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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Bioeng. Biotechnol.</journal-id>
<journal-title>Frontiers in Bioengineering and Biotechnology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Bioeng. Biotechnol.</abbrev-journal-title>
<issn pub-type="epub">2296-4185</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">840372</article-id>
<article-id pub-id-type="doi">10.3389/fbioe.2022.840372</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Bioengineering and Biotechnology</subject>
<subj-group>
<subject>Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Ceramic Toughening Strategies for Biomedical Applications</article-title>
<alt-title alt-title-type="left-running-head">Bai et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Biomedical Ceramic Toughening</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Bai</surname>
<given-names>Rushui</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Sun</surname>
<given-names>Qiannan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>He</surname>
<given-names>Ying</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Peng</surname>
<given-names>Liying</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>Zhang</surname>
<given-names>Yunfan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/824439/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhang</surname>
<given-names>Lingyun</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>Lu</surname>
<given-names>Wenhsuan</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>Deng</surname>
<given-names>Jingjing</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>Zhuang</surname>
<given-names>Zimeng</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" corresp="yes">
<name>
<surname>Yu</surname>
<given-names>Tingting</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/791994/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wei</surname>
<given-names>Yan</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/933273/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Department of Orthodontics</institution>, <institution>Peking University School and Hospital of Stomatology</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>National Engineering Laboratory for Digital and Material Technology of Stomatology and Beijing Key Laboratory of Digital Stomatology</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Department of Geriatric Dentistry</institution>, <institution>Peking University School and Hospital of Stomatology</institution>, <addr-line>Beijing</addr-line>, <country>China</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/674982/overview">Yanyu Yang</ext-link>, Zhengzhou University, China</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/689801/overview">Dan Wang</ext-link>, Beijing University of Chemical Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1340413/overview">Dongpeng Yan</ext-link>, Beijing Normal University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/257812/overview">Ahmed El-Fiqi</ext-link>, Dankook University, South Korea</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1657176/overview">Liu Weipeng</ext-link>, Hebei University of Technology, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Tingting Yu, <email>tingtingyu@bjmu.edu.cn</email>; Yan Wei, <email>kqweiyan@bjmu.edu.cn</email>
</corresp>
<fn fn-type="equal" id="fn1">
<label>
<sup>&#x2020;</sup>
</label>
<p>These authors have contributed equally to this&#x20;work</p>
</fn>
<fn fn-type="other">
<p>This article was submitted to Biomaterials, a section of the journal Frontiers in Bioengineering and Biotechnology</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>07</day>
<month>03</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>840372</elocation-id>
<history>
<date date-type="received">
<day>21</day>
<month>12</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>09</day>
<month>02</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Bai, Sun, He, Peng, Zhang, Zhang, Lu, Deng, Zhuang, Yu and Wei.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Bai, Sun, He, Peng, Zhang, Zhang, Lu, Deng, Zhuang, Yu and Wei</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&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>Aiming at shortage of metal materials, ceramic is increasingly applied in biomedicine due to its high strength, pleasing esthetics and good biocompatibility, especially for dental restorations and implants, artificial joints, as well as synthetic bone substitutes. However, the inherent brittleness of ceramic could lead to serious complications, such as fracture and disfunction of biomedical devices, which impede their clinical applications. Herein, several toughening strategies have been summarized in this review, including reinforcing phase addition, surface modification, and manufacturing processes improvement. Doping metal and/or non-metal reinforcing fillers modifies toughness of bulk ceramic, while surface modifications, mainly coating, chemical and thermal methods, regulate toughness on the surface layer. During fabrication, optimization should be practiced in powder preparation, green forming and densification processes. Various toughening strategies utilize mechanisms involving fine-grained, stress-induced phase transformation, and microcrack toughening, as well as crack deflection, bifurcation, bridging and pull-out. This review hopes to shed light on systematic combination of different toughening strategies and mechanisms to drive progress in biomedical devices.</p>
</abstract>
<kwd-group>
<kwd>ceramic</kwd>
<kwd>biomedical</kwd>
<kwd>fracture</kwd>
<kwd>toughening</kwd>
<kwd>reinforcing phase</kwd>
<kwd>surface modification</kwd>
<kwd>manufacture</kwd>
<kwd>toughening mechanism</kwd>
</kwd-group>
<contract-num rid="cn001">2020YFA0710401 2021YFC2400403</contract-num>
<contract-num rid="cn002">51972005 U21A2055 82101074&#x20;51903003</contract-num>
<contract-sponsor id="cn001">National Key Research and Development Program of China<named-content content-type="fundref-id">10.13039/501100012166</named-content>
</contract-sponsor>
<contract-sponsor id="cn002">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>With the aging of the population, the demand for maintaining the quality of life is in needed worldwide. The tooth loss (<xref ref-type="bibr" rid="B144">Zitzmann et&#x20;al., 2007</xref>), symptomatic osteoarthritis (<xref ref-type="bibr" rid="B117">Pivec et&#x20;al., 2012</xref>; <xref ref-type="bibr" rid="B63">Hunter and Bierma-Zeinstra, 2019</xref>), as well as bone defects and dysfunction (<xref ref-type="bibr" rid="B17">Carrington, 2005</xref>; <xref ref-type="bibr" rid="B111">Olshansky et&#x20;al., 2005</xref>) have become global health care problems, which lead to growing markets for high-quality biomedical devices (<xref ref-type="bibr" rid="B144">Zitzmann et&#x20;al., 2007</xref>; <xref ref-type="bibr" rid="B69">Kim et&#x20;al., 2008</xref>; <xref ref-type="bibr" rid="B22">Chevalier and Gremillard, 2009</xref>; <xref ref-type="bibr" rid="B16">Carr et&#x20;al., 2012</xref>; <xref ref-type="bibr" rid="B113">Patel et&#x20;al., 2015</xref>). Large amount of these devices are made of metal but their metal-color (<xref ref-type="bibr" rid="B10">Bayne et&#x20;al., 2019</xref>), high wear rates of bearing components and large amount of ion release (<xref ref-type="bibr" rid="B22">Chevalier and Gremillard, 2009</xref>) greatly impede their clinical applications. Thus, benefited from its excellent mechanical, esthetic (<xref ref-type="bibr" rid="B10">Bayne et&#x20;al., 2019</xref>) and biocompatible properties (<xref ref-type="bibr" rid="B48">Gao et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B124">Ruiz Henao et&#x20;al., 2021</xref>), ceramic becomes potential candidate for biomedical applications, such as dental restorations (<xref ref-type="bibr" rid="B85">Li et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B132">Spitznagel et&#x20;al., 2018</xref>), dental implants (<xref ref-type="bibr" rid="B70">Kohal et&#x20;al., 2008</xref>; <xref ref-type="bibr" rid="B125">Saadaldin and Rizkalla, 2014</xref>), heads and cups of joint replacements (<xref ref-type="bibr" rid="B118">Rahaman et&#x20;al., 2007</xref>), as well as bone fillers and scaffolds (<xref ref-type="bibr" rid="B95">Ma et&#x20;al., 2018</xref>) for tissue engineering. Although ceramic materials show their huge potential and preponderance, high brittleness of ceramic restrains its biomedical applications, which might result in severe clinical complications, such as fracture (<xref ref-type="bibr" rid="B13">Benaqqa et&#x20;al., 2005</xref>; <xref ref-type="bibr" rid="B73">Koo et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B102">Morimoto et&#x20;al., 2016</xref>; <xref ref-type="bibr" rid="B72">Kong et&#x20;al., 2019</xref>). Failures of ceramic mostly happen in the absence of extrinsic shielding mechanisms, where fracture invariably occurs catastrophically by cohesive bond breaking at the crack tip with a resulting very low intrinsic toughness of roughly 1&#x2013;3&#xa0;MPa m<sup>1/2</sup> (<xref ref-type="bibr" rid="B79">Launey and Ritchie, 2009</xref>). Therefore, the extreme brittleness of ceramic materials highlights the importance of ceramic toughening.</p>
<p>Toughness of materials could be thought as the ability to dissipate deformation energy without crack propagation (<xref ref-type="bibr" rid="B79">Launey and Ritchie, 2009</xref>). One of the widely recognized methods of computing toughness, denoted here as &#x3c4;, is by the area under the engineering stress &#x3c3; vs. engineering strain &#x3b5; curve determined in a tensile test (<xref ref-type="bibr" rid="B127">Sehaqui et&#x20;al., 2013</xref>). Thus<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi>&#x3c4;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:munderover>
