Abstract
Refractory high entropy alloys feature outstanding properties making them a promising materials class for nextgeneration hightemperature applications. At high temperatures, materials properties are strongly affected by lattice vibrations (phonons). Phonons critically influence thermal stability, thermodynamic and elastic properties, as well as thermal conductivity. In contrast to perfect crystals and ordered alloys, the inherently present mass and force constant fluctuations in multicomponent random alloys (high entropy alloys) can induce significant phonon scattering and broadening. Despite their importance, phonon scattering and broadening have so far only scarcely been investigated for high entropy alloys. We tackle this challenge from a theoretical perspective and employ ab initio calculations to systematically study the impact of force constant and mass fluctuations on the phonon spectral functions of 12 bodycentered cubic random alloys, from binaries up to 5component high entropy alloys, addressing the key question of how chemical complexity impacts phonons. We find that it is crucial to include both mass and force constant fluctuations. If one or the other is neglected, qualitatively wrong results can be obtained such as artificial phonon band gaps. We analyze how the results obtained for the phonons translate into thermodynamically integrated quantities, specifically the vibrational entropy. Changes in the vibrational entropy with increasing the number of elements can be as large as changes in the configurational entropy and are thus important for phase stability considerations. The set of studied alloys includes MoTa, MoTaNb, MoTaNbW, MoTaNbWV, VW, VWNb, VWTa, VWNbTa, VTaNbTi, VWNbTaTi, HfZrNb, HfMoTaTiZr.
Introduction
High entropy alloys (HEA) are of great technological interest due to their excellent mechanical^{1, 2} and electronic properties.^{3} Refractory HEAs, such as e.g. bcc NbMoTaW, possess extraordinary mechanical properties, comparable to current stateoftheart nickelbased superalloys.^{2, 4,5,6} This makes them promising candidates for nextgeneration hightemperature applications. The design of materials for extreme temperature environments requires an accurate knowledge of phase stabilities, thermodynamic properties and thermal conductivity,^{7} all of which are linked intrinsically to lattice vibrations, i.e. phonons.^{8, 9} Accurate modeling of phonon excitations and their interactions plays therefore a decisive role in the design, exploration and optimization of such materials.
Phonons can be altered by nanostructural features (e.g., nanoparticles, nanowires),^{10, 11} they interact with themselves (i.e., phononphonon interactions)^{9} and with chemical disorder, a key feature of HEAs.^{12,13,14} The interaction with chemical disorder can lead to significant phonon scattering and broadening, if elements of considerable mass difference are involved. In addition to the mass disorder, the locally distinct chemical environments in HEAs can induce force constant variations that also modify the phonon spectral distribution. These force constant variations may be enhanced by local lattice distortions that are known to be important in HEAs.^{13,14,15,16,17}
The large compositional space inherent to HEAs offers the possibility to tune phonon broadening by adjusting the chemical complexity via variation of the relative fractions of the constituent elements and the total number of elements. The mass and force constant induced scattering processes could be, for example, used to modify systematically thermal conductivity (inversely proportional to phonon bandwidth). This is of particular interest for HEAs that were recently suggested as candidates for thermoelectric^{18, 19} or heat shield materials.^{7}
Tuning chemical complexity in HEAs has been employed to tailor electron scattering and electronic properties^{20, 21} aiming at improved radiation resistant materials. Similar studies on disorder induced phonon scattering and phonon broadening in HEAs are so far lacking. Previous works addressing phonons in disordered alloys have been mostly limited to binaries.^{22,23,24,25,26,27} A few works have been devoted to vibrational properties of multicomponent alloys,^{16, 28,29,30,31} but were mainly focused on integrated quantities such as the phonon density of states^{28} or thermodynamic properties such as lattice specific heat, typically derived from simplified Debyelike models.^{29, 30} Phonon spectra and in particular mass and force constant induced phonon broadening remain unexplored.
