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Breathing distortions in the metallic, antiferromagnetic phase of LaNiO$_3$
by Alaska Subedi
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This Submission thread is now published as SciPost Phys. 5, 020 (2018)
Submission summary
As Contributors:  Alaska Subedi 
Arxiv Link:  http://arxiv.org/abs/1708.08899v1 (pdf) 
Date submitted:  20170830 02:00 
Submitted by:  Subedi, Alaska 
Submitted to:  SciPost Physics 
Academic field:  Physics 
Specialties: 

Approaches:  Theoretical, Computational 
Abstract
I study the structural and magnetic instabilities in LaNiO$_3$ using density functional theory calculations. From the nonspinpolarized structural relaxations, I find that several structures with different Glazer tilts lie close in energy. The $Pnma$ structure is marginally favored compared to the $R\overline{3}c$ structure in my calculations, suggesting the presence of finitetemperature structural fluctuations and a possible proximity to a structural quantum critical point. In the spinpolarized relaxations, both structures exhibit the $\uparrow\!\!0\!\!\downarrow\!\!0$ antiferromagnetic ordering with a rocksalt arrangement of the octahedral breathing distortions. The energy gain due to the breathing distortions is larger than that due to the antiferromagnetic ordering. These phases are semimetallic with small threedimensional Fermi pockets, which is largely consistent with the recent observation of the coexistence of antiferromagnetism and metallicity in LaNiO$_3$ single crystals by Li \textit{et al.} [arXiv:1705.02589].
Ontology / Topics
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Submission & Refereeing History
Published as SciPost Phys. 5, 020 (2018)
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Reports on this Submission
Anonymous Report 2 on 2017121 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1708.08899v1, delivered 20171201, doi: 10.21468/SciPost.Report.287
Strengths
1  very thorough study
2  useful for other researchers as it gives many details
3  deals with Nioxide compounds, which are currently of big interest
Weaknesses
1  the encyclopedic tone makes it a big hard to read
Report
This manuscript focuses mainly on LaNiO3 and YNiO3 which are analyzed within DFT. It studies the magnetic phases, calculates the Fermi surfaces and band structures and makes contact with a number of recent experiments on LaNiO3.
I have read the comments by the other referee and I agree essentially with all of them. I would like to add only the following point:
When discussing DFT+DMFT results, it would be good to mention that they depend crucially on the filling of the e_g manifold. The author cites Park et al. [19] and a study by himself [20]. In another study [PHYSICAL REVIEW B 88, 195116 (2013)] a model calculation showed that the relative energy position of the x2y2 and z2 orbitals strongly depends on whether the lowenergy model is close to quarter or half filling. This can be explained invoking a weaker or stronger effect of the Hund's coupling, respectively. The number of electrons sitting in the e_g manifold depends on how strong the hybridization to the pligand orbitals is. In the absence of pbands (e_g only model) the model is quarterfilled and J_Hund influences the physics very little. This results in a large energy separation between x2y2 and z2. The more electrons are donated to the e_g from the porbitals within a dpmodel, the stronger J_Hund can operate and x2y2 and z2 as a consequence are less separated and both contribute to the Fermi surface.
This aspect should be discussed to some extent, in my opinion.
Requested changes
1  add the comment on the DFT+DMFT calculation
Report 1 by Markus Aichhorn on 20171017 (Invited Report)
 Cite as: Markus Aichhorn, Report on arXiv:1708.08899v1, delivered 20171017, doi: 10.21468/SciPost.Report.262
Strengths
1) This paper is a very thorough study of the structural and magnetic properties of the rareearth nickelate LaNiO3, including a comprehensive comparison to other members of the nickelate family such as YNiO3. Alaska Subedi did take a lot of care in analysing the structural instabilities of the system, and gave an understandable explanation of how LaNiO3 is different to the other compounds.
2) The paper is well placed in the context of other current works, and discusses all relevant developments appropriately.
3) Alaska Subedi also openly discusses the failures of his approach, in the sense that he does not only tell what works. For instance, it is valueable that he mentions also structures that he tries to stabilize and did not succeed to do so.
Weaknesses
1) Given that Alaska Subedi did do many calculations, it is in some parts not so easy to follow the arguments. For example, I had to read page 8, which discusses all the different possible magnetic orderings and corresponding unit cells, several times until I got the point. At the current stage, I would encourage Alaska Subedi to make in this part more clear what he is aiming at, before entering all the details of the results. Reading these paragraphs would be much more easy if one knows what the main message should be.
Report
I think that this is a very timely work that discusses a very interesting compound, based on stateoftheart calculations. It tries to convey a complete picture of how structure and magnetism is intertwined, and how this is reflected in the electronic properties.
I have a concern about the accuracy of the calculations. At several points, Alaska Subedi discusses tiny differences of, e.g., total energies, for instance the 1eV difference of the Pnma and R3c structure of LaNiO3 (Table 1). As a matter of fact, these numbers have no real, or very difficult to estimate, error bars. In principle, they should be converged in several parameters, most importantly the energy cutoff and the kspace integration. I understand that this is complicated, and computational costs are prohibitive. Nevertheless, a discussion of the accuracy of the given numbers is necessary.
When comparing to the experimental works, two things come to my mind: PBE gives the wrong structure as the ground state, and stabilizes a magnetic ordering that is at least strongly debated. The first issue could be related to the above given possible problems with convergence. The second, however, needs a bit more discussion. As far as I understood the argument, the rocksalttype breathing distortions come hand in hand with chargedisproportionation and the up0down0 magnetic ordering. Now the question: Is it possible to stabilize this structure with the distortions also without magnetic ordering? This would strengthen the argument that magnetic ordering is not detrimental for the phase transition, but rather follows the effects in the structure.
Two general remarks on section 3.3: First, matrix elements are neglected in the Lindhard formula. We did some work recently showing that matrix elements can have a significant effect on the relative height of excitations in the Brillouin zone (Heil et al., Phys.Rev.B 90, 115142, 2014). Maybe some comments on this could be added here. Second, magnetic instabilities should follow from the RPAenhanced suszeptibility, and not the bare one. This is also discussed in above paper, where also references to work by the group of Hardy Gross can be found, which studied this problem in the context of ironchalcogenide superconductors.
In general, I am not sure if this section 3.3 is absolutely necessary for the manuscript.
Requested changes
1) Some discussion on the numerical accuracy of the total energies.
2) Some rewriting, in particular in section 3.2, to make the main points clearer.
3) It would be nice if Alaska could clarify if a disproportionated state exists without magnetic ordering.
Alaska Subedi on 20170918 [id 173]
I'd like to correct three small errors that I noticed in the manuscript that might cause confusion:
1) The imaginary frequencies have the imaginary "i" missing in page 6.
2) The a+bc tilt is not stabilized for YNiO3, and the corresponding entry in Table I should be "".
3) In Fig. 7, the "LAFM" and "TAFM" should be "RAFM" and "PAFM", respectively.