<mml:mstyle displaystyle="true">
<mml:mo>&#x222b;</mml:mo>
</mml:mstyle>
<mml:mn>0</mml:mn>
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b5;</mml:mi>
<mml:mi>b</mml:mi>
</mml:msub>
</mml:mrow>
</mml:munderover>
<mml:mi>&#x3c3;</mml:mi>
<mml:mi>d</mml:mi>
<mml:mi>&#x3b5;</mml:mi>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>Where &#x3b5;<sub>b</sub> is the elongation at break. The term &#x201c;toughness&#x201d; is also used to the critical outcome of impact testing, namely the energy required to generate fracture at high rates of force application (<xref ref-type="bibr" rid="B8">Bai et&#x20;al., 2012</xref>). Thus, there is fracture toughness, notch toughness, determined in impact testing for a predetermined geometry of the notch and testing methods, or else drop impact toughness (<xref ref-type="bibr" rid="B15">Brostow et&#x20;al., 2015</xref>). Fracture toughness is the focus of this review, and a variety of testing methods have been proposed, such as indentation fracture (IF) (<xref ref-type="bibr" rid="B34">Evans and Charles, 1976</xref>; <xref ref-type="bibr" rid="B80">Lawn et&#x20;al., 1980</xref>; <xref ref-type="bibr" rid="B6">Anstis et&#x20;al., 1981</xref>), single-edge notched beam (SENB) (<xref ref-type="bibr" rid="B25">Damani et&#x20;al., 1996</xref>), single-edge precracked beam (SEPB) (<xref ref-type="bibr" rid="B18">Cesar et&#x20;al., 2005</xref>), single-edge V-notched beam (SEVNB), chevron notch (CN), surface crack in flexure (SCF) and double cantilever beam (DCB) methods (<xref ref-type="bibr" rid="B138">Wang et&#x20;al., 2017</xref>).</p>
<p>Crack growth is promoted ahead of the crack tip by intrinsic microstructural damage, and impeded by extrinsic mechanisms acting primarily behind the crack tip, which serve to &#x201c;shield&#x201d; the crack tip from the far-field driving forces (<xref ref-type="bibr" rid="B122">Ritchie, 1988</xref>). Toughness can be enhanced by increasing the microstructural resistance, such as by changing the nature and distribution to suppress damage in the form of microcracking or microvoid formation ahead of the crack tip, which is termed intrinsic toughening. However, this approach is largely ineffective with brittle materials such as ceramic (<xref ref-type="bibr" rid="B35">Evans, 1990</xref>), which invariably must rely on extrinsic toughening. Extrinsic toughening involves microstructural mechanisms that act primarily behind the crack tip to effectively reduce the crack-driving force actually experienced at the crack tip; this is termed crack-tip shielding and can occur by such mechanisms as <italic>in situ</italic> phase transformations and crack bridging (<xref ref-type="bibr" rid="B79">Launey and Ritchie, 2009</xref>). Brittle materials, such as ceramics, are invariably toughened with extrinsic mechanisms (<xref ref-type="bibr" rid="B35">Evans, 1990</xref>; <xref ref-type="bibr" rid="B11">Becher, 1991</xref>), which depend on crack size and to some degree specimen geometry. A principle manifestation of this crack-size dependent fracture behavior is resistance-curve (R-curve) toughness behavior where the crack driving force to sustain cracking increases with crack extension. Extrinsic toughening mechanisms mainly affect the crack growth, while have little effect on crack initiation.</p>
<p>Biomedical used-ceramic is applied as structural material, where catastrophic fracture is strictly prohibited and might lead to medical malpractice. Therefore, systematic investigation on ceramic toughness and recent progress of its modulation strategies are vastly required. However, there is limited number of reviews concerning ceramic toughening strategies, especially for biomedical applications (<xref ref-type="bibr" rid="B107">Naslain, 2004</xref>; <xref ref-type="bibr" rid="B7">Asl et&#x20;al., 2018</xref>; <xref ref-type="bibr" rid="B131">Siddiqui et&#x20;al., 2018</xref>). Therefore, this review provides an overview of crack-tip shielding methods to realize extrinsic toughening for biomedical ceramic (<xref ref-type="fig" rid="F1">Figure&#x20;1</xref>), from adding reinforcing second phase (summarized in <xref ref-type="table" rid="T1">Table&#x20;1</xref>), surface modification to manufacturing optimization. And toughening mechanisms are also introduced briefly to deepen understanding of these strategies.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Medical applications of ceramics, corresponding clinical complications due to the low fracture toughness of ceramics, as well as toughening strategies and underlying mechanisms. <bold>(A)</bold> Fully contoured zirconia crown, <bold>(a)</bold> before polishing and <bold>(b)</bold> from the occlusal view (second lower left molar) (<xref ref-type="bibr" rid="B101">Miyazaki et&#x20;al., 2013</xref>). <bold>(B)</bold>, <bold>(a)</bold> Chipping of the ceramic veneer; <bold>(b)</bold> Framework fracture in the second upper left molar distal buccal (<xref ref-type="bibr" rid="B101">Miyazaki et&#x20;al., 2013</xref>). <bold>(C)</bold>, <bold>(a)</bold> Insertion of the ceramic implant; <bold>(b)</bold> Ceramic abutments (zirconia) attached to the implants intraorally (<xref ref-type="bibr" rid="B70">Kohal et&#x20;al., 2008</xref>). <bold>(D)</bold> Extracted fractured implant and crown, as well as fractured surface (<xref ref-type="bibr" rid="B72">Kong et&#x20;al., 2019</xref>). <bold>(E)</bold>, <bold>(a)</bold> Prosthetic hip implants with ceramic-on-ceramic (Al<sub>2</sub>O<sub>3</sub>-on-Al<sub>2</sub>O<sub>3</sub>) bearing couple; <bold>(b)</bold> Prosthetic knee implants with ceramic-on-UHMWPE bearing couple (<xref ref-type="bibr" rid="B118">Rahaman et&#x20;al., 2007</xref>). <bold>(F)</bold>, <bold>(a)</bold> Five large pieces of a fractured ceramic head and many small fragments; <bold>(b)</bold> Radiograph showing the fracture of the ceramic femoral head (<xref ref-type="bibr" rid="B135">Toran et&#x20;al., 2006</xref>; <xref ref-type="bibr" rid="B65">Hwang et&#x20;al., 2007</xref>). <bold>(G)</bold> Photograph of 3D-printed bioactive glass-ceramic scaffolds (<xref ref-type="bibr" rid="B92">Liu et&#x20;al., 2018</xref>). <bold>(H)</bold> Crack initiation and propagation path shown by <bold>(a&#x2013;c)</bold> XFEM analysis and <bold>(d&#x2013;f)</bold> FE-SEM images (<xref ref-type="bibr" rid="B32">Entezari et&#x20;al., 2016</xref>). UHMWPE, ultra-high-molecular-weight polyethylene; XFEM, extended finite element method; FE-SEM, field emission scanning electron microscopy.</p>
</caption>
<graphic xlink:href="fbioe-10-840372-g001.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Summary of adding reinforcing second phase in bioceramics.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Classification</th>
<th align="center">Second phase fillers</th>
<th align="center">Volume fraction of fillers</th>
<th align="center">Ceramic matrix</th>
<th align="center">Fabrication techniques</th>
<th align="center">K<sub>lc</sub> testing method</th>
<th align="center">Maximum K<sub>lc</sub> (MPa&#xb7;m<sup>1/2</sup>)</th>
<th align="center">K<sub>Ic</sub> of control</th>
<th align="center">Mentioned toughening mechanisms</th>
<th align="center">Ref.</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="15" align="left">Metal Oxide and Metal</td>
<td rowspan="2" align="left">Al<sub>2</sub>O<sub>3</sub> whiskers</td>
<td rowspan="2" align="left">2.5&#xa0;wt%</td>
<td rowspan="2" align="left">Al<sub>2</sub>O<sub>3</sub>/3Y-TZP</td>
<td rowspan="2" align="left">Conventional sintering (1,500&#xb0;C, 2h, in air)</td>
<td rowspan="2" align="left">IF</td>
<td rowspan="2" align="left">6.9&#x20;&#xb1; 0.8</td>
<td align="left">4.2&#x20;&#xb1; 0.4 (Pure Al<sub>2</sub>O<sub>3(n)</sub>)</td>
<td rowspan="2" align="left">Microcracking, crack deflection, phase transformation toughening</td>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B1">Aguilar-Elgu&#xe9;zabal and Bocanegra-Bernal, (2013)</xref>
</td>
</tr>
<tr>
<td align="left">6.4&#x20;&#xb1; 0.4 (Pure 3Y-TZP)</td>
</tr>
<tr>
<td align="left">Al<sub>2</sub>O<sub>3</sub> platelets</td>
<td align="left">25&#xa0;wt%</td>
<td align="left">(Ce,Y)-TZP</td>
<td align="left">Sintered at 1,500&#xb0;C, 2&#xa0;h</td>
<td align="left">IF</td>
<td align="left">11.3&#x20;&#xb1; 0.4</td>
<td align="left">7.2&#x20;&#xb1; 0.5 (3Y-TZP)</td>
<td align="left">Phase transformation toughening, microcracking, denomination coupled toughening, crack deflection, bridging and pull-out</td>
<td align="left">
<xref ref-type="bibr" rid="B126">Santos et&#x20;al. (2021)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">Al<sub>2</sub>O<sub>3</sub> &#x2b; SA6</td>
<td align="left">Al<sub>2</sub>O<sub>3</sub>: 0, 5,10, 15 vol%;</td>
<td rowspan="2" align="left">1Y6Ce-TZP</td>
<td rowspan="2" align="left">Pressureless sintering</td>
<td rowspan="2" align="left">IF</td>
<td rowspan="2" align="left">12.5</td>
<td rowspan="2" align="left">Not mentioned</td>
<td rowspan="2" align="left">Phase transformation toughening, crack deflection, crack bridging, microcracking</td>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B52">Gommeringer et&#x20;al. (2019)</xref>
</td>
</tr>
<tr>
<td align="left">SA6: 15, 10, 5, 0 vol%</td>
</tr>
<tr>
<td align="left">3Y-TZP</td>
<td align="left">0, 5, 10, 15, 20&#xa0;wt%</td>
<td align="left">Mica glass ceramic</td>
<td align="left">Two-stage heat treatment sequence</td>
<td align="left">IF</td>
