Abstract
Interfaces dramatically affect the properties of materials because their atomic configurations often differ from the bulk material. A determination of the atomic structure of the interface is, therefore, one of the most significant tasks in materials research. Electron microscopy and theoretical calculations have been effectively used to accomplish this important task. In addition, an informatics approach has recently been combined with theoretical calculations to efficiently determine the atomic structures of interfaces. This chapter introduces the determination of interface structures using an informatics approach (Bayesian optimization and virtual screening) along with advanced electron microscopy. In the informatics approach, calculation acceleration on the order of 10^{6} can be achieved. Determination of the interface structure with resolution better than ~45 pm is now possible using advanced electron microscopy. In this way, nanostructures at grain boundaries and heterointerfaces can be qualified. We will introduce these state of the art methods to investigate nanostructures.
Keywords
 Interface
 Electron microscopy
 Scanning transmission electron microscopy
 Bayesian optimization
 Virtual screening
Download chapter PDF
1 Atomic Structures of Interfaces
Interfaces are a kind of lattice defect inside materials and can have significant effects on the overall material properties. For instance, interfaces in polycrystalline materials, i.e., grain boundaries (GB), determine the ion transportation properties and high temperature mechanical properties [1,2,3,4]; an atomically controlled interface in a thin film often provides unique properties such as the formation of twodimensional gases [5, 6]. The fact that interfaces have different properties from the bulk is a consequence of the fact that they have different atomic structures from the bulk. Thus, for a comprehensive understanding of interface properties, determination of the atomic structure of the interface is crucial.
Since the atomic structure of the interface is strongly dependent on the crystal orientation, lattice planes, and terminations, a systematic study of the interface structure is indispensable for achieving a comprehensive understanding. Thus, the atomic structures of interfaces have already been extensively investigated. Because these characteristic atomic configurations at the interface appear within a very limited area (below 10 nm), high spatial resolution observations using transmission electron microscopy (TEM) and theoretical calculations using atomistic simulations have been effectively applied to investigate interfaces.
Similar to TEM, aberrationcorrected scanning transmission electron microscopy (STEM) has achieved sub0.45 Å spatial resolution [7], and direct atombyatom imaging is now routinely possible via annular darkfield (ADF) imaging. In addition, owing to the rapid improvement in detectors, interface chemical analysis using energydispersive Xray spectroscopy (EDS) and electron energy loss spectroscopy (EELS) can also achieve atomic resolution. In short, atomicresolution STEM has become a very powerful tool for characterizing the atomic structures of interfaces [8, 9].
In terms of calculations, extensive calculations are usually necessary to determine even one interface structure because of the geometrical freedom of the interface. Nine degrees of freedom (five macroscopic and four microscopic) are present in an interface. The number of atomic configurations to be considered often reaches 10^{4} in even the simplified coincidence site lattice (CSL) grain boundary, namely Σ grain boundaries [10, 11]. In a straightforward manner, as schematically illustrated in Fig. 8.1, structure and energy calculations for all candidates must be performed, and leading to optimized configurations and energies of these are obtained (E_{i,j} in Fig. 8.1). The most stable configuration with the minimal energy (E_{i, mim} in Fig. 8.1) can then be determined from the density functional theory/molecular dynamics (DFT/MD) simulation of the interface. Furthermore, the same “brute force” computation is necessary to determine other types of interfaces because the interface structure is dependent on the type of interface (ΣGB_{1}, ΣGB_{2}, … ΣGB_{N} in Fig. 8.1).
If the structure and energy of unknown interfaces could be determined more efficiently and accurately, the investigation of interfaces would be dramatically accelerated, which could lead to a deeper understanding of the mechanisms that give rise to interface properties. To more efficiently determine interface structures, a genetic algorithm method and a random structure searching algorithm method have been proposed [13, 14]. However, many trial calculations are still necessary to determine a single grain boundary structure. More recently, much more efficient methods based on machine learning techniques, including virtual screening and Bayesian optimization have been proposed by the present authors [12, 15,16,17]. Those methods are described below.
2 Informatics Approach for Interfaces
2.1 Virtual Screening
In this section, a virtual screening method for interface structure determination is described. Virtual screening is an effective method in timecritical problems and was applied to determine the structure and energy of an interface. This virtual screening technique has been used in drug discovery, where a prediction model was constructed using machine learning from a relatively small dataset and a large database consisting of the actual data and data predicted by the prediction model. Then, the candidate drug that is most likely to have the intended effectiveness is selected from the larger constructed database. More recently, this virtual screening method has been applied to discover new molecules for organic electroluminescence (EL) applications and has succeeded in its discovery aims [18]. We have applied this virtual screening technique to predict the structure and energy of certain interfaces [12].
The idea of our virtual screening method is illustrated in Fig. 8.2. A prediction model (predictor) is constructed via regression analysis of the training data, in this case ΣGB_{1} and ΣGB_{2}. Once the predictor is constructed, the grain boundary energies can be predicted from the initial configurations. Then, the candidate configuration that is most likely to give the minimal energy E_{i, mim (i=3, 4,… N)} can be determined. Next, the promising initial configuration is optimized using the structure and subsequent energy calculations. Finally, the accurate energy and stable structure are obtained (Stable ΣGB_{3 ~ N} in Fig. 8.2).
