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<article article-type="research-article" dtd-version="1.1" specific-use="sps-1.9" 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-id pub-id-type="publisher-id">00004</article-id>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Research Papers</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>Colloidal synthesis of C0A1<sub>2</sub>O<sub>4</sub> nanoparticles using dodecylamine and their structural characterization</article-title>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<name>
						<surname>Blanco</surname>
						<given-names>O.</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
					<xref ref-type="corresp" rid="c1"><sup>*</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Morán-Lázaro</surname>
						<given-names>J.P.</given-names>
					</name>
					<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
					<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Rodríguez-Betancourtt</surname>
						<given-names>V.M.</given-names>
					</name>
					<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Reyes-Gómez</surname>
						<given-names>J.</given-names>
					</name>
					<xref ref-type="aff" rid="aff5"><sup>5</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Barrera</surname>
						<given-names>A.</given-names>
					</name>
					<xref ref-type="aff" rid="aff6"><sup>6</sup></xref>
				</contrib>
			</contrib-group>
			<aff id="aff1">
				<label>1</label>
				<institution content-type="original">Departamento de Física, CUCEI Universidad de Guadalajara Guadalajara, Jal. 44410, México</institution>
				<institution content-type="normalized">Universidad de Guadalajara</institution>
				<institution content-type="orgdiv1">Departamento de Física</institution>
				<institution content-type="orgdiv2">CUCEI</institution>
				<institution content-type="orgname">Universidad de Guadalajara</institution>
				<addr-line>
					<state>Guadalajara</state>
					<city>Jal</city>
					<postal-code>44410</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff2">
				<label>2</label>
				<institution content-type="original">Posgrado en Ciencia de Materiales, CUCEI Universidad de Guadalajara Guadalajara, Jal. 44410, México</institution>
				<institution content-type="normalized">Universidad de Guadalajara</institution>
				<institution content-type="orgdiv1">Posgrado en Ciencia de Materiales</institution>
				<institution content-type="orgdiv2">CUCEI</institution>
				<institution content-type="orgname">Universidad de Guadalajara</institution>
				<addr-line>
					<state>Guadalajara</state>
					<city>Jal</city>
					<postal-code>44410</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff3">
				<label>3</label>
				<institution content-type="original">Departamento de Ciencias Computacionales e Ingeniería, CUVALLES Universidad de Guadalajara Ameca, Jal. 46600, México</institution>
				<institution content-type="normalized">Universidad de Guadalajara</institution>
				<institution content-type="orgdiv1">Departamento de Ciencias Computacionales e Ingeniería</institution>
				<institution content-type="orgdiv2">CUVALLES</institution>
				<institution content-type="orgname">Universidad de Guadalajara</institution>
				<addr-line>
					<city>Ameca</city>
					<state>Jal</state>
					<postal-code>46600</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff4">
				<label>4</label>
				<institution content-type="original">Departamento de Química, CUCEI Universidad de Guadalajara Guadalajara, Jal. 44410, México</institution>
				<institution content-type="normalized">Universidad de Guadalajara</institution>
				<institution content-type="orgdiv1">Departamento de Química</institution>
				<institution content-type="orgdiv2">CUCEI</institution>
				<institution content-type="orgname">Universidad de Guadalajara</institution>
				<addr-line>
					<state>Guadalajara</state>
					<city>Jal</city>
					<postal-code>44410</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff5">
				<label>5</label>
