Abstract
Determination of magnetic structure is an important analytical procedure utilized in various fields ranging from fundamental condensedmatter physics and chemistry to advanced manufacturing. It is typically performed using a neutron diffraction technique; however, finding global solutions of the magnetic structure optimization problem represents a significant challenge. Generally, it is not possible to mathematically prove that the obtained magnetic structure is a truly global solution and that no solution exists when no acceptable structure is found. In this study, the global optimization technique called semidefinite relaxation of quadratic optimization, which has attracted much interest in the field of applied mathematics, is proposed to use as a new analytical method for the determination of magnetic structure, followed by the application of polarized neutron diffraction data. This mathematical approach allows avoiding spurious local solutions, decreasing the amount of time required to find a tentative solution and finding multiple solutions when they exist.
Introduction
Development of method for determining crystal and magnetic structure is an important issue^{1,2,3}. The magnetic structure of a compound is directly related to the microscopic origins of various intriguing magnetic phenomena observed in physics, chemistry, biology and geology^{4,5,6,7,8,9,10,11}. Accurate information on the experimentally determined magnetic structures can be potentially used to effectively design functional materials and opens multiple opportunities for utilizing advanced firstprinciple calculations and informatics approaches. Furthermore, the responses of the analysed magnetic structure to external factors such as temperature, pressure, electromagnetic field, light and environment are usually related to the corresponding changes in the macroscopic properties of minerals and biomolecules.
Since the pioneering work of Shull et al. published in 1951^{1}, many studies on the determination of the magnetic structures of various materials by neutron diffraction have been performed. Thus, Izymov, Kovalev and Bertaut developed the irreducible representation (IR) theory, which successfully classified magnetic structures by their magnetic point symmetries obtained through the analysis of neutron diffraction data^{12,13,14}. Moreover, the modern neutron diffractometers exhibit relatively high statistical accuracy and resolution^{15,16}. However, analysing neutron diffraction data to determine the correct magnetic structure represents a challenging task. The major issue here is the existence of socalled local solutions to the optimization problem (Fig. 1A). The analysis procedure is mathematically categorized as the nonlinear optimization, in which the obtained diffraction data points are fitted with the function of neutron scattering crosssection characterized by highdimensional nonlinear parameters such as magnetic moment vectors^{17}. After performing nonlinear optimization, it is very difficult to prove that the best solution obtained via various numerical models is the global one. Furthermore, multiple or many solutions are hidden in some cases, and no solutions exist in other cases. To mitigate these issues, global optimization techniques including a simulated annealing method, the Monte Carlo method and genetic algorithms can be used^{18,19,20,21,22,23}. However, none of these approaches can determine the global solution(s) with 100% probability.
In this study, a new analytical method for the determination of magnetic structure is proposed, which allows (i) judging whether the obtained solution is a truly global one; (ii) evaluating the uniqueness of the solution obtained for a given set of experimental data; and (iii) completing the global optimization procedure in a very short time (typically, less than several seconds). Furthermore, the applicability of the proposed method is demonstrated using polarizedneutron powder diffraction data.
Mathematical Formulation for Applications of Semidefinite Relaxation Method
Relaxation techniques have been previously developed in the field of mathematical programming. In particular, semidefinite relaxation (SDR) combined with semidefinite programming (SDP) has found many applications in applied mathematics and engineering (for example, see Chapter 2.2 in ref.^{24}). SDR is an efficient technique for solving nonlinear optimization problems, such as quadratic programs (QPs), namely the minimization of multivariate quadratic polynomials under constraints. It should be noted that SDR could provide both fast convergence and a numerical proof of the global optimality of the obtained solutions using the global convergence property and duality theorem of the convex programming methods, as schematically shown in Fig. 1(B,C).
In the field of optical imaging, Candès et al. published a pioneering work (called the PhaseLift method), in which a sparse modelling approach was adopted for general phase retrieval^{25}. Furthermore, one of the authors (ROT) developed an SDRbased mathematical approach to investigate whether a crystal structure could be uniquely identified using only diffraction data and independent atomic model^{26}.
