Patent Application
20210118646
The invention relates generally to large area three-dimensional analysis in a charged particle microscope, and specifically to large area three-dimensional analysis in a charged particle microscope using glancing incidence focused ion beam milling.
Volume analysis of samples using charged particle systems is performed using a variety of techniques and charged particle microscopes. Most of these techniques, however, include delicate and demanding sample preparation that, if not performed correctly, can provide unusable results or destruction of critical sample material. For example, conventional slice-and-view techniques use a focused ion beam to mill away a slice of sample to expose a surface that is imaged, which can damage areas of interest. To protect the areas of interest, protective layers are used. Additionally, alignment to the edge of the area of interest is critical for subsequent FIB milling operations. If the protective layer is absent, not robust, and/or the alignment is not optimal, FIB milling may result in removal of desired areas for imaging. Additionally, conventional slice-and-view requires time-consuming preparation steps, is limited to high-energy (30 keV) FIB milling, relatively small volumes, cut placement accuracy FIB imaging resolution requirements are very high, and milling artifacts (e.g., “curtaining”) are common and problematic to subsequent 3D reconstructions. While there are other volume analysis techniques that may be better than slice-and-view, they too have their own drawbacks and difficult sample preparation requirements. As such, more straightforward and robust volume analysis techniques are desired, especially a technique that can process large areas of a sample.
Methods and apparatuses disclosed herein for large-area 3D analysis of samples using glancing incidence FIB milling. An example method at least includes milling, with a focused ion beam, a sample at a shallow angle and at a plurality of rotational orientations to remove a layer of the sample and to expose a surface, and after milling, imaging, with a charged particle beam, the exposed surface of the sample.
An example apparatus for implementing the disclosed techniques at least includes a focused ion beam column, an electron beam column, a stage and a controller. The controller including or coupled to non-transitory memory including code that, when executed by the controller, causes the apparatus to mill, with a focused ion beam, a sample at a shallow angle and at a plurality of rotational orientations to remove a layer of the sample, and after milling, image, with a charged particle beam, an exposed surface of the sample.
Like reference numerals refer to corresponding parts throughout the several views of the drawings.
Embodiments of the present invention are described below in the context of a dual-beam charged particle microscope configured to perform glancing angle, large area milling and imaging. The disclosed techniques may provide large area volume reconstruction data of materials of different types, and the type of material being studied may determine what ion species to use and at what ion milling energy. However, it should be understood that the methods described herein are generally applicable to a wide range of different tomographic methods and apparatus, including both cone-beam and parallel beam systems, and are not limited to any particular apparatus type, beam type, object type, length scale, or scanning trajectory
As used in this application and in the claims, the singular forms “a,” “an,” and “the” include the plural forms unless the context clearly dictates otherwise. Additionally, the term “includes” means “comprises.” Further, the term “coupled” does not exclude the presence of intermediate elements between the coupled items.
The systems, apparatus, and methods described herein should not be construed as limiting in any way. Instead, the present disclosure is directed toward all novel and non-obvious features and aspects of the various disclosed embodiments, alone and in various combinations and sub-combinations with one another. The disclosed systems, methods, and apparatus are not limited to any specific aspect or feature or combinations thereof, nor do the disclosed systems, methods, and apparatus require that any one or more specific advantages be present or problems be solved. Any theories of operation are to facilitate explanation, but the disclosed systems, methods, and apparatus are not limited to such theories of operation.
Although the operations of some of the disclosed methods are described in a particular, sequential order for convenient presentation, it should be understood that this manner of description encompasses rearrangement, unless a particular ordering is required by specific language set forth below. For example, operations described sequentially may in some cases be rearranged or performed concurrently. Moreover, for the sake of simplicity, the attached figures may not show the various ways in which the disclosed systems, methods, and apparatus can be used in conjunction with other systems, methods, and apparatus. Additionally, the description sometimes uses terms like “produce” and “provide” to describe the disclosed methods. These terms are high-level abstractions of the actual operations that are performed. The actual operations that correspond to these terms will vary depending on the particular implementation and are readily discernible by one of ordinary skill in the art.
In some examples, values, procedures, or apparatuses are referred to as “lowest”, “best”, “minimum,” or the like. It will be appreciated that such descriptions are intended to indicate that a selection among many used functional alternatives can be made, and such selections need not be better, smaller, or otherwise preferable to other selections.
