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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mater.</journal-id>
<journal-title>Frontiers in Materials</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mater.</abbrev-journal-title>
<issn pub-type="epub">2296-8016</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">863603</article-id>
<article-id pub-id-type="doi">10.3389/fmats.2022.863603</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Materials</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Prolonged and Enhanced Protection Against Corrosion Over Titanium Oxide-Coated 304L Stainless Steels Having Been Irradiated With Ultraviolet</article-title>
<alt-title alt-title-type="left-running-head">Sathasivam et al.</alt-title>
<alt-title alt-title-type="right-running-head">Prolonged Protection Against 304LSS Corrosion</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Sathasivam</surname>
<given-names>Kamalasekaran</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wang</surname>
<given-names>Mei-Ya</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Anbalagan</surname>
<given-names>Aswin kumar</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1656860/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Lee</surname>
<given-names>Chih-Hao</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/336962/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Yeh</surname>
<given-names>Tsung-Kuang</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/160363/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Nanoscience and Technology Program</institution>, <institution>Taiwan International Graduate Program</institution>, <institution>Academia Sinica</institution>, <addr-line>Taipei</addr-line>, <country>Taiwan</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Department of Engineering and System Science</institution>, <institution>National Tsing Hua University</institution>, <addr-line>Hsinchu</addr-line>, <country>Taiwan</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Nuclear Science and Technology Development Center</institution>, <institution>National Tsing Hua University</institution>, <addr-line>Hsinchu</addr-line>, <country>Taiwan</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Institute of Nuclear Engineering and Science</institution>, <institution>National Tsing Hua University</institution>, <addr-line>Hsinchu</addr-line>, <country>Taiwan</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/620442/overview">Michele Fedel</ext-link>, University of Trento, Italy</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1669367/overview">Ali G&#xfc;nen</ext-link>, Iskenderun Technical University, Turkey</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1676375/overview">Mohammad Jafar Hadianfard</ext-link>, Shiraz University, Iran</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Tsung-Kuang Yeh, <email>tkyeh@mx.nthu.edu.tw</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Environmental Degradation of Materials, a section of the journal Frontiers in Materials</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>07</day>
<month>04</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>9</volume>
<elocation-id>863603</elocation-id>
<history>
<date date-type="received">
<day>29</day>
<month>01</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>14</day>
<month>03</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Sathasivam, Wang, Anbalagan, Lee and Yeh.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Sathasivam, Wang, Anbalagan, Lee and Yeh</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Austenitic stainless steels are commonly used as the base material for dry storage canisters in nuclear power plants because of their excellent corrosion resistance and mechanical properties. Dry storage canisters are often exposed to chloride-containing atmosphere near seashores that could induce localized stress corrosion cracking in these stainless steels near the welded regions. Titanium dioxide (TiO<sub>2</sub>) coatings applied on stainless steel substrates (i.e. Type 304&#xa0;L stainless steels) along with ultraviolet irradiation have been proposed as a mitigation measure against corrosion in canister materials. In this study, TiO<sub>2</sub> coatings were applied on stainless steel samples using a dip-coating method. The coated samples were then thermally treated under different annealing temperatures. Corrosion behavior and photocatalytic responses of the coated samples with and without UV illumination were evaluated by electrochemical polarization analyses and open circuit potential measurements. Surface morphologies of the samples and the crystal structures were studied by scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDX), and X-ray diffraction (XRD). It was found that the TiO<sub>2</sub> coating not only showed markedly enhanced photocathodic protection on Type 304&#xa0;L stainless steels during UV illumination but also maintain more active open circuit potentials for several hours after the cutoff of UV illumination. Results from electrochemical polarization analyses further supported the superior corrosion resistance of the coated samples under UV illumination conditions. In addition, the specifically processed TiO<sub>2</sub> coatings once irradiated with UV could lead to a prolonged corrosion resistance of the samples even hours without UV illumination.</p>
</abstract>
<kwd-group>
<kwd>dry storage canister</kwd>
<kwd>304L austenitic stainless steel</kwd>
<kwd>TiO2 coating</kwd>
<kwd>photocathodic protection</kwd>
<kwd>UV illumination</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Decommissioning of nuclear reactors involves dismantling of the reactor components and the relocation of spent fuel to repository sites for final disposal. In case of the absence of a geological repository site, it is commonly accepted that dry storage inside nuclear power plants or at selected concentrated sites as an interim solution to handling spent fuel has been considered as an appropriate option (<xref ref-type="bibr" rid="B21">Wang et al., 2020</xref>). During the period of dry storage, metal canisters, sometimes with additional concrete or metal shields, are used to accommodate and preserve spent nuclear fuel for up to 40 years, prior to reprocessing or final disposal in a geological repository. Austenitic stainless steels are widely used as the substrate materials for dry storage canisters owing to its excellent corrosion resistance, thermal conductivity, and mechanical properties. The foregoing properties make stainless steels a desirable material for applications in various industrial plants, from food storage to solar power generation (<xref ref-type="bibr" rid="B6">G&#xfc;nen et al., 2014a</xref>). It is