In this study, this method was applied to magnetic structure analysis by replacing the optimized parameters with magnetic moments. The problem of magnetic structure determination can be mathematically described by the following set of N quadratic equations:
where \({I}_{\mathrm{mag},\mathrm{obs}}({Q}_{k})\,\)and \({I}_{\mathrm{mag},\mathrm{cal}}({Q}_{k})\) denote the observed and calculated integrated magnetic diffraction intensities at the magnetic reflection \({Q}_{k}={h}_{{\rm{mag}}}\,{k}_{{\rm{mag}}}\,{l}_{{\rm{mag}}}\), respectively; x = (x_{1}, …, x_{n})^{T} and \({S}_{k}\) represents the coefficient matrix numerically obtained using the scattering crosssection formula for each \({Q}_{k}\), which consists of the absolute intensity scale factor, magnetic form factor, Lorentz factor, multiplicity and structural weight factor (the details of this formula are summarized in Supplementary Information).
The symbol \(\approx \) indicates that each \({I}_{{\rm{mag}},{\rm{obs}}}({Q}_{k})\) value includes an experimental error. In order to incorporate all errors, the following optimization problem is solved:
The inequality \({x}_{i}\le {R}_{i}\) can be also removed if the permitted range of \({x}_{i}\) (\({R}_{i}\), for example, the upper limit of magnetic moment) is uncertain while maintaining the validity of the subsequent discussion of the SDR and SDP techniques.
Equation (2) is classified as a socalled l^{1}norm minimization problem, which is equivalent to the following form of the quadratic programming problem:
The problems described by equations (2) and (3) are equivalent since they have the same set of solutions x and the minimized values of the objective functions (more details are provided in Supplementary Information). The basic strategy utilized in this work is to apply SDR to equation (3) in order to solve equation (2) and then provide a computational proof on the global convergence property of the solution. The leastsquares minimization of the \(\,\sum _{k=1}^{N}{({I}_{\mathrm{mag},\mathrm{obs}}({Q}_{k}){{\boldsymbol{x}}}^{T}S{\boldsymbol{x}})/{\rm{Err}}[{I}_{\mathrm{mag},\mathrm{obs}}({Q}_{k})]}^{2}\) function is avoided because a small increase in the polynomial degree considerably magnifies the size of the SDR problem (it increases proportionally to the power of N). Thus, it is possible to locate the global optimum by performing l^{1}norm minimization, which can be subsequently used as the initial parameter of the normal leastsquares method to calculate the refined parameters and then compare them with literature data.
Application to Experimental Data Analysis
Experimental results
The developed SDR method was verified by applying it to the experimental data obtained for pyrochlore Nd_{2}Ir_{2}O_{7}, which served as a proximate material for a threedimensional Weyl semimetal and a component of spintronic devices on the basis of its geometrically frustrated magnetism and 5delectron configuration^{27,28,29,30,31,32}. This state theoretically corresponds to the allin allout type of magnetic structure described by the magnetic propagation vector k_{mag} = (0, 0, 0), in which all the magnetic moments are oriented either towards the centre of the participating tetrahedron or in the opposite direction^{30,32}. This prediction was experimentally confirmed in previous unpolarized neutron diffraction studies^{33,34}. However, the superposition of the nuclear and magnetic reflections observed for the magnetic structures with k_{mag} = (0, 0, 0) produces ambiguous results during their separation. Furthermore, it is not possible to mathematically prove with 100% certainty the absence of other acceptable solutions to the problem of magnetic structure determination. Thus, in this work, polarized neutron diffraction studies were performed for this material, and the obtained magnetic structure was verified mathematically.
