Mineral Characterization using Scanning Electron Microscopy (SEM): A Review of the Fundamentals, Advancements, and Research Directions

1. Introduction

The rapid pace of technological development requires a detailed study of minerals to a further extent, to meet the unprecedented material demands of the evolving world. There are more than 5956 species of minerals known today and the number of new identifications is evolving with as many as 50 new types identified each year [1,2]. The quantitative measurements and qualitative analyses of mineral compositions within mining ores and reservoirs contain valuable importance to practical applications. A piece of comprehensive and accurate information can be gathered for the identification of rocks and minerals, including structural characteristics and mineral composition, which can provide a worthy set of information about pore structure and reservoir heterogeneity [3,4,5].

The qualitative analysis of minerals is usually conducted through conventional optical microscopy (OM), also known as light microscopy (LM), scanning electron microscopy (SEM), and infrared spectroscopy methods [6,7,8]. Mineral characteristics and mutual relationships are broadly analyzed by OM, however, due to its resolution limitations, it lacks the qualitative analysis of micro-nanoscale particles including structural characteristics and mineral morphology [9,10]. OM can obtain a maximum useful magnification of 1000 times [11]. The wavelength of the imaging radiation can be decreased further for better resolution (i.e., higher useful magnification). OM uses light as imaging radiation, while electron microscopy makes use of electrons to magnify the specimen. Electron beams are accelerated with high energies (from 2 keV to 1000 keV, representing smaller wavelengths of 0.027 nm to 0.0009 nm) in electron microscopes [11].

The bombardment of high-energy electron beams on the atoms in the specimen can result in various possible interactions (Figure 1), which are subject to the thickness of the specimen. The electrons can be transmitted unabsorbed through the specimen, if its thickness is very small, and can be used to form an image in transmission electron microscopy (TEM) [12]. Contrarily, with thicker specimens, electrons are not transmitted and the particles (electrons, photons, x-rays, etc.) emerging from the surface of the specimen provide morphological and structural information. Low-energy electron beams ranging from 0.1 keV to 30 keV penetrate the sample from a few to tens of nanometers. Medium-energy ones ranging from 30 keV to 1,000 keV penetrate from tens of nanometers to micrometer scale, while high-energy beams, which are usually above 10,000 keV can go from several micrometers to millimeters within the sample. The retrieved information signals are used in SEM to provide sample characteristic information [13].

SEM can be used to analyze the crystalline structure, surface topography, electrical behavior, and chemical composition of around 1µm of the top part of the specimen [11]. The behavior of the specimen under several conditions can be investigated using SEM, as a variety of specialized stages can be attached to it, such as, cold [14], hot [15], or designed to allow in situ mechanical testing [16]. For instance, cathodoluminescence (emission of light) works very well for temperatures near absolute zero, as compared to room temperature [17,18]. Since the images formed are much less noisy from the light emitted by a cold specimen.

SEM has additional advantages over OM. For example, SEM has a powerful useful magnification of 1,000,000 times and can reach up to the nanometer scale [19]. This allows an in-depth examination of the specimen as compared to the OM. Surface smoothness affects the quality of micrographs taken with OM, as high-magnification OM possesses a very low depth of field. SEM, on the other hand, has a large depth of field and it benefits in simultaneous focus on the specimen surface, irrespective of the surface roughness [20]. SEM contains the possibility to go beyond analyzing the surface topography [21], such as chemical composition [22], crystal structure [23], and electrical properties [24]. The confidence of analysis can be gained further by switching between different imaging techniques, which enables cross-correlating the acquired information. SEM is also beneficial over TEM in several analytical scenarios. SEM can cater to larger-sized samples (wafers of 200 mm diameter, while specially adapted SEMs can go further up), in comparison to TEM, which can go to just 2.3 mm or 3 mm [19]. SEM is a non-destructive analytical technique [25], while the specimen preparation process of TEM makes it a destructive technique [26]. The time required for preparing the sample for SEM is also less when compared to the TEM technique.

Figure 1. Various possible interactions of high-energy electrons with atoms. The atomic shells are labeled with standard notation (i.e., K, L, M). The incident particle is shown with a solid arrow. (a) Low-angle scattering: very little energy loss is experienced by the incident electrons, and they scatter to the next layer of atoms; (b) High-angle (or back) scattering; (c) Emission of characteristic x-rays and a secondary electron; (d) Emission of an Auger electron and a secondary electron.

Figure 1. Various possible interactions of high-energy electrons with atoms. The atomic shells are labeled with standard notation (i.e., K, L, M). The incident particle is shown with a solid arrow. (a) Low-angle scattering: very little energy loss is experienced by the incident electrons, and they scatter to the next layer of atoms; (b) High-angle (or back) scattering; (c) Emission of characteristic x-rays and a secondary electron; (d) Emission of an Auger electron and a secondary electron.

SEM can be further classified into three types, i.e., conventional SEM (CSEM), low vacuum SEM (LVSEM), and environmental SEM (ESEM) [27,28,29]. CSEM usually possesses a high-vacuum (10^-6 torr) condition for the interaction of electron beam and specimen. This allows the emission of low-energy secondary electrons from the specimen, resulting in their minimum collisions with the gas molecules present in the chamber. The CSEM reinforces those analyses where dehydration and cracking of the sample (due to high vacuum) is not a problem such as the identification of alkali-silica reactivity in concrete [30]. The second type LVSEM is similar to CSEM, with adaptation of elevated pressure (0.2 to 1 torr) operations as well. The LVSEM environment slowly dissipates any liquid water present in the sample, and therefore the crack propagation in the sample moves very slowly. For non-conductive samples, it is important to add the conductive coating to avoid any charging effects. The third type ESEM permits imaging of the sample at high humidity and therefore, is considered as “wet mode”. ESEM has a relatively high-pressure environment i.e., 0.2 to 20 torr, which reduces or eliminates dehydration. The elevated pressure reinforces the ionization of gas molecules due to the emission of surface charges, thereby reducing the need for conductive coatings [31]. The strength of the electron signal increases with the ionization of gas molecules, providing better results. ESEM supports coherent imaging but ponders a limited ability for analyzing X-ray microanalysis, as frequent collisions lead to defocusing and scattering of the electron beam which makes the position of the beam on the specimen uncertain. Field emission gun SEM (FEG SEM) typically falls under the category of CSEM, as its operation includes high vacuum conditions. In conclusion, the type of SEM should be chosen based on the nature of the specimen and the required analysis.