important to note that some of the dry storage sites, such as the nuclear power plants, may be located at areas close to seashore and the metallic materials are thus more prone to salt deposition under highly humid environments in these areas. The deposited salt could induce localized stress corrosion cracking (SCC) near the welded regions of the metallic materials and could eventually lead to structural failure of the canisters. Serious failures of the canisters accompanying with through-wall cracks could lead to the release of radionuclides toward the environment. Therefore, adequate corrosion protection measures are required for the canister materials such as stainless steels (<xref ref-type="bibr" rid="B26">Yeom et al., 2020</xref>). Researchers also attempted to enhance the corrosion resistance of stainless steels by surface modification techniques such as boronizing and nitriding (<xref ref-type="bibr" rid="B7">G&#xfc;nen et al., 2014b</xref>; <xref ref-type="bibr" rid="B3">&#xc7;etin et al., 2021</xref>). However, these techniques usually lack flexibility and require abundant efforts that make them almost impossible for large scale application.</p>
<p>During the past decade, cathodic protections for corrosion mitigation in stainless steels by specific metal-oxide coatings such as TiO<sub>2</sub> (<xref ref-type="bibr" rid="B25">Yeh et al., 2013</xref>), ZnO<sub>2</sub> (<xref ref-type="bibr" rid="B20">Techapiesancharoenkij et al., 2017</xref>), or ZrO<sub>2</sub> (<xref ref-type="bibr" rid="B24">Yeh et al., 2008</xref>) irradiated with ultraviolet (UV) have drawn considerable interests. Among them, TiO<sub>2</sub> coatings are more popular due to their inherent advantages such as superior photoelectrical properties and long-term stability in corrosive environments (<xref ref-type="bibr" rid="B2">Bu and Ao, 2017</xref>). Under excitation in the presence of UV illumination, TiO<sub>2</sub> coatings can generate electron and hole pairs in the space charge layer. The generated photoelectrons are then transferred to the stainless steel surface that is exposed to a corrosive environment, making its open circuit potential more active than its original corrosion potential. The holes on the other hand would move toward the electrolyte leading to the oxidation of H<sub>2</sub>O (<xref ref-type="bibr" rid="B29">Yuan et al., 1994</xref>). In principle, the TiO<sub>2</sub> coating actually acts as a non-sacrificial anode for photo-cathodic protection against corrosion in stainless steels. Efforts were devoted to the application of TiO<sub>2</sub> coating over stainless steel substrates for corrosion mitigation, and positive results were reported (<xref ref-type="bibr" rid="B5">Fujisawa and Tsujikawa, 1994</xref>; <xref ref-type="bibr" rid="B10">Imokawa et al., 1994</xref>). However, due to the wide band gap energy of TiO<sub>2</sub> and the recombination of electron and hole pairs in the absence of UV illumination, practical applications of TiO<sub>2</sub> coatings have not been widely accepted (<xref ref-type="bibr" rid="B15">Shen et al., 2005</xref>). Other approaches have been made on metal oxides that also bear semiconductor property and have similar band gap energies compared to TiO<sub>2</sub>. Investigated examples included Fe<sub>2</sub>O<sub>3</sub> (<xref ref-type="bibr" rid="B12">Liu et al., 2014</xref>), SnO<sub>2</sub> (<xref ref-type="bibr" rid="B17">Subasri and Shinohara, 2003</xref>), CeO<sub>2</sub> (<xref ref-type="bibr" rid="B23">Yang and Cheng (2017)</xref>, and WO<sub>3</sub> (<xref ref-type="bibr" rid="B19">Tatsuma et al., 2001</xref>) that all acted as photo-anodes and were separately coupled with stainless steels for corrosion mitigation. This type of photo-cathodic protection would require a relatively complicated system setup and would need to deal with the degradation of organic substances in the photo-anodic half-cell, leading to increasing production costs for large-scale industrial applications. These shortcomings may simply be overcome by the use of TiO<sub>2</sub> coatings directly applied over stainless steels. Several techniques such as sol&#x2013;gel coating, chemical vapor deposition, sputtering, spray pyrolysis, anodization, and plasma spraying for TiO<sub>2</sub> deposition are currently available (<xref ref-type="bibr" rid="B22">Xu et al., 2021</xref>) (<xref ref-type="bibr" rid="B4">Erol et al., 2014</xref>). Among them, the sol&#x2013;gel method offers many advantages in terms of coating homogeneity, well-controlled TiO<sub>2</sub> phase structure, and good adherence over larger area. On the other hand, the factors that influence the functionality of these TiO<sub>2</sub> coatings over stainless steels, especially low carbon Type 304 stainless steel (304LSS), have not yet been investigated in detail. For example, TiO<sub>2</sub> coatings prepared by the sol&#x2013;gel method usually require a thermal treatment at 400&#x2013;500&#xa0;C to achieve a desirable photocatalytic effect under UV illumination. However, such a high-temperature treatment to TiO<sub>2</sub> coatings would also alter the microstructure of 304LSS surfaces, which could eventually lead to a poorer photocatalytic activity of these coatings (<xref ref-type="bibr" rid="B11">Konishi and Tsujikawa, 1997</xref>).</p>
<p>The undesirable outcomes of worsened catalysis in TiO<sub>2</sub> coatings on the 304LSS substrate during high-temperature treatments have to be addressed properly before such coatings being adopted for large-scale applications. In this study, we intend not only to retain the catalytic efficiency of plain TiO<sub>2</sub> coatings but also to prolong the cathodic protection period of the coatings even after the shutoff of UV illumination, by precisely controlling the diffusion of Fe ions from the 304LSS substrate into TiO<sub>2</sub> coatings during annealing treatments. For a precise control over the diffusion of Fe ions, a number of parameters such as annealing temperature, annealing time, and coating thickness were considered and tested. In addition, for comparison purposes, the influences of Fe ions on the photocatalytic activity and the cathodic protection period of Fe-doped plain TiO<sub>2</sub> coatings were investigated on indium-doped tin oxide (ITO) glass substrates. An external dopant such as ferric nitrate nanohydrate was used as a prime source of Fe in these TiO<sub>2</sub> coatings.</p>
<p>Multi-layered TiO<sub>2</sub> coatings were prepared by dipping the 304LSS substrates in TiO<sub>2</sub>-containing sol&#x2013;gel solutions for a number of times, followed by appropriate annealing treatments at various temperatures for different time durations.</p>