Charged particle beam microscopes come in a variety of types, such as transmission electron microscopes (TEMs), scanning electron microscopes (SEMs), focused ion beam (FIBs) microscopes, and dual-beam microscopes that include both an FIB and an SEM column, to name a few. While there are many different analysis and image acquisition techniques that can be performed using this array of microscopes, one type of analysis technique aims at obtaining an array of 2D images taken at different positions within a volume of a sample so that volume reconstruction can be performed of that volume of the sample. This technique is sometimes referred to as slice-and-view. Slice-and-view is conventionally implemented in dual-beam (DB) systems since they have the ability to both remove sample material using the FIB column and image the sample using the SEM column. While the samples may also be imaged with the FIB column, imaging with the SEM column may provide greater resolution in some instances.
The conventional slice-and-view technique includes many steps that require precision and that make the process lengthy and delicate. For example, slice-and-view requires lengthy sample preparation steps, such as excavation of large volumes of a sample around a region of interest and the need to deposit a protective layer over the region of interest. Fiducials are typically formed close to the region of interest as well to help with location detection for sample movement. Additionally, the volume of a sample analyzed by slice-and-view is typically small 50 to 100 μm in at least one dimension. For example, a large slice-and-view volume may be 100×50×50 μm in X, Y, Z, respectively, which is about 250,000 μm3. Larger volumes are possible, but the time constraint of the milling process becomes prohibitive. Smaller volumes might range down to a few thousand cubic-microns, and a targeted, high-resolution run may be 1000 μm3 or smaller. Moreover, depending on the FIB column and source used, the slice thickness may be limited to 5 nm, but may be more typically on the order of 10 nm. Other issues may arise with the ion milling of the slices, such as curtaining and non-uniformity of slice thickness. All of these issues, either on their own or in combination, make slice-and-view potentially problematic and difficult to implement effectively. Another potential limitation is that, owing to the high demands of imaging resolution and cut placement accuracy, the ion beam needs to be operated at maximum possible acceleration potential (i.e., 30 keV). However, this high energy can damage biological tissue and obscure visibility of some cellular structures. Avoidance of such damage is highly desirable, especially for soft materials.
One solution to the above discussed problems may be to perform glancing angle incident “spin milling” of the sample. The shallow angle spin milling may provide a large area of analysis, e.g., 100 μm to 1 mm in diameter, and layers as thin as 2 nm may be removed per “spin mill.” As used herein, spin mill refers to milling an area of a sample at a number of different rotational orientations using a shallow milling angle, e.g., 1 to 10 degrees from glancing incidence, relative to the sample surface. An example of the technique includes positioning the sample so that the FIB angle of incidence relative to the sample surface is near glancing. A brief FIB exposure (usually several seconds with beam currents of several nA to 2.5 uA) is performed over the desired area. The stage is rotated through a fixed angle, which is typically in the range 10-60 degrees. In some embodiments, the stage is rotated 72 degrees, for example, so that 5 sites are milled to encompass 360° of that surface. Milling five sites may reduce surface texturing artifacts, for example. Usually, this stage rotation process is repeated until a full 360 rotation of the sample has been realized. In some cases, multiple rotations may be preferred per milling cycle. As a result, ion flux is delivered to the sample from several different azimuthal directions, which greatly reduces milling artifacts (curtaining) as compared to conventional top-down cross sectional milling. One full rotation of milling constitutes a “slice.” Alternatively, a slice may be defined by the frequency the milling is interrupted to perform SEM imaging. As such, a slice is usually, but not always, defined by 1 full rotation. After each slice the sample is imaged, such as with SEM imaging, of one or more regions of interest (ROIs) within the milled area.
In some embodiments, the one or more ROIs may be imaged at high resolution while the surrounding area inside the milled area is imaged at a lower resolution. Of course, the entire milled area may be imaged at high resolution as well. As additional slices are removed and additional exposed surfaces are imaged, the number and location of the ROIs being tracked may change, where some ROIs may disappear due to removal (or due to extending beyond the milled area) and additional ROIs may appear due to exposure. Image recognition techniques and software may be enabled to track the various ROIs as additional slices are removed and images acquired.