Seventeen [001] axissymmetric tilt CSL grain boundaries of Cu were considered in this chapter: Σ5[001]/(210), Σ5[001]/(310), Σ13[001]/(230), Σ17[001]/(410), Σ17[001]/(350), Σ25[001]/(430), Σ25[001]/(710), Σ29[001]/(520), Σ29[001]/(730), Σ37[001]/(610), Σ37[001]/(750), Σ41[001]/(910), Σ41[001]/(540), Σ53[001]/(720), Σ53[001]/(950), Σ61[001]/(11 1 0), and Σ125[001]/(11 2 0). To obtain stable structures for these grain boundaries, approximately 1,000,000 configurations must be considered. Namely, structure and energy calculations (such as DFT and MD) must be performed 1,000,000 times to determine the structures of these grain boundaries. To construct the predictor, Σ5[001]/(210), Σ5[001]/(310), Σ17[001]/(350), and Σ17[001]/(410) were selected as the training data, corresponding to ΣGB_{1} and ΣGB_{2} in Fig. 8.2. Those grain boundaries were selected as the training data based on the variance of their tilt angles and computational costs for their calculations. Structure and energy calculations for a total of 150,000 configurations, corresponding to approximately 15% of all possible configurations, were performed. We can confirm that the calculated structures are almost identical to the previously reported structures [19, 20], indicating that these training data are suitable for constructing the predictor.
The selection of descriptors for regression analysis is important when predicting the grain boundary energy of noncalculated structures. In this study, geometrical data for the “initial atomic configurations” are used as the descriptors. This choice enables one to predict the grain boundary energy without performing structure and energy calculations. The selected descriptors, such as the minimum and maximum bond lengths are listed in Table 8.1.
In addition to these descriptors, their square, inverse, exponential and exponential inverse values were considered. As a result, 83 descriptors were obtained, which were standardized to align their average and variance to zero and one, respectively.
The nonlinear support vector machine (SVM) method was used for regression analysis. In this study, the most stable structures and metastable structures of Σ5[001]/(210), Σ 5[001]/(310), Σ17[001]/(410), and Σ17[001]/(350) were considered for construction of the prediction model. We have selected those grain boundaries as the training data based on the variance of tilt angles and computational costs for their calculations.
There are two parameters in the SVM, the margin of tolerance and penalty factor. The best parameters were selected from combinations where the margin of tolerance was 0.001, 0.01, 0.05 or 0.1, the penalty factor was 10, 100, 1000 or 10000, and the variance was 10^{−2}, 10^{−3}, 10^{−4} or 10^{−5}, for a total of 64 different patterns. As a result, a margin of tolerance of 0.01, a penalty factor of 1000 and a variance of 10^{−4} were used as SVR parameters.
The results of the regression analysis for the training data are shown in Fig. 8.3a. Most data lie along the grey line, indicating that the predicted energies are equal to the accurate energies and that the regression analysis succeeded in correctly constructing the predictor. To evaluate the accuracy of the constructed predictor, the predictor was applied to Σ13[001]/(230) as a test situation. The results predicted by the predictor are shown in Fig. 8.3b. Most of the predicted grain boundary energies also lie on the grey line, indicating that the constructed predictor is also suitable for the test data. This result implies that the constructed predictor has the potential to predict the energy of the grain boundaries prior to the structure and energy calculations.
Here, we focus on the blue data point marked by the blue arrow in Fig. 8.3b. Based on the constructed predictor, the blue data point was predicted to provide the minimum grain boundary energy. It should be mentioned that the virtual screening method and the calculations of all candidates give the minimum grain boundary energy at the same blue data point. The predicted grain boundary energy is 0.96 J/m^{2}, which is only 10% larger than that the minimum grain boundary energy obtained from allcandidate calculations. It is also noteworthy that the predicted rigid body translation state (X = 5.0 Å, Y = 1.0 Å, and Z = 0.0 Å) is identical to the most stable rigid body translation state determined by allcandidate calculations.
We succeeded in screening all possible candidates and selecting the most promising candidate configuration for accurately provide the most stable structure. By performing the structure and energy calculation once for this rigid body translation state, a grain boundary energy and structure identical to those obtained from allcandidate calculations can be obtained. Namely, the stable grain boundary structure and energy can be determined with only a onetime calculation using the present virtual screening method, which is significantly more efficient than previously reported methods.
Since the constructed prediction model (the predictor shown in Fig. 8.2) was established, this predictor was also applied to other GBs. Here, based on the constructed predictor, the structures and energies of 12 other [001]axissymmetric tilt CSL grain boundaries, Σ25[001]/(430), Σ25[001]/(710), Σ29[001]/(520), Σ29[001]/(730), Σ37[001]/(610), Σ37[001]/(750), Σ41[001]/(910), Σ41[001]/(540), Σ53[001]/(720), Σ53[001]/(950), Σ61[001]/(11 1 0), and Σ125[001]/(11 2 0), are predicted.
