<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">WJCMP</journal-id><journal-title-group><journal-title>World Journal of Condensed Matter Physics</journal-title></journal-title-group><issn pub-type="epub">2160-6919</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/wjcmp.2023.133007</article-id><article-id pub-id-type="publisher-id">WJCMP-127311</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  M&amp;#246;ssbauer Spectroscopic Characterization of Fe Occupation of Columns in the Nb&lt;sub&gt;28&lt;/sub&gt;O&lt;sub&gt;70&lt;/sub&gt; Structure
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Osvaldo</surname><given-names>F. Schilling</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Departamento de Fisica, UFSC, Florianópolis, Brazil</addr-line></aff><pub-date pub-type="epub"><day>05</day><month>07</month><year>2023</year></pub-date><volume>13</volume><issue>03</issue><fpage>105</fpage><lpage>110</lpage><history><date date-type="received"><day>7,</day>	<month>June</month>	<year>2023</year></date><date date-type="rev-recd"><day>22,</day>	<month>August</month>	<year>2023</year>	</date><date date-type="accepted"><day>25,</day>	<month>August</month>	<year>2023</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In search of an experimental route to produce linear arrays of spins without 
  the use of nanotechnological tools, we have doped Nb<sub>28</sub>O<sub>70</sub> with small amounts of transition metal oxides
   
  (TM; in this case Fe<sub>2</sub>O<sub>3</sub>) or rare-earth oxides<sub>3</sub>, and investigated the location of the alien metal (Fe in this case) in the structure. Previous AC magnetic susceptibility measurements at low temperatures have been consistent with the formation of arrays of TM magnetic moments along the widely spaced columns parallel to the crystallographic b-axis in the Nb<sub>28</sub>O<sub>70</sub> structure. To obtain further details about the TM distribution, the previous investigation has been extended now to include a room-temperature M&amp;#246;ssbauer spectroscopic analysis of the Fe-doped material. The data are consistent with the presence of low-spin Fe<sup>3+</sup> ions in both octahedral and tetrahedral coordinations of oxygens, and confirm
   
  (as suggested in the previous work) that Fe also interchanges positions with Nb ions located at tetrahedrally coordinated sites in the columns of the structure.
 