In this technique, conventional fiducials associated with an ROI may not be as useful for at least a couple of reasons. One, since the total milled area is typically very large, the small fiducials would lack visibility and would not help with alignment. Plus, the fiducials would likely be milled away unless they were placed along the perimeter of the milled area, which may make them less useful. Since the fiducials would be too small to be imaged with adequate resolution, subsequent positioning accuracy in the ROIs would be poor. To overcome this problem, images of individual ROIs are digitally stored and used as reference images for the subsequent slice images using pattern matching algorithms to locate the ROIs. As long as slice thickness is relatively small, the structural details of the sample changes very little from slice-to-slice, and therefore using the image of the nth slice is adequate for pattern matching to the n+1 slice. In some embodiments, however, local fiducial markers may be formed so that there is a reference position for reconstructing an array of 2D slices. Such a local fiducial may only be useful in the images of a specific ROI (or perhaps a cluster of closely-spaced ROIs), because of the limitations described above, but they could be useful locally in instances in which the target features within an ROI are positioned at an angle relative to the sample normal. In such embodiments, image registration techniques may not be able to distinguish a tilted feature from stage drift, and the placement of local fiducials may be helpful for references. Additionally, local fiducials may also be used as an internal way of monitoring slice thickness. For this embodiment, the local fiducial may be engineered in such a way that removal of a particular thickness of sample surface results in a predictable change to the measurable appearance of the local fiducial.
In addition to the above discussed aspects of the technique, e.g., glancing angle, large area milling, the technique may also include variation of milling parameters, e.g., ion species, number of milling sites per rotation, ion dose per site, and milling energy, based on the sample type. For example, in the case of biological samples, a plasma FIB system operating with O+ ions is preferred, thereby generating a mixture of molecular and atomic oxygen ions, typically at 12 keV or below. If, however, xenon (Xe+) is used for biological samples, the ion energy should be kept below 5 keV. For other sample types, such as metal alloys or minerology samples, argon (Ar+) or Xe+ may be preferred, and the ion energy can range widely, from 2-30 keV for example, depending on the characteristics of the individual sample. The metal and metal alloy category may include fabricated structures, e.g., battery electrodes, flexible displays, and Integrated circuits, to name a few.
A scanning electron microscope 141, along with power supply and control unit 145, is provided with the dual beam system 100. An electron beam 143 is emitted from a cathode 152 by applying voltage between cathode 152 and an anode 154. Electron beam 143 is focused to a fine spot by means of a condensing lens 156 and an objective lens 158. Electron beam 143 is scanned two-dimensionally on the specimen by means of a deflection coil 160. Operation of condensing lens 156, objective lens 158, and deflection coil 160 is controlled by power supply and control unit 145.
Electron beam 143 can be focused onto sample 122, which is on movable X-Y stage 125 within lower chamber 126. When the electrons in the electron beam strike substrate 122, secondary electrons are emitted. These secondary electrons are detected by secondary electron detector 140 as discussed below. STEM detector 162, located beneath the TEM sample holder 124 and the stage 125, can collect electrons that are transmitted through the sample mounted on the TEM sample holder as discussed above.
Dual beam system 100 also includes focused ion beam (FIB) system 111 which comprises an evacuated chamber having an upper neck portion 112 within which are located an ion source 114 and a focusing column 116 including extractor electrodes and an electrostatic optical system. In some embodiments, the axis of focusing column 116 is tilted 52 degrees from the axis of the electron column. Of course, other tilt angles between the FIB and SEM columns is possible as well. The ion column 112 includes an ion source 114, an extraction electrode 115, a focusing element 117, deflection elements 120, and a focused ion beam 118. Focused ion beam 118 passes from ion source 114 through focusing column 116 and between electrostatic deflection means schematically indicated at 120 toward sample 122, which can be, for example, a biological sample, a semiconductor sample, a metal or metal alloy sample, or a minerology sample, positioned on movable X-Y stage 125 within lower chamber 126.
Stage 125 can preferably move in a horizontal plane (X and Y axes) and vertically (Z axis). Stage 125 can also tilt approximately sixty (60) degrees and rotate about the Z axis. In some embodiments, negative stage tilts may be used to reach the desired glancing FIB milling incidence angle. Of course, both positive and negative tilts are contemplated herein. The desired tilt range for spin mill-enabled instruments is typically −38° to 60°, with 0 degrees being the “untilted,” SEM-normal orientation. In some embodiments, a positive tilt of 52° is normal to the ion beam. In some embodiments, stage 125 can be cooled to cryogenic temperatures by being coupled to a cold finger (not shown), the cold finger provided or in contact with a supply of liquid nitrogen, for example. By cooling the stage 125 to cryogenic temperatures, biological samples that are cooled to cryogenic temperatures, and possibly vitrified, can be milled and imaged as discussed herein.