Figure 8.4 shows the results of the predicted grain boundary energies and a comparison with previously reported grain boundary energies [19, 20]. Based on previous studies, the grain boundary energy exhibits a convex profile in relation to the misorientation angle θ. Small cusps are also present, namely energy drops at 16.26°, 28.07°, 36.87°, 53.13°, and 67.38° corresponding to Σ25[001]/(710), Σ17[001]/(410), Σ5[001]/(310), Σ5[001]/(210), and Σ13[001]/(230) respectively. The predicted grain boundary energies of all grain boundaries obtained using the predictor are also plotted in the same figure. Although the absolute value is not identical to the previous studies due to the differences in empirical potential, the overall profile of the grain boundary energy is in good agreement with previous reports. Notably, small cusps at 16.26° and 67.38° are also reproduced by the prediction model (other cusps at 28.07°, 36.87°, and 53.13° were used for training). In addition to the GB energy, it was also confirmed that those predicted models fit well to the other calculation and TEM observations. The above results clearly demonstrate that the presented virtual screening method based on machine learning is sufficiently robust and powerful for predicting stable interface structures and energies from initial atomic configurations. The success of this method implies that the initial atomic configuration is correlated to the grain boundary energy, and its correlation is studied by machine learning.
2.2 Bayesian Optimization (Kriging) [15]
In this section, we demonstrate an alternative and powerful method that can be used to search for stable interface structures with the aid of a geostatistics approach called kriging. Kriging is an effective interpolation method based on a Bayesian optimization and Gaussian process governed by prior covariances. This Kriging method has been previously used to predict the optimum access points for geological mining operations. Here, we apply this Kriging technique to determine the stable structures of interfaces.
To demonstrate the performance of the Kriging method, the Σ5[001](210) CSL GB of fccCu was again selected as the test case. The threedimensional translations were considered with 0.1 Å steps, resulting in the generation of a total of 17,983 configurations. The data space that must be searched to determine the most stable structure can be visualized as shown in Fig. 8.5a. In the conventional approach, namely allcandidate calculations, one must calculate the interface energies of all configurations and determine the most stable point within this space. In other words, the search space is occupied by the calculated results as shown in Fig. 8.5b.
To accelerate this search process, a Kriging method based on a Gaussian process was applied. The Gaussian process is a nonparametric regression analysis based on Bayesian statistics. This method allows for the prediction of values and uncertainties of a random field at a point. The steps of this Kriging process are as follows:

(1)
Several initial configurations (20 configurations here) are randomly selected from the search space shown in Fig. 8.5a.

(2)
The structure optimization and energy calculations for the selected configurations are performed, and a joint probability distribution is calculated with the Gaussian process considering the three rigid body translations along each direction as the descriptors. The grain boundary energy, E _{ GB }, is then estimated.

(3)
Based on the joint probability distribution, the possible GB energies are estimated at all points in the search space.

(4)
Zscores, calculated by the following equation, are estimated at all points in the search space.
$$ Z  score_{i} = (GB\,Energy_{current\,\hbox{min} }  GB\,Energy(x_{i} ))\,\text{/}\,\sqrt {\sigma (x_{i} )} $$where GB Energy _{current min} is the minimum GB energy at this moment, while GB Energy( x _{ i } ) and σ( x _{ i } ) are the mean and standard deviation at the point x _{i} in the search space respectively.

(5)
The point that has the maximum Zscore is selected as the next search point because that point is most likely to have the least GB energy at the moment.

(6)
It is confirmed whether or not the acquired GB energies meet the convergence conditions, such as energy difference between the ith calculation and the i + 1th calculation.
The cycle of above operations ((2)–(6)) is repeated until the convergence criteria have been satisfied. In the structure optimization and energy calculation for (2), we have performed a static lattice calculation using an empirical potential method with the general utility lattice program (GULP) code [21]. The embedded atom potential method reported by Cleri et al. was employed [22].
First, using the conventional approach, all configurations were calculated and the most stable point was determined from the search space shown in Fig. 8.5b. The obtained stable structure is shown in Fig. 8.6a, where the calculated GB energy was 0.96 J/m^{2}. As can be seen here, the GB is composed of an array with a sixmembered structure unit, in agreement with previously reported structures [23, 24]. However, 17,983 complete calculations were necessary to reach this stable structure using the conventional allcandidate calculation.
On the other hand, in the Kriging approach, the search space was interpolated based on the Gaussian process. We found that this Kriging approach greatly decreased the data necessary for calculations. In this case, the most stable point was determined after only 69 trials (including the initial 20 trials). The most stable structure obtained is shown in Fig. 8.6b; the GB is composed of a sixmembered structure unit that is very similar to the stable structure obtained by comprehensive data searching. Furthermore, the calculated GB energy is 0.96 J/m^{2}, which is identical to that determined by the conventional method, indicating that our present method can accurately determine the most stable structure.
The convergence processes for the allcandidate calculation and the Kriging method are displayed in Fig. 8.7. Although the conventional method requires the calculation of all 17,983 configurations, the present Kriging method requires only 69 calculations (Fig. 8.7a). Figure 8.7b shows the calculation trajectory in the Kriging method. The red numbers show the position in the random sampling, and the pink triangle shows the most stable structure found by the Kriging method. As can be seen in Fig. 8.7b, data space was randomly selected at the beginning of the Kriging method, and it gradually concentrates to neighboring points around the most stable point.