<p>Electrochemical polarization analyses were conducted to evaluate the corrosion behavior of the 304LSS substrates exposed to an aqueous alkaline solution without and with the TiO<sub>2</sub> coatings in the absence and presence of UV illumination. Surface morphologies of the substrate samples were studied by scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (EDX). Crystalline characteristics of TiO<sub>2</sub> coatings were evaluated by an X-ray diffraction (XRD) pattern. Depth profile analysis by secondary ion mass spectroscopy (SIMS) was conducted to quantify the amount of Fe ions having diffused into the TiO<sub>2</sub> coatings from the substrate materials.</p>
<p>TiO<sub>2</sub> coatings and coatings doped with Fe ions play important roles on both enhanced photocatalytic activity and prolonged cathodic protection for improving the corrosion resistance of coated 304LSS substrates exposed to corrosive environments. It is anticipated that this particular coating treatment could lead to a more effective reduction in the corrosion rate of the coated substrate in the presence of UV illumination and to a prolonged low corrosion rate even after the UV illumination has been switched off. During the consecutive annealing treatments for the inner anatase-type TiO<sub>2</sub> coating and the outer amorphous TiO<sub>2</sub> coating over the 304LSS substrate, it is expected that a considerable amount of Fe element present in the substrate would diffuse into the inner-coating layer and form Ti&#x2013;O&#x2013;Fe bonds, with the simultaneous formation of &#x3b1;-Fe<sub>2</sub>O<sub>3</sub> and Fe<sub>3</sub>O<sub>4</sub> in the interface between the substrate and the coating layer (<xref ref-type="bibr" rid="B32">Zhu et al., 2001</xref>; <xref ref-type="bibr" rid="B25">Yeh et al., 2013</xref>). In addition to Fe, Cr, and Ni would also diffuse into the TiO<sub>2</sub> coating, but Fe tends to react more readily with TiO<sub>2</sub> owing to its inherent tendency toward oxygen (<xref ref-type="bibr" rid="B13">Maruska and Ghosh, 1979</xref>). Furthermore, the diffusion coefficient of Fe is greater than that of Cr, which makes &#x3b1;-Fe<sub>2</sub>O<sub>3</sub> and Fe<sub>3</sub>O<sub>4</sub> to be predominant in the interfacial oxide layer. Although major ions in the interfacial oxide actually consists of both Fe<sup>2&#x2b;</sup> and Fe<sup>3&#x2b;</sup> ions, most Fe elements are present in the oxidation state of Fe<sup>3&#x2b;</sup> rather than Fe<sup>2&#x2b;</sup> since conversion from Fe<sup>2&#x2b;</sup> to Fe<sup>3&#x2b;</sup> would usually take place during planned calcination treatments (<xref ref-type="bibr" rid="B28">Yu et al., 2006</xref>). It is well known that Fe<sub>2</sub>O<sub>3</sub> and TiO<sub>2</sub> are both n-type semiconductors with two different band gap energies of 2.2 and 3.2 eV, respectively. Moreover the conduction band energy of &#x3b1;-Fe<sub>2</sub>O<sub>3</sub> is lower than that of TiO<sub>2</sub> by outer 0.38&#xa0;eV. Hence, the n&#x2013;n type heterojunction formed during the calcination treatment allows the photo-excited electrons to migrate easily from the outer and inner TiO<sub>2</sub> coatings to the substrate (<xref ref-type="bibr" rid="B9">Huang et al., 1997</xref>).</p>
<p>In this study, the key to achieving a better photocatalytic activity and a prolonged cathodic protection is the preparation of multi-layered TiO<sub>2</sub> coatings <italic>via</italic> the sol&#x2013;gel-based dipping process, followed by calcination treatments at various temperatures. Suggested multi-layered TiO<sub>2</sub> coatings depositing over the 304LSS substrate consist of two outer coatings of amorphous TiO<sub>2</sub> and one inner anatase-type TiO<sub>2</sub> coating underneath the amorphous coatings. It is presumed that this inner anatase-type TiO<sub>2</sub> layer, after accommodating the Fe<sup>2&#x2b;</sup> and Fe<sup>3&#x2b;</sup> ions diffusing from the interfacial oxide during the calcination treatment, would act as a free electron donor under UV illumination. In the meantime, this specifically engineered Fe-doped layer would also become a charge storage container to trap the free electrons produced on the site and from the outer amorphous TiO<sub>2</sub> layers, making the substrate&#x2019;s electrochemical corrosion potential shifted to a more active value. The two outer amorphous TiO<sub>2</sub> layers also serve as a barrier for preventing the stored electrons from escaping from the inner TiO<sub>2</sub> layer once the UV illumination is switched off.</p>
<p>In the simultaneous presence of Fe<sup>3&#x2b;</sup> and Fe<sup>2&#x2b;</sup> ions, the Fe<sup>3&#x2b;</sup> ions would undergo a reduction reaction and become Fe<sup>2&#x2b;</sup> ions <italic>via</italic> the process of intercalated cations capturing some of the photoelectrons generated inside the TiO<sub>2</sub> coatings during UV illumination. The remaining excess electrons would migrate through the interfacial oxide layer to the 304LSS substrate, offering photo-cathodic protection to the alloy (<xref ref-type="bibr" rid="B8">Huang et al., 1998</xref>). On the other hand, when the UV illumination is shutoff, Fe<sup>2&#x2b;</sup> ions tends to re-oxidize into Fe<sup>3&#x2b;</sup> ions by releasing the electrons that have been captured during UV illumination. The released electrons would continue to protect the substrate alloy from corrosion even in the absence of UV illumination. Furthermore, the two outer layers of amorphous TiO<sub>2</sub> coatings would make it difficult for the preserved electrons to escape from coatings and react directly with the oxidizing species in corrosive environments. Eventually, the electrochemical corrosion potential of the substrate, instead of instantly moving back to the original value, would slowly rise up once the UV illumination is shutoff (<xref ref-type="bibr" rid="B8">Huang et al., 1998</xref>). This unique charge storage and slow release characteristics of the multi-layered TiO<sub>2</sub> coatings, as shown in <xref ref-type="fig" rid="F1">Figure 1</xref>, may help maintain the effectiveness of cathodic protection over a prolonged period of time in the absence of UV illumination. The fundamental mechanism of electron capturing and releasing is as follows (<xref ref-type="bibr" rid="B16">Shinohara, 2001</xref>):<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi mathvariant="normal">Capturing:F</mml:mi>
<mml:msup>
<mml:mi mathvariant="normal">e</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">3&#x2b;</mml:mi>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:msup>
<mml:mi mathvariant="normal">e</mml:mi>
<mml:mi mathvariant="normal">-</mml:mi>
</mml:msup>
<mml:mo>&#x2192;</mml:mo>
<mml:mi mathvariant="normal">F</mml:mi>
<mml:msup>
