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<article article-type="research-article" dtd-version="1.1" specific-use="sps-1.8" xml:lang="en" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
	<front>
		<journal-meta>
			<journal-id journal-id-type="publisher-id">sv</journal-id>
			<journal-title-group>
				<journal-title>Superficies y vacío</journal-title>
				<abbrev-journal-title abbrev-type="publisher">Superf. vacío</abbrev-journal-title>
			</journal-title-group>
			<issn pub-type="ppub">1665-3521</issn>
			<publisher>
				<publisher-name>Sociedad Mexicana de Ciencia y Tecnología de Superficies y Materiales A.C.</publisher-name>
			</publisher>
		</journal-meta>
		<article-meta>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Research Papers</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>Amorphous Zr(OH)<sub>4</sub> to t-ZrO<sub>2</sub> transformed isothermally</article-title>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<name>
						<surname>Meza-Galvez</surname>
						<given-names>J.</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>
 <italic>1</italic>
</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Olea-Mejía</surname>
						<given-names>O.</given-names>
					</name>
					<xref ref-type="aff" rid="aff2"><sup>
 <italic>2</italic>
</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Hernández-López</surname>
						<given-names>S.</given-names>
					</name>
					<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Vigueras-Santiago</surname>
						<given-names>E.</given-names>
					</name>
					<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Camacho-López</surname>
						<given-names>M.</given-names>
					</name>
					<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
					<xref ref-type="corresp" rid="c1"><sup>*</sup></xref>
				</contrib>
			</contrib-group>
			<aff id="aff1">
				<label>1</label>
				<institution content-type="original"> Posgrado en Ciencia de Materiales, Facultad de Química, Universidad Autónoma del Estado de México, Tollocan s/n, esq. Paseo Colón, Toluca, Estado de México, 50110, México.</institution>
				<institution content-type="normalized">Universidad Autónoma del Estado de México</institution>
				<institution content-type="orgname">Universidad Autónoma del Estado de México</institution>
				<addr-line>
					<city>Toluca</city>
					<state>Estado de México</state>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff2">
				<label>2</label>
				<institution content-type="original"> Centro Conjunto de Investigación en Química Sustentable UAEM-UNAM, Universidad Autónoma del Estado de México, km 14.5 Carretera Toluca-Atlacomulco, San Cayetano 50200, México.</institution>
				<institution content-type="normalized">Universidad Autónoma del Estado de México</institution>
				<institution content-type="orgdiv1">Centro Conjunto de Investigación en Química Sustentable UAEM-UNAM</institution>
				<institution content-type="orgname">Universidad Autónoma del Estado de México</institution>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff3">
				<label>3 </label>
				<institution content-type="original">Laboratorio de Investigación y Desarrollo de Materiales Avanzados (LIDMA), Universidad Autónoma del Estado de México, Carretera Toluca-Atlacomulco Km 14.5, Unidad San Cayetano, Toluca, Estado de México 50295, México. </institution>
				<institution content-type="normalized">Universidad Autónoma del Estado de México</institution>
				<institution content-type="orgname">Universidad Autónoma del Estado de México</institution>
				<addr-line>
					<city>Toluca</city>
					<state>Estado de México</state>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<author-notes>
				<corresp id="c1">
					<label><sup>*</sup></label>
					<email>macamacholo@uaemex.mx</email>
				</corresp>
			</author-notes>
			<pub-date pub-type="epub-ppub">
				<season>Jul-Sep</season>
				<year>2018</year>
			</pub-date>
			<volume>31</volume>
			<issue>3</issue>
			<fpage>44</fpage>
			<lpage>47</lpage>
			<history>
				<date date-type="received">
					<day>12</day>
					<month>12</month>
					<year>2017</year>
				</date>
				<date date-type="accepted">
					<day>25</day>
					<month>06</month>
					<year>2018</year>
				</date>
			</history>