</p></abstract><kwd-group><kwd>M&amp;#246;ssbauer Spectroscopy</kwd><kwd> Niobium Oxides</kwd><kwd> Spin Arrays</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Two-dimensional magnetic structures are well known for their influence on several technologically important effects, like giant magnetoresistance [<xref ref-type="bibr" rid="scirp.127311-ref1">1</xref>] , high-tem- perature superconductivity in the cuprates [<xref ref-type="bibr" rid="scirp.127311-ref2">2</xref>] , and magnetocaloric effects [<xref ref-type="bibr" rid="scirp.127311-ref3">3</xref>] , just to mention the most widely investigated.</p><p>Investigations on one-dimensional spin arrays have also recently been published [<xref ref-type="bibr" rid="scirp.127311-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref5">5</xref>] . This subject has been of our interest for some time. In previous work we undertook an investigation on how to build one-dimensional magnetic “lines”, by exploiting a suitable crystal structure that might serve as a framework for lines of spins added by alien ions [<xref ref-type="bibr" rid="scirp.127311-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref7">7</xref>] . Materials like those employed as solid electrolytes contain wide channels along one of the crystallographic directions (Vanadium bronzes, for instance [<xref ref-type="bibr" rid="scirp.127311-ref8">8</xref>] ) and the objective in that case is achieving large directional conductivity.</p><p>In our case we look for channels in which alien ions support localized magnetic moments. The compound Nb<sub>28</sub>O<sub>70</sub> (also called H-Nb<sub>2</sub>O<sub>5</sub>, or simply the “niobate”, for short) indeed displays a suitable structure, since the unit cells are stacked along the b-axis in such way that columns with octahedrally coordinated vacant sites become available for alien magnetic ions and their spins. In our previous publications on this material we focussed on the low-temperature magnetic characterization of doped niobate, containing additions of either Fe or other TM and rare earth ions. AC magnetic susceptibity measurements under superimposed static fields up to 9T are fully consistent with magnetically-induced flipping of correlated spins aligned in one dimension (see <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>, from our previous work [<xref ref-type="bibr" rid="scirp.127311-ref7">7</xref>] ). However, such technique is not sufficiently sensitive to disclose the details of the environment around the alien ions.</p><p>The present work has been devised to fill this gap. Mossbauer spectroscopy of <sup>57</sup>Fe is an adequate tool to answer the main questions left from the previous investigation, as discussed below.</p></sec><sec id="s2"><title>2. Sample Details and Experimental Procedure</title><p>The left side of  <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref> shows the ac-plane view [<xref ref-type="bibr" rid="scirp.127311-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref8">8</xref>] of the structure of Nb<sub>28</sub>O<sub>70</sub>, displaying unit cells containing stacks of 4 &#215; 3 and 5 &#215; 3 NbO<sub>6 </sub>octahedra (hatched and dotted squares, respectively). The right side of the <xref ref-type="fig" rid="fig">Figure </xref>shows the view parallel to the crystallographic b-axis, normal to the ac-plane.</p><p>Each unit cell ideally contains a separate Nb atom in a NbO<sub>4</sub> tetrahedral environment, situated along a column with additional empty octahedral sites available around. Alien metals added to the structure might occupy such empty octahedral sites forming columns of localized spins (Structure A). The right side of <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref> shows also the case in which the alien atom exchanges position with a Nb atom in a tetrahedral site (Structure B), a move that depends on the radii difference between Nb and Fe. Therefore, (at least) two different environments (A and B) for alien atoms are expected. The susceptibility measurements in our previous work were not sensitive to such changes of environment though, so that a different technique would be required. Such technique is Mossbauer spectroscopy, which is sensitive to the anions arrangement (and d-orbital electrons occupation) around Fe, added as alien atoms in the sample.</p><p>The sample preparation was as follows. Fe<sub>2</sub>O<sub>3</sub> and Nb<sub>28</sub>O<sub>70</sub> powders were mixed in a proportion nominally sufficient to introduce one atom of iron per unit cell of the niobate matrix. The mixture was treated at 1000˚C for 24 hours in a box furnace. After the heat treatment a light-greenish powder was obtained. Since the originally white niobate powder is an insulator with a 3 eV gap, and the d-levels of Fe should fit just above the bottom of the gap, by absorption of violet and blue (of about 2.8 eV photons energy) from the incident visible light the reflected light would leave the powder with the observed greenish color.</p><p>X-ray diffraction of the powder using Cu-Kα radiation displayed the spectrum of the niobate only, without any evidence of phases associated with Fe.</p></sec><sec id="s3"><title>3. Experimental Results and Analysis</title><p>The Mossbauer spectra were collected at “room temperature” of about 298 K in the transmission geometry with a 50 mCi <sup>57</sup>Co source. The spectrometer was operated with a triangular velocity waveform in a constant accelerarion mode. Isomer shifts (δ) are referred to natural alpha iron at ambient temperature.</p><p>The spectroscopic data for this sample are similar to the ones obtained by Paduani et al. [<xref ref-type="bibr" rid="scirp.127311-ref9">9</xref>] for Fe in soil samples containing the minerals kaolinite, montmorillonite, goethite, and hematite, and we follow their analysis and references. The minerals structures contain tetrahedrally and octahedrally coordinated sites similar to what is found in the niobate. <xref ref-type="fig" rid="fig">Figure </xref>3 shows the Mossbauer spectrum of the sample at room temperature. The main features are a large doublet, and a weak superimposed sextet. The analysis was carried out with the MossWinn 4.0 software, which fits theoretical lorentzian curves to obtain the relevant parameters. The doublet can be fitted by two doublets attributable to Fe<sup>+3</sup>. With reference to the curves in <xref ref-type="fig" rid="fig">Figure </xref>3, one gets the following parameters from the fits: First doublet from top (in green): Isomer Shift (δ) = 0.338 mm/s; Electric Quadrupolar Splitting (QS) = 0.645 mm/s, and Subspectral Area Fraction (A) = 26%. Second doublet (in light blue): δ = 0.328, QS = 1.056, and A = 58%. For the Sextet: δ = 0.364, QS = −0.179, A = 16%, and Hyperfine Magnetic Field B = 51.5 T, which are close to the parameters for Fe<sub>2</sub>O<sub>3</sub>. This latter feature characterizes the presence of hyperfine magnetic interactions between Fe atoms.</p><p>The isomer shifts for the doublets are consistent with either Fe<sup>+2</sup> or Fe<sup>+3</sup> states; however, the values of QS are indeed characteristic of Fe<sup>+3</sup> rather than Fe<sup>+2</sup> [<xref ref-type="bibr" rid="scirp.127311-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref11">11</xref>] . The first doublet parameters correspond to Fe in octahedral sites (Structure A), and the Second doublet to Fe in tetrahedral stes (Structure B) [<xref ref-type="bibr" rid="scirp.127311-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.127311-ref11">11</xref>] , which gives support to the configurations proposed in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref> of this paper. There is a larger proportion of Fe in tetrahedral columnar sites.</p><p>Hyperfine magnetic interactions (revealed by the presence of the weak sextet) indicate the formation of clusters of Fe ions, probably close to one nanometer size. This might indicate localized inhomogeneities in Fe distribution during sample preparation and the minor presence of unreacted Fe<sub>2</sub>O<sub>3</sub>.</p></sec><sec id="s4"><title>4. Conclusion</title><p>This paper has presented a Mossbauer spectroscopic study of Fe-doped Nb<sub>28</sub>O<sub>70</sub>. This material was devised to provide an experimental “platform” for the magnetic investigation of linear (or columnar) arrays of spins. Previous measurements of magnetic AC susceptibility under static magnetic fields down to low temperatures gave results consistent with the formation of linear arrays of spins, but other details are not revealed by that technique. Mossbauer spectroscopy, however, is a sensitive tool to probe the actual coordination around the alien atoms. The Fe ions were identified as trivalent, and the study was capable of identifying two kinds of environment around Fe, namely those of octahedral (A) and those of tetrahedral (B) coordination, with a greater proportion of the tetrahedrally-coordinated type.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The Mossbauer spectroscopic measurements were carried out in the Laboratorio de Espectroscopia M&#246;ssbauer, at Universidade de Brasilia, by Prof. Aderbal C. de Oliveira.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Schilling, O.F. (2023) M&#246;ssbauer Spectroscopic Characterization of Fe Occupation of Columns in the Nb<sub>28</sub>O<sub>70</sub> Structure. 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