# A comparative study of the electronic and magnetic properties of BaFeAs and BaMnAs using the Gutzwiller approximation

## Abstract

To elucidate the role played by the transition metal ion in the pnictide materials, we compare the electronic and magnetic properties of BaFeAs with BaMnAs. To this end we employ the LDA+Gutzwiller method to analyze the mass renormalizations and the size of the ordered magnetic moment of the two systems. We study a model that contains all five transition metal 3d orbitals together with the Ba-5d and As-4p states (ddp-model) and compare these results with a downfolded model that consists of Fe/Mn d-states only (d-model). Electronic correlations are treated using the multiband Gutzwiller approximation. The paramagnetic phase has also been investigated using LDA+Gutzwiller method with electron density self-consistency. The renormalization factors for the correlated Mn 3d orbitals in the paramagnetic phase of BaMnAs are shown to be generally smaller than those of BaFeAs, which indicates that BaMnAs has stronger electron correlation effect than BaFeAs. The screening effect of the main As 4p electrons to the correlated Fe/Mn 3d electrons is evident by the systematic shift of the results to larger Hund’s rule coupling J side from the ddp-model compared with those from the d-model. A gradual transition from paramagnetic state to the antiferromagnetic ground state with increasing is obtained for the models of BaFeAs which has a small experimental magnetic moment; while a rather sharp jump occurs for the models of BaMnAs, which has a large experimental magnetic moment. The key difference between the two systems is shown to be the d-level occupation. BaMnAs, with approximately five d-electrons per Mn atom, is for same values of the electron correlations closer to the transition to a Mott insulating state than BaFeAs. Here an orbitally selective Mott transition, required for a system with close to six electrons only occurs at significantly larger values for the Coulomb interactions.

###### pacs:

71.10.Fd, 71.20.Be, 71.27.+a## I Introduction

The discovery of high T superconductivity in LaOFFeAs has initiated a detailed investigation of these and related iron based compounds with the ultimate aim to identify new high temperature superconductors(1). Many binary, ternary and quaternary compounds have been synthesized and investigated experimentally, some of which were quickly found to exhibit high T superconductivity with electron or hole doping or under pressure or intrinsically (2); (3); (4); (5); (6); (7). Meanwhile, several closely related and physically interesting systems have also been studied. An interesting example is the BaMnAs compound, which has the same layered tetragonal ThCrSi-type crystal structure as the BaFeAs at room temperature(8); (9); (10); (11). BaMnAs is an antiferromagnetic (AFM) insulator with a small gap; while BaFeAs, a parent compound of the Fe-based high T superconductors, is an AFM metal at low temperatures. The more localized behavior of the ordered magnetic state in the Mn-based system suggests that electronic correlations in this system are stronger or more efficient in changing the electronic properties of the material. A closer, comparative investigation of distinct transition metal ions therefore promises to reveal further whether iron is indeed special among its neighbors in the periodic table. This is also expected on qualitative grounds on the basis of the Hund’s rule picture(13).

Theoretically, the description of the normal states for iron pnictide superconductors is complicated by the multi-orbital nature and the presence of electron correlation effects. Interesting results can be obtained from low energy theories that are primarily concerned with states in the immediate vicinity of the Fermi surface(14); (15); (16); (17); (18); (19). However, material specific insight often requires a careful analysis of states over a larger energy window. In the iron pinctide and chalcogenides the strength of the correlations is controlled by the Hund’s rule coupling , rather than by the Hubbard or the p-d charge transfer energy(13). This makes these materials a new class of correlated metals, different from doped Mott or charge transfer insulators. Calculations based on density functional theory (DFT) usually yield too wide Fe 3d bands and too large magnetic moment in the AFM ground state(12). Recently the AFM phase of the iron pnictide parent compounds has been successfully described by using a combination of DFT and dynamical mean field theory (DMFT) with full charge self-consistency(20). These investigations clearly demonstrated the important role played by the Hund’s rule coupling for the magnetic and electronic properties of the iron pnictides. A systematic analysis of a large class of Fe-based materials further demonstrated that the nature and strength of local correlations are rather universal, while material specifics result from changes in the kinetic energy, amplified by the frustrated nature of electron hopping path due to Fe-As-Fe and direct Fe-Fe overlaps(21). This universality in the value of the local Coulomb interactions , , only exists if one includes in addition to the Fe-3d states at least the As 4p orbitals. Downfolding to models with iron states only is sufficient to lead to material specific variations in the local correlations. In view of these insights is it important to compare the behavior of Fe-based systems with systems based on other transition metals, also in view of the ongoing debate whether these systems should be considered weakly or strongly correlated.