1.1. Background Development of SEM

The idea of using electron microscopy dates back to the previous century when Ruska and Knoll conducted their experiments in 1932 [32,33]. This instrument was named as transmission electron microscope (TEM), based on its working principle and application, where electrons were transmitted through thin specimens to magnify beyond levels of the optical microscope of that time. In 1938, a scanning coil was added to the TEM by Von Ardenne, introducing the era of scanning transmission electron microscopy (STEM) [34,35]. It provided a magnification of 8000x with a resolution of 50-100 nm at 23 keV. Ardene developed the laboratory instrument with various features, which became standard for developing and inventing new SEM systems [36]. A new explanation of SEM for analyzing thick samples was presented by Zworykin, Hillier, and Snyder in 1942. It was found that the emission of secondary electrons can be used for topographic contrast. Oatley and McMullan in 1952 developed the electrostatic lens for SEM. Smith understood the role of signal processing in improving SEM micrographs and laid the foundation for non-linear signal amplification. Another contribution from Smith was the production of double deflection scanning for upgrading the scanning system [36]. Wells in 1953 designed a new stereoscopic pair for investigating the third dimension in SEM micrographs. The work of Everhart and Thornley indicates the development of a secondary detector, which served as a tool for improving the signal-to-noise ratio, and overall increasing the collected signals. Pease used the three magnetic lenses in building the SEM V system, which is considered the first commercial SEM instrument available under the name of “Stereoscan” Cambridge Scientific Instruments Mark 1 in markets from 1965 [37]. Since then, several advancements have been made to improve the SEM analysis, such as the upgradation of electron source for better electron emission resulting in efficient and clear SEM resolution. Another beneficial advancement in SEM development pertains to the invention of an energy-dispersive spectrometer (EDS). The system has been used in conjunction with SEM since 1968 and has been making use of solid-state detectors for measuring X-rays [36]. SEM has been developing with the advent of modern equipment. Danilatos studied the effect of the environment on analyzed samples during 1991-1993, which led to the development of an environmental scanning electron microscope (ESEM) for examining the surface of a specimen, whether it is dry or wet [38,39]. Among these advancements in SEM, the most recent one is the generation of digital images, which are then displayed on computers for analysis. At present, the majority of the SEM instruments have modern software, for analyzing obtained data, and EDS system, which makes the use of computer programming for evaluating the composition of various elements present in the sample [36]. The use of modern software provides improved quantitative analysis and converts the X-ray intensity into chemical compositions of the sample, in a relatively shorter period of time.

1.2. Basic SEM Operation

The typical energies of incident electrons coming from electron guns in SEM, in general range from 2 keV to 40 keV [11]. The SEM instrument can be classified based on the range of energies, which is subject to the type and nature of samples and analyses, such as low voltage SEM, standard SEM, high-resolution SEM, and field emission SEM. Electron guns are also chosen based on the intended application, and there are three types of electron guns usually used for SEM. Type one is the tungsten filament electron gun, which is heated over 2500℃ resulting in the thermal emission of electrons from its tip [40,41]. The second type of electron gun is lanthanum hexaboride filament which produces thermionic emissions, with the advantages of longer work-life time and a brighter beam of electrons from a larger maximum beam current [42,43]. These electron guns are relatively more expensive than the conventional tungsten filament ones. Field emission guns are the third type of electron guns, and are known as cold cathode electron emitters, as heating is not involved in the process [44,45]. It works with the application of a very high electric field to a finely pointed tip, which results in providing the brightest beam with a very small deviation in electron energy. Since the field emission guns need 10^-10 torr pressure for preserving the tip, the cost of SEM with these guns becomes expensive [11].

The electron beam is demagnified into a fine probe by two or three electromagnetic condenser lenses. Scan coils are used with fine probes for scanning across the selected surface area of the specimen. The electrons coming from the probe penetrate into the sample in a tear-dropped-shape volume (Figure 2). The overall dimensions of this volume are determined by various factors such as the electron beam energy and the atomic masses of the constituent elements present in the specimen. Higher energy and lighter atomic masses of elements tend to result in increased penetration depth inside the sample. The angle of incidence does not significantly affect the penetration depth, rather it affects the angle of deflection, scattering, and other electron interactions as the beam traverses through the specimen. The production of secondary, Auger, and backscattered electrons takes place due to the interaction of the electron beam with the sample surface. It also accompanies the production of characteristic, continuum, and fluorescent X-rays (Figure 2).

The elastic interaction between an electron beam and the sample results in electrons reflecting back, termed as backscattered electrons (Figure 2). These electrons are used for generating high-resolution images of the constituent elements present in the specimen. The inelastic collision results in relatively lower energy electrons originating from the atoms of the sample, are known as secondary electrons, and are helpful in investigating the topography of the specimen surface. Auger electrons are emitted when excited atoms release energy and are characteristic of the sample elements. These electrons help in understanding the elemental composition of the specimen. When the electron beam displaces an electron from the inner shell of an atom, another electron from a higher valence shell takes its place, resulting in a small loss of energy in the form of an X-ray photon. It is considered a characteristic X-ray and helps in investigating the particular element from which it is emitted. The electrostatic force experienced by the high-energy incident electron beam due to the presence of atomic nuclei, results in deflections/accelerations/decelerations of electrons. This results in the production of continuum X-rays (also known as Bremsstrahlung or Brems X-rays) having a continuous spectrum ranging from low to high energies (Figure 2). The continuum X-rays do not contribute towards primary elemental analysis; however, they help in studying the interaction between the sample and the electron beam. Fluorescent X-rays are a subset of characteristic X-rays, resulting from the filling up of the inner shell by outer shell electrons (Figure 2). Characteristic X-rays are emitted from the vacancy left by an ejected inner-shell electron, while fluorescent X-rays are produced when the outer-shell electron fills the vacancy. Fluorescent X-rays contribute valuable information about elemental information in addition to the main characteristic X-rays. They also help in studying the background radiation in the X-ray spectrum [11] (Figure 1).

The signals of this electron and X-ray production are collected by various detectors present in the specimen chamber of SEM. A monitor is fed with the signals from each detector, and a rectangular pattern of parallel scanning lines is synchronized with the electron beam [11]. The field emission gun SEM (FEG-SEM) can produce high-resolution secondary electron images, owing to the intense electron beam, and is capable of achieving sub-nanometer to nanometer-scale resolutions [46].

It is important to understand the meaning of magnification value in SEM images. In general, the magnification value provides information about the size ratio in between the actual and the enlarged image of specimen. SEM produces high-resolution images for visualizing the material surfaces. During the imaging process, the level of enlargement applied to the specimen is given by the magnified value of the SEM image. This magnification is usually expressed as a numerical value (such as 1,000x, or 10,000x) visualizing how many times larger the imaged structures or features are shown, as compared to the actual sample. It is one of the fundamental features of SEM to have the ability to control magnification. The level of magnification can be adjusted to have an overview of the specimen’s surface structure or to focus on any specific structural details. Figure 3 shows ilmenite micrographs having various magnification levels, aimed to analyze the existing (a) cracks, (b) furrows, and (c) particle shape in the sample [47].

