<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0370-3908</journal-id>
<journal-title><![CDATA[Revista de la Academia Colombiana de Ciencias Exactas, Físicas y Naturales]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. acad. colomb. cienc. exact. fis. nat.]]></abbrev-journal-title>
<issn>0370-3908</issn>
<publisher>
<publisher-name><![CDATA[Academia Colombiana de Ciencias Exactas, Físicas y Naturales]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0370-39082022000300617</article-id>
<article-id pub-id-type="doi">10.18257/raccefyn.1643</article-id>
<title-group>
<article-title xml:lang="es"><![CDATA[Efecto Hall cristalino en el antiferromagnético colineal no convencional NiF2]]></article-title>
<article-title xml:lang="en"><![CDATA[Crystal Hall effect in an unconventional collinear antiferromagnet NiF2]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[González-Hernandez]]></surname>
<given-names><![CDATA[Rafael]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[González]]></surname>
<given-names><![CDATA[Roberto]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[Libor]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
</contrib-group>
<aff id="Af1">
<institution><![CDATA[,Universidad del Norte Departamento de Física y Geociencias ]]></institution>
<addr-line><![CDATA[Barranquilla ]]></addr-line>
<country>Colombia</country>
</aff>
<aff id="Af2">
<institution><![CDATA[,Universität Mainz  ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
<country>Germany</country>
</aff>
<aff id="Af2">
<institution><![CDATA[,Czech Academy of Sciences Cukrovarnická  ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
<country>Czech Republic</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>09</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>09</month>
<year>2022</year>
</pub-date>
<volume>46</volume>
<numero>180</numero>
<fpage>617</fpage>
<lpage>627</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S0370-39082022000300617&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S0370-39082022000300617&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S0370-39082022000300617&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[Resumen A lo largo de un siglo, la corriente eléctrica transversal, sin disipación de energía, que genera el efecto Hall continúan desempeñando un papel central en la investigación de materia condensada por su intrigante naturaleza cuántica, relativista y topológica. El efecto Hall anómalo requiere la ruptura espontanea de la simetría de reversión temporal, lo cual es atribuido al ordenamiento magnético de los espines dentro del material cristalino (como es el caso del hierro). Recientemente, se identificó la presencia del efecto Hall anómalo, llamado efecto Hall cristalino, en ciertos materiales antiferromagnéticos no convencionales, donde la ruptura de simetría de inversión temporal es causada por la disposición de los átomos no magnéticos en estructura cristalina antiferromagnética. En el presente trabajo se estudia el efecto Hall cristalino en el fluoruro de níquel (NiF2) por medio de un análisis de simetría y cálculos de primeros principios. Se encuentra que la conductividad Hall anómala para el NiF2 podría alcanzar valores cercanos a 700 S/cm. Esta respuesta Hall se obtiene para el eje fácil de magnetización del material; esto no se presenta en otros cristales tipo rutilo estudiados recientemente donde el vector antiferromagnético tiene que reorientarse aplicando un campo externo. Además, se muestra el origen en el espacio reciproco de la conductividad Hall anómala y la manera en que se puede controlar mediante la rotación del vector de Néel, el cual da cuenta del ordenamiento antiferromagnético del material. Nuestros resultados indican que el NiF2 podría ser un elemento clave en el diseño de futuros dispositivos espintronicos basados en materiales antiferromagnéticos no convencionales.