On a technical level, quite a few efforts have been devoted to study the electronic and magnetic properties of the systems using the Gutzwiller variational method(22) and simplified tight-binding models(23); (24) with the particular appeal that the Gutzwiller approach is computationally cheaper if compared to more sophisticated DMFT approaches such as the usage of Quantum Monte Carlo algorithms. For example. the experimental magnetic moment was obtained in a three band Hubbard model of LaOFeAs which contains only Fe 3d orbitals(23). Calculations based on the five-band model show that the orbitals are also important and the system exhibits a sharp transition from paramagnetic (PM) state to AFM state with large magnetic moment when increases, which is different from the results of three-band model(24). Another important question is whether, in addition to the Fe 3d orbitals, the inclusion of As 4p elections is required for a more quantitative description of the AFM and paramagnetic phases. Finally, recent calculations for LaOFeAs based on the LDA+Gutzwiller approach that includes a Fe3d–As4p Wannier-orbital basis does indeed reproduce the experimentally observed small ordered magnetic moment over a large region of () parameter space(25).

In this paper, we report a comparative study of the BaFeAs and BaMnAs on the electronic and magnetic properties by investigating the Fe/Mn d-band model and the ddp-model that includes Fe/Mn 3d, Ba 5d, and As 4p orbitals with Gutzwiller approximation(26); (27); (28) which has been shown to be equivalent to a slave-boson mean field theory(29). The paramagnetic phase for the two systems has also been investigated using LDA+Gutzwiller method with electron density self-consistency(30); (31). BaMnAs is shown to be a more correlated material than BaFeAs. The screening effect of the As 4p electrons is evident by the comparison between the results of the Fe/Mn d-model and those of the ddp-model or LDA+Gutzwiller method. The key difference in the behavior of these systems is shown to be the distinct electron count of the 3d states, a result that is robust against changes in the detailed description of these systems. While the even number of electrons for an Fe site requires that the system undergoes an orbitally selective Mott transition, Mn with five electrons can more easily localize and therefore has a much stronger tendency towards large moment magnetism and Mott localization, even for the nominally same values of the Coulomb interactions. The prospect to tune the tendency towards localization by varying the transition metal ions may therefore play an important role in optimizing the strength of electronic correlations for high temperature superconductivity.

## Ii Formalism

For the sake of being self-contained, we outline the main formalisms for the multiband model with the Gutzwiller approximation(26); (27); (28) and the LDA+Gutzwiller approach with electron density self-consistency(30); (31).

### ii.1 Multiband model with the Gutzwiller approximation

The multi-band Hamiltonian with local many-body interactions is written as

(1) |

where the bare paramagnetic band Hamiltonian () is

(2) |

is the electron hopping element between orbital at site and orbital at site . is the orbital level.For the Fe/Mn d-model, and run over the Fe/Mn 3d orbitals. For the ddp-model, and run over the Fe/Mn 3d orbitals, Ba 5d orbitals, and As 4p orbitals. () is the electron creation (annihilation) operator. is the spin index.

The typical Hubbard density-density type interaction term () for Fe 3d electrons is

(3) |

which is usually sufficient for describing collinear magnetic order(23). Here is the correlated Fe/Mn 3d orbital index, , and .