<td align="left">3.6&#x20;&#xb1; 0.2</td>
<td align="left">0.8&#x20;&#xb1; 0.2 (mica glass ceramic)</td>
<td align="left">Phase transformation toughening</td>
<td align="left">
<xref ref-type="bibr" rid="B46">Gali et&#x20;al. (2018)</xref>
</td>
</tr>
<tr>
<td align="left">Nanocrystalline ZrO<sub>2</sub> (3Y)</td>
<td align="left">CaSiO<sub>3</sub>/ZrO<sub>2</sub> mole ratio of 80/20 (C8Z2), 60/40 (C6Z4), 40/60 (C4Z6)</td>
<td align="left">Micrometer sized &#x3b2;-CaSiO<sub>3</sub>
</td>
<td align="left">SPS</td>
<td align="left">IF</td>
<td align="left">4.08&#x20;&#xb1; 0.13 (C6Z4)</td>
<td align="left">1.54&#x20;&#xb1; 0.04 (&#x3b2;-CaSiO<sub>3</sub>)</td>
<td align="left">Few &#x3b2;-CaSiO<sub>3</sub> transformed into &#x3b1;-CaSiO<sub>3</sub>; the ZrO<sub>2</sub> phase showed a network structure in the matrix</td>
<td align="left">
<xref ref-type="bibr" rid="B93">Long et&#x20;al. (2008)</xref>
</td>
</tr>
<tr>
<td align="left">Needle-like ZnOw</td>
<td align="left">1, 3, 5, 10&#xa0;wt%</td>
<td align="left">Porous CaSO<sub>4</sub>/bioglass scaffolds</td>
<td align="left">SLS</td>
<td align="left">IF</td>
<td align="left">1.67&#x20;&#xb1; 0.04</td>
<td align="left">Not mentioned</td>
<td align="left">Whisker pull-out, crack bridging, crack deflection, crack branching</td>
<td align="left">
<xref ref-type="bibr" rid="B130">Shuai et&#x20;al. (2016)</xref>
</td>
</tr>
<tr>
<td align="left">&#x3b1;-Al<sub>2</sub>O<sub>3</sub>
</td>
<td align="left">5, 10, 15, 25, 50&#xa0;wt%</td>
<td align="left">&#x3b1;- CaSiO<sub>3</sub>
</td>
<td align="left">Sintered at 1,150&#xb0;C and 1,250&#xb0;C, 5&#xa0;h</td>
<td align="left">IF</td>
<td align="left">0.9&#x20;&#xb1; 0.1</td>
<td align="left">0.6&#x20;&#xb1; 0.12 (Pure &#x3b1;- CaSiO<sub>3</sub>)</td>
<td align="left">Forming new phase CaAl<sub>2</sub>O<sub>4</sub> from reaction of CaSiO<sub>3</sub> and Al<sub>2</sub>O<sub>3</sub>
</td>
<td align="left">
<xref ref-type="bibr" rid="B129">Shirazi et&#x20;al. (2014)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">Cs<sub>2</sub>O-stabilized leucite core particles</td>
<td rowspan="2" align="left">0.0&#x2013;2.0&#xa0;mol%</td>
<td rowspan="2" align="left">Commercial porcelain (VP); synthesized leucite-based porcelain (NP)</td>
<td rowspan="2" align="left">Vacuum fired (1,100&#xb0;C, 20min)</td>
<td rowspan="2" align="left">IF</td>
<td align="left">1.42&#x20;&#xb1; 0.21 (VP)</td>
<td align="left">0.85&#x20;&#xb1; 0.11 (VP)</td>
<td rowspan="2" align="left">Phase transformation toughening</td>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B121">Rasmussen et&#x20;al. (2004)</xref>
</td>
</tr>
<tr>
<td align="left">2.15&#x20;&#xb1; 0.33 (NP)</td>
<td align="left">1.51&#x20;&#xb1; 0.15 (NP)</td>
</tr>
<tr>
<td rowspan="2" align="left">AgNPs, PtNPs</td>
<td rowspan="2" align="left">500&#xa0;ppm</td>
<td rowspan="2" align="left">NS</td>
<td rowspan="2" align="left">Fired (vacuum: 730&#xa0;mmHg, 930&#xb0;C)</td>
<td rowspan="2" align="left">IF</td>
<td align="left">1.42&#x20;&#xb1; 0.02 (Pt-NS)</td>
<td rowspan="2" align="left">1.36&#x20;&#xb1; 0.03</td>
<td rowspan="2" align="left">Greater elasticity of the metal than the matrix glass; generation of hydrostatic stress</td>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B45">Fujieda et&#x20;al. (2012)</xref>
</td>
</tr>
<tr>
<td align="left">1.54&#x20;&#xb1; 0.05 (Ag-NS)</td>
</tr>
<tr>
<td rowspan="2" align="left">AgNPs</td>
<td rowspan="2" align="left">100, 200, 500, 1,000&#xa0;ppm (Ag100, Ag200, Ag500, Ag1000)</td>
<td rowspan="2" align="left">NS</td>
<td rowspan="2" align="left">Fired (vacuum: 730&#xa0;mmHg, 930&#xb0;C)</td>
<td rowspan="2" align="left">IF</td>
<td align="left">1.54&#x20;&#xb1; 0.05 (Ag500)</td>
<td rowspan="2" align="left">1.36&#x20;&#xb1; 0.03</td>
<td rowspan="2" align="left">Crack deflection, crack bridging</td>
<td rowspan="2" align="left">
<xref ref-type="bibr" rid="B136">Uno et&#x20;al. (2013)</xref>
</td>
</tr>
<tr>
<td align="left">1.51&#x20;&#xb1; 0.08 (Ag1000)</td>
</tr>
<tr>
<td rowspan="4" align="left">Non-metal</td>
<td align="left">CNT</td>
<td align="left">4&#xa0;wt%</td>
<td align="left">HA</td>
<td align="left">SPS</td>
<td align="left">IF</td>
<td align="left">2.40&#x20;&#xb1; 0.60</td>
<td align="left">1.25&#x20;&#xb1; 0.91 (HA)</td>
<td align="left">Interfacial shear strength and pull-out energy of CNT from the HA matrix</td>
<td align="left">
<xref ref-type="bibr" rid="B77">Lahiri et&#x20;al. (2010)</xref>
</td>
</tr>
<tr>
<td align="left">GPL</td>
<td align="left">0.81 vol%</td>
<td align="left">ZTA</td>
<td align="left">SPS</td>
<td align="left">SENB</td>
<td align="left">9.05&#x20;&#xb1; 0.55 (GPL/ZTA, 1,550&#xb0;C)</td>
<td align="left">6.46&#x20;&#xb1; 0.65 (Pure ZTA, 1,550&#xb0;C)</td>
<td align="left">Pull out, crack bridging, crack deflection</td>
<td align="left">
<xref ref-type="bibr" rid="B89">Liu et&#x20;al. (2012)</xref>
</td>
</tr>
<tr>
<td align="left">GNP</td>
<td align="left">0.5, 1.0, 1.5, 2.0&#xa0;wt%</td>
<td align="left">CaSiO<sub>3</sub>
</td>
<td align="left">HIP</td>
<td align="left">Nanoindentatio<italic>n</italic> experiments</td>
<td align="left">1.77&#x20;&#xb1; 0.05 (1&#xa0;wt% GNP)</td>
<td align="left">0.76&#x20;&#xb1; 0.18 (CaSiO<sub>3</sub>)</td>
<td align="left">Crack bridging, pull-out, branching and deflection</td>
<td align="left">
<xref ref-type="bibr" rid="B99">Mehrali et&#x20;al. (2014)</xref>
</td>
</tr>
<tr>
<td align="left">GO</td>
<td align="left">0-0.2&#xa0;wt%</td>
<td align="left">3Y-TZP</td>
<td align="left">Hot-press sintering</td>
<td align="left">IF</td>
<td align="left">8.95&#x20;&#xb1; 0.59 (0.1&#xa0;wt% GO)</td>
<td align="left">40.9% lower</td>
<td align="left">Crack deflection, crack bridging, GO put-out</td>
<td align="left">
<xref ref-type="bibr" rid="B142">Zhang et&#x20;al. (2020)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">Polymer</td>
<td align="left">PVA fibers</td>
<td align="left">2.5&#x2013;5&#xa0;wt%</td>
<td align="left">CPCs</td>
<td align="left">Set at room temperature (24&#xa0;h), immersed in PBS and placed on a shaker table set to 120&#xa0;rpm in an incubator (37&#xb0;C, 72&#xa0;h)</td>
<td align="left">Three-point flexural test</td>
<td align="left">WOF: 8.7&#x20;&#xb1; 2.5&#xa0;KJ&#xa0;m<sup>&#x2212;2</sup> (5&#xa0;wt% PVA fibers)</td>
<td align="left">WOF: 0.020&#x20;&#xb1; 0.008&#xa0;KJ&#xa0;m<sup>&#x2212;2</sup> (fiber free CPCs)</td>
<td align="left">Fiber bridging, crack deflection, frictional sliding</td>
<td align="left">
<xref ref-type="bibr" rid="B74">Kucko et&#x20;al. (2019)</xref>
</td>
</tr>
<tr>
<td align="left">PNIPAM-functionalized PVA fibers</td>
<td align="left">2.5&#xa0;wt%</td>
<td align="left">CPCs</td>
<td align="left">Set at room temperature (12&#xa0;h), then immersed in PBS (37&#xb0;C, 3&#xa0;days)</td>
<td align="left">Three-point flexural tests</td>
<td align="left">WOF&#x3e; 1500&#xa0;J&#xa0;m<sup>&#x2212;2</sup> (PVA)</td>
<td align="left">WOF&#x3c; 100J&#xb7;m<sup>&#x2212;2</sup> (CPCs)</td>
<td align="left">Thermoresponsive effect of PNIPAM to increase the fiber-matrix affinity of PVA fibers</td>
<td align="left">
<xref ref-type="bibr" rid="B114">Petre et&#x20;al. (2019)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">PICN</td>
<td align="left">Vita Enamic (commercial product)</td>
<td align="left">Not mentioned</td>
<td align="left">SEVNB</td>
<td align="left">1.09&#x20;&#xb1; 0.05</td>
<td align="left">Not mentioned</td>
<td align="left">Crack deflection, crack bridging</td>
<td align="left">
<xref ref-type="bibr" rid="B27">Della Bona et&#x20;al. (2014)</xref>
</td>
</tr>
<tr>
<td align="left">49.5&#xa0;wt% TEGDMA &#x2b;1&#xa0;wt% BPO &#x2b; Bis-GMA</td>
<td align="left">12.3&#x2013;18.4&#xa0;wt%</td>
<td align="left">ZrO<sub>2</sub>
</td>
<td align="left">Immersing ZrO<sub>2</sub> networks in the liquid polymer, polymerization under the atmospheric pressure by heat treatment (70&#xb0;C, 10&#xa0;h)</td>
<td align="left">SENB</td>
<td align="left">3.69&#x20;&#xb1; 0.15</td>
<td align="left">Not mentioned</td>
<td align="left">Polymer occupies pore sites, increased densification leads to reduction in the detrimental stress concentration</td>
<td align="left">
<xref ref-type="bibr" rid="B84">Li et&#x20;al. (2017)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">Others</td>
<td align="left">Si<sub>3</sub>N<sub>4</sub>
</td>
<td align="left">1, 3, 5&#xa0;wt%</td>
<td align="left">&#x3b2;-CaSiO<sub>3</sub>
</td>
<td align="left">Pressureless sintering</td>
<td align="left">SENB</td>
<td align="left">2.3 (3&#xa0;wt% Si<sub>3</sub>N<sub>4</sub>)</td>
<td align="left">1.1 (pure &#x3b2;-CaSiO<sub>3</sub>)</td>
<td align="left">Not mentioned</td>
<td align="left">
<xref ref-type="bibr" rid="B112">Pan et&#x20;al. (2015)</xref>
</td>
</tr>
<tr>
<td align="left">L- (&#x2b;)-Tar</td>
<td align="left">3, 3.5, 4, 4.3&#xa0;g/ml</td>
<td align="left">Brushite</td>
<td align="left">Set at room temperature (30min), then incubated in distilled water (37&#xb0;C, 24&#xa0;h)</td>
<td align="left">Three-point bending method</td>
<td align="left">0.6&#x20;&#xb1; 0.07 (0.5M L-(&#x2b;)-Tar at 4.3 powder-to-liquid ratio)</td>
<td align="left">Not mentioned</td>
<td align="left">L- (&#x2b;)-Tar can decrease the subunit size of brushite crystals</td>
<td align="left">
<xref ref-type="bibr" rid="B103">Moussa et&#x20;al. (2020)</xref>
</td>
</tr>
<tr>
<td rowspan="3" align="left">Multi-component</td>
<td align="left">Leucite</td>
<td align="left">0, 6, 15, 22 vol%</td>
<td align="left">Six porcelains<xref ref-type="table-fn" rid="Tfn1">
<sup>a</sup>
</xref>
</td>
<td align="left">Not mentioned</td>
<td align="left">SEPB</td>