1.2.1. Specimen Preparation

For the production of high-quality and accurate SEM images, the sample preparation stage is very important. The SEM analysis is susceptible to distortions, artifacts, and other issues in case of improper specimen preparation. The sample of interest can be a solid material, a biological specimen, or belonging to any other area of the object to be analyzed. The specimen material is mounted on a stub or holder using an adhesive conducting double-sided tape or with other mounting techniques. The SEM stubs are electrically conducting pads. No special specimen preparation is required for conductor or semiconductor materials. For insulator materials, the image is distorted by charging the sample, and therefore a conduction path to the ground is required for clear image production [11]. If the sample is moist, it is ensured that the sample is completely dry before going into the SEM analysis stage. The moisture can introduce charging effects thereby distorting the quality of the image. For materials of interest without or with lower electrical conductivity, a thin coating of metals such as gold, platinum, palladium, and chromium is applied to prevent charging effects [48,49,50]. Samples can be trimmed, fractured, or cut to the expose the surface of interest to the electron beam, and to make the geometry and size of the sample suitable for SEM analysis.

1.2.2. Imaging Process in the SEM

The SEM images are formed by using various signals (Figure 2) collected by the detectors, present in the collection chamber. Each signal offers different types of imaging information for the sample [11]. Secondary electron imaging (SEI) is an extensively utilized imaging mode in SEM, which produces images by detecting secondary electrons [51]. It provides topographic information such as surface textures, shapes, and features. Backscattered electron imaging (BSEI) is generated by detecting backscattered electrons coming from the surface of the sample due to interaction with the primary electron beam [52].

BSE images indicate compositional contrast, with respect to the atomic number of the elements present in the sample (Figure 4). This atomic number contrast provides tremendous value in detecting elements in the samples containing a variety of chemical compositions. Elements with higher atomic numbers appear brighter in BSE images, while darker appearance represents the elements having lower atomic numbers [53,54,55,56]. This feature is especially helpful for mineralogists and geologists as it allows the identification of various mineral phases present in a rock sample. BSE provides value in analyzing the sample surface topography by showing surface texture, morphology, and roughness, which may not be clear in secondary electron images. Certain features of the sample can be studied by BSE contrast enhancement, as it allows characterization of subtle compositional variations. BSE imaging is also helpful in studying the non-conductive elements, which is not the case with secondary electron images. BSE imaging can also be coupled with other diffraction and spectroscopy techniques, such as electron backscatter diffraction (EBD) for analyzing the crystallographic properties of materials at a granular level, and with energy-dispersive X-ray spectroscopy (EDS) for quantitative mapping of elemental distributions.

When high-energy electrons coincide with the sample, some materials have the tendency to emit light, imaging that signal is considered as cathodoluminescence imaging (CLI) [57]. The luminescent properties and defects of the sample material are revealed by CLI images. The electrical properties of materials are studied by using the electron beam-induced current (EBIC) technique [58]. It is specially used for semiconductor materials with localized charge carriers. Electron-hole pair in a semiconductor material is created with the help of the primary electron beam. With the application of external voltage, the created charge carriers start moving in response to the acting electrical field, indicating a measurable current, which is used to investigate the electrical properties of materials. This technique is also valuable in the identification of defects, grain boundaries, and other microstructural features affecting electrical behaviors. The electrical functionality of semiconductor devices is studied with the aid of voltage contrast imaging (VCI), which indicates the variations in electrical potential or voltage across the surface of the specimen [59].

1.3. Fundamental Theoretical Calculations

Crewe et al. in 1969 demonstrated the basic theoretical calculations that were helpful in the designing and selection process of SEM [60]. Their work helped in identifying the correct probe size for SEM. The aberrations of diffraction and electron gun, as well as the first order image of the field emission tip aid in determining the size of examining SEM probe at the specimen. The diameter ($d_s$) of an effective source leads toward an image with the following correlation:

$$d_s=2mR{\left(\frac{\overline{v_T}}{v_1}\right)}^{\raisebox{1ex}{$1$}\!\left/ \!\raisebox{-1ex}{$2$}\right.}$$

(1)

where $m$ is the magnification of the gun, R represents the actual radius of the tip, $\overline{v_T}$ indicates the average transverse energy of electrons coming out of the tip (~0.2 V), and $v_1$ is the emission voltage required to produce 1 µamp emission current. The term ${\left(\frac{\overline{v_T}}{v_1}\right)}^{\raisebox{1ex}{$1$}\!\left/ \!\raisebox{-1ex}{$2$}\right.}$ is the characteristic of a field emission source and indicates the reduction factor of effective source size.

The theoretical spot size is affected by the aberrations of the gun with the following two terms:

$$d_a=\frac{m{C}_s{\alpha }_1^3}{2}$$

(2)

$$d_c=m{C}_c{\alpha }_1∆V$$

(3)

where $d_a$ is spherical aberration, $d_c$ is chromatic aberration, $C_s$ is the spherical aberration constant, $C_c$ indicates the chromatic aberration constant, ${\alpha }_1$ is the entrance half angle of electron bean, and $∆V$ represents the total energy spread of electrons. $∆V$ is maintained such that the total energy spread of electrons leaving the tip remains 0.2V, while variations in $V_0$ and $V_1$ can be considered negligible [60].

At the defining aperture, the diffraction effect should be included. The diffraction contribution to the final spot size ($d_d$) can be calculated as follows:

$$d_d=\frac{0.6m{\mathsf{\lambda }}_1}{{\alpha }_1}$$

(4)

${\mathsf{\lambda }}_1$ represents the electron wavelength at the first anode. The focused spot diameter can be estimated by combining the four terms as follows [60]:

$$d_{rms}=\sqrt{d_s^2+d_a^2+d_c^2+d_d^2}$$

(5)

2. Scanning Electron Microscopy and Mineral Characterization

SEM makes use of secondary electron imaging to analyze the surface topology and morphology of micron/nanometer scale minerals [61]. For a comprehensive understanding of microstructure and mineral components, the SEM method is usually combined with X-ray techniques to complement the acquired information [62,63,64,65]. The infrared spectroscopy method is helpful in identifying chemical species and determining the molecular structure of the minerals. This technique has been widely used in mineral characterization [66,67,68,69].