An ion pump 168 is employed for evacuating neck portion 112. The chamber 126 is evacuated with turbomolecular and mechanical pumping system 130 under the control of vacuum controller 132. The vacuum system provides within chamber 126 a vacuum of between approximately 1×10-7 Torr and 5×10-4 Torr. If an etch assisting, an etch retarding gas, or a deposition precursor gas is used, the chamber background pressure may rise, typically to about 1×10-5 Torr.
The high voltage power supply provides an appropriate acceleration voltage to electrodes in focusing column 116 for energizing and focusing ion beam 118. When it strikes substrate 122, material is sputtered, that is physically ejected, from the sample. Alternatively, ion beam 118 can decompose a precursor gas to deposit a material.
High voltage power supply 134 is connected to liquid metal ion source 114 as well as to appropriate electrodes in ion beam focusing column 116 for forming an approximately 1 keV to 60 keV ion beam 118 and directing the same toward a sample. Deflection controller and amplifier 136, operated in accordance with a prescribed pattern provided by pattern generator 138, is coupled to deflection plates 120 whereby ion beam 118 may be controlled manually or automatically to trace out a corresponding pattern on the upper surface of substrate 122. In some systems the deflection plates are placed before the final lens, as is well known in the art. Beam blanking electrodes (not shown) within ion beam focusing column 116 cause ion beam 118 to impact onto blanking aperture (not shown) instead of substrate 122 when a blanking controller (not shown) applies a blanking voltage to the blanking electrode.
In some embodiments, ion source 114 is a liquid metal ion source that typically provides a metal ion beam of gallium. The source typically is capable of being focused into a sub one-tenth micrometer wide beam at substrate 122 for either modifying the substrate 122 by ion milling, enhanced etch, material deposition, or for the purpose of imaging the substrate 122. In other embodiments, however, ion source 114 is a plasma-based ion source, such as an inductively coupled plasma source or a radio frequency ion source, and is further capable of providing different ion species, such as oxygen, argon, xenon, and nitrogen to name a few. In such an embodiment, the plasma gas is switched to provide the desired ion species. As disclosed herein, the ion species being used when operating system 100 may depend on the sample type. For example, if the sample is a biological sample, oxygen or xenon may be the desired ion species. On the other hand, if the sample is a metal, metal alloy or mineral, then the desired ion species may be argon or xenon. As disclosed herein, basing the choice of ion species on the sample type helps to efficiently and optimally process a sample to alleviate the problems discussed above, such as surface texturing for example.
A charged particle detector 140, such as an Everhart Thornley or multi-channel plate, used for detecting secondary ion or electron emission is connected to a video circuit 142 that supplies drive signals to video monitor 144 and receiving deflection signals from a system controller 119. The location of charged particle detector 140 within lower chamber 126 can vary in different embodiments. For example, a charged particle detector 140 can be coaxial with the ion beam and include a hole for allowing the ion beam to pass. In other embodiments, secondary particles can be collected through a final lens and then diverted off axis for collection.
A micromanipulator 147 can precisely move objects within the vacuum chamber. Micromanipulator 147 may comprise precision electric motors 148 positioned outside the vacuum chamber to provide X, Y, Z, and theta control of a portion 149 positioned within the vacuum chamber. The micromanipulator 147 can be fitted with different end effectors for manipulating small objects. In the embodiments described herein, the end effector is a thin probe 150.
A gas delivery system 146 extends into lower chamber 126 for introducing and directing a gaseous vapor toward substrate 122. For example, iodine can be delivered to enhance etching, or a metal organic compound can be delivered to deposit a metal.
System controller 119 controls the operations of the various parts of dual beam system 110. Through system controller 119, a user can cause ion beam 118 or electron beam 143 to be scanned in a desired manner through commands entered into a conventional user interface (not shown). Alternatively, system controller 119 may control dual beam system 110 in accordance with programmed instructions stored in a memory 121. In some embodiments, dual beam system 110 incorporates image recognition software to automatically identify regions of interest, and then the system can manually or automatically extract samples in accordance with the invention. For example, the system could automatically locate desired features on a sample.