			<permissions>
				<license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by-nc/4.0/" xml:lang="en">
					<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution License</license-p>
				</license>
			</permissions>
			<abstract>
				<title>Abstract:</title>
				<p>With the aim to study the transformation from the commercially amorphous Zr(OH)<sub>4</sub> to the t-ZrO<sub>2</sub>, phase, the starting material was isothermally treated in a calorimeter at 350, 365, 370, 375 and 380 <sup>o</sup> C. The TGA coupled to the DSC technique was used to determine with high precision both the temperature and time necessary to achieve the amorphous Zr(OH)<sub>4</sub> to t-ZrO<sub>2</sub> transformation. The mass loss and heat flow, as a function of time, were monitored to study the dehydroxylation of Zr(OH)<sub>4</sub> and the crystallization processes, respectively. Raman spectroscopy was used to obtain evidence of the t-ZrO<sub>2</sub> formation. The DSC results show an exothermic peak (typical of amorphous-crystalline transitions) related to the formation of t-ZrO<sub>2</sub>. Our results indicate that the time necessary to obtain the t-ZrO<sub>2</sub> phase shortens when temperature increases.</p>
			</abstract>
			<kwd-group xml:lang="en">
				<title>Keywords:</title>
				<kwd>Zirconium hydroxide</kwd>
				<kwd>Tetragonal Zirconia</kwd>
				<kwd>Isothermal treatment</kwd>
				<kwd>Raman spectroscopy</kwd>
			</kwd-group>
			<counts>
				<fig-count count="5"/>
				<table-count count="0"/>
				<equation-count count="0"/>
				<ref-count count="20"/>
				<page-count count="4"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>Introduction</title>
			<p>Zirconia (t-ZrO<sub>2</sub>, m-ZrO<sub>2</sub> and c-ZrO<sub>2</sub>) is a very important material due to its wide range of applications, which include catalysis, gas sensors, solid-oxide fuel cells, biomaterials, among others [<xref ref-type="bibr" rid="B1">1</xref>-<xref ref-type="bibr" rid="B4">4</xref>]. For a long time ZrO<sub>2</sub> has been used as dental implants and recently Gutierrez <italic>et al.</italic>, have reported on the potential application of YSZ (yttria-stabilized zirconia) as cranial implants [<xref ref-type="bibr" rid="B5">5</xref>-<xref ref-type="bibr" rid="B6">6</xref>].</p>
			<p>It is well known that amorphous zirconium hydroxide can be transformed into t-ZrO<sub>2</sub> and subsequently this polymorph can be transformed into m-ZrO<sub>2</sub> [<xref ref-type="bibr" rid="B7">7</xref>-<xref ref-type="bibr" rid="B11">11</xref>]. Li <italic>et al.</italic> have determined that the complete transformation of Zr(OH)<sub>4</sub> follow the steps: Zr(OH)<sub>4</sub> to t-ZrO<sub>2</sub> to t-ZrO<sub>2</sub>+m-ZrO<sub>2</sub> and finally to m-ZrO<sub>2</sub> [<xref ref-type="bibr" rid="B7">7</xref>]. Sato has described the transformation as follows: Zr(OH)<sub>4</sub> to amorphous ZrO<sub>2</sub> to t-ZrO<sub>2</sub> to t-ZrO<sub>2</sub>+m-ZrO<sub>2</sub>.Various research groups have extensively studied the t-ZrO<sub>2</sub> to m-ZrO<sub>2</sub> transformation [<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B10">10</xref>,<xref ref-type="bibr" rid="B12">12</xref>]. While obtaining t-ZrO<sub>2</sub> from zirconium hydroxide, these studies do not include the determination of both the time and temperature required to achieve the transformation. Livage <italic>et al</italic>. have reported that amorphous zirconia initiates its crystallization at 290 <sup>°</sup>C, reaching no more than 25 % of crystallinity for 7 days of treatment. Applying a thermal treatment at 300 and 315 <sup>°</sup>C for several days still produces an incomplete crystallization. On the other hand, 100 % crystallization is completed under a thermal treatment at 348 <sup>°</sup>C during 8 hours, with 90 % achieved during the first 4 hours. [<xref ref-type="bibr" rid="B13">13</xref>]. Glushkova <italic>et al</italic>. have reported the crystallization process as a function of time at 200, 250, 275 and 300 <sup>°</sup>C, and they compare their results with those reported by Livage <italic>et al</italic>. [<xref ref-type="bibr" rid="B14">14</xref>].</p>