				<institution content-type="original">Facultad de Ciencias, Universidad de of Colima Colima, Col. 28040, México</institution>
				<institution content-type="normalized">Universidad de Colima</institution>
				<institution content-type="orgdiv1">Facultad de Ciencias</institution>
				<institution content-type="orgname">Universidad de of Colima</institution>
				<addr-line>
					<state>Colima</state>
					<postal-code>28040</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<aff id="aff6">
				<label>6</label>
				<institution content-type="original">Laboratorio de Materiales Catalíticos, CUCIENEGA Universidad de Guadalajara Ocotlán, Jal. 47820, México </institution>
				<institution content-type="normalized">Universidad de Guadalajara</institution>
				<institution content-type="orgdiv1">Laboratorio de Materiales Catalíticos</institution>
				<institution content-type="orgdiv2">CUCIENEGA</institution>
				<institution content-type="orgname">Universidad de Guadalajara</institution>
				<addr-line>
					<city>Ocotlán</city>
					<state>Jal</state>
					<postal-code>47820</postal-code>
				</addr-line>
				<country country="MX">Mexico</country>
			</aff>
			<author-notes>
				<corresp id="c1">
					<label><sup>*</sup></label>
					<email>oscar.blanco@cucei.udg.mx</email>
				</corresp>
			</author-notes>
			<pub-date date-type="pub" publication-format="electronic">
				<day>26</day>
				<month>06</month>
				<year>2020</year>
			</pub-date>
			<pub-date date-type="collection" publication-format="electronic">
				<month>09</month>
				<year>2016</year>
			</pub-date>
			<volume>29</volume>
			<issue>03</issue>
			<fpage>78</fpage>
			<lpage>82</lpage>
			<history>
				<date date-type="received">
					<day>02</day>
					<month>05</month>
					<year>2016</year>
				</date>
				<date date-type="accepted">
					<day>08</day>
					<month>07</month>
					<year>2016</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>A mechanism of formation of colloidal particles was proposed by LaMer and Dinegar in order try to explain the variation of the concentration of the reagents with the time in the colloidal solution. According to the LaMer mechanism, if the concentration of the reagents is increased gradually then this could reach the super-saturation limit and consequently, a nucleation and growth process occurs. From this point of view, in this work the formation of CoAl<sub>2</sub>O<sub>4</sub> nanoparticles in the under-supersaturation limit can be partially explained by this mechanism. A non-aqueous colloidal method was formulated using the organic compound dodecylamine as a surfactant agent. By a variation of dodecylamine concentration two distinct morphologies for the CoAl<sub>2</sub>O<sub>4</sub> spinel phase were obtained. The thermal decomposition of the precursor mixture resulted in the formation of the blue CoAl<sub>2</sub>O<sub>4</sub> spinel phase at a temperature of 800 °C.</p>
			</abstract>
			<kwd-group xml:lang="en">
				<title>Keywords:</title>
				<kwd>Dodecylamine</kwd>
				<kwd>colloidal</kwd>
				<kwd>spinel</kwd>
				<kwd>nanoparticles</kwd>
			</kwd-group>
			<funding-group>
				<award-group award-type="contract">
					<funding-source>F-PROMEP</funding-source>
					<funding-source>SEP</funding-source>
					<award-id>-23-005</award-id>
				</award-group>
			</funding-group>
			<counts>
				<fig-count count="6"/>
				<table-count count="0"/>
				<equation-count count="0"/>
				<ref-count count="26"/>
				<page-count count="05"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>Introduction</title>
			<p>Cobalt aluminate (CoAl<sub>2</sub>O<sub>4</sub>), known as Thenard's blue, is a normally spinel-type oxide that has the general formula AB<sub>2</sub>O<sub>4</sub>, where A represents a divalent cation in a tetrahedral site, and B is a trivalent cation located in an octahedral site. This compound has been applied as a catalyst [<xref ref-type="bibr" rid="B1">1</xref>], an electrode in photo-electrochemical cells [<xref ref-type="bibr" rid="B2">2</xref>] and as a ceramic [<xref ref-type="bibr" rid="B3">3</xref>,<xref ref-type="bibr" rid="B4">4</xref>], because of its high thermal stability, high catalytic activity and good electronic and optical properties.</p>