We take a variational wave function of the Gutzwiller form,

(4) |

with the Gutzwiller approximation to calculate the expectation values of Eq. 1 (26); (27); (28). is the uncorrelated wave function. is the Gutzwiller projection operator, which adopts the following form

(5) |

where is the Fock state generated by a set of

(6) |

with or , which identifies whether there is an electron with spin occupied in orbital for Fock state at the site. is a variational parameter which controls the weight of the local Fock state in the Gutzwiller wave function. for the empty and singly occupied configurations because in these cases there are no electron-electron repulsion involved. According to Ref. (28), the expectation value of the electron Hamiltonian can be expressed as

(7) |

where and . We define the Gutzwiller orbital renormalization factor for Ba 5d and As 4p orbitals in the ddp-model since they are not considered as strongly correlated orbitals. Following Ref. (28), for the Fe/Mn 3d orbitals

(8) |

with . is the occupation probability of configuration , which absorbs and serves as the additional variational parameter due to the Gutzwiller wave function.

Since in the Hamiltonian of Eq. 1 is obtained by downfolding the DFT band structure, some contributions from have already been taken into account by in a mean-field way. Such contributions are commonly referred to as the double counting term. Consequently, the total energy of the system is given by

(9) |

with

(10) |

following the treatment in DFT+U method(32); (33). Here () is the averaged Coulomb U (Hund’s rule coupling J) parameter, which for d orbitals is given as(31); (34)

(11) |

(12) |

is the expectation value of the total Fe/Mn d-orbital occupancy at site . The double counting term introduces some spin-independent chemical potential shift for the Fe/Mn 3d orbitals,

(13) |

In the Fe/Mn d-model that contains only 3d states, has no effect since it merely shifts all the Fe/Mn 3d levels by a constant. However, in the ddp-models becomes important because it changes the position of the Fe/Mn 3d levels with respect to Ba 4d and As 4p orbitals and hence affects the electron flow between these orbitals.

The minimization of with the constraints of and yields an effective single-particle Hamiltonian

(14) |

where if belongs to the correlated Fe/Mn 3d orbitals and otherwise. It has been shown that describes the Landau-Gutzwiller quasiparticle bands(37), and the square of the orbital renormalization factor corresponds to the quasiparticle weight(31). and are obtained by solving the following equations.

(15) |

where

(16) |

with . from Eq. 14 and from Eq. 15 need to be solved self-consistently to obtain the final solution(35).

### ii.2 LDA+Gutzwiller

The

above formalism based on the Gutzwiller approximation on the multiband model can be naturally combined with DFT, in which full electron density convergence can be achieved(30); (31); (36). The total energy density functional can be written as

(17) |

where is the kinetic energy operator and is the Hartree potential energy. The electron-ion and ion-ion potential energies are given by and , respectively. In the LDA+Gutzwiller method(30); (31), the approximate exchange-correlation energy takes the following form

(18) |

The electron density under the Gutzwiller approximation can be written as

(19) |

where is a general complete basis set including local correlated orbitals (e.g., Fe/Mn 3d orbitals) as well as nonlocal orbitals. indicates that the summation excludes the term with . The kinetic energy is also renormalized

(20) |

The total energy of the closed form can be similarly minimized as in the above multiband model with respect to and . The resultant effective single-particle Hamiltonian has the same form as Eq. 14 with the hopping element

(21) |

The LDA screening potential is the sum of the Hartree potential and the exchange-correlation potential . The renormalized orbital level if belongs to the correlated Fe/Mn 3d orbitals and otherwise. Here and and are obtained by solving the same equation as Eq.15. One can see that the major difference is that the hopping element and the orbital level will be updated self-consistently by the LDA screening potential in LDA+Gutzwiller method, while they are fixed in the multiband model.

## Iii Effects caused by downfolding

Fe/Mn | |||||

Fe/Mn: | -0.34/-0.32 (-0.35/-0.33) | 0.25/0.20 (0.21/0.17) | 0.31/0.28 (0.27/0.24) | -0.25/-0.20 (-0.21/-0.17) | 0 |

0.25/0.20 (0.21/0.17) | -0.22/-0.16 (-0.14/-0.10) | -0.11/-0.10 (-0.09/-0.08) | 0.12/0.11 (0.08/0.08) | 0.18/0.16 (0.17/0.15) | |

0.31/0.28 (0.27/0.24) | -0.11/-0.10 (-0.09/-0.08) | 0.06/0.03 (0.01/-0.01) | 0.11/0.10 (0.09/0.08) | 0 | |