In operation, the system 100 performs one or more “spin milling” processes on sample 122 and images an exposed layer after each spin milling process. The spin milling includes milling the sample 122 at a glancing angle and in a plurality of rotational orientations. For example, the stage 125 is tilted so that the ion beam 118 is at 1° to 10° from the surface of the sample 122 and then the surface is milled over a desired area (the desired area may be 100 μm to 1 mm and may further include the entire field of view at a given magnification). After milling over the desired area, the sample 122 is rotated 72°, for example, and the sample 122 is milled again at the same glancing angle and over the same size of area. Of course, other angles of rotation may be used within 360. This mill and rotate process may be repeated a desired number of times, such as 2, 3, 4, 5, 6 or more, and once a full 360 of rotation has occurred (or multiple rotations, if desired), the sample 122 is imaged with the electron beam 143. More specifically, after the full milling, an exposed surface of the sample 122 is imaged. The milling after the full 360° has occurred may be referred to herein as a “slice” of the sample. In some embodiments, the sample 122 may be repositioned in x, y, z and/or tilt angle to acquire the images, then repositioned to the desire glancing angle to mill another slice of the sample 122.
For the milling, the ion species used and the energy of the ion beam 118 may be based on the type of sample being milled and imaged. For example, a biological sample may be milled using O2+ at an energy of 12 keV or less, or, alternatively, be milled using Xe+ at an energy of less than 5 keV. If, for example, the sample is a metal or mineral, the ion species may be either Ar+ or Xe+ at an energy of 2 to 30 keV. Irrespective of ion species, sample and ion beam energy, the sample may also be cooled to cryogenic temperatures during milling an imaging. The cryo-cooling may be especially useful in studying biological samples, some of which may have been vitrified prior to loading into system 100, to preserve their structure. By implementing the “spin mill” process, large areas of sample 122 may be repeatedly imaged so that a volume of images may form a 3D reconstruction of the sample. Additionally, the use of the disclosed spin mill process reduces the need for depositing a protective layer, performing pre-excavations of large volumes surrounding the ROI, and depositing fiducials, which provides a straightforward and robust 3D analysis technique.
Each of the mill areas A-E will be milled by delivering the ion beam 218 to each pixel in the respective square. As used herein, the term “pixel” refers to a coordinate on the sample 222 inside of a mill area that receives the ion beam 218 for a designated amount of dwell time, such as several to hundreds of microseconds, but the dwell time may depend on beam current, to mill away some of the sample 222 at that coordinate. Stated differently, each pixel receives the ion beam 218 for a desired dwell time. As can be seen, areas outside of the “slice” circle also receive the ion beam 218, but because those areas do not receive the ion beam at each rotational orientation, they may not have a full thickness of the sample 222 milled away. Additionally, each mill areas A-E may fill the entire field of view of the microscope at the given magnification of the ion column, such as ion column 111. As such, very large areas may be milled at each rotational orientation.
The method 301 begins at optional process block 303, which includes determining sample material type. For example, determinations that the sample material type is biological, metal, semiconductor, mineral, etc., may be made. In some embodiments, this determination may be made by a user. In other embodiments, the determination may be made automatically by the system using some other analytical technique, such as a spectroscopic technique. For example, a spectroscopic analysis, using EBSD for example, may be performed to determine the chemical makeup of the sample. The chemical makeup may determine whether the sample is metal/alloy, semiconductor or biological sample, which may determine mill parameters and ion species.
Process block 303 may be followed by optional process block 305, which includes setting mill parameters based on the sample material. The mill parameters may include ion species, mill energy, and ion beam current, for example. In general, the sample material type determines the mill parameters so that high surface quality milling is obtained. For example, if the sample is biological, then the selected ion species may be either oxygen or xenon. If oxygen is selected, then the ion beam energy may be set to 12 keV or less. If xenon is selected, then the ion beam energy may be set to less than 5 keV. For metal or mineral type samples, for example, the ion species can be argon or xenon, and both can be delivered at a range of energies, such as 2 keV to 30 keV.
Process block 305 may be followed by process block 307, which includes milling the sample at a shallow angle and at a plurality of rotational orientations to remove a layer of the sample. Removing the layer exposes a surface of the sample. The shallow angle may be from 1 to 10 degrees, for example, and the number of rotational orientations may be from 2 to 10. Additionally, the milling may be performed stepwise in that each rotational orientation is maintained for a desired milling time before the sample is rotated to a subsequent rotational orientation. Alternatively, the sample may be continuously rotated while being milled for a desired amount of time.
Process block 307 may be followed by process block 309, which includes imaging the exposed surface of the sample after milling. The imaging may occur after milling all of the rotational orientations or after milling each individual rotational orientation. The images may then be stored, for example.