<mml:mi mathvariant="normal">e</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">2&#x2b;</mml:mi>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mi mathvariant="normal">Under</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi mathvariant="normal">UV</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi mathvariant="normal">illumination</mml:mi>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mi mathvariant="normal">Releasing:F</mml:mi>
<mml:msup>
<mml:mi mathvariant="normal">e</mml:mi>
<mml:mrow>
<mml:mi mathvariant="normal">2&#x2b;</mml:mi>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2192;</mml:mo>
<mml:mi mathvariant="normal">F</mml:mi>
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</mml:mrow>
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<mml:mi mathvariant="normal">e</mml:mi>
<mml:mi mathvariant="normal">-</mml:mi>
</mml:msup>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mi mathvariant="normal">Dark</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi mathvariant="normal">condition</mml:mi>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Schematic representation of amorphous TiO<sub>2</sub>/anatase-type TiO<sub>2</sub> coatings on a 304LSS substrate and the working principle of photo-catalysis on the substrate under UV illumination.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g001.tif"/>
</fig>
</sec>
<sec id="s2">
<title>Experimental</title>
<sec id="s2-1">
<title>TiO<sub>2</sub> Sol&#x2013;Gel Preparation</title>
<p>Two different TiO<sub>2</sub> coatings were prepared by the sol&#x2013;gel calcination method using two different compositions. A Fe-doped TiO<sub>2</sub> sol&#x2013;gel solution and a plain TiO<sub>2</sub> sol&#x2013;gel one were developed separately. All the reagents were purchased from Sigma-Aldrich analytical reagent grade and used without further purification.</p>
<sec id="s2-1-1">
<title>Fe-Doped TiO<sub>2</sub> Sol&#x2013;Gel Preparation</title>
<p>The Fe-doped TiO<sub>2</sub> sol&#x2013;gel solution was prepared with a designated amount of TiO<sub>2</sub> to achieve a 10% in weight. The solution contained 2.3&#xa0;g of ferric nitrate, 10.0&#xa0;g of ethanol, and 29.3&#xa0;g of titanium isopropoxide. The resultant brownish transparent solution was aged and used as Fe pre-doped TiO<sub>2</sub> sol&#x2013;gel for applications in the comparative study on ITO.</p>
</sec>
<sec id="s2-1-2">
<title>Plain TiO<sub>2</sub> Sol&#x2013;Gel Preparation</title>
<p>The plain TiO<sub>2</sub> sol&#x2013;gel solution for applications in preparing coatings on 304LSS substrates was a mixture of 29.3&#xa0;g of titanium tetrapropoxide precursor, 8.0&#xa0;g of anhydrous ethanol, 5&#xa0;g of nitric acid, and additional 24&#xa0;g of ethanol. The first two chemicals were mixed under vigorous stirring condition at 260&#xa0;rpm in an ice bath for 5&#xa0;min, with the solution temperature controlled at 0&#xa0;C. The latter two chemicals were then added into and well-mixed with the foregoing solution to finish the sol&#x2013;gel preparation. The transparent yellow sol&#x2013;gel solution obtained was aged and used in constructing plain TiO<sub>2</sub> coatings on 304LSS substrates.</p>
</sec>
</sec>
<sec id="s2-2">
<title>Substrate Sample Preparation</title>
<p>Square disks made of 304LSS with a dimension of 2&#xa0;cm by 2&#xa0;cm by 0.5&#xa0;cm were used as substrate samples. <xref ref-type="table" rid="T1">Table 1</xref> shows the composition of the 304LSS sample analyzed by glow discharge spectroscopy (GDS). Prior to the coating process, the samples were degreased and mechanically polished with emery paper up to 600 grits and then cleansed with acetone and distilled water in an ultrasonic bath. Afterward, the samples were dipped into the plain TiO<sub>2</sub> sol&#x2013;gel solution <italic>via</italic> a commercial dip coater. In each dipping process, every sample was fully immersed in the solution for 1&#xa0;min and then slowly withdrawn at a speed of 3&#xa0;mm per min. The samples, coated with different layers of TiO<sub>2</sub> and designated as 304LSS/1TO, 304LSS/2TO, and 304LSS/3TO, were subjected to annealing treatment at different temperatures of 400 and 200&#xb0;C for 1&#xa0;h, as listed in <xref ref-type="table" rid="T2">Table 2</xref> with a heating ramp rate fixed at 5&#xa0;C/min for all treatments. A layer of uniform, transparent, and adhesive coating was obtained over each 304LSS sample under every annealing condition. The same procedures of dip coating with various layers of plain TiO<sub>2</sub> and Fe-doped TiO<sub>2</sub> and thermal annealing were repeated on ITO glass substrates for pertinent comparative studies, as listed in <xref ref-type="table" rid="T3">Table 3</xref>. The annealed specimens were staged in a desiccator and then used for the photo electrochemical measurements.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Chemical composition of 304LSS specimens.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Chemical</th>
<th align="center">Fe</th>
<th align="center">C</th>
<th align="center">Cr</th>
<th align="center">Ni</th>
<th align="center">Si</th>
<th align="center">Mn</th>
<th align="center">P</th>
<th align="center">S</th>
<th align="center">Mo</th>
<th align="center">Cu</th>
<th align="center">V</th>
<th align="center">Co</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">(%)</td>
<td align="center">Bal</td>
<td align="char" char=".">0.025</td>
<td align="char" char=".">17.92</td>
<td align="char" char=".">8.17</td>
<td align="char" char=".">0.44</td>
<td align="char" char=".">1</td>
<td align="char" char=".">0.023</td>
<td align="char" char=".">0.003</td>
<td align="char" char=".">0.00</td>
<td align="char" char=".">0.02</td>
<td align="char" char=".">0.07</td>
<td align="char" char=".">0.21</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Annealing treatment conditions for TiO<sub>2</sub> over 304LSS.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Designated name</th>
<th align="center">Coating layer</th>
<th align="center">Temperature (<sup>0</sup>C)</th>
<th align="center">Annealing environment</th>
<th align="center">Flow rate (SCCM)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">304LSS/1TO</td>
<td align="left">304LSS/anatase</td>
<td align="center">400</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">304LSS/2TO</td>
<td align="left">304LSS/anatase/amorphous</td>
<td align="center">400/200</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">304LSS/3TO</td>
<td align="left">304LSS/anatase/amorphous/amorphous</td>
<td align="center">400/200/200</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Annealing treatment conditions for doped and plain TiO<sub>2</sub> over ITO.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Designated name</th>
<th align="center">Coating layer</th>
<th align="center">Temperature (<sup>0</sup>C)</th>
<th align="center">Annealing environment</th>