			<p>Several synthesis methods have been used for the preparation of cobalt aluminate, including combustion [<xref ref-type="bibr" rid="B5">5</xref>], the use of thermal complex precursors [<xref ref-type="bibr" rid="B6">6</xref>], sol-gel methods [<xref ref-type="bibr" rid="B7">7</xref>], co-precipitation [<xref ref-type="bibr" rid="B8">8</xref>], sonochemical decomposition [<xref ref-type="bibr" rid="B9">9</xref>], and the use of inverse micro-emulsions [<xref ref-type="bibr" rid="B10">10</xref>]. However, the use of colloidal methods for the preparation of cobalt aluminate has not been reported previously. Colloidal methods involve simple processes, and allow the preparation of a wide variety of inorganic composites such as hydrous sulfides, phosphates, hydroxides, and oxides [<xref ref-type="bibr" rid="B11">11</xref>,<xref ref-type="bibr" rid="B12">12</xref>]. These methods also offer advantages in terms of the higher purity and compositional homogeneity of the final products and they do not require expensive instruments or sophisticated procedures to generate nanostructured materials. Recently, CoSb<sub>2</sub>O<sub>6</sub> and ZnSb<sub>2</sub>O<sub>6</sub> with a trirutile-type structure were synthesized using a colloidal method [<xref ref-type="bibr" rid="B13">13</xref>-<xref ref-type="bibr" rid="B15">15</xref>]. In these studies, the colloidal method allowed unique microstructural morphologies to be obtained: microcolumns and microspheres were obtained for CoSb<sub>2</sub>O<sub>6</sub>, and microtubes and microwires were obtained for ZnSb<sub>2</sub>O<sub>6</sub>. The form of these microstructures depended largely on the type of surfactant used in the synthesis; ethylenediamine and n-dodecylamine were used for CoSb<sub>2</sub>O<sub>6</sub>, while PVP and n-dodecylamine were used in the preparation of ZnSb<sub>2</sub>O<sub>6</sub>. This synthetic method enabled the production of nanoparticles of these compounds; such nanoparticles are suitable for gas sensor applications, because of their large specific surface area. The ability to produce nanosized powders of a material makes it very attractive for various applications; the properties of the material could depend on the particle size.</p>
			<p>The goal of this work was to achieve the synthesis of nanoparticles of CoAl<sub>2</sub>O<sub>4</sub> using a simple colloidal method in a non-aqueous environment, using the organic compound dodecylamine as a surfactant agent. Also, the effect of the dodecylamine concentration on the microstructure of the CoAl<sub>2</sub>O<sub>4</sub> was investigated.</p>
		</sec>
		<sec sec-type="materials|methods">
			<title>Materials and methods</title>
			<sec>
				<title><italic>Synthesis</italic></title>
				<p>Cobalt aluminate with a spinel-type structure was synthesized using a colloidal method, following the method reported by Michel <italic>et al.</italic> [<xref ref-type="bibr" rid="B13">13</xref>]. The synthesis of CoAl<sub>2</sub>O<sub>4</sub> was carried out in two separate processes performed at room temperature. In the first, 1.45 g of cobalt nitrate hexahydrate (Mallinckrodt, USA, 99 %), 3.75 g of aluminum nitrate nonahydrate (Sigma Aldrich, México, 98 %), and 1 g of dodecylamine (Sigma Aldrich, México, 98 %), were separately dissolved in 5 mL of ethyl alcohol (Golden Bell, México, 98 %). Then, the cobalt nitrate solution was added to the dodecylamine solution under vigorous stirring. The aluminum nitrate solution was then added slowly, producing a transparent red colloidal solution with pH = 2. The resulting colloidal solution was subjected to an agitation process for 24 h. Solvent evaporation was then performed using a microwave oven (General Electric JES769WK, 700 W) at low power (140 W), leaving a solid precursor material. The resulting precursor was dried at 200 °C for 8 h using a furnace (Novatech muffle); finally, the powders were calcined at 800 °C for 5 h. In the second synthesis, the same process was followed but instead of 1 g, 2 g of dodecylamine was used. <xref ref-type="fig" rid="f1">Figure 1</xref> shows a flowchart for the synthesis of the CoAl<sub>2</sub>O<sub>4</sub> powders.</p>