We repeated the Kriging operation 74 times for the same GB and found that the 43 Kriging operations were completed using fewer than 50 time calculations. As a result, the average number of calculations for determining the stable structures is 70. Based on this, the Kriging method has succeeded in accelerating the process of interface structure determination by ~150 times.
Finally, to confirm the applicability of the Kriging method, a different GB was also examined. The Σ3[110]/(111) GB of bccFe was selected as a model because its stable structure has also been reported previously [25, 26]. The Kriging method was applied to search for the most stable configuration, just as in the case of the Σ5[001]/(210) copper GB described above. We succeeded in determining the stable structure after 105 calculations, and the calculated structure is shown in Fig. 8.8. The stable structure determined by the Kriging approach agrees well with that of the previous study [25, 26] (yellow circles in Fig. 8.8).
Since 17,466 configurations are present for this Σ3[110]/(111) GB bccFe grain boundary, the Kriging method again achieves two orders of magnitude better efficiency than the conventional method. This clearly indicates that the Kriging method is a very powerful technique to determine the stable interface structure.
2.3 Kriging Method for Oxide Interfaces [16]
Comparing the virtual screening method and the Kriging method, the efficiency of the virtual screening is superior to that of the Kriging method. However, one has to construct a predictor in order to maintain this great efficiency. The most important advantage of the Kriging method is its wide applicability. No training is needed for the Kriging method, and thus it can be easily applied to other GBs in other materials. To show the wider applicability of the Kriging method, we used it to conduct similar studies on oxide interfaces. In particular, we applied the Kriging approach to grain boundaries of metal oxides including MgO, TiO_{2}, and CeO_{2} which commonly exhibit more complex structures than metals.
Four kinds of metal oxide grain boundaries, namely rocksaltMgO Σ5[001]/(210) and Σ5[001]/(310), rutileTiO_{2} Σ5[001]/(210), and fluoriteCeO_{2} Σ3[110]/(111) were selected to test the applicability of the present method. These grain boundaries have different complexities; the number of termination planes for MgO Σ5[001]/(210) and Σ5[001]/(310) is one (Fig. 8.9a, b), whereas that for TiO_{2} Σ5[001]/(210) and CeO_{2} Σ3[110]/(111) is two (Fig. 8.9c, d).
The same Kriging method was applied to these oxides GBs. Two hyperparameters, predistribution and kernel parameter, were set to 0 and 3.0 respectively so that the kernel is not biased to 0 or 1. The random selection number for the initial calculation was set to 5, with the actual size of the threedimensional rigid body translations in each xyzdirection acting as descriptors. Namely, smaller numbers than the above metal cases were used due to the higher computational cost of the oxide simulations.
For structure optimization and energy calculation, static lattice calculations with an empirical potential were performed using a general utility lattice program (GULP) code [21]. Buckinghamtype potentials were used for MgO (Catlow et al. [27]), TiO_{2} (Bandura et al. [28]), and CeO_{2} (Minervini et al. [29]).
Regarding the convergence criteria in the Kriging method, the structure searching continues until five structures which have the identical lowest grain boundary energy are found. In this case, the grain boundary energies within ±0.005 J/m^{2} were judged to be the same. Until these convergence criteria are met, the Kriging algorithm continues searching for the lowest energy configuration.
Figure 8.10a, b show the obtained Σ5[001](210) and Σ5[001](310) grain boundaries of rocksaltMgO, which has a single grain boundary termination plane as shown in Fig. 8.9a, b. Previously reported structures are overlaid on the structures calculated herein using black or white circles [30, 31]. The number of candidate configurations for Σ5[001](210) and Σ5[001](310) structures equals 28,896 and 40,635 respectively. In the conventional method, structure optimization and energy calculations for all candidates need to be performed to determine the most stable structure. Conversely, using the Kriging method, we have succeeded in determining the most stable structures for Σ5[001](210) and Σ5[001](310) by performing only 18 and 15 calculations respectively, including initial random calculations.
We performed the Kriging method several times and confirmed that the number of calculations needed to reach convergence in these cases is 14–22, including the initial random sampling. This variation comes from the selection of the initial sampling. However, we would like to emphasize that the Kriging method is clearly powerful to search the most stable structure.
To confirm the applicability of this method to more complex structures, we applied it to TiO_{2} and CeO_{2} grain boundaries. The most stable structure of the rutileTiO_{2} Σ5[001]/(210) grain boundary is shown in Fig. 8.10c. To maintain charge neutrality, the termination planes were set to Ti and O on their respective sides. A total of 21,630 structures and energies need to be computed in order to find the most stable structure using conventional brute force calculations, while the Kriging method can find the most stable structure by performing only 42 calculations, achieving a more than 500fold efficiency. In addition, the obtained structure was compared with the previously reported one (Fig. 8.10c) [32], clearly showing that the structure determined by the present strategy was correct.
Next, the present method was applied to the fluoriteCeO_{2} Σ3[110](111) grain boundary. In contrast to the other three grain boundaries, this one possesses a [110] rotation axis. Notably, the Kriging method can determine the most stable structure (which is in agreement with the one reported previously [33]) using only 12 calculations. These results indicate that the Kriging method is applicable to complex oxides and can potentially achieve efficiency improvements by factors of ~10^{3}–10^{4} over the conventional allcandidate calculation method.