<th align="center">Flow rate (SCCM)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">ITO/1TO200</td>
<td align="left">ITO/amorphous</td>
<td align="center">200</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">ITO/1TO400</td>
<td align="left">ITO/anatase</td>
<td align="center">400</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">ITO/1TO-Fe</td>
<td align="left">ITO/Fe-TiO<sub>2</sub> anatase</td>
<td align="center">400</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">ITO/2TO-Fe</td>
<td align="left">ITO/400&#xb0;C 1&#xa0;h Fe-TiO<sub>2</sub> anatase/anatase</td>
<td align="center">400/400</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
<tr>
<td align="left">ITO/3TO-Fe</td>
<td align="left">ITO/400&#xb0;C 1&#xa0;h Fe-TiO<sub>2</sub> anatase/anatase/amorphous</td>
<td align="center">400/400/200</td>
<td align="center">Argon</td>
<td align="char" char=".">176</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-3">
<title>Analytical Measurements on Coating Properties</title>
<p>To determine an optimal calcination temperature for forming TiO<sub>2</sub> coatings, thermo-gravimetric analyses (TGA) using TA instruments Q80 were adopted to analyze the thermal behavior of as prepared TiO<sub>2</sub> sol&#x2013;gel in the temperature range of 50&#x2013;600&#xa0;C. Optical absorption properties of the plain and Fe-doped TiO<sub>2</sub>-coated samples were measured using HP8453 (HP Germany) UV-visible spectrometer. Surface morphologies of the substrate samples were analyzed by scanning electron microscopy (SEM) by using a field emission scanning electron microscope (FE-SEM, JEOL JSM-6330F). In addition, the chemical composition of the samples was analyzed by an energy dispersion spectroscopy (EDS, Oxford INCA300, England) attached to SEM. The crystalline nature of the TiO<sub>2</sub> coatings was evaluated by an X-ray diffraction (XRD) pattern. A depth profile analysis by secondary ion mass spectroscopy (SIMS) was conducted by using the CAMECA secondary ion mass spectrometer to quantify the amount of Fe ions having diffused into the TiO<sub>2</sub> coatings from the substrate materials. Atomic force microscopy (AFM) was performed using the Bruker&#x2019;s nanoscope to determine the coating thickness. Synchrotron X-ray diffraction (XRD) (using &#x3bb; &#x3d; 1.48787&#xa0;&#xc5;) was performed at the end station of the TPS 09A beamline at the National Synchrotron Radiation Research Center (NSRRC), Taiwan, to study the change in the crystallinity and structure of the samples after annealing treatment at 200 and 400&#xb0;C. The samples were characterized at a glancing angle of 0.5&#xb0; over a two theta range of 20&#x2013;35&#xb0;. Sol&#x2013;gel solutions were prepared using the dip coating machine sadhu design.</p>
</sec>
<sec id="s2-4">
<title>Electrochemical Analyses</title>
<p>Potential variation monitoring and electrochemical polarization analyses were conducted with a commercial potentiostat manufactured by Corrtest Instruments to characterize the impact of UV on the open circuit potentials (OCPs) and corrosion rates of the coated 304LSS substrates. The schematic of the setup for photo-electrochemical analyses is shown in <xref ref-type="fig" rid="F2">Figure 2</xref>. The analyses were conducted at room temperature in an electrolyte solution of 0.5&#xa0;M of sodium bicarbonate (NaHCO<sub>3</sub>) under deaerated conditions with a pH of 8.2. The test parameters adopted in the electrochemical potentiodynamic polarization analyses were set at a potential scanning range between 100&#xa0;mV lower and greater than the equilibrium potential vs. the saturated calomel electrode with a scan rate of 0.25&#xa0;mV/s. <xref ref-type="fig" rid="F2">Figure 2</xref> shows the setup schematic of the three electrode electrochemical system, in which the TiO<sub>2</sub> coated 304LSS acted as a working electrode, a saturated calomel electrode was the reference electrode, and the counter electrode was a platinum-coated titanium mesh. A 500&#xa0;W Hamamatsu-made light emitter with an intensity of 4,300&#xa0;mW/cm<sup>2</sup> and a wavelength of 254&#xa0;nm was used as the UV source. Prior to every measurement, all the samples were immersed in the electrolyte solution for a period of 3&#xa0;h to ensure that the steady-state equilibrium was obtained.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Schematic of the three-electrode electrochemical system with a potentiostat for polarization analyses. A flat transparent window was installed to provide a designated path for incident UV.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g002.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and Discussion</title>
<sec id="s3-1">
<title>Determination of Optimal Calcination Temperature by TGA</title>
<p>
<xref ref-type="fig" rid="F3">Figure 3</xref> shows the TGA curve of TiO<sub>2</sub> sol&#x2013;gel in powder form, after being dried at 50&#xa0;C for 4&#xa0;h. It is clearly seen that the curve, descending from the starting temperature until it becomes flat at around 400&#xb0;C, may be explained by three stages. The first stage in the temperature range of 50&#x2013;120&#xb0;C represents the evaporation of remaining ethanol, acid, and moisture in the powder, and around 10% weight loss was observed. Between 120 and 400&#xb0;C, the declining in weight was attributed to decomposition and desorption of the organic hydroxyl compounds adsorbed on the sample, with about 9% weight loss. The amorphous TiO<sub>2</sub> precursors was converted to anatase phase TiO<sub>2</sub> crystals as the temperature increases from 400 to 600&#xb0;C in the third stage. There was no further significant weight loss on the TGA curve after 400&#xb0;C indicating that the decomposition and desorption process had completed. Accordingly, this temperature was selected as the calcination temperature for forming anatase TiO<sub>2</sub> thin films on the substrate samples. The inferred outcome was further confirmed by XRD analyses and is discussed in the later section.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>TGA curve for TiO<sub>2</sub> sol&#x2013;gel powder formed due to drying at 50&#xa0;C for 4&#xa0;h.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g003.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>Optical Absorption Properties of the TiO<sub>2</sub> Coatings</title>