<td align="left">1.23&#x20;&#xb1; 0.12 (porcelain A)</td>
<td align="left">0.71&#x20;&#xb1; 0.05 (porcelain Cb); 0.75&#x20;&#xb1; 0.08 (porcelain V)</td>
<td align="left">Crack deflection around leucite particles and clusters</td>
<td align="left">
<xref ref-type="bibr" rid="B18">Cesar et&#x20;al. (2005)</xref>
</td>
</tr>
<tr>
<td align="left">Needle-like fluorapatites</td>
<td align="left">0, 1, 3&#xa0;wt%</td>
<td align="left">Mica-based glass-ceramics</td>
<td align="left">Casting and subsequent heat treatment</td>
<td align="left">IF</td>
<td align="left">3.1&#x20;&#xb1; 0.3 (Glass 3)</td>
<td align="left">0.8&#x20;&#xb1; 0.1 (Glass 1)</td>
<td align="left">Frictional bridging and pullout toughening</td>
<td align="left">
<xref ref-type="bibr" rid="B141">Xiang et&#x20;al. (2007)</xref>
</td>
</tr>
<tr>
<td align="left">MgO</td>
<td align="left">0.5&#xa0;wt%</td>
<td align="left">Al<sub>2</sub>O<sub>3</sub>-glass composite</td>
<td align="left">Sintering at 1,400&#xb0;C for 2h, infiltrating the molten glass into the partially sintered alumina compact</td>
<td align="left">SENB</td>
<td align="left">5.12&#x20;&#xb1; 0.35 (MgO-Al<sub>2</sub>O<sub>3</sub>/glass)</td>
<td align="left">0.58&#x20;&#xb1; 0.13 (partially sintered Al<sub>2</sub>O<sub>3</sub>)</td>
<td align="left">Crack deflection, crack bowing</td>
<td align="left">
<xref ref-type="bibr" rid="B94">Luo et&#x20;al. (2002)</xref>
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="Tfn1">
<label>a</label>
<p>Six porcelains: A (Ceramco I/Dentsply), B (Ceramco II/Dentsitply), C (Finesse/Dentsply), D (d.Sign/Ivoclar), Cb (Cerabien/Noritake) and V (Vitadur Alpha/Vita).</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s2">
<title>2 Adding Reinforcing Filler as Second Phase to Ceramic Matrix</title>
<p>Concept of ductile-phase toughening is to introduce metal component, non-metal component or ductile polymers into a brittle matrix, like ceramic, to increase its toughness. The development of metal-toughened ceramic mainly associates with alumina (Al<sub>2</sub>O<sub>3</sub>) and zirconia (ZrO<sub>2</sub>), which could act as either matrix or reinforcement. And a large family of non-metal components used to toughen ceramic are nanocarbon materials, from one-dimensional to three-dimensional. Additionally, polymers infiltrated ceramics gain lots of attention recently. Apart from adding every type of fillers alone, combined materials of several types could also achieve the toughening purpose (<xref ref-type="fig" rid="F2">Figure&#x20;2</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Adding reinforcing fillers as second phase to toughen ceramics. <bold>(A)</bold>, <bold>(a)</bold> transmission electron micrograph showing the microstructure for Al<sub>2</sub>O<sub>3</sub> containing well-dispersed unstabilized ZrO<sub>2</sub> particles; <bold>(b&#x2013;d)</bold> scanning electron micrographs showing the microstructures of Al<sub>2</sub>O<sub>3</sub> containing well-dispersed PSZ single crystals, TZP agglomerates and Al<sub>2</sub>O<sub>3</sub>-ZrO<sub>2</sub> duplex structured composites, respectively (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>). <bold>(B)</bold> A schematic of the toughening mechanism in GPL toughened ceramic (<xref ref-type="bibr" rid="B89">Liu et&#x20;al., 2012</xref>). <bold>(C)</bold> Polymer-infiltrated-ceramic-network structure (<xref ref-type="bibr" rid="B24">Coldea et&#x20;al., 2013</xref>). <bold>(D)</bold> Thermoresponsive brushes facilitate effective reinforcement of calcium phosphate cements (<xref ref-type="bibr" rid="B114">Petre et&#x20;al., 2019</xref>). PSZ, partially stabilized zirconia; TZP, tetragonal zirconia polycrastal; GPL, graphene platelet.</p>
</caption>
<graphic xlink:href="fbioe-10-840372-g002.tif"/>
</fig>
<sec id="s2-1">
<title>2.1 Metal Oxide and Metal Reinforcements</title>
<p>In 1976, ZrO<sub>2</sub> was revealed to display high toughness (R. C. <xref ref-type="bibr" rid="B50">Garvie and Hannink, 1975</xref>), which ushered in a decade of exceptional ceramic toughening development, culminating in materials having toughness on the order of 20&#xa0;MPa m<sup>1/2</sup> (<xref ref-type="bibr" rid="B35">Evans, 1990</xref>). Undoped ZrO<sub>2</sub> displays three phases at different temperature: the monoclinic (m) phase of undoped ZrO<sub>2</sub> is thermodynamically stable at temperatures below 1,170&#xb0;C; it is a tetragonal (t) phase from 1,170 to 2,370&#xb0;C, and a cubic (c) phase above 2,370&#xb0;C until the melt occurs at 2,706&#xb0;C (<xref ref-type="bibr" rid="B44">French et&#x20;al., 1994</xref>). Because the t-to-m phase transformation in zirconia may be used to toughen the material and enhance its mechanical properties, it has sparked a lot of technological interest in zirconia and composites incorporating zirconia (<xref ref-type="bibr" rid="B59">Heuer, 1987</xref>).</p>
<p>Using ZrO<sub>2</sub> alone have the shortage of low-temperature degradation (LTD) (<xref ref-type="bibr" rid="B71">Kohorst et&#x20;al., 2012</xref>), so Al<sub>2</sub>O<sub>3</sub> are doped to exert synergistic effect. Two composite materials can be made&#x20;in the ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> system as follows: Al<sub>2</sub>O<sub>3</sub> reinforced with ZrO<sub>2</sub> particles and denominated as zirconia toughened alumina (ZTA), or ZrO<sub>2</sub> reinforced with Al<sub>2</sub>O<sub>3</sub> particles, named alumina toughened zirconia (ATZ) (<xref ref-type="bibr" rid="B108">Nevarez-Rascon et&#x20;al., 2009</xref>). According to the findings of De Aza et&#x20;al. (<xref ref-type="bibr" rid="B122">Ritchie, 1988</xref>; <xref ref-type="bibr" rid="B26">De&#x20;Aza et&#x20;al., 2002</xref>) and Gregori et&#x20;al. (<xref ref-type="bibr" rid="B53">Gregori et&#x20;al., 1999</xref>), the fracture toughness of the ceramic matrix material rose in both cases. ZTA can be considered a new generation of toughened ceramic, with toughness exceeding 12&#xa0;MPa m<sup>1/2</sup>, compared to 3&#xa0;MPa m<sup>1/2</sup> for commercial alumina ceramic. The inclusion of discrete zirconia grains in the alumina matrix as a second phase allows the former to behave intrinsically, that is, to undergo the t-to-m transformation or to remain in the metastable tetragonal state after cooling of the composites from fabrication temperatures (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>). ZTA is microstructurally separated into four classes by Wang et&#x20;al. (<xref ref-type="fig" rid="F2">Figure&#x20;2A</xref>) (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>): (I) alumina with dispersed unstabilized zirconia (<xref ref-type="fig" rid="F2">Figures 2A,a</xref>); (II) alumina with dispersed partially stabilized zirconia (PSZ) (<xref ref-type="fig" rid="F2">Figures 2A,b</xref>); (III) alumina with PSZ agglomerates (<xref ref-type="fig" rid="F2">Figures 2A,c</xref>); (IV) alumina-zirconia duplex structures (<xref ref-type="fig" rid="F2">Figures&#x20;2A,d</xref>).</p>
<p>Except for these basic forms of ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> materials, the shapes of both components could be altered, or other metal compounds could be added, to achieve better toughening effect. <xref ref-type="bibr" rid="B1">Aguilar-Elgu&#xe9;zabal and Bocanegra-Bernal (2013)</xref> investigated the fracture toughness of an Al<sub>2</sub>O<sub>3</sub>(n)-70&#xa0;wt% ZrO<sub>2</sub> (ZrO<sub>2</sub> with 3&#xa0;mol% yttria, TZ-3Y)n nanocomposite with addition of 2.5% Al<sub>2</sub>O<sub>3</sub> whiskers. The fracture toughness was enhanced 62, 28, and 7% over pure Al<sub>2</sub>O<sub>3</sub>, the composite without additions of whiskers, and pure TZ-3Y for medical applications, respectively. They achieved a maximum fracture toughness of 6.9&#xa0;MPa m<sup>1/2</sup> with an average grain size of 0.4&#x20;&#xb1; 0.17&#xa0;&#x3bc;m, and found microcracking, crack deflection and phase transformation toughening mechanisms could contribute to the improvement of fracture toughness. Additionally, the Al<sub>2</sub>O<sub>3</sub> whiskers did not affect other intrinsic properties during the toughening process. <xref ref-type="bibr" rid="B126">Santos et&#x20;al. (2021)</xref> not only added Al<sub>2</sub>O<sub>3</sub> in ZrO<sub>2</sub>, but also replaced the conventional tetragonal zirconia stabilized with 3&#xa0;mol% yttria (3Y-TZP) with ceria and yttria stabilized zirconia, namely (Ce, Y)-TZP. And this new composite received higher fracture toughness, elastic modulus and hardness than those obtained for 3Y-TZP. In the meantime, its values of Weibull modulus (m &#x3e; 10) and flexural strength (&#x3e; 950&#xa0;MPa) were similar to the 3Y-TZP ceramics, with high resistance to degradation in saliva, indicating adequate properties for dental application. They thought several different toughening mechanisms acting simultaneously in the material. Apart from the above ingredients of Santos et&#x20;al.&#x2019;s study, <xref ref-type="bibr" rid="B52">Gommeringer et&#x20;al. (2019)</xref> reinforced 1Y6Ce-TZP materials with different amounts of alumina and/or strontium hexaalumina by slip casting and pressureless sintering at different temperatures. Then these materials underwent accession of their mechanical properties, microstructure, phase composition, and low-temperature degradation stability, which showed that they exhibited a high fracture resistance of 10&#x2013;12&#xa0;MPa m<sup>1/2</sup>. Partial substitution of the alumina dispersion by strontium hexaaluminate can improve the strength, while pres.erving toughness, hardness and low-temperature degradation resistance. The residual alumina provides grain growth inhibition. In summary, the improvement of structure or/and composition of the second phase is helpful to the toughening of ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> ceramic.</p>