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[Abstract Dissipation less transversal Hall currents are intensively researched for more than one century due to their intriguing quantum, relativistic, and topological origin. The spontaneous Hall effect requires time-reversal symmetry breaking, which is induced by the spin ordering and traditionally was attributed to the magnetization in ferromagnetic materials such as iron. Recently, spontaneous, so-called crystal, Hall effect was identified, which is induced by unconventional magnetism arising from the interplay of collinear antiferromagnetism tron filling, and we predict spontaneous Hall response can be as large as 700 S/cm. In NiF2, the antiferromagnetic vector is oriented along the crystal axis conducive for the Hall response. This property is elusive in other recently studied rutile crystals where the antiferromagnetic vector had to be reoriented by the applied field. Additionally, we analyze the momentum space resolved contribution to the spontaneous Hall conductivity and the Néel vector rotation dependence of the effect. Our calculations show that the NiF2 can be useful element in future spintronics based on unconventional antiferromagnets.]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[nimulaciton de materiales]]></kwd>
<kwd lng="es"><![CDATA[Efecto Hall cristalino]]></kwd>
<kwd lng="es"><![CDATA[Materiales antiferros magneticot]]></kwd>
<kwd lng="es"><![CDATA[NiF2]]></kwd>
<kwd lng="en"><![CDATA[Materials simulation, Crystal Hall effect]]></kwd>
<kwd lng="en"><![CDATA[Antiferromagnetic materials]]></kwd>
<kwd lng="en"><![CDATA[NiF2]]></kwd>
</kwd-group>
</article-meta>
</front><back>
<ref-list>
<ref id="B1">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Baltz]]></surname>
<given-names><![CDATA[V.]]></given-names>
</name>
<name>
<surname><![CDATA[Manchon]]></surname>
<given-names><![CDATA[A.]]></given-names>
</name>
<name>
<surname><![CDATA[Tsoi]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
<name>
<surname><![CDATA[Moriyama]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
<name>
<surname><![CDATA[Ono]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
<name>
<surname><![CDATA[Tserkovnyak]]></surname>
<given-names><![CDATA[Y.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Antiferromagnetic spintronics]]></article-title>
<source><![CDATA[Rev. Mod. Phys]]></source>
<year>2018</year>
<volume>90</volume>
<page-range>015005</page-range></nlm-citation>
</ref>
<ref id="B2">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Blöchl]]></surname>
<given-names><![CDATA[P. E.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Project of augmented-wave method]]></article-title>
<source><![CDATA[Phys. Rev]]></source>
<year>1994</year>
<volume>50</volume>
<page-range>17953</page-range></nlm-citation>
</ref>
<ref id="B3">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Chen]]></surname>
<given-names><![CDATA[H.]]></given-names>
</name>
<name>
<surname><![CDATA[Niu]]></surname>
<given-names><![CDATA[Q.]]></given-names>
</name>
<name>
<surname><![CDATA[MacDonold]]></surname>
<given-names><![CDATA[A H]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Anomalous hall effect arising from noncollinear antiferromagnetism]]></article-title>
<source><![CDATA[Phys. Rev. Lett]]></source>
<year>2014</year>
<volume>112</volume>
<page-range>017205</page-range></nlm-citation>
</ref>
<ref id="B4">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Corrêa]]></surname>
<given-names><![CDATA[C. A.]]></given-names>
</name>
<name>
<surname><![CDATA[Výborný]]></surname>
<given-names><![CDATA[K]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Electoonic estructure and magnetic enisotropies ed antiferromagndfc transition-metal difluorides]]></article-title>
<source><![CDATA[Phys. Rev]]></source>
<year>2018</year>
<volume>7</volume>
<page-range>235111</page-range></nlm-citation>
</ref>
<ref id="B5">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[González-Hernández]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<name>
<surname><![CDATA[&#352;nejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
<name>
<surname><![CDATA[Výborný]]></surname>
<given-names><![CDATA[K]]></given-names>
</name>
<name>
<surname><![CDATA[Yahcgi]]></surname>
<given-names><![CDATA[Y]]></given-names>
</name>
<name>
<surname><![CDATA[Sinova]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Jungwirth]]></surname>
<given-names><![CDATA[T. C V.]]></given-names>
</name>
<name>