One of the major quantitative analysis methods in mineral analysis is X-ray diffraction (XRD). It correlates the content of minerals with diffraction density, which helps in identifying and quantifying the minerals present in the sample [70,71]. For example, XRD can be used to analyze the calcite and nahcolite in saline brine [72], to evaluate the deposit by identifying minerals in phyllite [73], to examine the order degree of dolomite [74] and study the content of calcite and dolomite in carbonate rocks [75]. XRD is a rapid and accurate method for quantitative mineral analysis, however, some mineral compositional structures could lead to errors in analytical results [70].

Combining the qualitative analysis with quantification assessment methods can provide a better understanding of the investigated minerals. Such methods include SEM energy dispersive spectroscopy (SEM-EDS) [75,76,77,78], automated SEM mineral liberation analysis (SEM-MLA) [79,80,81], and quantitative evaluation of minerals by scanning electron microscopy (QEMSCAN) [82,83,84]. These methods incorporate a mineral quantitative analysis system by an using energy spectrometer and SEM. For accurate identification of minerals, backscattered electron (BSE) images are used, which can reflect the difference between the X-ray energy spectrum and mineral phase composition [85,86,87]. The quantitative analysis of rare earth minerals is a challenging task with conventional identification methods, the above-mentioned techniques have attained the rare earth minerals identification. The problems in the usage of these methods pertain to the difficulty in application, promotion, and high measurement cost.

2.1. SEM Energy Dispersive X-Ray Spectroscopy (SEM-EDS)

When the electron beam, emitted from the gun, penetrates and interacts with the volume beneath the sample surface, X-rays are generated. This is a well-established principle in physics, the deceleration of electrons due to their entrance in the Coulomb field of specimen, results in loss of electron energy and emits photons. In SEM analysis, similar X-ray photons are emitted which are characteristic of the sample under investigation [85], as shown in Figure 2.

The quantification scheme is delivered by measuring the X-ray intensity. This was illustrated by Heinrich and Yakowitz in 1968 in their publication namely, Quantitative Electron Probe Microanalysis [88], which later became the standard for developing X-ray fields. At that time, X-ray absorption, determination of correction factors at the instant of electron penetration and scattering, and conversion of X-ray intensity to the relative concentration were missing. Many problems pertaining to the electron probe field were solved with the development of energy dispersive spectrometry (EDS). At present, various studies have incorporated SEM-EDS for qualitative and semi-quantitative analysis in a variety of subject areas [89,90,91,92,93,94,95].

The schematic diagram of the energy dispersive spectrometer is shown in Figure 5. The X-ray detecting system (which is a solid-state detector) separates the characteristic X-rays of various elements present in the sample. Then the EDS system software analyzes the energy spectrum to determine the amplitude of particular elements, and electrical signals are generated from respective photon energy. This results in qualitative and quantitative determination of chemical composition maps of the elements present in the sample [85]. SEM-EDS have been used in a variety of fields for mineral characterization [96,97,98,99,100,101,102].

2.2. SEM-Based Automated Mineralogy (SEM-AM)

SEM-AM is a tool that was initially designed to characterize mineral processing products and ores. The measurement process starts with collecting backscattered electron (BSE) images, which are analyzed with image analysis software procedures. Based on BSE image adjustments, the energy dispersive X-ray spectra (EDS) are gained at selected points. The EDS spectra of the sample is then classified based on the list of approved reference EDS spectra. Relevant software providers offer services such as particle analysis, EDS spectral mapping, sparse phase search, and point counting modal analysis using four principal SEM-AM measurement routines and different classification algorithms, which can be used based on the analysis requirement. The main challenges of the process are materials with very different hardness, polishing of relief surfaces in particles, and electron beam stability and appropriate non-evaporating epoxy resin mixtures [80].

SEM-based automated mineralogy (SEM-AM) is still under-utilized, despite the fact that SEM instruments are widely distributed in industry, geosciences, and material research. SEM-AM can produce valuable results in a variety of major applications by characterizing the primary ores, and optimizing the mineral concentration, flotation, comminution, and metallurgical processes in the mining industry with the generation of quantified reliable data [103,104,105,106,107]. Beyond the classical fields, the potential of SEM-AM gains further interest on scientific and economic grounds. Some closely related topics are ore fingerprinting, metallurgy, and applications in petrology [108,109,110].

SEM-AM systems are a combination of hardware platforms, processing software, and specific image analysis. Any SEM with minor adjustments can be used as a hardware tool for SEM-AM. These adjustments include a high-vacuum operation mode and additional internal mainboards. The vacuum pressure of 10^-5 to 10^-7 Pa is required for its operation. The electron source of Tungsten cathodes and field emission guns can be employed. Tungsten cathodes can be used for economical operation; however, field emission guns are recommended for long-term stability of electron beams for automated measurements. The speed of analysis and the X-ray count rate are increased in SEM-AM by employing two or more EDS spectrometers in the SEM hardware. Multiple samples can be accommodated in a large sample chamber for simultaneous analysis in a single measurement session. A very accurate stage movement of SEM allows precise positioning using small intervals. For valuable analysis results, a fine-quality backscattered electron (BSE) detector is required. In SEM-AM analysis, BSE image quality and BSE image stability are important factors, as the resultant image (in combination with the EDS spectrum) is used for phase or mineral discrimination. Prior to the measurement, fixed working distances must be set to allow constant BSE image grey levels [80].

Keeping the image calibration constant makes sure that a specific phase or mineral always possesses the same BSE image grey level. The calibration process can be conducted with various BSE image grey levels of reference materials such as quartz (dark grey), copper (intermediate), and gold (very bright) [80]. A choice of calibration reference materials should be made based on the sample materials to be investigated. For example, many slags, industrial ashes, or particulate materials are investigated using SEM-AM, and quartz or copper are used for calibration with BSE image grey levels of dark grey to intermediate. This results in SEM images with better resolution and quality. For SEM-AM technology, four principal measurement routines can be outlined, which starts with collecting BSE grey-level image with respect to the calibrated grey level, as shown in Figure 6. The upper row represents the BSE images, while the bottom row indicates the EDS images of SEM-AM one measurement frame. White or black crosses denote the points of X-ray analyses (only some points are shown). Figure 6 represents the EDS point counting technique used for the quantification of modal composition. Figure 6 indicates particle analysis by EDS, which has been developed for fast automated characterization of grain mounts with up to 10⁶ particles, such as milled products from mineral processing and mining. Figure 6 denotes the sparse phase search method, which combines single spot EDS spectral analysis of grains with a BSE grey tone value trigger. It is valuable in massive rock applications, such as drill cores and in thin sections. Figure 6 expresses EDS spectral mapping which combines BSE image levels with the mapping of EDS spectrum. This method is helpful, especially in cases where fine details of mineral intergrowth are considered. In summary, SEM-AM is a powerful tool for mineral characterization and has actively been used in recent literature [111,112,113].