Figure 2 shows the representative neutron diffraction data obtained for Nd_{2}Ir_{2}O_{7} at the minimum temperature T = 1.4 K. The nonspinflip and spinflip parameters I_{OFF} and I_{ON} roughly correspond to the nuclear and magnetic reflection components I_{nuc} and I_{mag}, respectively. The magnitude of I_{OFF} is systematically larger than I_{ON} at all temperatures, thus confirming the necessity of conducting polarized neutron diffraction experiments. For I_{ON}, the intensity of the 113 reflection increases with decreasing temperature, indicating the existence of strong temperature dependence for this reflection, which is not observed for the 222 reflection. Moreover, as the flipping ratio of the neutron beam in the actual experiments is finite, the magnitudes of I_{ON} and I_{OFF} can be expressed by the following formulas:
$$\{\begin{array}{c}{I}_{{\rm{OFF}}}=(1{r}_{{\rm{mix}}}){I}_{{\rm{nuc}}}+\,{r}_{{\rm{mix}}}{I}_{{\rm{mag}}},\,\\ {I}_{{\rm{ON}}}={r}_{{\rm{mix}}}{I}_{{\rm{nuc}}}+\,(1{r}_{{\rm{mix}}}){I}_{{\rm{mag}}},\,\end{array}$$where r_{mix} = N_{−}/(N_{+} + N_{−}) is the mixing rate, and N_{+} (N_{−}) denotes the number of majorityspin (minorityspin) neutrons. The value of r_{mix} is selected to satisfy the condition I_{mag} = 0; hence, I_{ON} = r_{mix}·I_{nuc} at the paramagnetic T = 40 K. As a result, the pure magnetic intensity I_{mag} can be determined by combining I_{OFF} and I_{ON}. A more detailed explanation and data obtained for other reflections are presented in Supplementary Information, while the calculated I_{mag,obs} values are listed in Table 1.
Magnetic structure analysis results
The arbitrary magnetic structure with k_{mag} = (0, 0, 0) in the space group \(Fd\bar{3}m\) is described as the function of x_{arb} = (m^{(Nd)}_{1}, …, m^{(Nd)}_{12}, m^{(Ir)}_{1}, …, m^{(Ir)}_{12}) containing n_{arb} = 24 variables generated by the eight magnetic atoms of the unit cell and three Cartesian coordinates. Here, the magnetic symmetry was classified by performing IR analysis (this procedure is generally not required for the proposed method; however, it may be potentially useful because of the reduction of the number of variables if the number of observed reflection points is limited). The possible magnetic structures are described by the representations Γ_{Nd} = Γ_{3} + 2Γ_{5} + 3Γ_{7} + 6Γ_{9} and Γ_{Ir} = Γ_{3} + 2Γ_{5} + 3Γ_{7} + 6Γ_{9}, where Γ_{3} corresponds to the allin allout type of the magnetic structure, and the coefficients denote the numbers of basis vectors summarized in Table 2^{18,35}. Hence, the total numbers of variables are reduced to n_{Γ3} = 2, n_{Γ5} = 4, n_{Γ7} = 6 and n_{Γ9} = 12. Furthermore, representation Γ_{9} includes six ferromagnetic basis vectors. However, the Nd_{2}Ir_{2}O_{7} structure exhibits only extremely weak spontaneous magnetization (around 10^{−4}μ_{B}/formula unit)^{29}, which is significantly below the detection limit of the neutron diffraction technique. Therefore, the ferromagnetic basis vectors are precluded and the value of n_{Γ9} is further reduced from 12 to 6 during the analysis of the neutron diffraction data.
Thus, the variables used for the magnetic structure analysis in this work are defined as follows: x_{Γ3} = (m^{(Γ3,Nd)}_{1}, m^{(Γ3,Ir)}_{1}), x_{Γ5} = (m^{(Γ5,Nd)}_{1}, m^{(Γ5,Nd)}_{2}, m^{(Γ5,Ir)}_{1}, m^{(Γ5,Ir)}_{2}), x_{Γ7} = (m^{(Γ7,Nd)}_{1}, m^{(Γ7,Nd)}_{2}, m^{(Γ7,Nd)}_{3}, m^{(Γ7,Ir)}_{1}, m^{(Γ7,Ir)}_{2}, m^{(Γ7,Ir)}_{3}) and x_{Γ9} = (m^{(Γ9,Nd)}_{1}, m^{(Γ9,Nd)}_{2}, m^{(Γ9,Nd)}_{3}, m^{(Γ9,Ir)}_{1}, m^{(Γ9,Ir)}_{2}, m^{(Γ9,Ir)}_{3}). The goal is to determine the globally optimal solutions x for representations Γ_{3}, Γ_{5}, Γ_{7} and Γ_{9} using the I_{mag,obs} magnitudes listed in Table 1. After that, the solution characterized by the best fit can be selected.
The output values produced by the SDP solver are as follows.