Optionally, after process block 309 is performed, method 301 may return to process block 307 so that another layer of the sample is removed by milling in the plurality of rotational orientations. This optional loop may be performed a plurality of times until a desired depth of the sample is imaged. As such, an image of each respective surface of the sample is obtained.
Optionally, process block 309 may be followed by process block 311, which includes forming a 3D reconstruction of the imaged area of the sample. Images of the plurality of exposed surfaces are combined to form the 3D reconstruction.
Computer system 419 also includes a main memory 421, such as a random access memory (RAM) or other dynamic storage device, coupled to the bus for storing information and instructions to be executed by processor 470. Main memory 421 also may be used for storing temporary variables or other intermediate information during execution of instructions to be executed by processor 470. Such instructions, when stored in non-transitory storage media accessible to processor 470, render computer system 419 into a special-purpose machine that is customized to perform the operations specified in the instructions.
Computer system 419 further includes a read only memory (ROM) 472 or other static storage device coupled to bus for storing static information and instructions for processor 470. A storage device 474, such as a magnetic disk or optical disk, is provided and coupled to a bus for storing information and instructions.
Computer system 419 may be coupled via the bus to a display, such as a cathode ray tube (CRT), for displaying information to a computer user. An input device, including alphanumeric and other keys, is coupled to the bus for communicating information and command selections to processor 470. Another type of user input device is a cursor control, such as a mouse, a trackball, or cursor direction keys for communicating direction information and command selections to processor 470 and for controlling cursor movement on the display. This input device typically has two degrees of freedom in two axes, a first axis (e.g., x) and a second axis (e.g., y), that allows the device to specify positions in a plane.
Computer system 419 may implement the techniques described herein using customized hard-wired logic, one or more ASICs or FPGAs, firmware and/or program logic which in combination with the computer system causes or programs computer system 419 to be a special-purpose machine. According to one embodiment, the techniques herein are performed by computer system 419 in response to processor 470 executing one or more sequences of one or more instructions contained in main memory 421. Such instructions may be read into main memory 421 from another storage medium, such as storage device 474. Execution of the sequences of instructions contained in main memory 421 causes processor 470 to perform the process steps described herein. In alternative embodiments, hard-wired circuitry may be used in place of or in combination with software instructions.
The term “storage media” as used herein refers to any non-transitory media that store data and/or instructions that cause a machine to operate in a specific fashion. Such storage media may comprise non-volatile media and/or volatile media. Non-volatile media includes, for example, optical or magnetic disks, such as storage device 736. Volatile media includes dynamic memory, such as main memory 732. Common forms of storage media include, for example, a floppy disk, a flexible disk, hard disk, solid state drive, magnetic tape, or any other magnetic data storage medium, a CD-ROM, any other optical data storage medium, any physical medium with patterns of holes, a RAM, a PROM, and EPROM, a FLASH-EPROM, NVRAM, any other memory chip or cartridge, content-addressable memory (CAM), and ternary content-addressable memory (TCAM).
Storage media is distinct from but may be used in conjunction with transmission media. Transmission media participates in transferring information between storage media. For example, transmission media includes coaxial cables, copper wire and fiber optics, including the wires that comprise the bus. Transmission media can also take the form of acoustic or light waves, such as those generated during radio-wave and infra-red data communications.
Computer system 419 also includes a communication interface 476 coupled to the bus. Communication interface 476 provides a two-way data communication coupling to a network link (not shown) that is connected to a local network, for example. As another example, communication interface 476 may be a local area network (LAN) card to provide a data communication connection to a compatible LAN. Wireless links may also be implemented. In any such implementation, communication interface 476 sends and receives electrical, electromagnetic or optical signals that carry digital data streams representing various types of information.
Computer system 419 can send messages and receive data, including program code, through the network(s), a network link and communication interface 476. In the Internet example, a server might transmit a requested code for an application program through Internet, ISP, local network and communication interface 476. The received code may be executed by processor 470 as it is received, and/or stored in storage device 736, or other non-volatile storage for later implementation.
The embodiments discussed herein to illustrate the disclosed techniques should not be considered limiting and only provide examples of implementation. For example, different numbers of rotational orientations, ion species, ion beam energies and currents at various milling angles may be implemented and still fall within the scope of the present disclosure. Those skilled in the art will understand the other myriad ways of how the disclosed techniques may be implemented, which are contemplated herein and are within the bounds of the disclosure.