Finally, the reasons behind the broad applicability of the Kriging method are discussed. As mentioned above, the Kriging method searches for stable structures in a threedimensional data set, as shown in Fig. 8.5b, with extrapolation of this data space performed using the Gaussian process. The success of the Kriging method indicates the suitability of this extrapolation method for the present data space, with data spaces for MgO Σ5[001](310) and Cu Σ5[001](310) compared in Fig. 8.11a, b. The corresponding Cu data space was obtained in previous studies [12, 15]. Although these data spaces appear to be different from each other, their energy profiles are similar. Namely, the grain boundary energy gradually and continuously changes with changing rigid body translation, with no discrete large energy changes present in the data space. This fact indicates that the Kriging method is applicable for grain boundaries possessing a continuous energy surface.
3 Microscopic Approach for Interfaces
3.1 Scanning Transmission Electron Microscopy (STEM)
STEM is one branch of TEM techniques that has been extensively used for characterizing interface structures in many materials and devices. In recent years, STEM combined with aberration correction technology has enabled direct atombyatom imaging via annular darkfield (ADF) imaging. ADF imaging uses a doughnutshaped annular detector to selectively collect highangle scattered electrons, building up images from the variation in this signal with probe position in a raster scan. Since the integrated intensity of highangle scattered electrons strongly scales with the atomic number of the atoms under the probe, this imaging (socalled Zcontrast imaging) can sensitively visualize heavy element atoms [34]. However, ADF can seldom reliably visualize light elements due to their weak power to scatter electrons at higher angles. While ADF imaging mainly uses electrons scattered at highangles to form atom images, there are many other possible detector geometries for collecting electron signals and forming images. One is known as annular brightfield (ABF) imaging, which involves the selective collection of electrons inside the brightfield disk via a small annular detector [35]. It has been shown that ABF imaging can directly visualize light atoms and can even directly visualize H atom columns inside compound materials [36, 37]. Since ADF and ABF images can be obtained simultaneously from the same sample positions, both heavy and light element atomic structures can now be directly visualized by combining these two images. However, it is still very difficult to identify the atomic species using only the ADF and ABF image contrasts, especially at interface regions where structure and chemistry are drastically changing. Since STEM uses an atomicscale electron probe, STEMbased analytical techniques such as energydispersive Xray spectroscopy (EDS) and electron energy loss spectroscopy (EELS) can also achieve atomic resolution. In particular, by utilizing ultrasensitive silicon drift detectors (SDDs) with much higher count rates, atomicscale EDS mapping is now becoming possible [38]. This capability should be very powerful to directly characterize dopant/impurity segregation behaviors in grain boundaries and heterointerfaces. Thus, atomicresolution STEM combined with spectroscopy will become an indispensable technique for characterizing atomicscale structures and chemistry of interfaces.
3.2 Interface Structures Using AberrationCorrected STEM
Two interface characterization studies using aberrationcorrected STEM and EDS are highlighted in this section. One is on the solute segregation in a GB of ceramics [39] and the other is on the impurity segregation in a metal/ceramic heterointerface [40]. These studies demonstrate that atomicresolution STEM is a powerful tool for directly understanding very complex segregation phenomena in materials.
3.2.1 Solute Segregation Behavior of a ∑3 Grain Boundary in Yttria Stabilized Zirconia [39]
ZrO_{2} doped with Y_{2}O_{3} (YSZ) is one of the most important materials for use as an electrolyte in solid oxide fuel cells, where the overall ionic conductivity is strongly affected by the presence of GBs; such an effect may potentially originate from GB chemical inhomogeneity. Previous studies have shown that the Y solute atoms segregate to the GBs, and the amount of segregation is strongly dependent on the GB characteristics [41]. However, the atomicscale mechanism of how Y solute actually segregate to GBs is still not well understood. In this study, we show an atomicscale EDS mapping of a Ʃ3[110]/{111} model GB in YSZ.
Figure 8.12 shows an ADF STEM image of the Ʃ3[110]/{111} grain boundary of YSZ, where the GB atomic arrangement is in good agreement with previous highresolution TEM studies [41]. However, it is almost impossible to distinguish Zr and Y atoms from the STEM image alone. Then, atomicresolution STEMEDS mapping was carried out in order to distinguish the two atomic components. Figure 8.13a, b show atomicresolution EDS maps around the GB, where the Y and Zr maps clearly reveal the formation of characteristic ordered segregation structures. The intensity variation is further highlighted in the corresponding intensity profile shown in Fig. 8.13c, d.
It is noteworthy that in some atomic column layers, Y atoms are obviously depleted. This indicates that the Y atoms are not simply substituting in all of the cation sites around the GB to form segregation structures. Thus, we experimentally found that Y solute segregation formed atomically ordered extended structures across the GB within a range of approximately 3 nm. These experimental results are in good agreement with largescale Monte Carlo simulations [39]. The simulation suggested that such processes can be driven by both the sitedependent segregation of Y due to strain and YV _{ O } interactions. Thus, recent advanced microscopy combined with theory can shed new light on the fundamental mechanism of solute segregation behaviors in GBs.