-0.25/-0.20 (-0.21/-0.17) | 0.12/0.11 (0.08/ 0.08) | 0.11/0.10 (0.09/0.08) | -0.22/-0.16 (-0.14/-0.10) | 0.18/0.16 (0.17/0.14) | |

0 | 0.18/0.16 (0.17/0.15) | 0 | 0.18/0.16 (0.17/0.15) | -0.13/-0.07 (-0.09/-0.03) | |

Fe/Mn: | -0.07/-0.05 (-0.06/-0.05) | 0.14/0.11 (0.10/0.08) | 0 | 0 | 0 |

-0.14/-0.11 (-0.10/-0.08) | 0.15/0.11 (0.08/0.07) | 0 | 0 | 0 | |

0 | 0 | -0.01/-0.02 (0/-0.01) | 0.17/0.15 (0.13/0.12) | -0.18/-0.13 (-0.12/-0.08) | |

0 | 0 | -0.16/-0.15 (-0.13/-0.12) | 0.32/0.27 (0.20/0.17) | 0.04/0.06 (0.04/0.05) | |

0 | 0 | -0.17/-0.13 (-0.12/-0.08) | -0.04/-0.06 (-0.04/-0.05) | 0.11/0.09 (0.09/0.07) | |

As: | (-0.50/-0.42) | (0.39/0.33) | 0 | 0 | 0 |

0 | 0 | (0.34/0.29) | (0.09/0.12) | (-0.49/-0.41) | |

0 | 0 | (0.14/0.13) | (-0.69/-0.58) | (0.32/0.25) |

The Fe/Mn d-model and ddp-model for BaFeAs and BaMnAs have been obtained by downfolding the first-principles LDA electron bands of the experimentally determined crystal structures(38); (9) using the quasi-atomic minimal basis-set orbitals (QUAMBOs)(39); (40); (41); (42). The main idea of the QUAMBO approach is to recover a set of local quasi-atomic orbitals by performing an inverse unitary transformation for the “bonding” and “anti-bonding” states. In practice, the “bonding states” are some occupied bands or low energy bands which are intended to be preserved in the new local orbital representation. The “anti-bonding” states are constructed from the orthogonal subspace of the “bonding” subspace and are optimized such that resultant QUAMBOs have maximal similarity with the free atomic orbitals. The orthogonal subspace is spanned by the wave functions in some energy window. It becomes complete in the infinite energy or band limit, where succinct closed form for QUAMBOs can still be obtained(41). In principle, different choices of the “bonding” states and the energy window for the “anti-bonding” states will yield different set of QUAMBOs and tight-binding parameters, which is reasonable and acceptable since the downfolding of the band structure should not be unique. We find that the ddp model will give too many Fe/Mn d-electrons if it is obtained by treating all the occupied states and virtual states up to eV above Fermi level as the “bonding” states in the infinite band limit: d-electrons per Fe atom for BaFeAs (close to the analysis of Ref.(43)) and for BaMnAs, while the nominal value would be and , respectively. Such large deviation of the correlated electron number clearly do not properly reflect the correct physics of these materials. This problem does not exist for the Fe/Mn d-model where the electron filling is fixed by assumption. In order to have a general tight-binding model suitable for the correlated local orbital-based approaches, we choose a finite energy window around the Fermi level for the generation of the “anti-bonding” states and another smaller energy window to control the Bloch bands which will contribute to the Fe/Mn d orbitals. We can then construct tight-binding models with reasonable number of correlated d-electrons. As a result, we have Fe 3d-electrons and Mn 3d-electrons for the ddp-model. Those are the initial occupancies that are further reduced due to the self-consistent determination of the occupancies within the Gutzwiller approach and the double counting corrections, reaching values close to Fe 3d-electrons and Mn 3d-electrons.