<p>ZrO<sub>2</sub> and Al<sub>2</sub>O<sub>3</sub> could also be added to toughen ceramics except for ZTA or ATZ. <xref ref-type="bibr" rid="B46">Gali et&#x20;al. (2018)</xref> investigated ZrO<sub>2</sub> toughened mica glass ceramics for dental restorations. It was recorded that mica glass ceramics with 20&#xa0;wt% yttria stabilized zirconia (YSZ) reached Vickers hardness of 9.2&#xa0;GPa, elastic modulus of 125&#xa0;GPa, indentation toughness of 3.6&#xa0;MPa m<sup>1/2</sup>, and chemical solubility of 30&#xa0;g/cm<sup>2</sup> (well below the permissible limit), respectively. The phenomenon of transformation toughening of YSZ was observed in enhancing the toughness properties of ceramic. Because of its osseointegration property, Calcium silicate (CaSiO<sub>3</sub>, CS), has been investigated as a bioactive biomaterial for bone tissue repair and replacement (<xref ref-type="bibr" rid="B99">Mehrali et&#x20;al., 2014</xref>). <xref ref-type="bibr" rid="B93">Long et&#x20;al. (2008)</xref> successfully fabricated &#x3b2;-CaSiO<sub>3</sub>/ZrO<sub>2</sub> (3Y) nanocomposites via spark plasma sintering. Adding ZrO<sub>2</sub> could enhance the phase transitional temperature of CaSiO<sub>3</sub> and inhibit its phase transition. When the &#x3b2;- CaSiO<sub>3</sub>/ZrO<sub>2</sub> mole ratio was 60/40, the fracture toughness and strength of the nanocomposites were as high as 4.08&#xa0;MPa m<sup>1/2</sup> and 395&#xa0;MPa, respectively. <xref ref-type="bibr" rid="B130">Shuai et&#x20;al. (2016)</xref> used zinc oxide whisker (ZnOw) to improve CaSO<sub>4</sub>/bioglass scaffolds which were prepared via selective laser sintering (SLS). And the ZnOw improved fracture toughness and compression strength significantly. The combination of several toughening mechanisms, including whiskers pull-out, crack bridging, crack deflection, and crack branching, might be attributed to the increase of mechanical characteristics. <xref ref-type="bibr" rid="B129">Shirazi et&#x20;al., (2014)</xref> investigated the effect of Al<sub>2</sub>O<sub>3</sub> on &#x3b1;-CaSiO<sub>3</sub> ceramic and found that 15&#xa0;wt% of Al<sub>2</sub>O<sub>3</sub> addition at 1,250&#xb0;C enhanced fracture toughness as well as hardness of CaSiO<sub>3</sub>.</p>
<p>Apart from ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> system, other reinforcement-ceramic matrix systems have also been studied. <xref ref-type="bibr" rid="B121">Rasmussen et&#x20;al. (2004)</xref> mixed core particles of cesium (Cs<sub>2</sub>O) -containing synthetic leucite with two cesium-free matrix porcelains, a commercial porcelain (VP) and a synthesized leucite-based porcelain (NP). The toughness of both types of composite materials was dependent on Cs<sub>2</sub>O content of the added core particles, and the ceramic containing 0.75&#xa0;mol% Cs<sub>2</sub>O reached a maximum toughness. The possible toughening mechanism was transformation toughening. <xref ref-type="bibr" rid="B94">Luo et&#x20;al. (2002)</xref> modified glass-infiltrated Al<sub>2</sub>O<sub>3</sub> with 0.5&#xa0;wt% MgO. And the fracture toughness of this composite (5.12&#xa0;MPa m<sup>1/2</sup>) is obviously higher than the partially sintered Al<sub>2</sub>O<sub>3</sub> (0.58&#xa0;MPa m<sup>1/2</sup>), MgO-modified partially sintered Al<sub>2</sub>O<sub>3</sub> (1.86&#xa0;MPa m<sup>1/2</sup>), or glass-infiltrated Al<sub>2</sub>O<sub>3</sub> (3.91&#xa0;MPa m<sup>1/2</sup>).</p>
<p>Most above mentioned second phases for toughening are metal compounds rather than metals alone. Besides, the research of <xref ref-type="bibr" rid="B45">Fujieda et&#x20;al. (2012)</xref> and <xref ref-type="bibr" rid="B136">Uno et&#x20;al. (2013)</xref> showed that metal nanocomposites (NPs) could also be used to increase the fracture toughness of ceramic. <xref ref-type="bibr" rid="B45">Fujieda et&#x20;al. (2012)</xref> found that the addition of silver (Ag) and platinum (Pt) NPs improved the mechanical properties, including the fracture toughness and the Young&#x2019;s modulus, of commercial ceramic. The fracture toughness of AgNPs was higher than that of PtNPs. This could be due to the difference in positive compressive stress generation, which is projected to be greater for silver due to its higher coefficient of thermal expansion. <xref ref-type="bibr" rid="B136">Uno et&#x20;al. (2013)</xref> researched the effects of adding AgNPs on the toughening of dental porcelain, Noritake Super (NS) Porcelain AAA. When the concentration of Ag in the solution was 500 and 1,000&#xa0;ppm (Ag500 and Ag1000), toughness values of 1.54&#xa0;MPa m<sup>1/2</sup> and 1.51&#xa0;MPa m<sup>1/2</sup> were observed, respectively, which were higher than that of the control (1.36&#xa0;MPa m<sup>1/2</sup>). The inclusion of Ag500 and Ag1000 NPs, on the other hand, resulted in a color shift. Some AgNPs remained nanoparticles, whereas others interacted with matrix elements and turned into silver ions. As a result of the ion exchange reaction and differential thermal expansion of the silver metal nanoparticles, a residual compressive stress was created. <xref ref-type="bibr" rid="B134">Swain S.K et&#x20;al. (2016)</xref> developed a novel biocompatible &#x3b2;-tricalcium phosphate (&#x3b2;-TCP)-based composited by reinforcing ceramic matrix with 30 vol% of a biodegradable iron-magnesium (Fe-Mg) metallic phase, scilicet &#x3b2;-TCP-15Fe15&#xa0;Mg and &#x3b2;-TCP-24Fe6&#xa0;Mg (vol%) composites. Both these composites had increasing mechanical properties.</p>
</sec>
<sec id="s2-2">
<title>2.2&#x20;Non-Metal Reinforcements</title>
<sec id="s2-2-1">
<title>2.2.1 Nanacarbon</title>
<p>Nanocarbon materials have ever-increasing applications in ceramic toughening (<xref ref-type="bibr" rid="B131">Siddiqui et&#x20;al., 2018</xref>), for displaying a special set of characteristics, namely high elasticity modulus, specific thermophysical, electrophysical and sorption properties (<xref ref-type="bibr" rid="B38">Falcao and Wudl, 2007</xref>). According to their spatial structures, nanocarbon materials can be classified as one-dimensional, two-dimensional and three-dimensional materials (<xref ref-type="bibr" rid="B61">Hirsch, 2010</xref>).</p>
<p>One of the representatives of one-dimensional carbon structures is carbon nanotubes (CNTs), possessing a tubular structure made by rolling single/multi-layer graphite sheets. Large specific surface areas (50&#x2013;1,315&#xa0;m<sup>2</sup> g<sup>&#x2212;1</sup>), a high aspect ratio (as they have their diameters at the nano-scale but their lengths, are, by contrast, at the micron-scale), high tensile strength, high resilience, and flexibility are its typical properties (<xref ref-type="bibr" rid="B30">Dong et&#x20;al., 2012</xref>). On the basis of this physical structure, carbon nanotubes can be single-walled carbon nanotubes (SWNTs) (single tube)&#x2014;or multi-walled carbon nanotubes (MWNTs) (concentric cylinders of carbon) (T. F. <xref ref-type="bibr" rid="B76">Kuo et&#x20;al., 2001</xref>; <xref ref-type="bibr" rid="B3">Akasaka et&#x20;al., 2006</xref>). <xref ref-type="bibr" rid="B77">Lahiri et&#x20;al. (2010)</xref> synthesized MWNTs reinforced hydroxyapatite (HA) composite <italic>via</italic> spark plasma sintering. The fracture toughness and elastic modulus increased by 92 and 25%, respectively, compared to the HA matrix without CNT, which is due to the uniform distribution of 4&#xa0;wt% CNTs in the HA matrix, good interfacial bonding and fine HA grain size. It was explained that interfacial shear strength and pull-out energy of MWNTs from HA contributed to toughening.</p>
<p>Graphene is a leading nanomaterial of two-dimensional carbonaceous materials (<xref ref-type="bibr" rid="B5">Allen et&#x20;al., 2010</xref>). Compared to monolayer graphene, graphene platelets (GPLs), also referred as graphene nanoplatelets (GNPs), graphene nanosheets (GNS), or multilayer graphene nanosheets (MGN), are formed by several layers of graphene with thickness of up to100&#xa0;nm (<xref ref-type="bibr" rid="B131">Siddiqui et&#x20;al., 2018</xref>). GPLs have not only a large specific surface area, but also two dimensional high aspect ratio, as well as outstanding mechanical properties, which make them excellent potential nanofillers in composite materials (<xref ref-type="bibr" rid="B90">Liu Y et&#x20;al., 2013</xref>). For dental ceramics, <xref ref-type="bibr" rid="B89">Liu et&#x20;al. (2012)</xref> carried out a study on graphene platelet/zirconia-toughened alumina (GPL/ZTA) composites, which were sintered at different temperatures <italic>via</italic> spark plasma sintering. Measured by the single-edge notched beam method, it is found that at 1,550&#xb0;C, GPL/ZTA composites reached almost full density, maximum fracture toughness (with 40% improvement) and hardness. Multi-toughening mechanisms, such as pull out, bridging and crack deflection, were observed. In the bone repair area, <xref ref-type="bibr" rid="B99">Mehrali et&#x20;al. (2014)</xref> reinforced CaSiO<sub>3</sub> ceramic with graphene nanoplatelets (GNPs) using hot isostatic pressing (HIP) method at 1,150&#xb0;C. The homogeneous distribution of 1&#xa0;wt% GNP in the CaSiO<sub>3</sub> matrix, fine CaSiO<sub>3</sub> grain size and high densification helped to increase the fracture toughness, brittleness index and hardness by 130, 40 and 30%, respectively, in contrast to the CaSiO<sub>3</sub> matrix without GNPs. Similar to <xref ref-type="bibr" rid="B89">Liu et&#x20;al. (2012)</xref>, the toughening mechanisms also included crack bridging, pull-out, branching and deflection.</p>