			<p>Roberts <italic>et al</italic>. have analyzed the influence of the thermal ageing on the tetragonal to monoclinic phase transformation in the near-surface regions of ZrO<sub>2</sub> [<xref ref-type="bibr" rid="B15">15</xref>]. Denkewicz <italic>et al</italic>. have investigated the isothermal transformation of t-ZrO<sub>2</sub> and m-ZrO<sub>2</sub> prepared by the hydrothermal method [<xref ref-type="bibr" rid="B16">16</xref>]. Nishizawa <italic>et al.</italic> have obtained hydrothermally the cubic phase of zirconia (c-ZrO<sub>2</sub>) and studied its transformation to m-ZrO<sub>2</sub>[<xref ref-type="bibr" rid="B17">17</xref>]. To study the crystallization process for Ni<sub>78</sub>Si<sub>8</sub>B<sub>14</sub> alloys, Baró <italic>et al</italic>. have used the DSC technique, by applying isothermal treatments [<xref ref-type="bibr" rid="B18">18</xref>]. They showed that the crystallization process can be studied if monitoring the heat flow as a function of time. The presence of an exothermic peak indicates the glass to crystal transition. To the best of our knowledge the DSC technique, as a function of time, has not yet been used to study the amorphous Zr(OH)<sub>4</sub> to t-ZrO<sub>2</sub> transformation.</p>
			<p>In this work, we determined both the time and temperature necessary to transform commercially available zirconium hydroxide into tetragonal zirconia. Isothermal treatments were applied to the starting material using a calorimeter. The heat flow was monitored as a function of time by DSC. Finally, Raman spectroscopy helped following the formation of t-ZrO<sub>2</sub>. Our results show that the starting material transforms as follow: amorphous Zr(OH)<sub>4</sub> to amorphous ZrO<sub>2</sub> (a-ZrO<sub>2</sub>) to t-ZrO<sub>2</sub>, this is in well agreement with previously published results by several research groups.</p>
		</sec>
		<sec>
			<title>Experimental details</title>
			<sec>
				<title><italic>Sample preparation</italic></title>
				<p>Commercially available Zr(OH)<sub>4</sub> (Sigma-Aldrich, 97 % purity) without further treatment was used as the starting material. Isothermal treatments at 350, 365, 370, 375 and 380 <sup>°</sup>C were done utilizing a calorimeter (TA instruments, SDT Q600). A heating rate of 20 <sup>°</sup>C/min was applied to reach the temperature of the isothermal treatment. The thermal treatment time was variable depending on the temperature. Finally, the sample was slowly cooled down to room temperature. All experiments were carried out in an O<sub>2</sub> flow (100 ml/min).</p>
			</sec>
			<sec>
				<title><italic>Sample characterization</italic></title>
				<p>Zr(OH)<sub>4</sub> was studied by calorimetry with the equipment described earlier. Simultaneous TG and DSC measurements were done as a function of time. The time in each measurement varied depending on temperature. Raman spectra were acquired with a spectrometer Labram HR800 of Jobin-Yvon-Horiba. A He-Ne laser (wavelength: 632.8 nm and laser power: 25 μW) was focused on the sample with the objective lens of an Olympus BX-41 microscope. Finally, IR spectra were measured by using a FT-IR Spectrometer (IR Prestige 21, Shimadzu).</p>
			</sec>
		</sec>
		<sec sec-type="results|discussion">
			<title>Results and Discussion</title>
			<p>
				<xref ref-type="fig" rid="f1">Figure 1</xref> shows (a) Raman and (b) IR spectra corresponding to the commercial zirconium hydroxide. The Raman band at 560 cm<sup>-1</sup> indicates that Zr(OH)<sub>4</sub> is amorphous and it is in good agreement with the results reported by Picquart <italic>et al</italic>. [<xref ref-type="bibr" rid="B9">9</xref>]. Bands corresponding to OH vibrations (3315 and 1629 cm<sup>-1</sup>) are present in the IR spectrum 1(b), these bands are typical for zirconium hydroxide [<xref ref-type="bibr" rid="B10">10</xref>]. The total mass loss of the commercial Zr(OH)<sub>4</sub> was 26 % when heated up to 1200 <sup>°</sup>C, obtaining the monoclinic phase (results not showed here). However, the tetragonal intermediate phase appears and disappears in the 300-400 °C range. Therefore, the aim of this work was to study the Zr(OH)<sub>4</sub> to a-ZrO<sub>2</sub> to t-ZrO<sub>2</sub> transformation. Commercial zirconium hydroxide was isothermally treated at 350, 365, 370, 375 and 380 <sup>°</sup>C. These temperatures were chosen according to the work of Livage <italic>et al</italic>. [<xref ref-type="bibr" rid="B13">13</xref>].</p>