2.3. Automated SEM Mineral Liberation Analysis (SEM-MLA)

Recent software developments in SEM have incited a dominant growth in applications of solid matter investigations. One of the economic solutions is the use of mineral liberation analysis (MLA) for optimizing the mineral processing methodology of metallic ores. SEM-MLA has been an important drive for transforming numerous software versions of SEM applications [80]. SEM-MLA was designed to quantify the mineralogy of ores. After the mining process, the ore is processed to increase the concentration of minerals of interest (and value). The processing of the ore is also important for removing minerals of no value or those having detrimental effects on the required mineral products. This processing of grinding the ore and liberating the mineral of interest provided rapid automated analysis of target minerals and extensively improved the process.

Mineral liberation analyzer (MLA) based on SEM was developed in the late 1990s by the JKRMC (Julius Kruttschnitt Mineral Research Centre, Australia) and it is commercially available now [114]. In MLA, minerals are differentiated by attaining and combining the information gathered from the EDS and BSE. Depending on the size range of particles in the sample, size fractions from the samples are produced. Then liberation is measured in each size fraction, followed by the liberation reconstruction of the whole sample. The measurement of mineral liberation is usually carried out through one of the two methods, i.e., either the area method or the linear intercept method. Liberation by area measurements has shown lower stereological error as compared to the linear measurements.

It is important to note that the liberation measurements by linear intercepts are known as one-dimensional, while the area method ones are called two-dimensional liberation. Both of the measured liberations are lower dimensional projections of the true volumetric liberation (which is three-dimensional). Stereological correction is based on the stereological transformation and prediction of liberation measurements. This stereological correction can be based on entropy regularization [115]. The correction of the apparent liberation and the production of three-dimensional liberation have also been described in several other investigations [116,117,118]. Various operating modes for the MLA system are available, i.e., X-ray modal analysis (XMOD), particle X-ray mapping (PXMAP), selected particle X-ray mapping (SXMAP), sparse phase liberation analysis (SPL), standard BSE liberation analysis (BSE), extended BSE liberation analysis (XBSE), and rare phase search (RPS) [119]. The use of SEM-MLA is shown in Figure 7, for quantifying the mineralogy of a hydrothermally overprinted alkali plutonite [81].

2.4. Quantitative Evaluation of Minerals by Scanning Electron Microscopy (QEMSCAN)

Traditional mineral analysis based on microscopy could not provide the required data because of the absence of quantitative information and the very small size of the particles of interest. QEMSCAN technology, initially termed QEM*SEM, demonstrated the potential of revolutionizing automated mineralogy [120]. In a mold, the particulate mineral sample is mixed with epoxy resin, and the sample surface is prepared using cutting, polishing, and carbon coating. The sample is scanned using SEM in backscatter mode, enabling the differentiation of particles with the background. After the identification of particles on the resin block, their composition is systematically mapped using EDS. In contrast to the most modern SEMs containing single EDX, QEMSCAN possesses the attribute of having multiple EDX at the same time, enabling rapid quantitative mineralogy. The acquired EDX signals are then compared with reference known materials in the database and assigned a mineral name or to a chemical compositional grouping. With this process, the mineralogy of the sample can be conducted, particle by particle, analysis by analysis [120]. QEMSCAN locates the particles using a BSE signal, while identifying the mineral by an EDS signal. It can be compared to the SEM-MLA which makes more use of the BSE signal than EDS one for identifying the mineral. SEM-MLA works very well for bright phases (such as platinum group element minerals).

Among SEM-EDS techniques, QEMSCAN is one of the most widely used, which offers quantitative characterization of minerals, ores, and other mineralogical compounds [121,122,123,124,125]. QEMSCAN is usually used in conjunction with other analytical techniques such as electron probe microanalysis (EPMA) and X-ray diffraction (XRD), as shown in Table 1 [126]. Figure 8 indicates the use of QEMSCAN for identifying the mineral distribution of four samples [126]. It shows the presence of geothite, quartz, clay, limonite, and other silicate minerals.

Table 1. Techniques used for investigating mineralogy and their comparison. ✔ indicates good, ● represents poor, while (✔) suggests it is possible but not recommended [126].

Investigation	Electron microprobe	XRD	QEMSCAN
Mineral textures	(✔)	●	✔✔✔
Mineral distributions and associations	(✔)	●	✔✔
Mineral specific particle size information	(✔)	●	✔✔
Mineral abundances	●	✔✔✔	✔✔✔
Amorphous minerals (geothite, silica)	✔✔✔	●	✔✔✔
Distribution of minor metals within minerals	✔✔✔	●	✔
Crystallinity (clays, silica, geothite, and limonite)	●	✔✔✔	●

Table 1. Techniques used for investigating mineralogy and their comparison. ✔ indicates good, ● represents poor, while (✔) suggests it is possible but not recommended [126].

Investigation	Electron microprobe	XRD	QEMSCAN
Mineral textures	(✔)	●	✔✔✔
Mineral distributions and associations	(✔)	●	✔✔
Mineral specific particle size information	(✔)	●	✔✔
Mineral abundances	●	✔✔✔	✔✔✔
Amorphous minerals (geothite, silica)	✔✔✔	●	✔✔✔
Distribution of minor metals within minerals	✔✔✔	●	✔
Crystallinity (clays, silica, geothite, and limonite)	●	✔✔✔	●

The above-described four analytical techniques are distinct but complement each other in comprehensive mineralogical analysis. High-resolution images are provided by SEM, elemental composition analysis is provided by EDS, while SEM with automated mineralogy involves a thorough mineral characterization. Most of the SEM with automated mineralogy equipment use have EDS incorporated, where software utilization provides objective and quick mineral characterization and other analytical results. QEMSCAN is a specific instance of the broader concept of automated mineralogy, which represents a specific system and brand used for comprehensive mineral characterization. MLA systems are used in geology, mining, and mineral analyses for ore processing and beneficiation, as they provide insights into the degree of liberation of valuable minerals from the host rock. Combining these techniques together offers constructive value to the mineral characterization and analysis process, by not only providing high-resolution surface images, but also offering the elemental composition of the samples, the degree of liberation of minerals, and saving time in determining the presence of valuable minerals present in the ores. In short, SEM demonstrates itself as a powerful technique for the characterization and analysis of various minerals [127,128,129].

Mineral characterization is usually carried out with more than one technique, for clear identification and quantification. Therefore, the SEM analysis for mineral characterization is accompanied by several other analytical techniques, as mentioned in Table 2, which have been applied in some of the recent publications.