<p>The UV&#x2013;visible absorption spectra of the Fe-doped and plain TiO<sub>2</sub> coatings applied over the ITO glass substrates were measured in the wavelength range of 300&#x2013;600&#xa0;nm, as shown in <xref ref-type="fig" rid="F4">Figure 4</xref>. The linear extrapolation method was adopted to determine the absorption onset wavelength of the samples. The plain crystalline TiO<sub>2</sub> coating shows an intense absorption in the UV region (around 360&#xa0;nm), whereas the amorphous TiO<sub>2</sub> coating exhibits its characteristic spectrum with an absorption onset wavelength of around 340&#xa0;nm. The foregoing results indicate that both the anatase and amorphous TiO<sub>2</sub> coatings do not have any absorption edge in the visible range. However, the absorption onset wavelength of the Fe-doped TiO<sub>2</sub> coating is slightly shifted to about 390&#xa0;nm, which lies in the visible light range and would lead to a poorer photocatalytic activity of this coating during UV illumination.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>UV&#x2013;visible absorption spectra for different TiO<sub>2</sub> thin films on ITO glass.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g004.tif"/>
</fig>
</sec>
<sec id="s3-3">
<title>Surface Morphologies of the Coatings</title>
<sec id="s3-3-1">
<title>Surface Analysis</title>
<p>SEM analysis was performed to determine the structural morphology of the three-layer TiO<sub>2</sub> coating on the 304LSS substrate. The coating did not show any presence of cracks or adhesion failure after the planned annealing treatments, as shown in <xref ref-type="fig" rid="F5">Figure 5</xref>. It was reported that the thermal expansion coefficient of Type 304 stainless steel is usually greater than that of a TiO<sub>2</sub> coating, causing an interfacial stress between the substrate and the TiO<sub>2</sub> coating (<xref ref-type="bibr" rid="B1">Balasubramanian et al., 2003</xref>). The TiO<sub>2</sub> coating would thus lose its adherence on the substrate during annealing treatments if this interfacial stress is higher than the coating adherent strength. Nevertheless, no spallation or cracking was observed on the coated sample in our study. The SEM-EDS data show significant evidence of Ti and O on the sample surface, and the TiO<sub>2</sub> coating surface was smooth without any wrinkles or non-uniform features. Furthermore, the AFM analysis results showed that the thickness of a single layer of amorphous TiO<sub>2</sub> coating was around 105&#xa0;nm whereas the thickness of the anatase TiO<sub>2</sub> coating was too small to estimate by AFM.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>SEM image and EDX analyses results of the three-layer TiO<sub>2</sub> coating on the 304LSS sample.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g005.tif"/>
</fig>
</sec>
<sec id="s3-3-2">
<title>Depth Profile Analysis</title>
<p>
<xref ref-type="fig" rid="F6">Figure 6</xref> shows the results of depth profile analysis for the plain three-layer TiO<sub>2</sub> coating (304LSS/3TO). It was observed that significant amounts of Fe and Cr along with Ni in a lower level are present in the coating. These foreign metal atoms diffused from the 304LSS substrate into the coating during the thermal annealing treatments (<xref ref-type="bibr" rid="B27">Yu et al., 2003</xref>). The amount of Fe having diffused into the TiO<sub>2</sub> coatings is greater than those of the other two elements because the diffusion coefficient of Fe in the coating is the greatest of all (<xref ref-type="bibr" rid="B13">Maruska and Ghosh, 1979</xref>). It is comparatively more likely for Fe to form iron oxide at the interface between the coating and the substrate during annealing, and this would actually allow more Fe ions to diffuse into the coating. In the meantime, Ni and Cr would remain in the metallic state as they are not easily oxidized at the selected annealing temperatures. On the other hand, indications of Ti are seen in the 304LSS substrate in a very low concentration which suggests that the interdiffusion of Fe and Ti would render the TiO<sub>2</sub> coating more adherent to the 304LSS substrate (<xref ref-type="bibr" rid="B14">Shang et al., 2003</xref>). Hence, the thermal annealing treatment not only helps in the crystallization of TiO<sub>2</sub> but also makes the coating firmly reside on the substrate. As also seen in <xref ref-type="fig" rid="F6">Figure 6</xref>, not the entire coating is doped with the metallic elements. A small portion near the outer surface of the coating remains uncontaminated, suggesting Fe doping might have acted as a barrier for further diffusion of the metallic elements at all thermal treatments between 400 and 200&#xa0;C.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Depth profiles of Fe, Cr, and Ni in the 304LSS/3TO sample.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g006.tif"/>
</fig>
</sec>
<sec id="s3-3-3">
<title>XRD Analysis</title>
<p>To characterize the structures of the TiO2 coatings under different calcination temperatures, coated ITO substrates were annealed at either 400&#xa0;C or 200&#xa0;C for 1&#xa0;h. The technique of glancing angle XRD was adopted to analyze these samples and an uncoated ITO substrate. The results, as summarized in <xref ref-type="fig" rid="F7">Figure 7</xref>, show that the crystallinity of the TiO<sub>2</sub> coating strongly depends on annealing heat treatment temperature. The sample annealed at 200&#xa0;C did not exhibit any obvious diffraction peak for TiO<sub>2</sub> except those corresponding to the uncoated ITO substrate, indicating that this coating was amorphous in nature. On the other hand, when the annealing temperature was set at 400&#xa0;C, the coating exhibited a crystalline structure. The diffraction peak at 24.5 <sup>o</sup> (101) corresponds to the tetragonal anatase phase of TiO<sub>2</sub>. The outcome is consistent with the results obtained from the TGA.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>XRD analysis results of the annealed TiO<sub>2</sub> coatings and the uncoated ITO.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g007.tif"/>
</fig>
</sec>
</sec>
<sec id="s3-4">
<title>OCP Responses of TiO<sub>2</sub>-Coated Samples to UV Illumination</title>
<p>The photocatalytic activities of the coatings were evaluated by OCP measurements in the designated electrolyte solution for both the ITO and 304LSS substrates.</p>
<sec id="s3-4-1">
<title>Variations in OCP of ITO Substrates Coated With Plain TiO<sub>2</sub>
</title>
<p>
<xref ref-type="fig" rid="F8">Figure 8</xref> shows the OCP responses of the ITO/1TO200 and ITO/1TO400 samples under dark and UV illumination conditions. Prior to UV illumination, the OCPs of the two samples were nearly the same at &#x2212;0.05 V<sub>SCE</sub>. Upon the start of UV illumination, the OCPs of both samples decrease significantly to more active values, exhibiting an instantaneous photocatalytic effect. ITO/1TO400 eventually attained a stable OCP value at &#x2212;0.50 V<sub>SCE</sub>. ITO/1TO200 actually reached an even more active potential of &#x2212;0.62 V<sub>SCE</sub> at the beginning but slightly increased to &#x2212;0.58 V<sub>SCE</sub> during the period of UV illumination. As soon as the UV was switched off, the OCP of ITO/1TO400 immediately returned to the original value because the free electrons readily recombined with the charge carriers. However, the OCP of ITO/1TO200 promptly increased to &#x2212;0.15 V<sub>SCE</sub> in 30&#xa0;min, about 0.1&#xa0;V lower than the original value.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>OCP responses of ITO/1TO400 and ITO/1TO200 in the designated electrolyte solution to the absence and presence of UV illumination.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g008.tif"/>