Therefore, we have performed an extensive firstprinciples study to evaluate phonon broadening for 12 different bodycentered cubic (BCC) refractory random alloys, from binaries up to 5component high entropy alloys. Our set of alloys includes in particular the 4component NbMoTaW, NbTaTiV, NbTaVW, and 5component NbMoTaWV, NbTaTiVW, HfMoTaTiZr alloys, which attracted attention recently.^{4, 16, 30, 32,33,34} On the basis of our results, we address the following fundamental questions: How strongly are phonon spectra affected in high entropy alloys by chemical disorder induced scattering? What is the detailed contribution due to mass and force constant fluctuations? Are both equally important or could one or the other be neglected? And what is the role of the number of constituent elements for phonon broadening?
Results
Figure 1 shows the computed phonon spectra for two sets of alloys, namely MoTa, MoTaNb, MoTaNbW, MoTaNbWV in (a)–(d) and VW, VWNb, VWNbTa, VWNbTaTi in (g)–(j) (added elements in bold), i.e., starting with binaries, moving to ternaries, then quaternaries, and finally to the fivecomponent quinaries. This strategy of adding one element after the other allows us to study systematically the impact of the total number of principal elements on the phonon broadening. For all considered alloys, the longwavelength limit (region close to Γ) is unaffected, i.e., no broadening is visible and the spectral function is sharply peaked as exemplified in the two 3D insets (e) and (f) for MoTaNbW and MoTaNbWV. This longwavelength behavior is a consequence of the Rayleigh law (~ ω ^{4}) for impurity scattering.^{35} For the mid and highfrequency region (above ~ 4 THz), the broadening turns out to be very strong for all alloys, reaching widths of up to a few THz. Inspecting the first sequence of alloys (Figs. 1a–d), the broadening of the 4 and 5component alloy spectra appears to be larger compared to the 2 and 3component ones as exemplified by the grey arrows at the Hpoint. This dependence is even better visible in the upper panel of Fig. 2 where the spectral function is drawn for the Hpoint. The impact of the number of components is qualitatively different for the second alloy series (Figs. 1g–j), where a phonon band gap appears for the phonon spectrum of VW around the Hpoint (grey dashed lines and arrow). This band gap disappears when more elements are added and the overall broadening is slightly contracted.
To analyze the observed behavior we will proceed in several steps, starting with a comparison to the most simplified approximation of chemical disorder. For that purpose we derived the phonon spectra based on the virtualcrystal approximation (VCA, black solid lines in Fig. 1 and black dashed lines in Fig. 2), where we replaced the force constants with averaged values according to the crystal symmetries (i.e. by not distinguishing the different constituents) and the atomic masses with averaged masses over the constituents. In the longwavelength limit and for frequencies below ~ 4 THz the averaged spectra agree very well with the full calculation. However, for frequencies above ~ 4 THz, where the broadening sets in, the averaged dispersions fail in capturing the correct physics. Clearly, due to the averaging procedure broadening cannot be described. Moreover, the averaged dispersions do not match well in position with the corresponding (broadened) peaks in the full dispersion. The discrepancy is most obvious for VW where the averaged dispersion falls into the band gap region of the full calculation. We conclude that the VCA is a too simplified approximation. Similar observations have been recently made for facecentered cubic (FCC) random FePt alloys.^{36}
The effective singlespecies approximation neglects mass fluctuations. A convenient quantity to characterize the latter is the massfluctuation phonon scattering parameter,^{35}
where c _{ i } and M _{ i } denote the concentration and atomic mass of the ith component and \(\bar M\) the averaged mass of the alloy. Within the original Klemens model,^{35} Γ_{ M } is proportional to the inverse relaxation time, which is often associated with the overall phonon broadening. We therefore employ our computed spectral functions to investigate a possible relationship.
The scattering parameter, Γ_{ M }, for the first alloy series in Fig. 1 upper panel is 0.09, 0.11, 0.10 and 0.19. The minor variation of Γ_{ M } between the 2, 3, and 4component alloys (Γ_{ M } ≈ 0.1) seems to be inconsistent with our observation above that the 4component alloy (together with the 5component one) reveals a more broadened spectrum than the 2 and 3component ones. Inspecting the second alloy series, where Γ_{ M } varies as 0.32, 0.26, 0.20, 0.29, substantiates the conclusion that Γ_{ M } alone cannot cover all aspects of phonon broadening. The 2 and 5component alloys, i.e. VW and VWNbTaTi, reveal qualitatively different phonon broadening although their Γ_{ M } parameters are similar (0.32 vs. 0.29). The reason that the Γ_{ M } parameter is insufficient to capture all the complexity of the broadening is force constant fluctuations that modify the mass induced fluctuations.