3. Uncertainties in SEM Measurements

The advancement of SEM with automated mineralogy has provided a quick and relatively economical quantitative mineral analysis solution. However, the absence of statistical errors makes the robustness of the results uncertain. This could damage the reliability of the technical solutions taken on the onus of these quantitative outcomes [153]. The automated mineralogy-based measurements have been studied with several methods for the estimation of uncertainties. For instance, a statistical approach was developed by Benvie et al. in 2013, for using SEM automated mineralogy in accordance with the diagnostic leaching tests [154]. It was concluded that, for deriving the standard deviation and the background variance, at least two-grain mount measurements were required for each head and leach residue sample. In another study, the variability in mineral liberation analyses and mineral quantity was investigated by Lastra and Paktunc in 2016 [155]. They studied a fraction of sulfide flotation rougher concentrate of -509 to 208 µm size through inter-laboratory testing. It was found that mineral quantities are having good agreement with the data, but mineral association and liberation analyses showed less agreement. It portrays a hint towards the idea that it is not necessary that correct mineral liberation and association can be found with correct mineral quantities. Guseva et al. in 2021 evaluated analytical errors in mineralogical measurements by applying the point counting method via binomial distribution approximation [156]. It came out that binomial approximation may not fit well with all the cases, especially with coarse materials, and other methods more suitable to the case should be used, such as the estimation of the confidence method [157] or bootstrap resampling method [158].

The estimation of errors in textural characteristics measured by automated mineralogy can be identified efficiently with the bootstrap resampling method [159]. For instance, the bootstrap approach can help in evaluating the uncertainties related to particle properties measured by SEM automated mineralogy for the evaluation of magnetic separation efficiency [160,161], density separation processes [162], and the simulation and statistical modeling of mechanical separation processes [163]. The bootstrap resampling method considers a population of N samples, takes M random subsets and replaces the randomly selected samples in order to make sure that the entire population is available for sampling [164,165]. The accepted statistical methods which use the point counting method on polished sections and assess errors in mineral grades, agree well with this bootstrap method [166,167,168]. This method has the advantage of being assumption-free and can be applied to a wide range of particle characteristics [158]. It does not assume a bionomical distribution. These methods imply that the standard deviation of mineral grades is proportional to the square root of the number of particles measured, or the total area of particles measured. The relative standard deviation of measurements for any mineral grade can be estimated as follows [169]:

$$RSD=a{x}^{-0.5}$$

(6)

Where, $RSD$ is the relative standard deviation, $a$ is a coefficient, and $x$ is the mineral grade. The bootstrap method can also provide information about the measurement of how much total area (grains) to reach a given uncertainty. In addition to the uncertainty, SEM also has some drawbacks including, but not limited to, a limited depth of penetration majorly providing the surface information and low accelerating voltages providing low-resolution images, while increasing the voltage starts damaging the surface of the sample.

3.1. Constraints in Phase Identification by EDS Spectra

It is a common claim in SEM-based automated mineralogy studies that minerals can be detected, identified, and quantified by their characteristic EDS spectrum (an example is shown in Figure 9 indicating feldspar mineral albite [80]). However, this claim cannot be fully correct, as minerals are characterized by their lattice structure indicated by XRD first, and then comes the use of elemental composition information provided by EDS spectrum quantification. Therefore, mineral identification remains incomplete with the use of the EDS spectrum only, based on its foundations on elemental composition. Identifying a mineral with chemical composition alone can be misdirecting, as there are examples of minerals with similar chemical composition but different crystal structures, based on the crystallization conditions of minerals. For instance, pseudorutile and ilmenite, are titanium-iron oxide minerals, but both exhibit different crystal structures [80].

Another challenge to the mineral detection, identification, and distinguishing using EDS spectra is with minerals having very similar elemental composition, such as hematite (Fe₂O₃) and magnetite (Fe₃O₄). Hematite is composed of 70% by weight Fe and 30% by weight O, while magnetite is made up of 72% by weight Fe and 28% by weight O. The EDS spectra for both minerals appear to be very similar, and the very trivial differences in Fe and O peaks cannot be resolved apparently. In such scenarios, it is a good idea to use the BSE image grey level as an additional distinguishing standard. It must be noted that for such a measurement, a specific BSE brightness and contrast calibration is required. Another challenge is the detection range of EDS spectra, as it does not cover the whole elemental periodic system. For example, the first light elements cannot be detected by EDS, such as H, He, Li, and Be. It is, therefore, recommended to complement EDS spectra with XRD and XRF methodologies for mineral identification and quantification [80]. Some other the limitations of EDS spectra include longer mapping causing damage to the samples, low sensitivity of light elements, quantitative accuracy is not very high, information about the chemical composition only (not about functional groups or chemical bonds) and overlapping peaks making it difficult to distinguish among elements present in the sample.

3.2. Sample Preparation and Related Issues

For the success of any SEM analysis, an optimal sample preparation process is essential. A wide variety of samples can be analyzed using SEM. The configuration of the sample holder systems and the size of the SEM sample chamber are the defining parameters for choosing the type of samples for investigation. Grain mounts in round epoxy blocks are usually used for particulate or granular samples. If the samples are massive and compact matter, such as rocks, petrographic glass-mounted sections can be used. Depending on the type of the sample, the production of thin grain mounts on glass is also possible. Two important configurations must be maintained, whether it is samples on glass or round block sample holders i.e., the holder ought to be mounted perpendicular to the electron beam and parallel to the BSE detector [80].

Figure 10. Epoxy adhesives shown using SEM having (a) epoxy resin only, (b) epoxy resin with aluminum nitride particles, (c) Epoxy resin with aluminum nitride and graphene oxide, and (d) Thermal conductivities of various test samples. CC-BY [170,175].

Figure 10. Epoxy adhesives shown using SEM having (a) epoxy resin only, (b) epoxy resin with aluminum nitride particles, (c) Epoxy resin with aluminum nitride and graphene oxide, and (d) Thermal conductivities of various test samples. CC-BY [170,175].