			<p>
				<fig id="f1">
					<label>Figure 1</label>
					<caption>
						<title>(a) Raman and (b) IR spectra of commercial Zr(OH)<sub>4</sub></title>
					</caption>
					<graphic xlink:href="1665-3521-sv-31-03-44-gf1.jpg"/>
				</fig>
			</p>
			<p>
				<xref ref-type="fig" rid="f2">Figure 2</xref> shows three graphs as a function of time: the temperature ramp 1 applied in the thermal treatment (black lines), the thermogravimetric curve (blue line) and the DSC profile (red line). This is an example of the thermal treatment as a function of time applied to the commercial zirconium hydroxide. As one can see the temperature ramp consist of three steps. First, an increment on the temperature under a heating rate of 20 <sup>°</sup>C/min, after that, an isothermal treatment for a fixed time is applied, and finally the cooling stage of the sample. The isothermal treatment time is established by the up rise of the exothermic peak as it can be observed in the DSC profile. In the first 18 minutes, during the heating, one can notice that the starting material losses 24 % of its mass (see blue line). In the same period of time, an endothermic peak appears in the DSC profile due to the heat consumption during the dehydroxylation of the Zr(OH)<sub>4</sub>. After that, the mass stays constant during the isothermal treatment and an exothermic peak appears. This peak indicates that an amorphous material to crystalline t-ZrO<sub>2</sub> transformation takes place. Also, from this graph we can conclude that the material after the dehydroxylation is amorphous-ZrO<sub>2</sub> (the mass is kept constant). We have corroborated by Raman spectroscopy that the t-ZrO<sub>2</sub> phase is present when the exothermic peak has been formed. The presence and features of the exothermic peak depend on the isothermal treatment temperature. With these experiments one can determine with high precision the temperature and the time necessary for the t-ZrO<sub>2</sub> formation.</p>
			<p>
				<fig id="f2">
					<label>Figure 2</label>
					<caption>
						<title>Temperature ramp (black lines), thermogravimetric curve (blue line) and the DSC profile (red line) during the thermal treatment of commercial Zr(OH).</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-31-03-44-gf2.jpg"/>
				</fig>
			</p>
			<p>
				<xref ref-type="fig" rid="f3">Figure 3</xref> shows a set of graphs of heat flow as a function of time, only for the isothermal interval (see <xref ref-type="fig" rid="f2">Figure 2</xref>). Various experiments were carried out in a similar way to that described in the former paragraph. In all graphs, an exothermic peak is present, this behaviour is in good agreement with that reported by Baró <italic>et al</italic>. found in the crystallization process for Ni<sub>78</sub>Si<sub>8</sub>B<sub>14</sub> alloys [<xref ref-type="bibr" rid="B18">18</xref>]. Therefore, the presence of the exothermic peak indicates the transition from amorphous-ZrO<sub>2</sub> to t-ZrO<sub>2</sub>. The exothermic peak shifts to shorter times and becomes narrower when temperature Increases, as it can be observed in <xref ref-type="fig" rid="f3">Figures 3(a)-3(e)</xref>. The maxima of the peaks are at: 114.39, 41.26, 26.55, 18.56 and 11.85 min for 350, 365, 370, 375 and 380 <sup>°</sup>C, respectively. The broadening of the exothermic peak is related to the time necessary to complete the crystallization process.</p>
			<p>
				<fig id="f3">
					<label>Figure 3</label>
					<caption>
						<title>Heat flow as a function of time of zirconium hydroxide samples isothermally treated at different temperatures. </title>
					</caption>
					<graphic xlink:href="1665-3521-sv-31-03-44-gf3.jpg"/>
				</fig>
			</p>
			<p>