<surname><![CDATA[&#381;ezelezný]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Efficient electrical spin spsittef based on non- relativistic collinear antiferromagnetism]]></article-title>
<source><![CDATA[Phys. Rev. Lett]]></source>
<year>2021</year>
<volume>126</volume>
<page-range>127701</page-range></nlm-citation>
</ref>
<ref id="B6">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Halilov]]></surname>
<given-names><![CDATA[S. V.]]></given-names>
</name>
<name>
<surname><![CDATA[Perlov]]></surname>
<given-names><![CDATA[A Y.]]></given-names>
</name>
<name>
<surname><![CDATA[Oppeneer]]></surname>
<given-names><![CDATA[P. M.]]></given-names>
</name>
<name>
<surname><![CDATA[Yaresko]]></surname>
<given-names><![CDATA[A. N.]]></given-names>
</name>
<name>
<surname><![CDATA[Antonov]]></surname>
<given-names><![CDATA[V. N.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Magnetocrystalline anisotropy energy in cubic fe, co, and ni: Applicability of local-spin-density theory reexamined]]></article-title>
<source><![CDATA[Phys. Rev]]></source>
<year>1998</year>
<volume>57</volume>
<page-range>9557-60</page-range></nlm-citation>
</ref>
<ref id="B7">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Hall]]></surname>
<given-names><![CDATA[E. H]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[On a new vction of the magiet on electric cunents]]></article-title>
<source><![CDATA[American Journal of Mathematics]]></source>
<year>1879</year>
<volume>2</volume>
<numero>3</numero>
<issue>3</issue>
<page-range>287-92</page-range></nlm-citation>
</ref>
<ref id="B8">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Herath]]></surname>
<given-names><![CDATA[U.]]></given-names>
</name>
<name>
<surname><![CDATA[Tavadze]]></surname>
<given-names><![CDATA[P.]]></given-names>
</name>
<name>
<surname><![CDATA[He]]></surname>
<given-names><![CDATA[X.]]></given-names>
</name>
<name>
<surname><![CDATA[Bousquet]]></surname>
<given-names><![CDATA[E.]]></given-names>
</name>
<name>
<surname><![CDATA[Singh]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[Munoz]]></surname>
<given-names><![CDATA[F.]]></given-names>
</name>
<name>
<surname><![CDATA[Romero]]></surname>
<given-names><![CDATA[A H.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Pyprocar: A python library for electronic structure pre/post-processing]]></article-title>
<source><![CDATA[Computer Physics Communications]]></source>
<year>2020</year>
<volume>251</volume>
<page-range>107080</page-range></nlm-citation>
</ref>
<ref id="B9">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
<name>
<surname><![CDATA[Hellenes]]></surname>
<given-names><![CDATA[A. B.]]></given-names>
</name>
<name>
<surname><![CDATA[González-Hernández]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<name>
<surname><![CDATA[Sinova]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Jungwirth]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Giant and tunneling magnetoresistance in unconventional collinear antiferromagnets with nonrelativistic spin-momentum coupling]]></article-title>
<source><![CDATA[Phys. Rev. X]]></source>
<year>2022</year>
<volume>12</volume>
<page-range>011028</page-range></nlm-citation>
</ref>
<ref id="B10">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Kohn]]></surname>
<given-names><![CDATA[W.]]></given-names>
</name>
<name>
<surname><![CDATA[Sham]]></surname>
<given-names><![CDATA[L. J.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Self-consistent equations including exchange and correlation effects]]></article-title>
<source><![CDATA[Phys. Rev]]></source>
<year>1965</year>
<volume>140</volume>
<page-range>A1133-8</page-range></nlm-citation>
</ref>
<ref id="B11">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Kresse]]></surname>
<given-names><![CDATA[G.]]></given-names>
</name>
<name>
<surname><![CDATA[Furthmüller]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set]]></article-title>
<source><![CDATA[Phys. Rev. B]]></source>
<year>1996</year>
<volume>54</volume>
<numero>16</numero>
<issue>16</issue>
<page-range>11169-86</page-range></nlm-citation>
</ref>
<ref id="B12">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Kresse]]></surname>
<given-names><![CDATA[G.]]></given-names>
</name>
<name>