The grain mounts in epoxy blocks are the best form to prepare samples, if the sample material is non-compact, particulate, or granular matter, which can be ground, or hand-picked single, or broken grains [171]. A potential problem occurs when the grains are not easily separated with the same colored grey-scale BSE image, as most of the SEM-AM software packages are unable to distinguish between them. The use of pure graphite is beneficial in such cases, as it can be utilized in stirred form as a distance material into the epoxy resin blocks [171]. In some granular sample cases, a wide range of densities can exist among the phases present in the sample. With the stirring process of the sample grains with graphite-saturated epoxy resins, grains with larger size and high densities tend to move towards the bottom of the holding block, and it is more probable that the small grains will be missed from the analysis. One good practice for dealing with such kinds of samples is cutting the round blocks in vertical slices, which can be remounted as vertical sections [80]. It is also possible to study other materials such as polymers and coals, with the use of some EDS detectors. Since the BDE grey value of this organic matter is similar to the one of epoxy resin, an alternative embedding material should be used [172]. Carnauba wax is an alternative material that can be used for embedding in these cases [173]. Carnauba wax is a very soft material, which makes it difficult to be polished. One possible solution is to double-mount the Carnauba wax in epoxy resin blocks. Another prospective solution could be the doping of iodoform in epoxy resin [172,174]. The organic matter has, therefore, a lower atomic number than the epoxy resin, which makes epoxy to be considered as a background material. A wide variety of epoxy resins are available for this purpose [175]. The SEM images of some epoxy resins and their respective thermal conductivities are shown in Figure 10. In addition to the variety, the proportions of the hardener and the filler can be varied. The challenges in choosing the epoxy resins are ones that remain stable under the 25 kV electron beam, which do not evaporate under high vacuum conditions, and which harden within convenient temperature conditions and time frames. The recommended ways of solving such problems are continuous application tests.

The complication of the sample preparation procedure depends on the type of the sample material. If it is solid, dry, compact, and massive, the preparation of thin and thick sections is quite simple. In the case of brittle and/or porous material, epoxy resin is impregnated with a previous material for stabilization before sawing. Thin and thick section production has been reported by several studies [176,177,178]. Usually, silicon carbide SiC (with 600 to 1000 mesh) is used for lapping of the sample material behind the mounting on glass. In the standard lapping procedure, a SiC 1000 works best for brittle and soft materials, with a minimum substance loss, as compared to the SiC 600. If the sample contains minerals with different optical properties but a closer chemical composition, thin sections are advantageous, as an optical microscope can also be used to check the minerals and phases. Besides, the microscope with polarized light can be used for recognizing the samples with glassy phases owing to their optical isotropy. The reference EDS spectra list can be compiled based on this set of information [80].

A plane and well-polished surface is required for SEM-AM to analyze grain mounts of thin and thick sections and mounts in epoxy resins. Every material needs a specific treatment, so it is safe to state that the polishing part is a work of craftsmanship. In most cases, water is used in the polishing procedure. If there is a chance of water reacting or mixing with the minerals or materials, the sample preparation procedure can be carried out with water-free liquids such as ethylene glycol [80]. A variety of industrial ashes such as power plant and sewage ashes, can contain anhydrite, and the use of water-free liquids is recommended in such cases. For the samples having varying degrees of particles’ hardness, the polishing plates covered with hard textile clothes are proposed. The plates with soft clothes having long fiber do work well for the samples containing minerals, soft metals, or ore minerals. The procedure of polishing the sample works well with decreasing grain sizes, for example, using abrasive papers first, then grinding, and then polishing powders on textile clothing. It is important to mention avoiding the use of lead-bearing polishing plates for general sample preparation, as it may cause sample contamination with lead. For the last step of sample polishing, the use of diamond powder with diamond paste or lubricant is very effective. The polishing procedure can be controlled using a reflected light microscope for inspecting the level of successive polishing steps. The impinging electrons in SEM should be dissipated well to obtain optimal BSE images. The use of carbon coating of the polished samples does provide the solution, which can be accomplished by either the evaporation of carbon-loaded thread, or electronic carbon thickness control, or carbon rods, etc. [80].

The quality of SEM images in publications is essential for clear communication and interpretation. It is also significant to ensure reproducibility and can avoid hinderance in the way of future research directions. Blurry SEM images also cause limitation in quantitative data extraction, and cause challenges to peer reviewers in analyzing and interpreting the results and understandings. Low-resolution images in scientific papers appear due to several reasons, some of which may be unintentional, while others are the result of constraints or limitations of the research process. The common reasons for the presence of low-quality SEM images in papers may include (but not limited to) instrument limitations, sample conditions, resource constraints including time and budget, image processing and acquisition, sample size, scope of the paper, image compression, historical or legacy data, and data storage and file size. For producing focused and clear SEM images for efficient transfer of information, the stigmator tool in SEM instrument should be properly utilized.

The stigmator is one of the critical components of SEM instrument, which is responsible for maintaining the astigmatism of the electron beam and adjusting the focus of the SEM equipment. While examining the fine details of mineral structures, astigmatism can cause distorted and blurry images. The stigmator ensures the symmetry and focus of electron beam, consequently producing quality SEM images. The proper use of well-adjusted stigmator allows characteristic mineral identification, enhanced elemental analysis, quantitative analysis, and precise imaging of microstructures. It also helps in enhanced imaging of thin sections, and provide crystal clear information about crystal faces, surface roughness and other textural attributes, which are essential for understanding the formation of minerals and digging deep into the geological history of the minerals.

Figure 11 shows wollastonite samples mounted on three stubs, as described in Table 3. Figure 12 shows the effect of layers and sputter-coating on SEM analysis by comparing wollastonite samples A, B, and C for three magnifications i.e., 5kx, 60kx, and 250kx. In the sample preparation stage, sample C was left uncoated to investigate the effect of sputter-coating, while samples A and B were coated with gold-platinum coating. It can be clearly illustrated in Figure 12 that all sample C SEM images are fuzzy, and dark with few very bright spots, and having few lines making it difficult to visualize the sample morphology. This is the charging effect, logically occurring due to the absence of conductive material coating. Another important aspect can be found by comparing the 60k and 250k SEM images of sample C with its 5k image. While charging effects are prominent in all, the SEM image with lower resolution provides better visualization features when compared to the ones at higher resolution. It suggests that whenever there are some samples where it is difficult to coat them with conductive materials, it is useful to snap SEM images at lower resolution. When comparing SEM images of samples A and B, it is observed that the morphology of the sample can be studied well with single-layered samples when compared with multiple-layered ones.

Table 3. Wollastonite samples prepared for SEM analyses.

Sample	Layer	Sputter Coating
A	Multiple	Applied
B	Single	Applied
C	Single	Not Applied

Table 3. Wollastonite samples prepared for SEM analyses.