3.2.2 Dopant Segregation Behavior in a Metal/Ceramic Interface [40]
Heterostructures between metals and ceramics have been widely used for power electronic devices requiring both high thermal performance and reliability in harsh environments. Since interfaces play a critical role in many properties, a fundamental understanding of the interface structure and formation mechanism is vitally important. One important possibility for obtaining heterointerfaces with better properties is to control dopant/impurity segregation behaviors. However, it has been very challenging to directly observe segregation structures at atomic dimensions in heterointerfaces. Here, atomicresolution STEMEDS mapping is shown to be a powerful tool for directly determining segregation structures in metal/ceramic heterointerfaces.
Figure 8.14 shows simultaneous crosssectional (a) ADF and (b) ABF STEM images of an Al alloy (containing Si and Mg as major dopants) /AlN interface formed using a liquid phase bonding technique [40]. In the AlN bulk region, compared to the ADF image, the columns with weaker intensities in the ABF image correspond to the N columns, and the interface of AlN should be Alpolar. The atomic structures of the Al alloy region were not clearly resolved because the present viewing direction is not wellaligned along the certain high symmetry crystallographic axis. To clearly identify the interface atomic structure, we show noisefiltered images of the interface core region in Fig. 8.14c, d. From these images, we can divide the interface core region into three different layered structures labeled as the 1st, 2nd, and 3rd layers. Considering both ADF and ABF STEM images, the 1st, 2nd and 3rd layer interface structures are anioncationanion, cationanion, and anion layers, respectively. However, it is difficult to determine the detailed atomic structure of the three layers from the STEM image contrast since dopant elements such as Al and Mg with close atomic numbers may coexist. Thus, we performed atomicresolution chemical mapping using STEMEDS.
Figure 8.15 shows atomically resolved chemical maps of the Al alloy/AlN interface using STEMEDS. The elemental maps of Al, N, O, Mg, and Si are shown in comparison with an ABF STEM image and structure model [40]. We found that the highest signal in Mg and O maps is located at the 1st interfacial layer, but that of Si is slightly shifted within the Al alloy region. This indicates that these dopant elements should occupy different atomic layers at the interface region. In the 1st layer, Mg atoms are concentrated to a single atomic column layer, whereas O atoms are concentrated to the top and bottom of the Mg layer. Considering the bonding distances and angles between Mg and O columns in the 1st layer, this structure is very similar to a MgO_{6} octahedron with rock salt structure. In the 2nd layer, a local maximum of Al can be found at the cation columns. Thus, the cation columns can be identified as Al columns. O and N could not be separated in the 2nd layer, but the ABF image contrast of the 2nd layer is similar to the AlN contrast in the AlN bulk structure, although with inverted polarity (Npolar). Thus, we consider that the main structure of the 2nd layer is an AlN_{4} tetrahedral monolayer. The polarity of this layer is inverted from the AlN substrate due to the presence of the MgO interlayer. Theoretical simulations suggested that the interface between Al metal and Npolar AlN is much more energetically stable than that between Al metal and Alpolar AlN.
Thus, Al alloy /AlN heterointerfaces should be stabilized by the formation of selforganized atomicscale layered structures with Mg dopant segregation. Atomicresolution STEMEDS is a powerful tool for directly determining heterointerface structures with dopant/impurity segregation.
References
Y. Ikuhara, Grain boundary atomic structures and lightelement visualization in ceramics: combination of Cscorrected scanning transmission electron microscopy and firstprinciples calculations. J. Electron. Microsc. (Tokyo) 60, 173–188 (2011). https://doi.org/10.1093/jmicro/dfr049
A. Sutton, R. Balluffi, Interfaces in Crystalline Materials (Clarendon, 1995)
J.P. Buban, K. Matsunaga, J. Chen, N. Shibata, W.Y. Ching, T. Yamamoto, Y. Ikuhara, Grain boundary strengthening in alumina by rare earth impurities. Science 311(2006) 212–215. https://doi.org/10.1126/science.1119839
K. Matsunaga, H. Nishimura, H. Muto, T. Yamamoto, Y. Ikuhara, Direct measurements of grain boundary sliding in yttriumdoped alumina bicrystals. Appl. Phys. Lett. 82, 1179–1181 (2003). https://doi.org/10.1063/1.1555690