Figure 1 and 2 show the bare band structures () of the d-model and the ddp-model for BaFeAs and BaMnAs, respectively. The LDA band structures have also been plotted for comparison. One can see that the band structure from the ddp-model agrees very well with the LDA result in the low energy window for both systems. The Fe/Mn d-model, however, fails to reproduce one low energy unoccupied band near -point which is mainly contributed by the Ba 5d orbitals. The total number of electrons is per Fe(Mn) atom for the d-model and per Fe(Mn) atom for the ddp-model. The tight-binding parameters between one Fe/Mn atom and its nearest Fe/Mn atom, second the nearest Fe/Mn atom and the nearest As atom are listed in Table 1, with the atomic configuration and the coordinate system shown in Fig.3. The hopping parameters of the BaFeAs system are overall larger in magnitude than those of BaMnAs system, which is mainly owing to the fact that BaMnAs has a much larger volume than BaFeAs although the ionic radii of Fe and Mn are very close. The direct Fe-Fe/Mn-Mn hopping parameters become smaller in the ddp-model, as expected. The Fe d-model has been compared with the one downfolded using maximally localized Wannier function (MLWF)(44); (45). Although the MLWF approach can achieve better fitting after some fine tuning(46), we find that the results reported here are not sensitive to this detail.

## Iv Comparative study of the d and ddp model for PM phase

Figure 4 and 5 show the variation of the -factors for the correlated d-orbitals with increasing Hund’s rule coupling J and Hubbard U fixed at 2eV, 3eV and 4eV in the paramagnetic state of the Fe/Mn d-model and the ddp-model, respectively. On the small J side, the -factors for both models of the compounds stay almost the same. With increasing J, the -factors start to drop rapidly but remain finite for the two models of BaFeAs. In contrast, the -factors exhibit a sharp decrease to zero for both models of BaMnAs, i.e., Mott localization for all the orbitals sets in beyond a threshold value of . This indicates that BaMnAs is a more correlated system than BaFeAs. By increasing from eV to eV, the transition of the -curves occurs at somewhat smaller -values for all the model calculations. The results show a much stronger dependence on the Hund’s rule coupling rather than Hubbard , which is typically the case in correlated multiband systems. Comparing the Fe/Mn d-model and the ddp-model, we observe a systematic shift of the -curves to larger value with the inclusion of the Ba 5d and As 4p orbitals to the Fe/Mn d-model. Thus, a larger value of is needed in a ddp-model to obtain the similar -factors as in the Fe/Mn d-model. This can be attributed to the screening effect of additional electrons in the ddp-model as caused the hybridization of the Fe/Mn 3d orbitals with other, less correlated degrees of freedom.

The general feature of the local d-orbital occupations in the model calculations as shown in Fig. 6 and 7 is consistent with that of the -factors described above. While the Hubbard U parameter tends to polarize the orbitals, the Hund’s rule coupling J favors the equalization of the local orbital occupations. All local d-orbitals become half occupied as the system approaches the Mott transition for the models of BaMnFe which has 5 electrons in each 5 Mn 3d orbitals. For the BaFeAs system, there is 6 electrons in each 5 Fe 3d orbitals. Hence we expect an orbital selective Mott transition would occur with large and (47); (48). We did perform model calculations at even larger and find an orbitally selective transition where the factors of all orbitals except the -orbital vanish, while as the orbital becomes completely filled. This behavior requires however unphysically large values of . Indeed some signature can be identified as one can see that becomes closest to 0.5 and drops most rapidly with increasing and for the Fe d-model. When comparing the results of Mn/Fe d-model and the ddp-model, a similar systematic shift of the local orbital occupation curves to the large side is observed due to the screening and hybridization effect. We conclude that BaMnFe is approaching a Mott insulator with large localized moment. Combining our calculations in the magnetically ordered state and in the paramagnetic state we obtain eV to yields the experimentally observed ordered moment, values that are not yet in the Mott insulating regime, yet they are rather close. In contrast, BaFeAs is significantly away from Mott localization, yet there are clearly visible polarizations of the orbital populations that demonstrate that the system is in an intermediate regime. To demonstrate that this is indeed the case we determined the quasiparticle weight of a system with the tight binding parameters (ddp-model) of BaFeAs, yet with a total electron count of 11 per Fe atom as appropriate for BaMnAs (see Fig. 8). Now a Mott transition similar to the actual BaMnAscalculation occurs, albeit at a somewhat larger value of .