An example method implementing the disclosed techniques includes milling, with a focused ion beam, a sample at a shallow angle and at a plurality of rotational orientations to remove a layer of the sample, and after milling, imaging, with a charged particle beam, an exposed surface of the sample.
The example method of above where each of the plurality of rotational orientations are milled separately before rotating the sample to a subsequent rotational orientation of the plurality of rotational orientations.
The method of above where the plurality of rotational orientations are milled while the sample is rotated.
The example method of above where the sample is a biological sample.
The example method of above where the focused ion beam provides oxygen ions at an energy of 12 keV or less.
The example method of above where the focused ion beam provides xenon ions at an energy of less than 5 keV.
The example method of above where the sample is a metal or metal alloy.
The example method of above where the focused ion beam provides Argon or Xenon at an energy in the range of 2 to 30 keV.
The example method of above where the sample is a mineral.
The example method of above where the focused ion beam provides Argon or Xenon at an energy in the range of 2 to 30 keV.
The example method of above where the sample is held on a cryo-stage cooled to cryogenic temperatures.
The example method of above where the sample is cooled to cryogenic temperatures while milling and imaging.
The example method of above where the sample is moved during imaging to acquire images of a region of interest.
The example method of above where an area as large as 1 mm in diameter is milled.
The example method of above where milling the sample at the shallow angle and at the plurality of rotational orientations removes a 2 nm thick layer.
The example method of above where the shallow angle is in a range from 1 to 6 degrees from a surface of the sample.
The example method of above where the focused ion mill is a plasma focused ion mill.
The example method of above where the plasma focused ion mill is capable of switching between different ion species.
The example method of above where the different ion species includes oxygen, argon, and xenon.
The example method of above further including repeating the milling and imaging steps a plurality of times.
The example method of above further including identifying sample material type.
The example method of above further including based on the sample material type, setting mill parameters, such as ion species, mill energy, ion beam current, and dwell time.
An example apparatus for implementing the disclosed techniques at least includes a focused ion beam column, an electron beam column, a stage and a controller. The controller including or coupled to non-transitory memory including code that, when executed by the controller, causes the apparatus to mill, with a focused ion beam, a sample at a shallow angle and at a plurality of rotational orientations to remove a layer of the sample, and after milling, image, with a charged particle beam, an exposed surface of the sample.
The example apparatus of above where each of the plurality of rotational orientations are milled separately before rotating the sample to a subsequent rotational orientation of the plurality of rotational orientations.
The example apparatus of above where the plurality of rotational orientations are milled while the sample is rotated.
The example apparatus of above where the sample is a biological sample.
The example method of above where the focused ion beam provides oxygen ions at an energy of 12 keV or less.
The example apparatus of above where the focused ion beam provides xenon ions at an energy of less than 5 keV.
The example apparatus of above where the sample is a metal or metal alloy.
The example apparatus of above where the focused ion beam provides Argon or Xenon at an energy in the range of 2 to 30 keV.
The example apparatus of above where the sample is a mineral.
The example apparatus of above where the focused ion beam provides Argon or Xenon at an energy in the range of 2 to 30 keV.
The example apparatus of above where the sample is held on a cryo-stage cooled to cryogenic temperatures.
The example apparatus of above where the sample is cooled to cryogenic temperatures while milling and imaging.
The example apparatus of above where the sample is moved during imaging to acquire images of a region of interest.
The example apparatus of above where an area as large as 1 mm in diameter is milled.
The example apparatus of above where milling the sample at the shallow angle and at the plurality of rotational orientations removes a 2 nm thick layer.
The example apparatus of above where the shallow angle is in a range from 1 to 6 degrees from a surface of the sample.
The example apparatus of above where the focused ion mill is a plasma focused ion mill.
The example apparatus of above where the plasma focused ion mill is capable of switching between different ion species.
The example apparatus of above where the different ion species includes oxygen, argon, and xenon.
The example apparatus of above further including repeating the milling and imaging steps a plurality of times.
The example apparatus of above further including identifying sample material type.
The example apparatus of above further including based on the sample material type, setting mill parameters, such as ion species, mill energy, ion beam current, and dwell time.
The present application claims the priority benefit of provisional U.S. Patent Application Ser. No. 62/923,231, filed Oct. 18, 2019. The disclosures of the foregoing application are incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| 62923231 | Oct 2019 | US |