</fig>
<p>When the UV was turned on for the second time, the OCP of ITO/1TOC immediately reached &#x2212;0.50 V<sub>SCE</sub> again. In the meantime, the OCP of ITO/1TOM promptly decreased to &#x2212;0.58 V<sub>SCE</sub>, the last recorded potential during the previous UV illumination period, which was due to the degradation of amorphous coating, also termed as photo-corrosion of TiO<sub>2</sub> (<xref ref-type="bibr" rid="B30">Zhang et al., 2015</xref>). This phenomenon suggests that it would be inappropriate to use amorphous TiO<sub>2</sub> coatings for deterring corrosion under UV illumination. The ITO/1TO400 sample, with its better crystallinity in the TiO<sub>2</sub> coating, would allow UV-generated electrons to migrate through the space charge layer to the substrate in a relatively more stable manner. The foregoing results prove that both the crystalline and amorphous TiO<sub>2</sub> coatings showed photocatalytic activity in generating free electrons. However, they did not bear the capability to trap electrons during UV illumination and thus could not protect the substrate materials under dark conditions.</p>
</sec>
<sec id="s3-4-2">
<title>OCP Responses to UV Illumination of Samples Coated With Fe-Doped TiO<sub>2</sub>
</title>
<p>It is anticipated that with a proper dopant such as Fe, TiO<sub>2</sub> coating may be able to bear the charge storage property. The Fe ions as dopants in the TiO<sub>2</sub> coating may serve to trap and store the UV-generated electrons, thus reducing their recombination with the charge carriers. The more active OCP of the coated sample during UV illumination would then return to its original value slowly once the UV is switched off, offering a prolonged protection against corrosion under dark condition. It should be also noted that even a small amount of Fe dopants incorporated within a plain TiO<sub>2</sub> coating would drastically degrade the photocatalytic activity of the coating, leading to a much less decrease in OCP. <xref ref-type="fig" rid="F9">Figure 9</xref> shows the variations in OCP of the ITO/1TO-Fe, ITO/2TO-Fe, and ITO/3TO-Fe samples after being irradiated with UV for 1&#xa0;h. It was observed that the presence of Fe ions in the TiO<sub>2</sub> coatings led to slow increases in OCP of the three samples for more than 10&#xa0;h, and one additional anatase TiO<sub>2</sub> coating would result in a comparatively more decrease in OCP on ITO/2TO-Fe, and ITO/3TO-Fe under UV illumination. The Fe-doped TiO<sub>2</sub> coating contained the redox couple of Fe<sup>2&#x2b;</sup>/Fe<sup>3&#x2b;</sup>, and Fe<sup>3&#x2b;</sup> is reduced to Fe<sup>2&#x2b;</sup> with the aid of free electrons generated under UV illumination (<xref ref-type="bibr" rid="B9">Huang et al., 1997</xref>). Further addition of an amorphous TiO<sub>2</sub> coating as in ITO/3TO-Fe not only increased the photocatalytic activity but also inhibited the oxygen reduction reaction on the coating surface (<xref ref-type="bibr" rid="B8">Huang et al., 1998</xref>). Moreover, the amorphous coating still contained which would make the space charge layer even thicker. It would hence be more difficult for the stored electrons to escape from the Fe-doped TiO<sub>2</sub> layer in the absence of UV illumination (<xref ref-type="bibr" rid="B18">Subasri and Shinohara, 2005</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>OCP responses of ITO/1TO-Fe, ITO/2TO-Fe, and ITO/3TO-Fe in the designated electrolyte solutions to the absence and presence of UV illumination.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g009.tif"/>
</fig>
</sec>
<sec id="s3-4-3">
<title>Variations in OCP of 304LSS Substrates Coated With Various Layers of TiO<sub>2</sub>
</title>
<p>The 304LSS/1TO, 304LSS/2TO, and 304LSS/3TO samples were separately immersed in the same electrolyte solutions for potentiodynamic polarization analyses, and the results of OCP variations of these samples in the absence and presence of UV are shown in <xref ref-type="fig" rid="F10">Figure 10A</xref> Prior to the start of UV illumination, all three samples showed similar OCPs at around &#x2212;0.1 V<sub>SCE</sub>, which were slightly higher than that of the uncoated 304LSS substrate (not shown in the figure). Upon the start of UV illumination, the OCPs of all samples promptly moved toward the more active (negative) direction. Among them, the OCP of 304LSS/1TO showed the least decrease of 0.1 V, and those of the other two decreased by more than 0.2&#xa0;V. The same crystalline TiO<sub>2</sub> coatings were applied to 304LSS/1TO and ITO/1TO400, but their responses of OCP to UV illumination were distinctly different. Between the off and on moments of UV, while the OCP decrease on ITO was greater than 0.4 V, and the decrease on Type 304LSS was slightly greater than 0.1&#xa0;V. The less OCP decrease on 304LSS/1TO was due to the formation of an interfacial oxide layer between the substrate and the coating during the 400&#xa0;C calcination treatment. At 400&#xb0;C, there would be interaction between the oxide layer and the TiO<sub>2</sub> coating, inducing the diffusion of metal ions, mainly Fe, into the TiO<sub>2</sub> coating and degrading the photocatalytic activity (<xref ref-type="bibr" rid="B11">Konishi and Tsujikawa, 1997</xref>).</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>
<bold>(A)</bold> OCP responses of 304LSS/1TO, 304LSS/2TO, and 304LSS/3TO in the designated electrolyte solutions to the absence and presence of UV illumination. <bold>(B)</bold> OCP responses of 304LSS/2TO and 304LSS/3TO in the designated electrolyte solutions to the absence and presence of UV illumination for two cycles.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g010.tif"/>
</fig>