## V Effects of charge self-consistency

The variation of the -factors and occupations of the correlated Fe/Mn 3d orbitals with U and J has further been investigated by the LDA+Gutzwiller method(30); (31), which is built upon the LDA+U approach(49); (50). We use the same correlated orbitals obtained via the QUAMBO procedure as in the Fe/Mn d-models for the calculations and achieve the electron density self-consistency. As shown in Fig. 9, the -curves exhibit a similar trend but vary in a way much slower than that in the Fe/Mn d-models, which can again be attributed to the screening effect of the other electrons in the systems. Our results on the BaFeAs system are in good agreement with those reported in Ref. (22). Overall, the -factors for BaMnAs are systematically smaller than those for BaFeAs. Note that the calculated screened U(J) is 3.6(0.76)eV for Fe and 3.2(0.70)eV for Mn based on the constrained random phase approximation and the maximally localized Wannier function(51), it is fairly reasonable to assume that the screened interaction parameters in the models investigated here are also very close. Therefore BaMnAs is a more correlated material than BaFeAs.

## Vi Comparative study of the d and ddp model for AFM phase

The ground state AFM phase has also been studied for the models of the two systems. Figure 11 shows the behavior of the magnetic moment as a function of J with U fixed at 2eV, 3eV and 4eV in the stripe-type AFM ground state for BaFeAs. In contrast to the Fe d-model including complete local interactions for LaOFeAs in which the system exhibits a sharp transition from PM state to AFM state with large magnetic moment using the Gutzwiller approximation(24), the models with only density-density type interactions for BaFeAs describe the PM-AFM transition fairly well as the magnetic moment increases rapidly yet smoothly when J rises as indicated by the solid symbols in the upper panel. The magnetic moment varies from to in the range of eV with eV. For reference the experimental magnetic moment is for BaFeAs(52). With the inclusion of the Ba 5d and As 4p orbitals in the ddp-model, the magnetic moment increases slower as seen in the lower panel. The high sensitivity of the magnetic moment to Hund’s rule coupling J is consistent with the DFT+DMFT calculation results(20). For comparison, Fig. 11 also shows the magnetic moment of the AFM phase in the Fe d-model with Hartree-Fock approximation by the open symbols in the upper panel. Within Hartree-Fock approximation, the PM-AFM transition takes place at much smaller J. The magnetic moment exhibits quite smooth variation with increasing J at U=2eV. However, an abrupt transition from PM to AFM state with large magnetic moment occurs at U=3eV. In comparison, the models of BaMnAs yield a very sharp transition from PM to the G-type AFM ground state with magnetic moment as shown in Fig. 12. However, it is still reasonable since the experimental magnetic moment is 3.88(9). The -factors for the models of BaFeAs in the AFM ground state are always or order unity ().

## Vii Conclusion

In summary, we have studied the Fe/Mn d-model and the ddp-model on the electronic and magnetic properties of the BaFeAs and BaMnAs systems. The renormalization factors of the correlated Mn 3d orbitals are found to be systematically smaller than those of Fe 3d orbitals, implying that the electron correlation for BaMnAs are much more efficient to cause Mott localization physics compared to BaFeAs. Ultimately this is due to the fact that Fe, with its close to six electrons, must undergo an orbital selective Mott transition while the odd number of electrons in case of Mn allow for a more ordinary Mott transition. While the strength of the interactions are not sufficient for Mott localization in either system the Mn-based material is significantly closer to localization. The LDA+Gutzwiller results on the paramagnetic phase with electron density self-consistency also confirm the conclusion. The variation of the magnetic moment in the AFM ground state of the two compounds seems in accordance with the experimental results: a smooth increase of the magnetic moment with rising for the stripe-AFM ground state of BaFeAs with small experimental magnetic moment and an abrupt jump of the magnetic moment from to about for the G-AFM ground state of BaFeAs with large experimental magnetic moment. We also checked that the two different ordered states are indeed energetically lower in the respective systems. The Gutzwiller approximation, however, is not able to provide a quantitatively consistent description of the AFM ground state for the iron pnictide systems with both correct magnetic moment and band renormalization factor for the same parameters. Nevertheless it is a comparatively easy to implement and powerful tool that allows for a first analysis of the role of magnetic correlations, the nature of magnetically ordered states in strongly correlated multi-orbital materials.