<surname><![CDATA[Hafner]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Ab initio molecular dynamics for liquid metals]]></article-title>
<source><![CDATA[Phys. Rev. B]]></source>
<year>1993</year>
<volume>47</volume>
<numero>1</numero>
<issue>1</issue>
<page-range>558-61</page-range></nlm-citation>
</ref>
<ref id="B13">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Li]]></surname>
<given-names><![CDATA[X.]]></given-names>
</name>
<name>
<surname><![CDATA[MacDonald]]></surname>
<given-names><![CDATA[A. H.]]></given-names>
</name>
<name>
<surname><![CDATA[Chen]]></surname>
<given-names><![CDATA[H.]]></given-names>
</name>
</person-group>
<source><![CDATA[Quantum anomalous hall effect through canted antiferromagnetism]]></source>
<year>2019</year>
<publisher-name><![CDATA[arxiv:1902.10650]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B14">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Manchon]]></surname>
<given-names><![CDATA[A.]]></given-names>
</name>
<name>
<surname><![CDATA[Koo]]></surname>
<given-names><![CDATA[H. C.]]></given-names>
</name>
<name>
<surname><![CDATA[Nitta]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Frolov]]></surname>
<given-names><![CDATA[S. M.]]></given-names>
</name>
<name>
<surname><![CDATA[Duine]]></surname>
<given-names><![CDATA[R. A.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[New perspectives for rashba spin-orbit coupling]]></article-title>
<source><![CDATA[Nature Materials]]></source>
<year>2015</year>
<volume>14</volume>
<numero>9</numero>
<issue>9</issue>
<page-range>871-82</page-range></nlm-citation>
</ref>
<ref id="B15">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Marzari]]></surname>
<given-names><![CDATA[N.]]></given-names>
</name>
<name>
<surname><![CDATA[Mostofi]]></surname>
<given-names><![CDATA[A. A.]]></given-names>
</name>
<name>
<surname><![CDATA[Yates]]></surname>
<given-names><![CDATA[J. R.]]></given-names>
</name>
<name>
<surname><![CDATA[Souza]]></surname>
<given-names><![CDATA[I.]]></given-names>
</name>
<name>
<surname><![CDATA[Vanderbilt]]></surname>
<given-names><![CDATA[D.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Maximally localized wannier functions: Theory and applications]]></article-title>
<source><![CDATA[Rev. Mod. Phys]]></source>
<year>2012</year>
<volume>84</volume>
<page-range>1419-75</page-range></nlm-citation>
</ref>
<ref id="B16">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Mazin]]></surname>
<given-names><![CDATA[I. I.]]></given-names>
</name>
<name>
<surname><![CDATA[Koepernik]]></surname>
<given-names><![CDATA[K.]]></given-names>
</name>
<name>
<surname><![CDATA[Johannes]]></surname>
<given-names><![CDATA[M. D.]]></given-names>
</name>
<name>
<surname><![CDATA[González-Hernández]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Prediction of unconventional magnetism in doped FeSb2]]></article-title>
<source><![CDATA[Proceedings of the National Academy of Sciences]]></source>
<year>2021</year>
<volume>118</volume>
<numero>42</numero>
<issue>42</issue>
</nlm-citation>
</ref>
<ref id="B17">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Momma]]></surname>
<given-names><![CDATA[K.]]></given-names>
</name>
<name>
<surname><![CDATA[Izumi]]></surname>
<given-names><![CDATA[F.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Vesta3 for three-dimensional visualization of crystal, volumetric and morphology data]]></article-title>
<source><![CDATA[Journal of Applied Crystallography]]></source>
<year>2011</year>
<volume>44</volume>
<numero>6</numero>
<issue>6</issue>
<page-range>1272-6</page-range></nlm-citation>
</ref>
<ref id="B18">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Mostofi]]></surname>
<given-names><![CDATA[A. A.]]></given-names>
</name>
<name>
<surname><![CDATA[Yates]]></surname>
<given-names><![CDATA[J. R.]]></given-names>
</name>
<name>
<surname><![CDATA[Pizzi]]></surname>
<given-names><![CDATA[G.]]></given-names>
</name>
<name>
<surname><![CDATA[Lee]]></surname>
<given-names><![CDATA[Y.-S.]]></given-names>
</name>
<name>
<surname><![CDATA[Souza]]></surname>
<given-names><![CDATA[I.]]></given-names>
</name>
<name>
<surname><![CDATA[Vanderbilt]]></surname>
<given-names><![CDATA[D.]]></given-names>
</name>
<name>