In order to separate the impact of mass and force constant fluctuations, we derived partially averaged phonon spectra with the averaging performed only over the force constants leaving the mass fluctuations unaffected. Subsequently, we applied a recently introduced projection procedure^{37} that resolves the contribution into the different pair interactions (MoMo, MoTa, etc.). The results for the MoTaNbWV series at the Hpoint are shown in the lower panel of Fig. 2. The Hpoint is particularly convenient because, for a oneatomic or an averaged bcc bulk system, only a single frequency mode is present enabling an unbiased analysis of the broadening without intervention from other modes. Taking only the mass fluctuations into account all elementprojected contributions to the spectral functions can be directly related to their individual atomic masses. Generally, the lower the atomic mass the higher the frequency and vice versa. For example, Ta has a mass of 181 u and its spectral function (red) is placed in a region of about 4 to 5 THz, shifting somewhat down as the number of elements is increased. Mo is significantly lighter with 96 u and its spectral function (blue) is in the range of 6 to 7 THz. Such a mass analysis makes a straightforward interpretation of the observed Γ_{ M } parameter dependence possible: The 2, 3 and 4component alloys can be considered as binary or quasibinary, due to the overlap of some of the atomic masses, thus justifying the similar Γ_{ M } ≈ 0.1. It is only the 5component alloy where a “new” mass of 51 u is introduced. This renders the alloy a quasiternary and increases Γ_{ M } to 0.19. The spectral functions involving mass fluctuations only (lower panel of Fig. 2) are nicely consistent with this analysis. However, the full spectral functions (upper panel) are quite different and this is caused by force constant fluctuations.
To explain how the force constant fluctuations modify the mass induced broadening, we focus on the VW alloy where the effect is strongest. Figure 3a shows the partially averaged spectral function for VW along the high symmetry directions. The phonon band gap is very large, from about 5 to 8 THz at the H point, due to the significant mass difference between V (51 u) and W (184 u). Figure 3b also shows a partially averaged spectral function. This time however, the mass fluctuations are averaged out leaving the force constant fluctuations unaffected. Although the resulting broadening is smaller than the one caused by the mass fluctuations, it is still significant with a width of about 3 THz. Such a significant impact of force constant fluctuations on the phonon broadening is generally found for the alloys studied here (see Supplementary Information). Inspecting the complete spectral function including both mass and force constant fluctuations (Fig. 3c) reveals that the phonon band gap and the overall broadening are contracted with respect to the spectral function with mass fluctuations only. Similar findings have been reported for random FCC NiPt and CuAu alloys.^{22,23,24} Our results indicate that such counteractions are also present in multicomponent alloys.
In order to substantiate this finding, we focus in Figs. 4a, b on the Hpoint. Figure 4a emphasizes the phonon band gap when only mass fluctuations are considered and clarifies that the lower peak is originating from vibrations of W (184 u) and the upper peak from vibrations of V (51 u). Figure 4b shows that considering only force constant fluctuations the two elements switch positions, VV interactions are responsible for the lower and WW interactions for the upper peak. This suggests that the lighter element V has smaller force constants and the heavier W has larger force constants. As a consequence, the force constants counteract the mass induced splitting of the spectral function contracting the band gap and the overall broadening. The resulting full spectral function is shown in Fig. 4a by the grey line. In contrast to the masses, for the force constants the mutual VW interactions are very important (purple line in Fig. 4b). They lead to a strong damping of the lowerfrequency peak and an enhancement of the higherfrequency peak in the final, full spectral function. Similar negative contributions to the spectral function of the mutual interactions have been found and discussed for CuAu recently.^{37}
The mass fluctuation induced broadening and splitting of the spectral functions can be rather straightforwardly analyzed and understood in terms of the atomic masses, as illustrated above for the MoTaNbWV series (Fig. 2, lower panel). In contrast, the nature of force constant fluctuations is, in general, much more obscure. Such force constant fluctuations are generated from the locally different chemical environments, which can be further modified by the variation of bond lengths (local lattice distortion). Often, however, the main contribution is given by the nearest neighbor force constants and we have therefore investigated this possibility for the present alloys. Specifically, we have computed spectral functions excluding all force constants but the ones with the nearest neighbors. The results (shown in the Supplementary Information) reveal that many features of the phonon spectra and broadening can be observed in these reduced nearestneighbor calculations, but longerranged interactions are needed for quantitative predictions. An example of the first nearest neighbor force constants is given in Figs. 4c, d. Consistent with the above discussion, the VV interactions reveal smaller force constants than the WW ones. The relative peak positions for the VV and WW force constant distributions in Fig. 4d clearly correlate with the related projections of the spectral functions due to the forceconstant fluctuations shown in Fig. 4b.