(1)
The convergence procedure results in the following coefficients:
$$\begin{array}{c}{{X}_{{\rm{\Gamma }}3}}^{({\rm{opt}})}\approx {{{\boldsymbol{x}}}_{{\rm{\Gamma }}3}}^{({\rm{opt}}1)}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}3}}^{({\rm{opt}}1)T};\\ {{X}_{{\rm{\Gamma }}5}}^{({\rm{opt}})}\approx ({{{\boldsymbol{x}}}_{{\rm{\Gamma }}5}}^{({\rm{opt}}1)}{{x}_{{\rm{\Gamma }}5}}^{({\rm{opt}}1)T}+{{{\boldsymbol{x}}}_{{\rm{\Gamma }}5}}^{({\rm{opt}}2)}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}5}}^{({\rm{opt}}2)T})/2;\\ {{X}_{{\rm{\Gamma }}7}}^{({\rm{opt}})}\approx 0;\\ {{X}_{{\rm{\Gamma }}9}}^{({\rm{opt}})}\approx ({{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}1)}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}1)T}+{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}2)}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}2)T}+{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}3)}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}3)T})/3;\end{array}$$and
$$\begin{array}{c}{{{\boldsymbol{x}}}_{{\rm{\Gamma }}3}}^{({\rm{opt}})}=(\,1.20,\,0.19);\\ {{{\boldsymbol{x}}}_{{\rm{\Gamma }}5}}^{({\rm{opt}}1)}=(0.55,\,0.,\,0.48,\,0.),\,{{{\boldsymbol{x}}}_{{\rm{\Gamma }}5}}^{({\rm{opt}}2)}=(0.,\,0.55,\,0.,\,0.48);\\ {{{\boldsymbol{x}}}_{{\rm{\Gamma }}7}}^{(opt)}=(0.,\,0.,\,0.,\,0.,\,0.,\,0.);\\ {{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}1)}=(0.55,\,0.,\,0.,\,\,0.52,\,0.,\,0.),\,{{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}2)}=(0.,\,0.55,\,0.,\,0.,\,\,0.52,\,0.),\\ {{{\boldsymbol{x}}}_{{\rm{\Gamma }}9}}^{({\rm{opt}}3)}=(0.,\,0.,\,0.55,\,0.,\,0.,\,\,0.52);\end{array}$$where the values of x are expressed the μ_{B} units, and the negative sign indicates the nearest ferromagnetic Nd–Ir correlation. While a single optimum solution is determined for representation Γ_{3}, multiple solutions are obtained for Γ_{5} and Γ_{9}, respectively, in accordance with the rank values of X_{Γ5}^{(opt)} and X_{Γ9}^{(opt)}, which indicate the existence of an infinite number of solutions with the same objective functions \({{\boldsymbol{x}}}_{{\rm{\Gamma }}5}^{({\rm{opt}})}=\,\cos \,\theta {{\boldsymbol{x}}}_{{\rm{\Gamma }}5}^{({\rm{opt}}1)}+\,\sin \,\theta {{\boldsymbol{x}}}_{{\rm{\Gamma }}5}^{({\rm{opt}}2)}\) and \({{\boldsymbol{x}}}_{{\rm{\Gamma }}9}^{({\rm{opt}})}=\,\cos \,\theta {{\boldsymbol{x}}}_{{\rm{\Gamma }}9}^{({\rm{opt}}1)}+\,\sin \,\theta \,\cos \,\varphi {{\boldsymbol{x}}}_{{\rm{\Gamma }}9}^{({\rm{opt}}2)}+\,\sin \,\theta \,\sin \,\varphi {{\boldsymbol{x}}}_{{\rm{\Gamma }}9}^{({\rm{opt}}3)}\), where \(\theta \) and \(\varphi \) are arbitrary. Without SDR, it is difficult to find the optimum solutions for this type of problems and prove that better solutions do not exist. Furthermore, the zero magnitude of x_{Γ7}^{(opt)} is obtained for representation Γ_{7}. Indeed, when x_{Γ7} values are finite (nonzero), the \({I}_{{\rm{mag}},{\rm{cal}}}\) values for \({I}_{{\rm{mag}},{\rm{obs}}}=0\) indices increase more rapidly than those for \({I}_{{\rm{mag}},{\rm{obs}}}\ne 0\) indices. Thus, the SDR method automatically overcomes these issues.

(2)
The obtained indicator values for representations Γ_{3}, Γ_{5}, Γ_{7} and Γ_{9} are as follows.