<p>An important derivative of graphene is graphene oxide (GO), consisting of graphene sheets covered with oxygen-based functional groups (<xref ref-type="bibr" rid="B120">Raslan et&#x20;al., 2020</xref>). Utilized in dental ceramic toughening, <xref ref-type="bibr" rid="B142">Zhang et&#x20;al. (2020)</xref> distributed GO uniformly in 3Y-ZrO<sub>2</sub> powders, forming the C-O-Zr bond during the sintering process. As a result, the fracture toughness increased 40.9% (8.95&#x20;&#xb1; 0.59&#xa0;MPa m<sup>1/2</sup>) when adding 0.1&#xa0;wt% GO, and the flexural strength improved up to 200% (1,489.96&#x20;&#xb1; 35.71&#xa0;MPa) when adding 0.15&#xa0;wt% GO, in comparison to raw 3Y-ZrO<sub>2</sub> ceramics. The toughening mechanisms, namely crack deflection, crack bridging, and GO put-out are&#x20;found.</p>
</sec>
<sec id="s2-2-2">
<title>2.2.2 Polymer</title>
<p>Calcium phosphate cements (CPCs) are a class of injectable bone substitute bioceramics (<xref ref-type="bibr" rid="B74">Kucko et&#x20;al., 2019</xref>). To toughen this kind of bioceramic, <xref ref-type="bibr" rid="B74">Kucko et&#x20;al. (2019</xref>, <xref ref-type="bibr" rid="B75">2020</xref>) added surface-modified poly (vinyl alcohol) (PVA) fibers to CPCs and improved toughness and flexural strength of CPCs by more than 435-fold and 3-fold, respectively. The fiber-matrix affinity is thought to be paramount in designing highly toughened CPCs. So, the surface of PVA fibers was modified to improve their hydrophilicity and affinity to the CPC matrix, which facilitated energy dissipation during fracture of CPCs. Furthermore, other crack-arresting mechanisms may also play a significant role in mechanically reinforcing CPCs, because the fracture toughness improved significantly even for CPCs reinforced with fibers of lengths greater than their critical fiber embedment length. The surface of PVA fibers could be further modified with environmentally responsive materials to improve their ceramic toughening effect. <xref ref-type="bibr" rid="B114">Petre et&#x20;al. (2019)</xref> functionalized the surface of PVA fibers with thermoresponsive poly (N-isopropylacrylamide) brushes of tunable thickness to enhance simultaneously fiber dispersion and fiber-matrix affinity. At temperatures above their lower critical solution temperature of 32&#xb0;C, these brushes shifted from hydrophilic to hydrophobic. This dual thermoresponsive shift favored fiber dispersion throughout the hydrophilic CPCs (at 21&#xb0;C) and toughened these cements when reaching their hydrophobic state (at 37&#xb0;C). And fibers at 37&#xb0;C showed nearly double reinforcement efficacy than that of 21&#xb0;C.</p>
<p>Different from conventional dispersed-filler toughened ceramics, a kind of dual-phase material consists of two continuous interpenetrating networks, namely polymer infiltrated ceramic network (PICN) material, has been developed to emulate the properties and physical properties of natural teeth (<xref ref-type="bibr" rid="B98">Mainjot et&#x20;al., 2016</xref>). PINCs can be sorted as interpenetrating phase composites, which possess a three-dimensional interconnected geometry. The two continuous networks in PICNs are porous pre-sintered ceramic networks and infiltrated polymers (commonly resin for dental applications), which are shown in <xref ref-type="fig" rid="F1">Figure&#x20;1</xref> (<xref ref-type="bibr" rid="B24">Coldea et&#x20;al., 2013</xref>). Crack propagation is often limited in PICNs due to interfacial crack deflection, which is caused by the existence of two linked phases. By bridging the cracks introduced to the other phase, the phase with the higher strain to failure improves fracture resistance (<xref ref-type="bibr" rid="B62">Horvitz et&#x20;al., 2002</xref>; <xref ref-type="bibr" rid="B106">Nalla et&#x20;al., 2003</xref>). Furthermore, <xref ref-type="bibr" rid="B41">Feng et&#x20;al. (2003)</xref> found that the reinforcing phase could distribute stresses more efficiently in all directions in interpenetrating networks. Released in 2012, Vita Enamic (Vita Zahnfabrik, Bad S&#xe4;ckingen, Germany) is the successful representative of commercial PICN, consisting of 86&#xa0;wt% or 75&#xa0;vol% inorganic phase and 14&#xa0;wt% or 25&#xa0;vol% organic phase (<xref ref-type="bibr" rid="B133">Swain M. V. et&#x20;al., 2016</xref>). <xref ref-type="bibr" rid="B27">Della Bona et&#x20;al. (2014)</xref> examined the microstructure and fracture toughness (K<sub>Ic</sub>) of Vita Enamic, <italic>via</italic> scanning electron microscopy (SEM) and V-notched-beam test, respectively. The microstructure was shown in <xref ref-type="fig" rid="F3">Figure&#x20;3</xref> and the K<sub>Ic</sub> was 1.09&#x20;&#xb1; 0.05&#xa0;MPa m<sup>1/2</sup>. <xref ref-type="bibr" rid="B31">El Zhawi et&#x20;al. (2016)</xref> tested the resistance to fatigue fracture and wear of Vita Enamic and used step-stress accelerated life testing to show that failure could only be found under very high loads (&#x3e;1000&#xa0;N). The result inferred that it was unlike for the Enamic posterior crowns to experience early clinical abrupt fractures, which may only happen under extremely high traumatic loads when the radius of the antagonist cusp was relatively small. <xref ref-type="bibr" rid="B133">Swain M. V et&#x20;al. (2016)</xref> investigated seven kinds of PICN materials, whose single edge V-notched bend (SEVNB) fracture toughness varied from 0.82 to 4.94&#xa0;MPa m<sup>1/2</sup>. And they indicated that factors influencing the extent of the&#x20;crack included the residual stress in the resins, the bonding quality with the ceramic matrixes, the extent of polymeric conversion of the monomer or oligomer, as well as the yield stress and strain to failure of the bridging polymer. <xref ref-type="bibr" rid="B84">Li et&#x20;al. (2017)</xref> fabricated a polymer-infiltrated zirconia ceramic for dental crown restoration, with zirconia network porosity varying from 46.3 to 34.7% and the relevant polymer content ranging from 18.4&#xa0;wt% to 12.3&#xa0;wt%. At pre-sintered temperature was 1,150&#xb0;C, the facture toughness was 3.69&#x20;&#xb1; 0.15&#xa0;MPa&#xa0;m<sup>1/2</sup>, about twice or three times higher than those of the polymer-infiltrated feldspar ceramics.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Toughening ceramics by coating, chemical and thermal surface treatments. <bold>(A)</bold> Monoclinic ZrO<sub>2</sub> and SiO<sub>2</sub> particle coating, toughening highly translucent ZrO<sub>2</sub>. <bold>(a&#x2013;d)</bold> scanning electron micrographs, <bold>(e&#x2013;h)</bold> Zr and Si elemental mapping of samples coated with mZrO<sub>2</sub>/SiO<sub>2</sub> and heat treated at 1,500&#xb0;C (<xref ref-type="bibr" rid="B137">Uno et&#x20;al., 2020</xref>). <bold>(B)</bold> Ion-exchange toughened lithium disilicate glass-ceramic. Changing tendencies of VIF toughness of the glass-ceramic with increasing <bold>(a)</bold> the ion-exchange time and <bold>(b)</bold> the depth of Li<sup>&#x2b;</sup>/Na<sup>&#x2b;</sup> exchange obtained, at 450, 385 and 315&#xb0;C, respectively, in a pure NaNO<sub>3</sub> bath (<xref ref-type="bibr" rid="B86">Li et&#x20;al., 2020</xref>). <bold>(C)</bold> Scanning electron microscope fractographs of the lithium disilicate glass-ceramic: <bold>(a,c)</bold> in annealing state; <bold>(b,d)</bold> tempered in 250&#xb0;C silicone oil. Reproduced with permission from <xref ref-type="bibr" rid="B82">Li et&#x20;al. (2021)</xref>. VIF, Vickers indentation fracture.</p>
</caption>
<graphic xlink:href="fbioe-10-840372-g003.tif"/>
</fig>
</sec>
<sec id="s2-2-3">
<title>2.2.3 Others</title>
<p>On the periodic table of the elements, silicon and carbon are both on the fourth group, which indicates that silicon may have similar effect as carbon and could also be used in ceramic toughening. Silicon nitride (Si<sub>3</sub>N<sub>4</sub>) is a kind of ceramics with high performance characterized by fracture toughness, high wear resistance and low coefficient of friction (<xref ref-type="bibr" rid="B115">Pezzotti, 2019</xref>). <xref ref-type="bibr" rid="B112">Pan et&#x20;al. (2015)</xref> doped different content of Si<sub>3</sub>N<sub>4</sub> in &#x3b2;-CaSiO<sub>3</sub> ceramics at the sintering temperature ranging from 1,000&#xb0;C to 1,150&#xb0;C. Through being oxidized to form SiO<sub>2</sub>, Si<sub>3</sub>N<sub>4</sub> can be successfully used as sintering additive. And with 3&#xa0;wt% Si<sub>3</sub>N<sub>4</sub> addition, the &#x3b2;-CaSiO<sub>3</sub> ceramics sintered at 1,100&#xb0;C got fracture toughness of 2.3&#xa0;MPa m<sup>1/2</sup>, flexural strength of 157.2&#xa0;MPa and hardness of 4.4&#xa0;GPa, which was much higher than that of pure &#x3b2;-CaSiO<sub>3</sub> ceramics (1.1&#xa0;MPa m<sup>1/2</sup>, 41.1&#xa0;MPa and 1.0&#xa0;GPa).</p>
<p>In organic compounds, chirality is a very important property, which seems to also play a role in ceramic toughening materials. <xref ref-type="bibr" rid="B103">Moussa et&#x20;al. (2020)</xref> showed that the addition of homochiral L-(&#x2b;)-tartaric acid (Tar) increased the mechanical properties of&#x20;brushite bioceramics by decreasing their crystal size, following the&#x20;classic Hall-Petch strengthening effect; however, D-(-)-tartaric acid displayed the opposite effect. In comparison with brushite bioceramics without additives, adding L-(&#x2b;)-Tar increased the fracture toughness (0.3&#xa0;&#xa0;MPa m<sup>1/2</sup>) and compressive strength (26&#xa0;MPa) of this ceramic composite by 62 and 33%, respectively.</p>
</sec>