The relationship between mass and force constant fluctuations is a general phenomenon for the studied alloys. Figure 5 exemplifies this relationship for the 5component alloys. It shows the mean value of the computed magnitude of nearestneighbor force constants of all pairs in the 5component alloys versus the atomic masses. In addition to the already discussed NbTaTiVW and MoNbTaVW alloys, the HfMoTaTiZr alloy^{38} has been included, motivated by recent interest^{38} sparked by yield strengths comparable to current stateoftheart superalloys. Note that the ternary HfNbZr subsystem is discussed in the Supplementary Information. The solid lines represent second order polynomial fits to the computed data and they reveal a clear relation of the masses and force constants for all quinaries. The larger the atomic masses the larger are the computed force constants. This relationship is the underlying reason for the partial compensation of the mass fluctuations by the force constant fluctuations.
An important tool in the above analysis of the phonon spectral function was the decomposition into the contributions of the various elementelement interactions. For the VW binary the projection procedure^{37} resulted in partial spectral functions for VV, VW, and WW interactions. The virtue of such a decomposition is the close correspondence to force constants between the elements as exploited above. However, for multicomponent alloys the analysis and interpretation based on pair interactions including crossterms (such as VW) becomes increasingly cumbersome. For a 5component alloy already 15 various elementelement interactions are present. We therefore propose an alternative projection scheme that allows one to map the total phonon spectral function onto single elements (not elementelement pairs). Within this projection scheme, the unfolded partial spectral function for each element X is obtained as
where K is a general wave vector, k _{ k } a wave vector in the first Brillouin zone of the underlying crystal structure (here bcc), J a phonon mode index, ω(K, J) the phonon frequency at K and J, and w _{X}(K, J) and \({w_{{{\bf{k}}_k}}}\left( {{\bf{K}},J} \right)\) corresponding weights given by:
Here, \({{\tilde{\bf v}}}\left( {{\bf{K}},J} \right)\) is the phonon eigenmode at K and J, and \({\hat P^{\rm{X}}}\) and \({\hat P^{{{\bf{k}}_k}}}\) are projection operators onto the species X and the wave vector k _{ k }. The subscript “0” indicates that the norms are taken for the original unit cell of the supercell model. A detailed derivation of the equations and explicit expressions for the projection operators are given in the Supplementary Information.
The above projection scheme allows us to decompose the full phonon spectra into the individual contributions of each element without requiring crossterms, thus facilitating the interpretation. To demonstrate the projection scheme we consider the second alloy series in Fig. 1, i.e. VW to VWNbTaTi, but now resolved into the individual contributions of each chemical element. The results are shown in Fig. 6 with the full spectra in the first column and their individually resolved contributions in the corresponding rows. Note that the partial phonon spectral functions include both mass and force constant fluctuations. The decomposition clearly reveals that the highest frequencies for each alloy are predominantly determined by the lightest elements whereas the heavier ones determine the lowfrequency parts. This is fully consistent with our findings above. We further see that, apart from the reduced concentration when going from top to bottom, the element specific contributions turn out to be rather independent of the actual alloy. This may open an efficient route for predicting phonon spectra of alloys that have not yet been explored.