a)
The corresponding duality gaps determined by the SDP solver are equal to \({\rm{\Delta }}f=2.1\times {10}^{7}\), \(1.4\times {10}^{6}\), \(3.1\times {10}^{6}\) and \(8.0\times {10}^{7}\), respectively. Their magnitudes are close to zero, indicating that the convergence to the global optimums is achieved.

b)
The minimized objective function \({f}^{({\rm{gl}})}\underline{\underline{{\rm{def}}}}\,\sum _{k=1}^{N}\,{I}_{{\rm{mag}},{\rm{obs}}}({Q}_{k}){I}_{{\rm{mag}},{\rm{cal}}}({Q}_{k})/{\rm{Err}}[{I}_{{\rm{mag}},{\rm{obs}}}({Q}_{k})]\) = 4.5, 19, 32 and 27, and the more familiar Rfactor, \({R}_{{\rm{Bragg}}}\underline{\underline{{\rm{def}}}}\,(\sum _{k=1}^{N}{I}_{\mathrm{mag},\mathrm{obs}}({Q}_{k}){I}_{\mathrm{mag},\mathrm{cal}}({Q}_{k}))/(\sum _{k=1}^{N}\,{I}_{\mathrm{mag},\mathrm{obs}}({Q}_{k}))\) = 0.13, 0.63, 1.0 and 0.81, respectively. These results show that the smallest values are obtained for representation Γ_{3}.

c)
The goodness of the fit \({\chi }^{2}\underline{\underline{{\rm{def}}}}\,(\sum _{k=1}^{N}{{I}_{{\rm{mag}},{\rm{obs}}}({Q}_{k}){I}_{{\rm{mag}},{\rm{cal}}}({Q}_{k})}^{2}\,/\,\,{\rm{Err}}{[{I}_{{\rm{mag}},{\rm{obs}}}({Q}_{k})]}^{2})/(N{n}_{{\rm{\Gamma }}})\) = 2.6, 14, 25 and 20, and the related statistical parameter \({f}^{({\rm{gl}})}/(N{n}_{{\rm{\Gamma }}})=0.75\), 4.8, 16 and 14, respectively. The value closest to the expected value (1 for \({\chi }^{2}\); \(\sqrt{2/\pi }\approx 0.798\) for the latter parameter) is obtained for Γ_{3}.
All these facts suggest that Γ_{3} represents the best solution, whereas representations Γ_{5}, Γ_{7} and Γ_{9} are excluded for the first time. For clarity, the values of I_{mag,cal} are listed in Table 2 and also shown in Fig. 3. The magnitude of I_{mag,calΓ3} matches I_{mag,obs} very well, whereas the globally optimal I_{mag,calΓ5}, I_{mag,calΓ7} and I_{mag,calΓ9} parameters substantially differ from the corresponding I_{mag,obs} values.
After proving mathematically the uniqueness of representation Γ_{3}, the refined values m_{Nd} = −1.22(5)μ_{B} and m_{Ir} = 0.14(5)μ_{B} are obtained using the x_{Γ3}^{(opt)} values as the initial parameters in the normal leastsquares method. These results are comparable with the reported values of m_{Nd} = −1.27(1)μ_{B} and m_{Ir} = 0.34(1)μ_{B}^{34}.
Discussion
Representation Γ_{9} (the only IR containing ferromagnetic basis vectors^{35}) is rejected as the optimal solution despite the existence of weak ferromagnetism^{29}. The observed inconsistency suggests that this ferromagnetism is symmetrically decoupled from the bulk magnetic structure (for example, as a surface or interfaceprotected property). In fact, by performing careful measurements of the macroscopic magnetization and electrical resistivity of isomorphic Cd_{2}Os_{2}O_{7}, it was found that the surface ferromagnetism coupled with novel spinpolarized conductivity emerged on the walls between the allin allout and allout allin antiferromagnetic domains^{36}. The macroscopic observation is consistent with the findings of this study verified both microscopically and mathematically, indicating their potential applicability in domain wall spin electronics.