<surname><![CDATA[Marzari]]></surname>
<given-names><![CDATA[N.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[An updated version of wannier90: A tool for obtaining maximally-localised wannier functions]]></article-title>
<source><![CDATA[Computer Physics Communications]]></source>
<year>2014</year>
<volume>185</volume>
<numero>8</numero>
<issue>8</issue>
<page-range>2309-10</page-range></nlm-citation>
</ref>
<ref id="B19">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Nagaosa]]></surname>
<given-names><![CDATA[N.]]></given-names>
</name>
<name>
<surname><![CDATA[Sinova]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Onoda]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[MacDonald]]></surname>
<given-names><![CDATA[A. H.]]></given-names>
</name>
<name>
<surname><![CDATA[Ong]]></surname>
<given-names><![CDATA[N. P.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Anomalous Hall effect]]></article-title>
<source><![CDATA[Rev. Mod. Phys]]></source>
<year>2010</year>
<volume>82</volume>
<page-range>1539-92</page-range></nlm-citation>
</ref>
<ref id="B20">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Nakatsuji]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[Kiyohara]]></surname>
<given-names><![CDATA[N.]]></given-names>
</name>
<name>
<surname><![CDATA[Higo]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Large anomalous hall effect in a non-collinear antiferromagnet at room temperature]]></article-title>
<source><![CDATA[Nature]]></source>
<year>2015</year>
<volume>527</volume>
<numero>7577</numero>
<issue>7577</issue>
<page-range>212-5</page-range></nlm-citation>
</ref>
<ref id="B21">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Neel]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
</person-group>
<source><![CDATA[Magnetism and the local molecular field]]></source>
<year>1970</year>
<publisher-name><![CDATA[Nobel Foundation]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B22">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Perdew]]></surname>
<given-names><![CDATA[J. P.]]></given-names>
</name>
<name>
<surname><![CDATA[Burke]]></surname>
<given-names><![CDATA[K.]]></given-names>
</name>
<name>
<surname><![CDATA[Ernzerhof]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Generalized gradient approximation made simple]]></article-title>
<source><![CDATA[Phys. Rev. Lett]]></source>
<year>1996</year>
<volume>77</volume>
<page-range>3865-8</page-range></nlm-citation>
</ref>
<ref id="B23">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Samanta]]></surname>
<given-names><![CDATA[K.]]></given-names>
</name>
<name>
<surname><![CDATA[Lezaic]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
<name>
<surname><![CDATA[Merte]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
<name>
<surname><![CDATA[Freimuth]]></surname>
<given-names><![CDATA[F.]]></given-names>
</name>
<name>
<surname><![CDATA[Blügel]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[Mokrousov]]></surname>
<given-names><![CDATA[Y.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Crystal hall and crystal magneto-optical effect in thin films of srruo3]]></article-title>
<source><![CDATA[Journal of Applied Physics]]></source>
<year>2020</year>
<volume>127</volume>
<numero>21</numero>
<issue>21</issue>
<page-range>213904</page-range></nlm-citation>
</ref>
<ref id="B24">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Seemann]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
<name>
<surname><![CDATA[Ködderitzsch]]></surname>
<given-names><![CDATA[D.]]></given-names>
</name>
<name>
<surname><![CDATA[Wimmer]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[Ebert]]></surname>
<given-names><![CDATA[H.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Symmetry-imposed shape of linear response tensors]]></article-title>
<source><![CDATA[Phys. Rev]]></source>
<year>2015</year>
<volume>92</volume>
<page-range>155138</page-range></nlm-citation>
</ref>
<ref id="B25">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
<name>
<surname><![CDATA[Mokrousov]]></surname>
<given-names><![CDATA[Y.]]></given-names>
</name>
<name>
<surname><![CDATA[Yan]]></surname>
<given-names><![CDATA[B.]]></given-names>
</name>
<name>
<surname><![CDATA[MacDonald]]></surname>