				<p>
					<fig id="f1">
						<label>Figure 1</label>
						<caption>
							<title>Flowchart illustrating the process used for the preparation of the CoAl<sub>2</sub>O<sub>4</sub> nanoparticles.</title>
						</caption>
						<graphic xlink:href="1665-3521-sv-29-03-78-gf1.png"/>
					</fig>
				</p>
			</sec>
			<sec>
				<title><italic>Characterization</italic></title>
				<p>X-ray diffraction measurements were performed using a Siemens D500 diffractometer (radiation Cu Ka). The θ/2θ diffraction pattern was recorded from 20 to 70 degrees, in 0.02 ° increments. The microstructure of the powders was observed by SEM, using a JEOL JSM 6390LV microscope. The nanostructure was identified by TEM, using a JEOL JEM 1010 microscope. The UV-vis spectra were recorded using a Perkin-Elmer/Lambda2 spectrometer (λ = 200 to 1000 nm). For this analysis, a small amount of powder was ground in an agate mortar and then suspended in ethyl alcohol. The Raman spectra from 100 to 1000 cm<sup>-1</sup> were measured at room temperature using a Renishaw 1000B Raman spectrometer (laser diode, λ = 830 nm).</p>
			</sec>
		</sec>
		<sec sec-type="results|discussion">
			<title>Results and discussion</title>
			<p>
				<xref ref-type="fig" rid="f2">Figure 2</xref> shows the XRD patterns for the CoAl<sub>2</sub>O<sub>4</sub> powder calcined at 800 °C, for 1 g and 2 g of dodecylamine. In these patterns the main phase was the cubic CoAl<sub>2</sub>O<sub>4</sub> spinel phase, which was identified using the JCPDF #44-0160 file. The spinel phase can be confirmed by the incipient presence of the (331) plane situated at 2θ = 49.2 °, and by the visual observation of its blue color, which is characteristic of cobalt aluminate. The average crystal sizes, which were calculated using Scherrer's formula, using the XRD (311) plane, were ~ 19 and 24 nm for 1 and 2 g of dodecylamine, respectively.</p>
			<p>
				<fig id="f2">
					<label>Figure 2</label>
					<caption>
						<title>XRD patterns for the CoAl<sub>2</sub>O<sub>4</sub> powders obtained using 1 and 2 g of dodecylamine, and subsequent calcination at 800 °C.</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-29-03-78-gf2.png"/>
				</fig>
			</p>
			<p>The surface microstructure of the CoAl<sub>2</sub>O<sub>4</sub> powders calcined at 800 °C was
				observed using SEM. <xref ref-type="fig" rid="f3">Figure 3</xref> shows micrographs
				of the powders prepared using 1 g of dodecylamine; the powders were formed from
				semispherical particles with sizes between 1 and 9 µm, with an average size of 3.7
				µm (<xref ref-type="fig" rid="f3">Figure 3A</xref>). The powders prepared using 2 g
				of dodecylamine were formed from thin laminas with a uniform thickness (<xref
					ref-type="fig" rid="f3">Figure 3B</xref>). The length of the laminas was between
				10 and 60 μm and the width of the laminas was in the range of 5 - 13 µm</p>
			<p>
				<fig id="f3">
					<label>Figure 3</label>
					<caption>
						<title>Surface morphology observed using SEM for the CoAl<sub>2</sub>O<sub>4</sub> powders synthesized using 1 g of dodecylamine (A) and 2 g of dodecylamine (B); the powders were calcined at 800 °C.</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-29-03-78-gf3.png"/>
				</fig>
			</p>