T. Mizoguchi, H. Ohta, H.S. Lee, N. Takahashi, Y. Ikuhara, Controlling interface intermixing and properties of SrTiO3based superlattices. Adv. Funct. Mater. 21, 2258–2263 (2011). https://doi.org/10.1002/adfm.201100230
H. Ohta, S. Kim, Y. Mune, T. Mizoguchi, K. Nomura, S. Ohta, T. Nomura, Y. Nakanishi, Y. Ikuhara, M. Hirano, H. Hosono, K. Koumoto, Giant thermoelectric Seebeck coefficient of a twodimensional electron gas in SrTiO3. Nat. Mater. 6, 129–134 (2007). https://doi.org/10.1038/nmat1821
H. Sawada, N. Shimura, F. Hosokawa, N. Shibata, Y. Ikuhara, Resolving 45pmseparated SiSi atomic columns with an aberrationcorrected STEM. Microscopy 64, 213–217 (2015). https://doi.org/10.1093/jmicro/dfv014
S.J. Pennycook, P.D. Nellist, Scanning Transmission Electron Microscopy (Springer New York, New York, 2011). https://doi.org/10.1007/9781441972002
N. Tanaka, Scanning transmission electron microscopy of nanomaterials, in ed. by N. Tanaka (Imperial College Press, London, 2014), pp. i–xliv. https://doi.org/10.1142/9781848167902_fmatter
S. Ranganathan, On the geometry of coincidencesite lattices. Acta Crystallogr. 21, 197–199 (1966). https://doi.org/10.1107/S0365110X66002615
D. Brandon, The structure of highangle grain boundaries. Acta Metall. 14, 1479–1484 (1966). https://doi.org/10.1016/00016160(66)901684
S. Kiyohara, H. Oda, T. Miyata, T. Mizoguchi, Prediction of interface structures and energies via virtual screening. Sci. Adv. 2, e1600746–e1600746 (2016). https://doi.org/10.1126/sciadv.1600746
A.L.S. Chua, N.A. Benedek, L. Chen, M.W. Finnis, A.P. Sutton, A genetic algorithm for predicting the structures of interfaces in multicomponent systems. Nat. Mater. 9, 418–422 (2010). https://doi.org/10.1038/nmat2712
G. Schusteritsch, C.J. Pickard, Predicting interface structures: from SrTiO3 to graphene. Phys. Rev. B. 90, 35424 (2014). https://doi.org/10.1103/PhysRevB.90.035424
S. Kiyohara, H. Oda, K. Tsuda, T. Mizoguchi, Acceleration of stable interface structure searching using a kriging approach. Jpn. J. Appl. Phys. 55, 2–6 (2016). https://doi.org/10.7567/JJAP.55.045502
S. Kikuchi, H. Oda, S. Kiyohara, T. Mizoguchi, Bayesian optimization for efficient determination of metal oxide grain boundary structures. Phys. B Condens. Matter. (2017) (in press). https://doi.org/10.1016/j.physb.2017.03.006
T. Ueno, T.D. Rhone, Z. Hou, T. Mizoguchi, K. Tsuda, COMBO: an efficient Bayesian optimization library for materials science, Mater. Discov. 10–13, (2016). https://doi.org/10.1016/j.md.2016.04.001
R. GómezBombarelli, J. AguileraIparraguirre, T.D. Hirzel, D. Duvenaud, D. Maclaurin, M.A. BloodForsythe, H.S. Chae, M. Einzinger, D.G. Ha, T. Wu, G. Markopoulos, S. Jeon, H. Kang, H. Miyazaki, M. Numata, S. Kim, W. Huang, S.I. Hong, M. Baldo, R.P. Adams, A. AspuruGuzik, Design of efficient molecular organic lightemitting diodes by a highthroughput virtual screening and experimental approach. Nat. Mater. 15, 1120–1127 (2016). https://doi.org/10.1038/nmat4717
D. Wolf, Structureenergy correlation for grain boundaries in F.C.C. metals—III. Symmetrical tilt boundaries. Acta Metall. Mater. 38, 781–790 (1990). https://doi.org/10.1016/09567151(90)90030K
G. Hasson, J.Y. Boos, I. Herbeuval, M. Biscondi, C. Goux, Theoretical and experimental determinations of grain boundary structures and energies: correlation with various experimental results. Surf. Sci. 31, 115–137 (1972). https://doi.org/10.1016/00396028(72)902567
J.D. Gale, GULP: a computer program for the symmetryadapted simulation of solids. J. Chem. Soc. Faraday Trans. 93, 629–637 (1997)
F. Cleri, V. Rosato, Tightbinding potentials for transition metals and alloys. Comput. Simul. Mater. Sci. 205, 233–253 (1991). https://doi.org/10.1007/9789401135467_11
P. Ballo, V. Slugeň, Grain boundary sliding and migration in copper: the effect of vacancies. Comput. Mater. Sci. 33, 491–498 (2005). https://doi.org/10.1016/j.commatsci.2004.09.049
M.A. Tschopp, D.L. Mcdowell, Asymmetric tilt grain boundary structure and energy in copper and aluminium. Philos. Mag. 87, 3871–3892 (2007). https://doi.org/10.1080/14786430701455321
H. Nakashima, M. Takeuchi, Grain boundary energy and structure of αFe < 110 > symmetric tilt boundary, TetsutoHagane. 86(2000) 357–362. https://doi.org/10.2355/tetsutohagane1955.86.5_357
R. Kurtz, H. Heinisch, The effects of grain boundary structure on binding of He in Fe. J. Nucl. Mater. 329–333, 1199–1203 (2004). https://doi.org/10.1016/j.jnucmat.2004.04.262