<p>On the other hand, all samples exhibited gradual increases in OCP when UV illumination was switched off. This slow recovery phenomenon in OCP is similar to that of the ITO/1TO-Fe sample and it took almost 2&#xa0;h for the OCP to reach the original value. This again confirmed that the Fe ions having diffused into the coating played an important role in the slow increase in OCP. The Fe ions served to trap and store the UV-generated electrons, thus limiting their recombination with the charge carriers. With an additional amorphous TiO<sub>2</sub> layer over the Fe-doped anatase layer, an improved photocatalytic effect was observed on 304LSS/2TO, and the OCP was further reduced to a more negative value to &#x2212;0.38 V<sub>SCE</sub>. The addition of amorphous TiO<sub>2</sub> also led to a slow recovery in OCP and it took nearly 8&#xa0;h for the sample to return to the original OCP, due to in part the suppression of oxygen reduction reaction by this additional coating with a mechanism similar to that of the ITO/3TO-Fe sample (<xref ref-type="bibr" rid="B8">Huang et al., 1998</xref>). One more layer of amorphous TiO<sub>2</sub> as in the 304LSS/3TO sample seemed even more effective in promoting photocatalytic effect and prolonging the OCP recovery time when UV was switched off. The OCP variation experiments were repeated for several cycles over the 304LSS/2TO and 304LSS/3TO specimens, and no degradation in UV-induced electrochemical characteristics of the coatings were observed as shown in <xref ref-type="fig" rid="F10">Figure 10B</xref>
</p>
</sec>
</sec>
<sec id="s3-5">
<title>Corrosion Rates of the TiO<sub>2</sub> Coated Samples</title>
<p>Potentiodynamic polarization analyses were conducted for the 304LSSS/3TO sample and the uncoated 304LSS sample exposed to a 0.5&#xa0;M of sodium bicarbonate electrolyte solution in the absence of UV illumination, and the results are shown in <xref ref-type="fig" rid="F11">Figure 11A</xref> Prior to each polarization analysis, the sample was immersed in the solution for a time period of 3&#xa0;h to ensure that a stabilized equilibrium was reached. According to the polarization curves, the electrochemical corrosion potential ECP (&#x2212;0.14 V<sub>SCE</sub>) of 304LSS/3TO is higher than that (&#x2212;0.21 V<sub>SCE</sub>) of the uncoated sample by 0.07&#xa0;V. The corrosion current density of the uncoated sample was 9.82 &#xd7; 10<sup>&#x2013;8</sup> A/cm<sup>2</sup>. In the meantime, the 304LSS/3TO sample exhibited comparative less anodic current density of 2.07 &#xd7; 10<sup>&#x2013;8</sup> A/cm<sup>2</sup>, revealing an inhibitive property of the coating and consistent with what had been observed in the literature (<xref ref-type="bibr" rid="B31">Zhou et al., 2009</xref>).</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>
<bold>(A)</bold> Polarization curves of the uncoated 304LSS sample and the 304LSS/3TO sample. <bold>(B)</bold> Polarization curves of the uncoated 304LSS sample in the absence of UV illumination and of the 304LSS/3TO samples at different stages.</p>
</caption>
<graphic xlink:href="fmats-09-863603-g011.tif"/>
</fig>
<p>The polarization curves for the 304LSS/3TO sample under different conditions in the absence and presence of UV illumination are shown in <xref ref-type="fig" rid="F11">Figure 11B</xref>, and the test conditions are summarized in <xref ref-type="table" rid="T4">Table 4</xref>. Under UV illumination, the 304LSS/3TO sample showed a markedly negative shift in corrosion potential to &#x2212;0.53 V<sub>SCE</sub>, which was 0.39&#xa0;V more active than that of the uncoated sample, also signifying the accumulation of UV-generated electrons. The pertinent corrosion current density was significantly lowered to 2.31 &#xd7; 10<sup>&#x2013;12</sup> A/cm<sup>2</sup>. On the other hand, the increase in anodic current density was attributed to the release of these electrons from the space charge layer. The change in ECP was consistent with the OCP variation in the same sample explained in the previous section. To investigate the time-dependent change in electrochemical corrosion potential and the pertinent corrosion current density of the sample, polarization analyses were further conducted at 1&#xa0;h and 10&#xa0;h after UV illumination was switched off. The ECP of the sample increased to &#x2212;0.42 V<sub>SCE</sub> 1&#xa0;h later and further increased to &#x2212;0.22 V<sub>SCE</sub> 10&#xa0;h later, which was in good agreement with the OCP variation of the same sample. The respective corrosion densities of the sample were determined to be 2.62 &#xd7; 10<sup>&#x2013;11</sup> A/cm<sup>2</sup> and 3.36 &#xd7; 10<sup>&#x2013;9</sup> A/cm<sup>2</sup>. It was noted that the corrosion current density of the coated sample could still remain one order of magnitude less than that of the uncoated one for 10&#xa0;h in the absence of UV, indicating that the protection against corrosion in the substrate alloy was effectively prolonged with the specifically engineered TiO<sub>2</sub> coating.</p>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>Conditions set for potentiodynamic polarization analyses.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Condition</th>
<th align="center">Synonyms</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Electrochemical potential under stable equilibrium condition before UV irradiation</td>
<td align="center">No UV</td>
</tr>
<tr>
<td align="left">Electrochemical potential during UV illumination for 1&#xa0;h</td>
<td align="center">UV on</td>
</tr>
<tr>
<td align="left">Electrochemical potential after 1&#xa0;h of UV illumination off</td>
<td align="center">1&#xa0;h UV off</td>
</tr>
<tr>
<td align="left">Electrochemical potential after 10&#xa0;h of UV illumination off</td>
<td align="center">10&#xa0;h UV off</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>A continuous, uniform, and compact TiO<sub>2</sub> coating was prepared on Type 304LSS substrates by the sol&#x2013;gel method for prolonged corrosion mitigation. The TiO<sub>2</sub> coating on the 304LSS/3TO sample exhibited the best photo-cathodic protection property in the corrosive environment. The 304LSS/3TO sample was cathodically protected for more than 10&#xa0;h even after the cutoff of UV illumination. The corrosion current density of the 304LSS/3TO sample was still one order of magnitude less than that of the uncoated sample for 10&#xa0;h without UV illumination. The novel multi-layered TiO<sub>2</sub> coating developed in this study is able to provide an effective and prolonged photo-cathodic protection for the stainless steel substrate.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>KS: investigation, formal analysis, methodology, and writing the original draft. M-YW: supervision, resources, funding acquisition, and project administration. AA: investigation and formal analysis. C-HL: supervision and resources. T-KY: supervision, conceptualization, data curation, writing&#x2014;review and editing.</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<ack>
<p>The authors thank the Nanoscience and Technology Program, Taiwan International Graduate Program, Academia Sinica, Taiwan. The beamtime offered by NSRRC is also highly acknowledged.</p>
</ack>
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