			<p>The mechanism of formation of colloidal particles was studied by LaMer and Dinegar [<xref ref-type="bibr" rid="B16">16</xref>]. This mechanism was established to explain the variation of the concentration of the reagents with the time. According to this mechanism the concentration of the reagents in the colloidal solution increased quickly. Then the concentration of reagents rising about the supersaturation limit for a short period of time and a rapid nucleation process occurs with the formation of large number of crystal nuclei. This leads to a decrease of the concentration. Later, the process of growth of the particles is developed by diffusion. In our case, the final colloidal solution does not present the supersaturation although the nucleation process may occur when the aluminum nitrate solution was added to the cobalt and dodecylamine solution; meanwhile, the process of growth was developed during the stirring of the colloidal solution. The amount of dodecylamine in the colloidal solution could affect the particle growth due to the suturing of nanocrystal surfaces [<xref ref-type="bibr" rid="B17">17</xref>] and hence results in the formation of CoAl<sub>2</sub>O<sub>4</sub> nanoparticles with different sizes and morphologies. In this work, semispherical particles and laminas of CoAl<sub>2</sub>O<sub>4</sub> were obtained when 1 and 2 g of dodecylamine were used, respectively.</p>
			<p>
				<xref ref-type="fig" rid="f4">Figure 4</xref> shows TEM images of the powders
				prepared using 1 and 2 g of dodecylamine calcined at 800 °C. When 1 g of
				dodecylamine was used, the obtained material consisted of agglomerates of
				nanoparticles, as shown in <xref ref-type="fig" rid="f4">Figure 4A</xref>. The
				particle sizes were in the range of 5 - 45 nm, with an average size of 17 nm (<xref
					ref-type="fig" rid="f4">Figure 4B</xref>). When 2 g of dodecylamine was used,
				fine agglomerates of nanoparticles with an average size of 13 nm were observed
					(<xref ref-type="fig" rid="f4">Figure 4C</xref>). The sizes of the
					CoAl<sub>2</sub>O<sub>4</sub> nanoparticles were in the ranged from 6 to 24 nm
					(<xref ref-type="fig" rid="f4">Figure 4D</xref>). However, several particles
				with a size of approximately 50 nm were also observed. The TEM images revealed that
				the microstructures observed in the SEM images were formed from nanosized
				particles.</p>
			<p>
				<fig id="f4">
					<label>Figure 4</label>
					<caption>
						<title>TEM images and particle size distributions of CoAl<sub>2</sub>O<sub>4</sub> prepared using 1 g of dodecylamine (A,B) and 2 g of dodecylamine (C,D).</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-29-03-78-gf4.png"/>
				</fig>
			</p>
			<p>UV-vis spectra from CoAl<sub>2</sub>O<sub>4</sub> powders prepared using 1 and 2 g of
				dodecylamine are show in <xref ref-type="fig" rid="f5">Figure 5</xref>. In the
				samples (both calcined at 800 °C), three absorption bands were observed in the
				visible region, at approximately 548, 591, and 639 nm. These absorption bands are
				characteristic of the CoAl<sub>2</sub>O<sub>4</sub> blue-phase, and had their origin
				in the spin transitions allowed for the Co<sup>2+</sup> tetrahedron (3d<sup>7</sup>
				configuration); these transitions were assigned to <sup>4</sup>A2(F) →
					<sup>4</sup>T<sub>1</sub>(P) [<xref ref-type="bibr" rid="B18">18</xref>].
				Rangappa <italic>et al.</italic> [<xref ref-type="bibr" rid="B19">19</xref>]
				reported a similar spectrum when they prepared nano-CoAl<sub>2</sub>O<sub>4</sub>
				pigment using using a supercritical water method involving organic binding. The same
				behavior was reported by Feldmann [<xref ref-type="bibr" rid="B4">4</xref>].</p>
			<p>
				<fig id="f5">
					<label>Figure 5</label>
					<caption>
						<title>UV-vis absorption spectra for CoAl<sub>2</sub>O<sub>4</sub> synthesized using 1 and 2 g of dodecylamine.</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-29-03-78-gf5.png"/>
				</fig>
			</p>