###### Acknowledgements.

This work was supported by the U.S. Department of Energy, Office of Basic Energy Science, Division of Materials Science and Engineering including a grant of computer time at the National Energy Research Supercomputing Center (NERSC) at the Lawrence Berkeley National Laboratory under Contract No. DE-AC02-07CH11358.### References

- Y. Kamihara, T. Watanabe, M. Hirano, and H. Hosono, Journal of the American Chemical Society 130, 3296-3297 (2008).
- M. Rotter, M. Tegel, and D. Johrendt, Phys. Rev. Lett. 101, 107006 (2008).
- F.-C. Hsu, J.-Y. Luo, K.-W. Yeh, T.-K. Chen, T.-W. Huang, P. M. Wu, Y.-C. Lee, Y.-L. Huang, Y.-Y. Chu, D.-C. Yan, and M.-K. Wu, Proceedings of the National Academy of Sciences 105, 14262-14264 (2008).
- J. H. Tapp, Z. Tang, B. Lv, K. Sasmal, B. Lorenz, P. C. W. Chu, and A. M. Guloy, Phys. Rev. B 78, 060505 (2008).
- M. S. Torikachvili, S. L. Bud’ko, N. Ni, and P. C. Canfield, Phys. Rev. Lett. 101, 057006 (2008).
- X. H. Chen, T. Wu, G. Wu, R. H. Liu, H. Chen, and D. F. Fang, Nature 453, 761-762 (2008).
- Z. Ren, W. Lu, J. Yang, W. Yi, X. Shen, Z. Li, G. Che, X. Dong, L. Sun, F. Zhou, and Z. Zhao, Chinese Physics Letters 25, 2215-2216 (2008).
- Y. Singh, A. Ellern, and D. C. Johnston, Phys. Rev. B 79, 094519 (2009).
- Y. Singh, M. A. Green, Q. Huang, A. Kreyssig, R. J. McQueeney, D. C. Johnston, and A. I. Goldman, Phys. Rev. B 80, 100403 (2009).
- J. An, A. S. Sefat, D. J. Singh, and M.-H. Du, Phys. Rev. B 79, 075120 (2009).
- D. Johnston, Adv. in Phys. 59, 803-1061 (2010).
- I. Mazin, M. D. Johannes, L. Boeri, K. Koepernik, and D. J. Singh, Phys. Rev. B 78, 085104 (2008).
- K. Haule and G. Kotliar, New Journal of Physics 11, 025021 (2009).
- K. Kuroki, S. Onari, R. Arita, H. Usui, Y. Tanaka, H. Kontani, and H. Aoki, Phys. Rev. Lett. 101, 087004 (2008).
- S. Raghu, X.-L. Qi, C.-X. Liu, D. J. Scalapino, and S.-C. Zhang, Phys. Rev. B 77, 220503(R) (2008).
- A. V. Chubukov, D. V. Efremov, and I. Eremin, Phys. Rev. B 78, 134512 (2008).
- V. Cvetkovic and Z. Tesanovic, Europhys. Lett. 85, 37002 (2009).
- H. Zhai, F. Wang, and D.-H. Lee, Phys. Rev. B 80, 064517 (2009).
- R. Sknepnek, G. Samolyuk, Y.-b. Lee, and J. Schmalian, Phys. Rev. B 79, 054511 (2009).
- Z. P. Yin, K. Haule, and G. Kotliar, Nat Phys 7, 294-297 (2011).
- Z. P. Yin, K. Haule, and G. Kotliar, to appear in Nature Materials (2011).
- G. Wang, Y. Qian, G. Xu, X. Dai, and Z. Fang, Phys. Rev. Lett. 104, 047002 (2010).
- S. Zhou and Z. Wang, Phys. Rev. Lett. 105, 096401 (2010).
- T. Schickling, F. Gebhard, and J. Bünemann, Phys. Rev. Lett. 106, 146402 (2011).
- T. Schickling, F. Gebhard, J. Bünemann, L. Boeri, O. K. Andersen, W. Weber, arXiv:1109.0929