				<xref ref-type="fig" rid="f4">Figure 4</xref> shows Raman spectra for commercial Zr(OH)<sub>4</sub> and the samples obtained at various isothermal treatments in the calorimeter. When zirconium hydroxide was isothermally treated at 350 <sup>°</sup>C for 240 min, the Raman spectrum 4(a) shows bands corresponding to the t-ZrO<sub>2</sub>. All the Raman bands in the spectrum 4(a) correspond to the t-ZrO<sub>2</sub> crystalline phase [<xref ref-type="bibr" rid="B19">19</xref>,<xref ref-type="bibr" rid="B20">20</xref>]. This Raman spectrum corresponds to the sample after thermal treatment accordingly to the DSC profile (<xref ref-type="fig" rid="f2">Figure 2</xref>(a)). Therefore, this result indicates that the presence of the exothermic peak is directly related to the formation of t-ZrO<sub>2</sub>. At 365 and 370 <sup>°</sup>C treatment temperature for 120 min the Raman spectra 4(b)-4(c) present almost the same bands that the one at 350 <sup>°</sup>C.</p>
			<p>
				<fig id="f4">
					<label>Figure 4</label>
					<caption>
						<title>Raman spectra of zirconium hydroxide samples at different treatment temperatures. </title>
					</caption>
					<graphic xlink:href="1665-3521-sv-31-03-44-gf4.jpg"/>
				</fig>
			</p>
			<p>These Raman spectra indicate that ordering of the atoms to form the crystalline structure can initiate at temperatures as low as 350 <sup>°</sup>C, but the time of thermal treatment has to be longer. For the highest temperatures 375 <sup>°</sup>C and 380 <sup>°</sup>C, the isothermal treatment time necessary to crystallize the a-ZrO<sub>2</sub> becomes shorter. The Raman spectra 4(d)-4(e) show peaks, which correspond to the t-ZrO<sub>2</sub>, indicating that 30 min of treatment are sufficient time to obtain the t-ZrO<sub>2</sub> crystalline phase. We must notice that some of the peaks in the spectra 4(b)-4(e) correspond to the monoclinic phase of ZrO<sub>2</sub> (m-ZrO<sub>2</sub>) [<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B12">12</xref>]. This shows that the thermal stability interval of t-ZrO<sub>2</sub> is very narrow.</p>
			<p>
				<xref ref-type="fig" rid="f5">Figure 5</xref> show Raman spectra corresponding to Zr(OH)<sub>4</sub> isothermally treated at 370 <sup>°</sup>C for different times. For 10 min, spectrum 5(a), the presence of a wide band indicates that the material is amorphous ZrO<sub>2</sub> [<xref ref-type="bibr" rid="B9">9</xref>]. For longer times, the crystallization process is completed, as it is evidenced by the presence of peaks in Raman spectra 5(b)-5(d), corresponding to the t-ZrO<sub>2</sub> phase. For 30 min and 60 min, spectra 5(b) and 5(c), Raman peaks appear which correspond to the ZrO<sub>2</sub> tetragonal phase. For 120 min, spectrum 5(d), the presence of two peaks at 181 and 380 cm<sup>-1</sup> indicates that the monoclinic phase of ZrO<sub>2</sub> can be induced by increasing the isothermal treatment time, producing a mixture of tetragonal and monoclinic phases of ZrO<sub>2</sub> [<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B12">12</xref>].</p>
			<p>
				<fig id="f5">
					<label>Figure 5</label>
					<caption>
						<title>Raman spectra for Zr(OH)<sub>4</sub> thermally treated at 370 °C for different times. (a) 10 min, (b) 30 min, (c) 60 min, (d) 120 min. </title>
					</caption>
					<graphic xlink:href="1665-3521-sv-31-03-44-gf5.jpg"/>
				</fig>
			</p>
		</sec>
		<sec sec-type="conclusions">
			<title>Conclusions</title>
			<p>The potential of the time-resolved DSC to study the dehydroxilation process, and the amorphous-crystalline transitions to obtain metallic oxide crystalline phases, has been presented in this work. The Zr(OH)<sub>4</sub> to a-ZrO<sub>2</sub> to t-ZrO<sub>2</sub> transformation thermally induced was studied in detail for the temperature range 350 to 380 <sup>°</sup>C. A calorimetric method to thermally treat commercial zirconium hydroxide was successfully employed. In this manner, dehydroxylation takes place in the first instance, while in the second step the crystallization of amorphous-ZrO<sub>2</sub> gives rise to the formation of t-ZrO<sub>2</sub>. By means of isothermal treatments, it was possible to determine with high precision both the time and temperature necessaries to obtain the t-ZrO<sub>2</sub> crystalline phase. Our Raman spectroscopy results indicate that it takes longer to form the crystalline structure at 350 <sup>°</sup>C. In contrast, it takes only a few minutes to obtain crystalline t-ZrO<sub>2</sub> at 380 <sup>°</sup>C.</p>
		</sec>
	</body>
	<back>
		<ack>
			<title>Acknowledgments</title>
			<p>J. M-G acknowledge CONACyT-México for the financial support his Master studies.</p>
		</ack>
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