So far in this section, we have focused on the impact of chemical disorder on spectral functions, i.e., on the detailed wavevectorresolved frequencydependence of the vibrational spectrum. For thermodynamic equilibrium properties, such as phase stabilities, the spectral function is less clarifying because it enters only after integration over wavevectors and frequencies. To elucidate this issue we computed the vibrational entropy, S _{vib}, in the harmonic approximation using the phonon density of states obtained from the abovediscussed spectral functions (see Figs. S1 through S4 in the Supplemental Information).
Figure 7 shows the results for S _{vib} at 1500 K for the MoTa to MoTaNbWV and the VW to VWNbTaTi alloy series in (a) and (b), respectively. The black filled circles and lines represent the full calculations including both, mass and force constant fluctuations, and the other colored lines represent the various approximations as investigated for the phonon broadening. Interestingly, on an absolute scale, even the virtualcrystalapproximation (VCA; orange lines), i.e., the average over mass and force constant fluctuations, provides a reasonable accuracy, in particular for the MoTa to MoTaNbWV series, with errors of about 0.1 k _{B}. The VCA error is larger for the other series, reaching up to 0.3 k _{B} for the VW binary. The fact that the VW binary shows the largest VCA error can be qualitatively understood with reference to the previous analysis of the spectral function for VW that shows a phonon band gap which cannot be captured by the VCA like phonon dispersion (black line in Fig. 1).
Although an error of 0.3 k _{B} may seem small in view of the absolute vibrational entropy of 8…9 k _{B} at 1500 K, it can become significant when considering competition between phases. Going beyond the VCA approach by including force constant fluctuations and averaging only over the masses (blue lines in Figs. 7a, b) does not lead to a significant improvement. A much better approximation is achieved by including the mass fluctuations and averaging over the force constants (red lines). This is consistent with our spectral function analysis that the dominating contribution to the phonon broadening is given by the mass fluctuations.
The dependence of the vibrational entropy on the number of constituents differs for the two alloy series. For the MoTa to MoTaNbWV series the changes are relatively small, while for the VW to VWNbTaTi series the vibrational entropy increases monotonically by a substantial amount from the binary (8.2 k _{B}) to the quinary (8.9 k _{B}). These dependencies can be, to a good extent, understood by inspecting the variation of the equilibrium volume and the averaged mass of the alloys, with the volume effect being the dominant one. Generally, increasing the volume results in decreasing phonon frequencies and an enhanced vibrational entropy, which is responsible for the thermal expansion of materials as captured by the quasiharmonic approximation. In this spirit, the strong volume increase when going from VW over to VWNb and then to VWNbTa (black filled circles and lines in Fig. 7f) is responsible for the significant increase in the vibrational entropy for this alloy sequence (black filled circles and lines in Fig. 7b).
The volume effect is modified by the impact of the atomic masses on the phonon frequencies. With reference to the decomposition performed in Fig. 6 and the corresponding discussion, we note again that light elements, i.e., the ones that decrease the average alloy mass, generally correspond to higher frequency regions and heavier elements, i.e., the ones that tend to increase the average alloy mass, to low frequency regions. The connection to the vibrational entropy is then such that it tends to increase when the average alloy mass decreases. The changes in the average atomic mass can counteract the volume effect (as is the case for VW to VWNb, or the sequence MoTa to MoTaNb to MoTaNbW), or can amplify the volume effect (as for VWNb to VWNbTa). Some additional details of these relationships are given in the Supplementary Information.
Finally, to put the changes observed for the vibrational entropy into a proper perspective, we plot the configurational entropy (in the ideal approximation) in Figs. 7c, d using purposefully the same scale as in Figs. 7a, b. The comparison reveals that changes in the vibrational entropy can be of the same magnitude as for the configurational entropy, and thus we conclude that configurational entropy cannot be a priori assumed to be the single dominating contribution to phase stabilities. This conclusion is further supported by explicitly considering the influence of ordering, which we have investigated by performing an additional calculation for the B2 (NbTa)(MoW) alloy, reported to be thermodynamically stable at low temperatures.^{16, 33} This alloy has two sublattices, with one sublattice containing a random distribution of Nb and Ta, and the other sublattice containing a random distribution of Mo and W. Although the ideal configurational entropy of this alloy is reduced by a factor of 1/2 (green cross in Fig. 7c) as compared to the fully disordered A2 NbMoTaW alloy, the computed phonon spectral functions turn out to be very similar (see Fig. S6 in Supplementary Information). This can be understood by the similar mass disorder on each sublattice in the B2 (NbTa)(MoW) as compared to A2 NbMoTaW. As a consequence the derived vibrational entropy (green cross in Fig. 7a) is hardly affected. This corroborates the statement that configurational entropy is not the sole factor in determining phonon broadening and derived thermodynamic properties.