- M. C. Gutzwiller, Phys. Rev. Lett. 10, 159 (1963).
- M. C. Gutzwiller, Phys. Rev. 137, A1726 (1965).
- J. Bünemann and F. Gebhard, Phys. Rev. B 76, 193104-4 (2007).
- G. Kotliar and A. E. Ruckenstein, Phys. Rev. Lett. 57, 1362 (1986).
- X. Y. Deng, X. Dai, and Z. Fang, EPL (Europhysics Letters) 83, 37008 (2008).
- X. Y. Deng, L. Wang, X. Dai, and Z. Fang, Phys. Rev. B 79, 075114-20 (2009).
- V. I. Anisimov, I. V. Solovyev, M. A. Korotin, M. T. Czyzdotyk, and G. A. Sawatzky, Phys. Rev. B 48, 16929 (1993).
- M. T. Czyżyk and G. A. Sawatzky, Phys. Rev. B 49, 14211 (1994).
- G. Kotliar, S. Y. Savrasov, K. Haule, V. S. Oudovenko, O. Parcollet, and C. A. Marianetti, Rev. Mod. Phys. 78, 865 (2006).
- Y. X. Yao, C. Z. Wang, and K. M. Ho, Phys. Rev. B 83, 245139 (2011).
- K. M. Ho, J. Schmalian, and C. Z. Wang, Phys. Rev. B 77, 073101 (2008).
- J. Bünemann, F. Gebhard, and R. Thul, Phys. Rev. B 67, 075103 (2003).
- M. Rotter, M. Tegel, D. Johrendt, I. Schellenberg, W. Hermes, and R. Pöttgen, Phys. Rev. B 78, 020503 (2008).
- W. C. Lu, C. Z. Wang, T. L. Chan, K. Ruedenberg, and K. M. Ho, Phys. Rev. B 70, 041101 (2004).
- T. L. Chan, Y. X. Yao, C. Z. Wang, W. C. Lu, J. Li, X. F. Qian, S. Yip, and K. M. Ho, Phys.Rev.B 76, 205119 (2007).
- X. F. Qian, J. Li, L. Qi, C. Z. Wang, T. L. Chan, Y. X. Yao, K. M. Ho, and S. Yip, Phys.Rev.B 78, 245112 (2008).
- Y. X. Yao, C. Z. Wang, G. P. Zhang, M. Ji, and K. M. Ho, Journal of Physics-Condensed Matter 21, 235501 (2009).
- E. Aktürk and S. Ciraci, Phys. Rev. B 79, 184523 (2009).
- N. Marzari, and D. Vanderbilt, Phys.Rev.B 56, 12847 (1997).
- I. Souza, N. Marzari, and D. Vanderbilt, Phys.Rev.B 65, 035109 (2001).
- S. Graser, A. F. Kemper, T. A. Maier, H.-P. Cheng, P. J. Hirschfeld, and D. J. Scalapino, Phys. Rev. B 81, 214503 (2010).
- V. I. Anisimov, I. A. Nekrasov, D. E. Kondakov, T. M. Rice, and M. Sigrist, The European Physical Journal B - Condensed Matter and Complex Systems 25, 191-201 (2002).
- A. Koga, N. Kawakami, T. M. Rice, and M. Sigrist, Phys. Rev. Lett. 92, 216402 (2004).
- V. I. Anisimov, J. Zaanen, and O. K. Andersen, Phys. Rev. B 44, 943 (1991).
- V. I. Anisimov, F. Aryasetiawan, and A. Lichtenstein, Journal of Physics-condensed Matter 9, 767-808 (1997).
- T. Miyake and F. Aryasetiawan, Phys. Rev. B 77, 085122-9 (2008).
- Q. Huang, Y. Qiu, W. Bao, M. A. Green, J. W. Lynn, Y. C. Gasparovic, T. Wu, G. Wu, and X. H. Chen, Phys. Rev. Lett. 101, 257003 (2008).
- P. Richard, K. Nakayama, T. Sato, M. Neupane, Y.-M. Xu, J. H. Bowen, G. F. Chen, J. L. Luo, N. L. Wang, X. Dai, Z. Fang, H. Ding, and T. Takahashi, Phys. Rev. Lett. 104, 137001 (2010).