We discuss the expected application scope of the SDR method. After determining the list of (h_{mag}, k_{mag}, l_{mag}, I_{mag,obs}) values, the described SDR method can be used to find the corresponding magnetic structures as the global solutions. First, the configurations with k_{mag} = (0, 0, 0) are considered, indicating their high potential applicability in various fields (including magnet materials). Second, this method is not restricted to polarized neutron diffraction experiments, but can be also used in studies involving unpolarized neutrons when the magnetic structure is characterized by k_{mag} ≠ (0, 0, 0) or k_{mag} = (0, 0, 0) with detectable magnetic moment. Both the magnetic and crystallographic structures can be simultaneously refined by the normal leastsquares method, in which the obtained SDR solutions are utilized as the initial values of the magnetic structural parameters. Third, the SDR technique is able to easily process thousands of independent variables. Therefore, magnetic structures of arbitrary types can be theoretically determined using the advanced diffractometers that provide a relatively large number of reflection points (even for the target materials with complex compositions).
The diffraction intensities are not represented by quadratic functions of the atomic positions r_{j}; hence, the SDR technique seems to be inapplicable for determining the values of r_{j} (crystal structure). However, the neutron and Xray diffraction intensities are represented by those of the nuclear and electron densities (generalized crystal structure), respectively. Likewise, a magnetic structure is also generalized to the magnetic moment density. Thus, the SDR technique is expected to enable analysing the global solutions of the generalized structures together with the aforementioned highvolume processing ability, such as protonic/ionic distributions in the conductors and electronic spinorbital distributions.
Materials and Methods
Calculations
The system of quadratic equations was solved using the SDP solver SDPA^{37}. To find the global optima of SDP problems, interior point methods were efficiently used^{38}.
Experiments
The polarized neutron elastic scattering experiments were performed using the HB1 thermal neutron threeaxis spectrometer located at the High Flux Isotope Reactor (HFIR) of the Oak Ridge National Laboratory (ORNL). Heusler alloy 111 reflection crystals were utilized as the monochromator and analyser. The flipping ratio R = 10 was obtained using the nuclear 222 reflection at a paramagnetic temperature of 40 K corresponding to the beam polarization P = 0.82. The polarization vector was set parallel to the scattering vector (P//Q). The incident energy of neutrons was E_{i} = 13.5 meV. The horizontal collimator sequence was 48′(open)–80′–80′–240′. A pyrolytic graphite Braggreflection filter was used to efficiently eliminate the contamination caused by higherorder wavelengths.
A powder Nd_{2}Ir_{2}O_{7} sample was synthesized by a solidstate reaction method inside a quartz tube. About 4.8 g of the sample was wrapped in thin aluminium foil and shaped to a hollow cylinder with a thickness of 0.8 mm and diameter of 20 mm to mitigate the effect of the strong neutron absorption of Ir nuclei. The cylinder was stored in an aluminium container filled with He gas and placed under the cold heads of a Heclosedcycle (Displex) or liquidHetype (Orange) cryostat.
Additional information
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Acknowledgements
Neutron diffraction experiments were conducted using the High Flux Isotope Reactor, a user facility of the DOE Office of Science operated by the Oak Ridge National Laboratory (USA). This study was partially supported by the U.S.Japan Cooperative Program on Neutron Scattering. This study was financially supported by the MEXT/JSPS KAKENHI (grant Nos JP18K03503, JP17H06137 and JP15H03692), JST PRESTO (grant No. JPMJPR14E6), JapanUS program administrated by ISSP at the University of Tokyo and FRIS program for the creation of interdisciplinary research at the Tohoku University.
Author information
Affiliations
Department of Physics, Tohoku University, Aoba, Sendai, 9808578, Japan
 K. Tomiyasu
Faculty of Science, Yamagata University, Yamagata, 9908560, Japan
 R. OishiTomiyasu
JST, PRESTO, Saitama, 3320012, Japan
 R. OishiTomiyasu
Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN, 37831, USA
 M. Matsuda
Faculty of Engineering, Kyusyu Institute of Technology, Kitakyusyu, 8048550, Japan
 K. Matsuhira
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Contributions
K.T. conceived and conducted this study. R.O.T. performed the mathematical optimization. K.M. synthesized the sample. K.T. and M.M. performed the neutron diffraction experiments. K.T. and R.O.T. analysed the data. K.T. and R.O.T. wrote the manuscript based on the feedback provided by all authors.
Competing Interests
The authors declare no competing interests.
Corresponding authors
Correspondence to K. Tomiyasu or R. OishiTomiyasu.
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