</sec>
<sec id="s2-3">
<title>2.3&#x20;Multi-Component Reinforcements</title>
<p>Both metal and non-metal reinforcements have their advantages&#x20;and disadvantages. Metal fillers like ZrO<sub>2</sub> or Al<sub>2</sub>O<sub>3</sub> have esthetic color but unexpected LTD or lower strength, while&#x20;non-metal fillers like nanocarbon materials possess high&#x20;elasticity modulus but susceptible to high sintering temperature. Proper combination of metal and non-metal components could be a promising approach to toughen bioceramics. <xref ref-type="bibr" rid="B18">Cesar et&#x20;al. (2005)</xref> modified six kinds of dental porcelains with the addition of leucite. Leucite (K<sub>2</sub>O&#xb7;Al<sub>2</sub>O<sub>3</sub>&#xb7;4SiO<sub>2</sub>) is a potassium&#x2013;aluminum&#x2013;silicate phase that can be incorporated into the dental porcelain in two ways: the incongruent melting of potash feldspar (K<sub>2</sub>O&#xb7;Al<sub>2</sub>O<sub>3</sub>&#xb7;6SiO<sub>2</sub>) or as a synthetic powder. For the materials investigated, the higher the leucite content in the porcelain, the higher the fracture toughness, implying that they would have better clinical performance. <xref ref-type="bibr" rid="B141">Xiang et&#x20;al. (2007)</xref> fabricated mica-based glass-ceramics containing needle-like fluorapatites. They found that the ceramics with higher fluorapatite content (mainly containing CaO and P<sub>2</sub>O<sub>5</sub>) presented higher fracture toughness and Vickers hardness, due to a large amount of needle-like fluorapatite crystals and the fine microstructure. <xref ref-type="bibr" rid="B94">Luo et&#x20;al. (2002)</xref> fabricated MgO-modified glass infiltrated Al<sub>2</sub>O<sub>3</sub> for CAD/CAM. There are two main functions of glass infiltration: the first is to eliminate almost all porosities, which are prone to crack initiation; secondly, the difference in the coefficients of thermal expansion between Al<sub>2</sub>O<sub>3</sub> and glass produces compressive stresses, further enhancing strength at the Al<sub>2</sub>O<sub>3</sub>-glass interface. Furthermore, MgO improved grain size uniformity, controlled grain growth, and promoted homogeneous wetting of Al<sub>2</sub>O<sub>3</sub> grains by the liquid through an alternation in interfacial energies, allowing the manufacture of high-density ceramics.</p>
</sec>
</sec>
<sec id="s3">
<title>3 Surface Modification of Ceramic</title>
<p>Surface modification mainly includes coating, chemical and thermal surface treatments (<xref ref-type="bibr" rid="B68">Kelly et&#x20;al., 1996</xref>) (<xref ref-type="fig" rid="F3">Figure&#x20;3</xref>).</p>
<p>Coating is also an important and widely used method in surface modification. Based on the toughening mechanism of strengthened glass, where the outer surface is compressed to impede breakage because of the outside stress, <xref ref-type="bibr" rid="B137">Uno et&#x20;al. (2020)</xref> used a dispersion containing mZrO<sub>2</sub> and SiO<sub>2</sub> as a surface coating agent for partially stabilized zirconia (PSZ). When the crystal phase changed from tetragonal to monoclinic, the mZrO<sub>2</sub> underwent volume change to generate a compressive stress layer on the material&#x2019;s surface. The SiO<sub>2</sub> serves as a binder to improve wettability and to accelerate the sintering of mZrO<sub>2</sub>.</p>
<p>Because many (but not all) ceramic and glass structures collapse due to surface imperfections, and surface compressive stresses must be exceeded before cracks can propagate, this approach permits treated structures to withstand higher loads before failing (<xref ref-type="bibr" rid="B68">Kelly et&#x20;al., 1996</xref>). Ion-exchange has become a major method for chemical toughening, the mechanism of which could be attributed to &#x201c;stuffing effect&#x201d;&#x2014;&#x2014;exchange of smaller alkaline metal ions in glasses with larger ones from molten salt baths can cause residual compressive stresses on the surfaces at temperatures below the glass transition temperatures (Tg), resulting in significant toughening of the glasses under the condition without sacrificing their light transmittance (translucency) (<xref ref-type="bibr" rid="B86">Li et&#x20;al., 2020</xref>). This mechanism indicates that ion-exchange is suitable for ceramics containing glass (glass-ceramics), dual-phase materials consisting of glassy matrix and embedded crystalline phases (<xref ref-type="bibr" rid="B28">Deubener et&#x20;al., 2018</xref>). They could combine the attractive properties of crystalline ceramics with those of glasses. Ion-exchange has been a popular way to strengthen monolithic silicate glasses containing alkaline oxides (<xref ref-type="bibr" rid="B42">Fillery and Lange, 2007</xref>; <xref ref-type="bibr" rid="B66">Jiang et&#x20;al., 2017</xref>). In Li et&#x20;al.&#x2019;s study (<xref ref-type="bibr" rid="B86">Li et&#x20;al., 2020</xref>), a multi-component lithium disilicate (LD) glass-ceramic with interlocking microstructure consisting of rod-like LD crystals and glassy matrix was ion-exchanged over wide temperature and time range in pure NaNO<sub>3</sub> or mixed NaNO<sub>3</sub> and KNO<sub>3</sub> baths below the glass transition temperature. Moreover, an experimental dual ion exchange toughening treatment was developed for feldspathic porcelains that surpassed the toughening of a single ion treatment and survived air abrasion (<xref ref-type="bibr" rid="B68">Kelly et&#x20;al., 1996</xref>).</p>
<p>Thermal treatment could also effectively toughen glass ceramics. <xref ref-type="bibr" rid="B82">Li et&#x20;al. (2021)</xref> toughened lithium disilicate (LD) glass-ceramic by tempering processes, which were conducted by heating the bar-like and disc-like specimens to a temperature below the dynamic softening point, and then rapid cooling in&#x20;silicone oil with different temperatures ranging from room-temperature to 300&#xb0;C to regulate the cooling rate. The specimens were effectively toughened, but the bar-like specimen displayed obvious anisotropy in fracture toughness, attributed to the &#x201c;edge cooling effect&#x201d; of the specimens with uneven geometry.</p>
<p>Comparing the chemical and thermal toughening methods, the former has the particular benefit of efficiently toughening glass-ceramic products of nearly any geometry and thickness (<xref ref-type="bibr" rid="B29">Donald, 1989</xref>), which is critical for many types of medical devices with customized geometries and thicknesses. However, this toughening effect could be susceptible to contact damage during service (<xref ref-type="bibr" rid="B55">Gy, 2008</xref>), or it will be completely lost in clinical practice by surface grinding during the manufacture of devices, like dental restorations, owing to the small micron level case depth of ion-exchange (<xref ref-type="bibr" rid="B43">Fischer et&#x20;al., 2008</xref>). On the contrary, the thermal tempering could create significantly deeper surface layers with residual compressive stresses (millimeter level), making the toughening effect less susceptible to contact damage (<xref ref-type="bibr" rid="B39">Fan et&#x20;al., 2016</xref>). Unfortunately, it was observed that the residual stresses created by fast cooling were geometry-dependent, and that they might vary in different directions as a result of differences in heat exchange conditions caused by different geometries (<xref ref-type="bibr" rid="B4">Al-Amleh et&#x20;al., 2014</xref>). Therefore, mechanical anisotropy of the tempered glass-ceramics would emerge from these geometry-dependent residual stresses, lowering their mechanical reliability.</p>
</sec>
<sec id="s4">
<title>4 Improving Manufacturing Processes</title>
<p>The fabrication of ceramics is concerned with powder preparation, green forming and the densification processes (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>): (I) powder preparation processes include mechanical mixing, sol-gel processes, partial chemical methods, chemical vapor deposition (CVD) process, rapid solidification, hydrothermal oxidation, wear of ZrO<sub>2</sub> milling media, etc. (II) forming methods mainly involve regular sintering, spark plasma sintering (SPS) (<xref ref-type="bibr" rid="B56">Han et&#x20;al., 2017</xref>), hot pressing, hot isostatic pressing and so&#x20;on.</p>
<p>Considering optimization of powder preparation processes, grain sizes could affect mechanical properties of ceramics. Larger particles undergo the martensitic t-to-m transformation more quickly than smaller particles in partially stabilized ZrO<sub>2</sub> and Al<sub>2</sub>O<sub>3</sub>-ZrO<sub>2</sub> composites (<xref ref-type="bibr" rid="B58">Heuer et&#x20;al., 1982</xref>). By decreasing the corresponding grain sizes and enhancing the homogeneity of the phase dispersion, the mechanical characteristics of ZrO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub> dispersion ceramics may be significantly improved. <xref ref-type="bibr" rid="B9">Bartolom&#xe9; et&#x20;al. (2016)</xref> prepared nanoparticles with an intraparticular phase distribution of Zr<sub>(1-x)</sub>Al<sub>x</sub>O<sub>(2-x/2)</sub> and (&#x3b3;-,&#x3b4;-)Al<sub>2</sub>O<sub>3</sub> by the simultaneous gas phase condensation of CO<sub>2</sub> laser co-vaporized (CoLAVA) zirconia and alumina raw powders. In general, the CoLAVA nanoparticles are spherically shaped, narrowly size-distributed, crystalline, and merely softly agglomerated by weak van der Waals forces. And fracture toughness of the CoLAVA composite significantly exceeds the ones of the wet mechanically mixed Al<sub>2</sub>O<sub>3</sub>/ZrO<sub>2</sub> reference powder (WM) by 45%, and reaches levels of 6.8&#xa0;MPa&#x20;m<sup>1/2</sup>.</p>