			<p>According to the group theory for oxides with a spinel structure, five active Raman vibration modes can be expected: A<sub>1g</sub> + E<sub>g</sub> + 3F<sub>g</sub> [<xref ref-type="bibr" rid="B20">20</xref>]. However, previous studies have shown that most of these five vibration modes can arise owing to a reduction in the crystal symmetry of the spinel structure [<xref ref-type="bibr" rid="B21">21</xref>]. <xref ref-type="fig" rid="f6">Figure 6</xref> shows the Raman spectra for the CoAl<sub>2</sub>O<sub>4</sub> spinel (blue powder) synthesized using 1 and 2 g of dodecylamine. For the powders synthesized using 1 g of dodecylamine, seven bands located at 194, 417, 485, 519, 618, 686, and 770 cm<sup>-1</sup> were observed; bands located at 196, 411, 483, 523, 620, 690, and 756 cm<sup>1</sup> were observed for the powders synthesized using 2 g of dodecylamine. The low intensity bands located around 417 and 770 cm<sup>-1</sup>, and 411 and 756 cm<sup>-1</sup>, for the samples prepared using 1 and 2 g of dodecylamine, respectively, are consistent with those reported by Jongsomith [<xref ref-type="bibr" rid="B22">22</xref>] and Kock [<xref ref-type="bibr" rid="B23">23</xref>] for the formation of CoAl<sub>2</sub>O<sub>4</sub>, and with the vibration bands observed for other aluminates such as MgAl<sub>2</sub>O<sub>4</sub> or ZnAl<sub>2</sub>O<sub>4</sub>, which are located near 410 and 755 cm<sup>-1</sup> [<xref ref-type="bibr" rid="B24">24</xref>,<xref ref-type="bibr" rid="B25">25</xref>]. The slight shift observed in the bands was owed to the atomic mass of Co. Based on previous studies made by Stanojevic [<xref ref-type="bibr" rid="B21">21</xref>] and Julien [<xref ref-type="bibr" rid="B26">26</xref>] on ZnCr<sub>2</sub>O<sub>4</sub> and LiMn<sub>2</sub>O<sub>4</sub> spinel oxides, it was possible to assign the active Raman vibration modes for the CoAl<sub>2</sub>O<sub>4</sub> as follows: one of the most intense peaks, located at 196 cm<sup>-1</sup>, is assigned to the Co-O deformation vibration with symmetry F<sub>2g</sub>. Another intense peak observed at 483 cm<sup>-1</sup> is related to the combination of the Al-O and Co-O symmetrical stretching vibrations with symmetry E<sub>g</sub>. Mean intensity peaks located at 523 and 620 cm<sup>-1</sup> are generated by asymmetric and symmetric Al-O stretching vibrations, respectively, which corresponded to an F<sub>2g</sub> symmetry. The highly symmetric A1g vibration, which is related to the contraction of the Al-O linkage, generated a very intense peak at 690 cm<sup>-1</sup>. Therefore, the Raman spectroscopy studies confirmed the formation of the CoAl<sub>2</sub>O<sub>4</sub> spinel phase as a result of the method presented in this work.</p>
			<p>
				<fig id="f6">
					<label>Figure 6</label>
					<caption>
						<title>Raman spectra for CoAl<sub>2</sub>O<sub>4</sub> powders calcined at
							800 °C (1 and 2 g of dodecylamine).</title>
					</caption>
					<graphic xlink:href="1665-3521-sv-29-03-78-gf6.png"/>
				</fig>
			</p>
		</sec>
		<sec sec-type="conclusions">
			<title>Conclusions</title>
			<p>Cobalt aluminate with a spinel type structure was synthesized by a colloidal method, using dodecylamine as a surfactant. Using this method, a pure CoAl<sub>2</sub>O<sub>4</sub> phase was obtained at 800 °C with a cubic spinel phase, as identified by DRX analysis. The spinel phase was confirmed by the presence of the (331) plane at 2θ = 49.2 °. SEM analysis revealed that the size and morphology of the cobalt aluminate particles were strongly influenced by the amount of dodecylamine used in the synthesis. When 1 g of dodecylamine was used, nanostructured semispherical particles (~17 nm) were produced, while nanostructured laminas (~13 nm) were obtained when 2 g of dodecylamine was used. The formation of the cobaltate blue phase was confirmed using UV-Vis and Raman spectroscopy. We expect that the colloidal method presented could be applied for the preparation of other oxides, because this method gives good control over the stoichiometry, provides unique morphological characteristics, and shows good repeatability for the formation of a pure CoAl<sub>2</sub>O<sub>4</sub> phase.</p>
		</sec>
	</body>
	<back>
		<ack>
			<title>Acknowledgments</title>
			<p>The authors are grateful to Dr. Israel Ceja (U. de G.), Dr. Armando Perez (U. de G.), Dr. Claudio Frausto (CIO) and Dario Pozas (U. de C.), by TEM, UV-Vis, Raman and SEM analysis, respectively. J.P. Morán acknowledges financial support from F-PROMEP-39/Rev-04, SEP-23-005.</p>
		</ack>
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