Discussion
The series of ab initio calculations for phonon spectra of refractory high entropy alloys presented here reveals that it is not only the mere number of constituents, which dominates the chemical disorder induced phonon scattering, but rather the inherent fluctuations in the masses and force constants of the elements. For all considered alloys, strong phonon broadening is observed in the range of mid to high frequencies (above ~ 4 THz). Mass fluctuations dominate the phonon broadening. However, for quantitative predictions force constant fluctuations cannot be neglected. In fact, for some alloys the neglect of force constant fluctuations can result in predictions of artificial phonon band gaps. In all of the considered alloys the force constant fluctuations counteract the mass disorder induced fluctuations. This might be intuited by the fact that we considered elements from the early transition metal series. Qualitatively the relation between atomic mass and force constants can be understood as follows: Increasing the band filling by going from left to right in the periodic table (e.g. from Hf over Ta to W), not only the atomic masses increase, but also the interatomic bonds are enhanced resulting in increased force constants, which correlates with a decreasing equilibrium volume. Going from top to bottom, e.g. from V over Nb to Ta, the inner core charge and atomic masses increase, resulting in an enhanced local electronic density and thus increased force constants too.
Since atomic mass and force constants jointly contribute to the dynamical matrix and hence phonon energies, this has direct implications for theoretical modeling tools, such as the coherent potential approximation which usually neglect force constant fluctuations.^{25} The present results further show that conclusions based on a single parameter (e.g. the massfluctuation scattering parameter) have little predictive capability because such parameters can neither fully account for the multicomponent element character inherent of high entropy alloys nor account for simultaneous mass and force constant fluctuations.
For thermodynamic equilibrium properties, such as the vibrational entropy, one may expect that details of the wavevectorresolved spectral functions are of less importance due to the involved integration. Our analysis shows that this expectation is indeed fulfilled for the force constant fluctuations that show only a small contribution to the vibrational entropy. In contrast, the integration argument does not work well for the mass fluctuations which are found to be significantly more important. When comparing the vibrational entropy with the configurational entropy for a varying number of constituents, we find changes of the same magnitude highlighting the importance of vibrational entropy for phase stability considerations of multicomponent alloys.
For some alloys chemical ordering^{39} has been reported at lower temperatures. This raises the issue in how far chemical ordering affects phonon broadening and vibrational entropies. Since chemical disorder is the key prerequisite for the derived broadening one might intuit that it would be strongly suppressed by any kind of chemical ordering. We find, however, that such conclusions do in general not apply for HEAs as our B2 (NbTa)(MoW) example reveals. Even though the partial ordering reduces the configurational entropy by a factor of 1/2 compared to the fully disordered alloy, almost no impact on the overall phonon broadening and vibrational entropy is found. Based on our analysis we can therefore conclude that it is not the configurational entropy inherent to HEAs, which controls the vibrational properties such as broadening or vibrational entropy, but rather the specific alloy combination of the involved alloy components.
The present study is a first step towards a full description of lattice excitations in HEAs. Chemical disorder induced scattering is an important part of such a description. The overall phonon broadening at elevated temperatures will be affected by multiple sources (phononphonon interactions, extended defect scattering, vacancies). Magnetic fluctuations can be an additional source too.^{36} Alloys featuring multiplephases^{40} will give rise to phonon scattering mechanisms on the nanoscale. Recently, an AlHfScTiZr alloy with partial sublattice ordering has been reported.^{41} At the same time recent computer simulations suggest the possibility of selective phonon broadening.^{42} Noteworthy, the disorderinduced broadened high frequency modes carry the highest energies and therefore constitute a very effective frequency range for such a selective filter. The combination of computationally engineered materials with designed phonon broadening may open the route towards a new generation of tailored hightemperature HEAs.
