, and is operated upon by an FIB to form the cross-section pre-lamella within the sample, followed by an approximate 90° rotation with no tilt of the stage for cut out by the FIB. Asymmetric trenches are milled to have a three-dimensional depth profile to ensure that the FIB has clear line of sight to a face of the resulting pre-lamella when the sample has been rotated. The three-dimensional depth profile further minimizes overall milling time required for the preparation of the pre-lamella.

Abstract: Linear fiducials including notches or chevrons with known angles relative to each other are formed such that each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Linear fiducials including notches or chevrons with known angles relative to each other are formed such that each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: A novel method for cross-section sample preparation has a sample oriented normal to an SEM/GFIS or other imaging column via a stage, and is operated upon by an FIB to form the cross-section pre-lamella within the sample, followed by an approximate 90° rotation with no tilt of the stage for cut out by the FIB. Asymmetric trenches are milled to have a three-dimensional depth profile to ensure that the FIB has clear line of sight to a face of the resulting pre-lamella when the sample has been rotated. The three-dimensional depth profile further minimizes overall milling time required for the preparation of the pre-lamella.

Abstract: Linear fiducials including notches or chevrons with known angles relative to each other are formed such that each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Notches or chevrons with known angles relative to each other are formed on a surface of the sample, where each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Notches or chevrons with known angles relative to each other are formed on a surface of the sample, where each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Notches or chevrons with known angles relative to each other are formed on a surface of the sample, where each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Notches or chevrons with known angles relative to each other are formed on a surface of the sample, where each branch of a chevron appears in a cross-sectional face of the sample as a distinct structure. Therefore, when imaging the cross-section face during the cross-sectioning operation, the distance between the identified structures allows unique identification of the position of the cross-section plane along the Z axis. Then a direct measurement of the actual position of each slice can be calculated, allowing for dynamic repositioning to account for drift in the plane of the sample and also dynamic adjustment of the forward advancement rate of the FIB to account for variations in the sample, microscope, microscope environment, etc. that contributes to drift. An additional result of this approach is the ability to dynamically calculate the actual thickness of each acquired slice as it is acquired.

Abstract: Generally, the present disclosure provides a method and system for improving imaging efficiency for CPB systems while maintaining or improving imaging accuracy over prior CPB systems. A large field of view image of a sample is acquired at a low resolution and thus, at high speed. The low resolution level is selected to be sufficient for an operator to visually identify structures or areas of interest on the low resolution image. The operator can select one or more small areas of arbitrary shape and size on the low resolution image, referred to as an exact region of interest (XROI). The outline of the XROI is mapped to an x-y coordinate system of the image, and the CPB system is then controlled to acquire a high resolution image of only the XROI identified on the low resolution image. For 3D imaging, once the XROI is identified, each section of the sample can be iteratively imaged in the previously described manner, with the operator having the option to redefine the XROI later.

Abstract: Generally, the present disclosure provides a method and system for improving imaging efficiency for CPB systems while maintaining or improving imaging accuracy over prior CPB systems. A large field of view image of a sample is acquired at a low resolution and thus, at high speed. The low resolution level is selected to be sufficient for an operator to visually identify structures or areas of interest on the low resolution image. The operator can select one or more small areas of arbitrary shape and size on the low resolution image, referred to as an exact region of interest (XROI). The outline of the XROI is mapped to an x-y coordinate system of the image, and the CPB system is then controlled to acquire a high resolution image of only the XROI identified on the low resolution image. For 3D imaging, once the XROI is identified, each section of the sample can be iteratively imaged in the previously described manner, with the operator having the option to redefine the XROI later.

Abstract: Generally, the present disclosure provides a method and system for improving imaging efficiency for CPB systems while maintaining or improving imaging accuracy over prior CPB systems. A large field of view image of a sample is acquired at a low resolution and thus, at high speed. The low resolution level is selected to be sufficient for an operator to visually identify structures or areas of interest on the low resolution image. The operator can select one or more small areas of arbitrary shape and size on the low resolution image, referred to as an exact region of interest (XROI). The outline of the XROI is mapped to an x-y coordinate system of the image, and the CPB system is then controlled to acquire a high resolution image of only the XROI identified on the low resolution image. For 3D imaging, once the XROI is identified, each section of the sample can be iteratively imaged in the previously described manner, with the operator having the option to redefine the XROI later.

Abstract: An apparatus and method for using high beam currents in FIB circuit edit operations, without the generation of electrostatic discharge events. An internal partial chamber is disposed over the circuit to be worked on by the FIB. The partial chamber has top and bottom apertures for allowing the ion beam to pass through, and receives a gas through a gas delivery nozzle. A non-reactive gas, or a combination of a non-reactive gas and a reactive gas, is added to the FIB chamber via the partial chamber, until the chamber reaches a predetermined pressure. At the predetermined pressure, the gas pressure in the partial chamber will be much greater than that of the chamber, and will be sufficiently high such that the gas molecules will neutralize charging induced by the beam passing through the partial chamber.

Abstract: Methods for using sub-100V electron beam landing energies for performing circuit edit operations. Circuit edit operations can include imaging for navigation and etching in the presence of a suitable gas. Low landing energies can be obtained by modifying a decelerator system of native FESEM equipment, or by using biasing means near the sample surface for decelerating electrons of the primary beam. At low landing energies near the operating voltage of a semiconductor circuit, voltage contrast effects can be visually seen for enhancing operator navigation. Low landing energies can be used during etching processes for minimizing the interaction volume of the beam and obtaining accurate and localized etching.