<given-names><![CDATA[A. H.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Topological anti-ferromagnetic spintronics]]></article-title>
<source><![CDATA[Nature Physics]]></source>
<year>2018</year>
<volume>14</volume>
<numero>3</numero>
<issue>3</issue>
<page-range>242-51</page-range></nlm-citation>
</ref>
<ref id="B26">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Stout]]></surname>
<given-names><![CDATA[J. W.]]></given-names>
</name>
<name>
<surname><![CDATA[Reed]]></surname>
<given-names><![CDATA[S. A.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[The crystal structure of mnf2, fef2, cof2, nif2 and znf2]]></article-title>
<source><![CDATA[Journal of the American Chemical Society]]></source>
<year>1954</year>
<volume>76</volume>
<numero>21</numero>
<issue>21</issue>
<page-range>5279-81</page-range></nlm-citation>
</ref>
<ref id="B27">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Strempfer]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Rütt]]></surname>
<given-names><![CDATA[U.]]></given-names>
</name>
<name>
<surname><![CDATA[Bayrakci]]></surname>
<given-names><![CDATA[S. P.]]></given-names>
</name>
<name>
<surname><![CDATA[Brückel]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
<name>
<surname><![CDATA[Jauch]]></surname>
<given-names><![CDATA[W.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Magnetic properties of transition metal fluorides mf2 (m = Mn, fe, co, ni) via high-energy photon diffraction]]></article-title>
<source><![CDATA[Phys. Rev. B]]></source>
<year>2004</year>
<volume>69</volume>
<page-range>014417</page-range></nlm-citation>
</ref>
<ref id="B28">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
<name>
<surname><![CDATA[González-Hernández]]></surname>
<given-names><![CDATA[R.]]></given-names>
</name>
<name>
<surname><![CDATA[Jungwirth]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
<name>
<surname><![CDATA[Sinova]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Crystal time-reversal symmetry breaking and spontaneous hall effect in collinear antiferromagnets]]></article-title>
<source><![CDATA[Science Advances]]></source>
<year>2020</year>
<volume>6</volume>
<numero>23</numero>
<issue>23</issue>
</nlm-citation>
</ref>
<ref id="B29">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Wu]]></surname>
<given-names><![CDATA[Q.]]></given-names>
</name>
<name>
<surname><![CDATA[Zhang]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
<name>
<surname><![CDATA[Song]]></surname>
<given-names><![CDATA[H.-F.]]></given-names>
</name>
<name>
<surname><![CDATA[Troyer]]></surname>
<given-names><![CDATA[M.]]></given-names>
</name>
<name>
<surname><![CDATA[Soluyanov]]></surname>
<given-names><![CDATA[A. A.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Wanniertools: An open-source software package for novel topological materials]]></article-title>
<source><![CDATA[Computer Physics Communications]]></source>
<year>2018</year>
<volume>224</volume>
<page-range>405-16</page-range></nlm-citation>
</ref>
<ref id="B30">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Xiao]]></surname>
<given-names><![CDATA[D.]]></given-names>
</name>
<name>
<surname><![CDATA[Chang]]></surname>
<given-names><![CDATA[M.-C.]]></given-names>
</name>
<name>
<surname><![CDATA[Niu]]></surname>
<given-names><![CDATA[Q.]]></given-names>
</name>
</person-group>
<article-title xml:lang=""><![CDATA[Berry phase effects on electronic proper- ties]]></article-title>
<source><![CDATA[Rev. Mod. Phys]]></source>
<year>2010</year>
<volume>82</volume>
<page-range>1959-2007</page-range></nlm-citation>
</ref>
<ref id="B31">
<nlm-citation citation-type="">
<person-group person-group-type="author">
<name>
<surname><![CDATA[&#352;mejkal]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
<name>
<surname><![CDATA[Sinova]]></surname>
<given-names><![CDATA[J.]]></given-names>
</name>
<name>
<surname><![CDATA[Jungwirth]]></surname>
<given-names><![CDATA[T.]]></given-names>
</name>
</person-group>
<source><![CDATA[Altermagnetism: spin-momentum locked phase protected by non-relativistic symmetries]]></source>
<year>2021</year>
<page-range>arxiv:2105.05820</page-range></nlm-citation>
</ref>
</ref-list>
</back>
</article>