Sample	Layer	Sputter Coating
A	Multiple	Applied
B	Single	Applied
C	Single	Not Applied

For making sure the stigmator is well-adjusted for taking quality SEM images, the SEM instrument should be allowed to stabilize and warm up, which will comply that the electron source and other components of the instrument are in steady state before any adjustment. There are usually two stigmation modes in SEM, i.e., objective lens stigmation and condenser stigmation. The specific requirement of the imaging task will require the selection of appropriate stigmation mode. Misalignment in electron column and detectors can adversely affect the SEM image quality, that’s why it is important to ensure the proper alignment of these components before starting the imaging process. Some of the latest SEMs are coming with automated alignment features. Sample preparation stage is also important for avoiding any contamination and charging effects hindering image quality. Dry, clean, and well-mounted samples provide a foundation for high-resolution SEM imaging. While focusing the electron beam on the sample, it is required to adjust the astigmatism controls to obtain a sharp image at low magnification. It is considered a good practice to select a well-defined edge or feature on the investigated sample as a reference point for stigmation control adjustments. Astigmatism is usually indicated by distortions in the SEM image, such as asymmetrical or elliptical features. In the SEM imaging process, it is important to observe such biases. The X- and Y-stigmation (representing horizontal and vertical stigmation respectively) need to be adjusted for eliminating any distortions. The focus of the electron beam should be rechecked and adjusted if necessary for proper and clear imaging. For optimal SEM imaging, several iterative adjustments might be required. Figure 13 compares the stigmator adjustment effect on SEM images, which vividly indicates the importance of stigmator adjustment in SEM analysis. Also, Figure 14 shows the effect of maintaining electron beam for a longer period of time at a single point, which damages the surface of the sample. This issue can be resolved by reducing the voltage of electron beam, but that comes at an expense of lower resolution of the SEM image. Therefore, it is recommended to find an optimum voltage-resolution combination which works well for a specific type of sample material.

4. Future Research and Directions

SEM is a powerful and resourceful tool that can be employed in various fields for the analysis and characterization of minerals such as mining [179,180,181], oil and gas [182,183,184], forensic science [185,186,187], biomedical research [188,189,190], geology [191,192,193], material science [194,195,196], and environmental science [197,198,199]. There is an evolution witnessed in the mineral processing engineering system. Previously, there were extended levels of complexities and practical challenges in managing and optimizing a mineral processing plant, which did not make way for data-based optimization development. The empirical characterization tests were used for designing and the operator intuition played a key role in plant operation, which is subjective and varies from case to case. Now, the technology is present to make the whole process objective, which has the capability to collect, manage, and analyze the retrieved information in large amounts. These technologies, artificial intelligence (AI) and machine learning (ML) possess the revolutionizing capacity for designing, managing, operating, and analyzing mineral processing plants [200].

With the advancement of ML and deep-learning technologies, the automation of many complex tasks with human execution accuracy is becoming possible, which can replace repeating repetitive and tedious tasks, mitigate subjective human errors, lower the analysis costs, and improve the time efficiency of the characterization process. Deep-learning methods in microscopic imaging are now developed to automate mineral grain segmentation and recognition [201,202,203]. With the recent AI developments, the intelligent identification and quantification of minerals is becoming possible [204,205,206]. There are voids in-between geological and artificial intelligence sciences, which can be filled with the latest research advancements. This can take the SEM mineral characterization to another level, with a greater level of objective autonomy and quicker solutions for mineral analyses.

The intelligent identification of minerals can be conducted in a generally consistent process, which can be divided into five segments, i.e., mineral datasets acquisition, preprocessing mineral datasets, training the mineral identification models, validating the accuracy of mineral identification tool, and ensuring the synchronization and integration of the intelligent tool with existing SEM systems. Cai et al. recently used a multi-scale dilated convolutional attention network for rapid identification of minerals with portable Raman spectroscopy [207]. A similar approach can be used for the development of a portable intelligent SEM system. Hao et al., in the recent past, used SEM/EDS data in machine learning applications for automatically classifying the heavy minerals in river sand [208]. Likewise, models can be trained for quantifying the mineral composition of ores. In another recent work, X Zeng et al. made use of a deep convolutional neural network by combining mineral image features and hardness data, for mineral identification purposes [209]. This investigation is an intuitive way of utilizing deep learning methods for mineral characterization by integrating the mineral data sets comprising various properties. Intelligent systems based on a cascade approach for mineral identification in thin sections are already on their way for space explorations [210].

It is a matter of extending it to the SEM systems for more in-depth insights. The future research directions in SEM lead towards the possible incorporation or upgradation of such tools in SEM for enhancing the effectiveness of SEM as a material characterization tool. This would not only help in reducing the factor of human error by providing objectivity to the mineral analysis, but also by providing cost-effective solutions to those extents where human intervention has never been thought of before. It could include investigating the mineral concentration at the nano-level present in living organisms and the robotic integration of SEM tool with AI and ML for studying the mineral compositions on other planets and stars. Another idea is the integration of SEM with other material characterization tools such as XRD, and by adding the incorporation of robotics, AI, and ML, the process can be automated to a further extent. One big challenge amongst several in this research direction is the proper use of robotics for sample preparation. The system needs to be designed in a way that it first measures the conductivity and other essential properties of the objective material, then following the respective algorithms for a particular material type. The pinnacle of robotics and instrumentation can play a very important role in this development. This idea on formalization can be especially helpful for visualizing the mineral composition in locations where human intervention is usually not possible. Consider a robotic SEM-based characterization tool, trained with generative ML and AI, containing depths of mineral databases, and programmed in such a way that it is semi-controlled to choose the location of interest for scanning, and then it can go on auto-mode for scanning the raw samples and communicating real-time SEM and XRD information from depths of mines on Earth or on other terrestrial surfaces, such as the moon, mars, and other planets. In-situ and environmental SEM will facilitate the changes during the reactions. This set of information would transform the mining industry on Earth but will also revolutionize astronomical and space engineering. The developed portable SEM/ML/AI systems can help save millions of dollars for mining and space agencies. The human researchers would then be able to focus more attention on analyses, research insights, and further development of technology.

5. Conclusion

The present research review offered the synopsis of SEM fundamentals, working, sample preparation, and the imaging process. The theoretical calculations underlying basic SEM operation are discussed. This foundational set of information would be helpful for the engineers and scientists, who are inspired by the mammoth potential of SEM but have never gotten a chance to dig in-depth about the SEM operation and process. This comprehensive review briefly summarizes these multiple facets for efficient transfer of knowledge. In addition, the use of techniques such as energy dispersive X-ray spectroscopy EDS, automated mineralogy (AM), and mineral liberation analysis (MLA), in conjunction with SEM is discussed and research fronts are analyzed. SEM lacks statistical error, and therefore it is very important to especially look towards the uncertainties in SEM measurements. The present paper discusses the constraints in mineral phase identification by EDS. It also covers sample preparation and other analytical issues that come across while performing mineral characterization. The review then examines the possible integration of deep learning (DL), machine learning (ML), and artificial intelligence (AI) techniques into SEM to improve the robustness and objectivity of the mineral characterization process. It also discusses the idea of robotics integration with SEM for the development of portable and automated SEM units, which can collect, analyze samples, and communicate information with researchers, from locations that are difficult to explore on Earth (such as deep mines) and on other terrestrial grounds.