A. Catlow, Chapter I0 Interionic Potentials in Ionic Solids, (n.d.)
A.V. Bandura, J.D. Kubicki, Derivation of force field parameters for TiO2–H2O systems from ab initio calculations (2003). https://doi.org/10.1021/JP034093T
L. Minervini, M.O. Zacate, R.W. Grimes, Defect cluster formation in M2O3doped CeO2. Solid State Ionics 116, 339–349 (1999). https://doi.org/10.1016/S01672738(98)003592
B.P. Uberuaga, X.M. Bai, P.P. Dholabhai, N. Moore, D.M. Duffy, Point defect–grain boundary interactions in MgO: an atomistic study. J. Phys. Condens. Matter 25, 355001 (2013). https://doi.org/10.1088/09538984/25/35/355001
Y. Yan, M.F. Chisholm, G. Duscher, A. Maiti, S.J. Pennycook, S.T. Pantelides, Impurityinduced structural transformation of a MgO grain boundary, Phys. Rev. Lett. 81(1998), 3675–3678. https://doi.org/10.1103/PhysRevLett.81.3675
S.B. Sinnott, R.F. Wood, S.J. Pennycook, Ab initio calculations of rigidbody displacements at the Σ5 (210) tilt grain boundary in TiO2. Phys. Rev. B. 61, 15645–15648 (2000). https://doi.org/10.1103/PhysRevB.61.15645
B. Feng, H. Hojo, T. Mizoguchi, H. Ohta, S.D. Findlay, Y. Sato, N. Shibata, T. Yamamoto, Y. Ikuhara, Atomic structure of a Σ3 [110]/(111) grain boundary in CeO2. Appl. Phys. Lett. 100, 73109 (2012). https://doi.org/10.1063/1.3682310
S.J. Pennycook, L.A. Boatner, Chemically sensitive structureimaging with a scanning transmission electron microscope. Nature 336, 565–567 (1988). https://doi.org/10.1038/336565a0
S.D. Findlay, N. Shibata, H. Sawada, E. Okunishi, Y. Kondo, T. Yamamoto, Y. Ikuhara, Robust atomic resolution imaging of light elements using scanning transmission electron microscopy. Appl. Phys. Lett. 95, 2–4 (2009). https://doi.org/10.1063/1.3265946
S.D. Findlay, T. Saito, N. Shibata, Y. Sato, J. Matsuda, K. Asano, E. Akiba, T. Hirayama, Y. Ikuhara, Direct imaging of hydrogen within a crystalline environment. Appl. Phys. Express 3, 6–9 (2010). https://doi.org/10.1143/APEX.3.116603
R. Ishikawa, E. Okunishi, H. Sawada, Y. Kondo, F. Hosokawa, E. Abe, Direct imaging of hydrogenatom columns in a crystal by annular brightfield electron microscopy. Nat. Mater. 10, 278–281 (2011). https://doi.org/10.1038/nmat2957
M.W. Chu, S.C. Liou, C.P. Chang, F.S. Choa, C.H. Chen, Emergent chemical mapping at atomiccolumn resolution by energydispersive Xray spectroscopy in an aberrationcorrected electron microscope, Phys. Rev. Lett. 104(2010), 1–4. https://doi.org/10.1103/PhysRevLett.104.196101
B. Feng, T. Yokoi, A. Kumamoto, M. Yoshiya, Y. Ikuhara, N. Shibata, Atomically ordered solute segregation behaviour in an oxide grain boundary. Nat. Commun. 7, 11079 (2016). https://doi.org/10.1038/ncomms11079
A. Kumamoto, N. Shibata, K. Nayuki, T. Tohei, N. Terasaki, Y. Nagatomo, T. Nagase, K. Akiyama, Y. Kuromitsu, Y. Ikuhara, Atomic structures of a liquidphase bonded metal/nitride heterointerface. Sci. Rep. 6, 22936 (2016). https://doi.org/10.1038/srep22936
N. Shibata, F. Oba, T. Yamamoto, Y. Ikuhara §, Structure, energy and solute segregation behaviour of [110] symmetric tilt grain boundaries in yttriastabilized cubic zirconia. Philos. Mag. 84, 2381–2415 (2004). https://doi.org/10.1080/14786430410001693463
Acknowledgements
This work was supported by a GrantinAid for Scientific Research on Innovative Areas “Nano Informatics” (Grant No. JP25106003) from the Japan Society for the Promotion of Science (JSPS).
Author information
Authors and Affiliations
Corresponding author
Editor information
Editors and Affiliations
Rights and permissions
This chapter is published under an open access license. Please check the 'Copyright Information' section either on this page or in the PDF for details of this license and what reuse is permitted. If your intended use exceeds what is permitted by the license or if you are unable to locate the licence and reuse information, please contact the Rights and Permissions team.
Copyright information
© 2018 The Author(s)
About this chapter
Cite this chapter
Mizoguchi, T., Kiyohara, S., Ikuhara, Y., Shibata, N. (2018). AtomicScale Nanostructures by Advanced Electron Microscopy and Informatics. In: Tanaka, I. (eds) Nanoinformatics. Springer, Singapore. https://doi.org/10.1007/9789811076176_8
Download citation
DOI: https://doi.org/10.1007/9789811076176_8
Published:
Publisher Name: Springer, Singapore
Print ISBN: 9789811076169
Online ISBN: 9789811076176
eBook Packages: Chemistry and Materials ScienceChemistry and Material Science (R0)