Methods
Electronic structure calculations have been performed with the vasp code^{43, 44} employing the projectoraugmented wave method^{45} and the generalized gradient approximation.^{46} To ensure high accuracy, the semicore pstates of Hf, Mo, Nb, Ta, Ti, V, and W were treated as valence in the employed paw potentials. For Zr, semicore sstates were treated as valence. A plane wave cutoff energy of 400 eV was chosen throughout all calculations. Chemical disorder was simulated by special quasi random structures (SQS).^{47} The SQS have been constructed by minimizing the correlation functions of the first two nearestneighbor shells employing the spcm program. The SQS cells for the equimolar 2, 3, 4, and 5component alloys contain 128, 54, 128, and 125 atoms. For further informations on the spcm program please contact Prof. Andrei V. Ruban (a.v.ruban@gmail.com) .
The equilibrium volume has been determined by computing total energies for at least nine volumes around the equilibrium volume. The atomic coordinates of each supercell were fully optimized with energy convergence criteria set to be less than 10^{−5} eV per atom while keeping the cubic cell shape. The MethfesselPaxton technique^{48} with a smearing value of 0.1 eV has been used. For the total energy calculations of the 54, 125 and 128atom cells, kpoint grids of 6 × 6 × 6, 4 × 4 × 4, and 4 × 4 × 4 (>8000 kpoint*atom) have been employed.
The phonon calculations have been performed at the theoretical equilibrium lattice constant obtained by fitting the Vinet equation of state^{49} to the total energy calculations. For each alloy, every atom has been displaced in x, y, zdirection by a finite displacement of 0.02 Bohr. To ensure a high numerical precision, these calculations have been performed with enhanced energy convergence criteria (<10^{−7} eV) and kpoint grids of 7 × 7 × 7 and 5 × 5 × 5 for the 54atom and 125, 128atom cells, respectively (>16,000 kpoint*atom). In addition, an additional support grid for the evaluation of the augmentation charges has been employed. The phonon density of states has been computed employing the phonopy program package.^{50}
The firstprinciples derived force constants have been employed in the band unfolding method.^{51,52,53,54} In this method, phonon spectra of random alloys are obtained by decomposing the phonon modes of SQS models onto the Brillouin zone of their underlying crystal structures according to their translational symmetry. Pairprojected contributions of the spectral functions are derived by the recently developed mode decomposition technique^{37} and by the proposed modified projection scheme. A detailed description is given in the Supplementary Information.
Data availability
The authors declare that all data supporting the findings of this study are available within the paper and its supplementary information files.
Additional information
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Acknowledgements
We thank Prof. Andrei V. Ruban for providing the spcm program for generating special quasirandom structures. Discussions with B. Dutta and T. Hickel are acknowledged. Funding by the Deutsche Forschungsgemeinschaft (DFG) through the scholarship KO 5080/11, by the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (Grant agreement No. 639211), by the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan, through the Elements Strategy Initiative for Structural Materials (ESISM) of Kyoto University, and by the Japan Society for the Promotion of Science (JSPS) KAKENHI GrantinAid for Young Scientist (B) (Grant No. 16K18228) are gratefully acknowledged.
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Affiliations
Materials Science and Engineering, Delft University of Technology, 2628 CD, Delft, The Netherlands
 Fritz Körmann
 & Marcel H. F. Sluiter
Center for Elements Strategy Initiative for Structural Materials, Kyoto University, Kyoto, 6068501, Japan
 Yuji Ikeda
Computationals Materials Design, MaxPlanckInstitut für Eisenforschung GmbH, 40237, Düsseldorf, Germany
 Blazej Grabowski
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Contributions
F.K. and M.S. designed the research, F.K. performed the DFT calculations, Y.I. implemented and applied the band unfolding approach. The results were visualized and analyzed together with B.G. All authors discussed the results and wrote the manuscript.
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The authors declare that they have no competing financial interests.
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Correspondence to Fritz Körmann or Yuji Ikeda.
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Temperaturedependent phonon spectra of magnetic random solid solutions
npj Computational Materials (2018)