<p>In addition to particle sizes, degree of crystallization also affects ceramic toughness, which could be referred to as crystallization toughening. <xref ref-type="bibr" rid="B128">Serbena et&#x20;al. (2015)</xref> employed stoichiometric lithium disilicate glasses as a model system, which were crystallized using two-stage heat treatments that were carefully developed and controlled to yield varied crystallized volume fractions while maintaining a constant grain size of around 12&#xa0;&#x3bc;m. The fracture toughness of a completely crystalline sample improves about fivefold, from 0.75 to 3.5&#xa0;MPa m<sup>1/2</sup>. Crack deflection, crack bowing and trapping, and crack bridging are three methods that contribute to toughening.</p>
<p>Regarding the densification of materials, sintering methods influence the final properties and microstructure of the obtained material (<xref ref-type="bibr" rid="B19">Chaim, 2008</xref>; <xref ref-type="bibr" rid="B108">Nevarez-Rascon et&#x20;al., 2009</xref>; <xref ref-type="bibr" rid="B37">Faga et&#x20;al., 2012</xref>). <xref ref-type="bibr" rid="B97">Magnani and Brillante (2005)</xref> found that post-hot isostatic pressing treatment resulted in the formation of a small amount of monoclinic phase in Al<sub>2</sub>O<sub>3</sub>-ZrO<sub>2</sub> composites that decreased fracture toughness. <xref ref-type="bibr" rid="B51">Gil-Flores et&#x20;al. (2020)</xref> densified ATZ nanocomposites via nonconventional microwave sintering technology at relatively low temperatures (1,200 and 1,300&#xb0;C). The results indicated that the density increased as the sintering temperature was higher, which lead to improved mechanical properties, reaching a maximum fracture toughness (5.7&#x20;&#xb1; 0.3&#xa0;MPa m<sup>1/2</sup>) and hardness (18.4&#x20;&#xb1; 0.4&#xa0;GPa).</p>
</sec>
<sec id="s5">
<title>5 Toughening Mechanisms</title>
<p>In short, the major toughening mechanism of ceramics is to absorb energy of crack initiation or propagation to impede ceramic fracture. Different toughening methods have their specific mechanisms, but may also share similar mechanisms, vice versa, one toughening method typically contains several mechanisms at the same time (<xref ref-type="fig" rid="F4">Figure&#x20;4</xref>).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Toughening mechanisms in ceramic composites. <bold>(A)</bold> Representation of stress-induced phase transformation toughening process (<xref ref-type="bibr" rid="B116">Piconi and Maccauro, 1999</xref>). <bold>(B)</bold> A typical representation of strengthening and toughening by fibers. <bold>(a,c)</bold> represent two views of crack in a body being perturbed by fibers, <bold>(b,d)</bold> represents the see-through image of the body presented in <bold>(a,c)</bold> (<xref ref-type="bibr" rid="B131">Siddiqui et&#x20;al., 2018</xref>). <bold>(C)</bold> Reinforcing mechanisms of low-dimensional nanomaterials (LDNs) in bioactive ceramics. <bold>(a,c)</bold> scanning electron micrographs and <bold>(b,d)</bold> schematic diagram showing the pull-out, crack bridging, crack deflection and crack tip shielding mechanisms (<xref ref-type="bibr" rid="B49">Gao et&#x20;al., 2017</xref>).</p>
</caption>
<graphic xlink:href="fbioe-10-840372-g004.tif"/>
</fig>
<sec id="s5-1">
<title>5.1&#x20;Fine-Grained Toughening</title>
<p>The underlying toughening mechanism of controlling grain size is mainly fine-grained toughening. The reinforcement fillers located at the grain boundary provide a pinning effect, which can not only inhibit grain growth but also promote filler dispersion (<xref ref-type="bibr" rid="B67">Karthiselva et&#x20;al., 2018</xref>). The toughening effect of fine-grain reinforcement is quite obvious according to the Hall-Petch formula. And the vital factors influencing the efficiency of fine-grained toughening include the content of second phase, the geometric shape, as well as the temperature and impurities (<xref ref-type="bibr" rid="B91">Liu et&#x20;al., 2020</xref>).</p>
</sec>
<sec id="s5-2">
<title>5.2&#x20;Stress-Induced Phase Transformation Toughening</title>
<p>Transformation toughening mainly occurs in ceramics consisting of ZrO<sub>2</sub>, and could sometimes happen for other components as well. When an external tensile stress is applied to a crack tip, metastable tetragonal ZrO<sub>2</sub> inclusions scattered in a ceramic matrix are known to convert to their thermodynamically stable monoclinic form (R. C. <xref ref-type="bibr" rid="B50">Garvie and Hannink, 1975</xref>; <xref ref-type="bibr" rid="B78">Lange, 1982</xref>). The stress to initiate transformation is lower than the fracture stress, and transformation happens preferentially and proceeds until the transformable t phase is exhausted (<xref ref-type="bibr" rid="B57">Hannink et&#x20;al., 2000</xref>). Therefore, the phase transformation, which is accompanied by a volume expansion of 4% and shear strain of 6%, creates a compressive stress that slows and eventually stops the crack propagation, while the strain energy associated with any net shear component of the transformation strain in the transformation zone contributes an effective increase in the energy of fracture (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>). The contribution of stress-activated transformation, &#x2206;K<sub>cT</sub>, to the toughness is usually expressed in the form<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mi mathvariant="bold">&#x394;</mml:mi>
<mml:msub>
<mml:mi mathvariant="bold">K</mml:mi>
<mml:mrow>
<mml:mi mathvariant="bold">c</mml:mi>
<mml:mi mathvariant="bold-italic">T</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi mathvariant="bold-italic">&#x3b7;</mml:mi>
<mml:msup>
<mml:mi mathvariant="bold-italic">E</mml:mi>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msub>
<mml:mi mathvariant="bold-italic">e</mml:mi>
<mml:mi mathvariant="bold-italic">T</mml:mi>
</mml:msub>
<mml:msub>
<mml:mi mathvariant="bold-italic">V</mml:mi>
<mml:mi mathvariant="bold-italic">f</mml:mi>
</mml:msub>
<mml:msup>
<mml:mi mathvariant="bold-italic">h</mml:mi>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>/</mml:mo>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="bold-italic">&#x3bd;</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>Where &#x3b7; is a factor depending on the zone shape at the crack tip and the nature of the stress field in that zone, E<sup>&#x2217;</sup> the effective modulus of the material, e<sub>T</sub> the dilatational strain, V<sub>f</sub> the transformed volume fraction of the particles, h the width of the transformation zone from the crack surface, and &#x3bd;the Poisson ratio (<xref ref-type="bibr" rid="B57">Hannink et&#x20;al., 2000</xref>).</p>
</sec>
<sec id="s5-3">
<title>5.3 Microcrack Toughening</title>
<p>Microcracks in ceramic materials can be subdivided as residual microcracks and stress-induced microcracks. Take the ZrO<sub>2</sub> ceramic as an example, the residual microcracks are those caused by the volume expansion and shear strain associated with t-to-m phase transformation mentioned in section above, while the stress-induced microcracks are from the volume expansion and shear strain associated with the subsequent stress-induced transformation during fracture process. During phase transformation, tangential stresses are generated around the transformed m-ZrO<sub>2</sub> particles. Microcrack toughening mainly relies on two shielding sources. One is the main-crack and microcrack interaction which causes stress redistribution ahead of the main-crack tip and thus lowers the continuum stiffness of the microcracked material. The other is the stress redistribution at the main-crack tip due to the release of residual stress when a microcrack is nucleated (<xref ref-type="bibr" rid="B64">Hutchinson, 1987</xref>). Microcracks form at the intersections of the fillers and the matrix as a result of this, which can absorb fracture energy by extending in the stress field of a propagating crack or deflecting the propagating crack (<xref ref-type="bibr" rid="B139">Wang and Stevens, 1989</xref>). Microcracks behind the main-crack tip provide the most shielding, while microcracks ahead of the main-crack tip contribute no shielding effect. What&#x2019;s more, compressive normal residual stress may attribute to an anti-shielding effect at the main-crack tip, which should be paid attention for the design of ceramic materials (<xref ref-type="bibr" rid="B20">Chen, 2005</xref>).</p>
</sec>
<sec id="s5-4">
<title>5.4 Crack Deflection and Crack Bifurcation</title>
<p>Crack deflection refers to the condition that the reinforcement fillers will generally deflect the crack at a certain angle when the crack propagates in the ceramic matrix and meets fillers (<xref ref-type="bibr" rid="B145">Zou et&#x20;al., 2018</xref>). So the fracture energy of crack propagating is consumed and the rate of crack propagating is reduced, as a result, the fracture toughness is increased (<xref ref-type="bibr" rid="B145">Zou et&#x20;al., 2018</xref>). Specifically, deflection toughening occurs whenever interaction between the crack front and the minor phase produces a non-planar crack, subject to a stress intensity lower than that experienced by the corresponding planar crack. And the non-planar crack arises either from the existence of weakened interfaces or from residual strains present in the material. Considering shape, the rod of high aspect ration is the most effective morphology to deflect propagating cracks, which could account for four-fold increases in fracture toughness (<xref ref-type="bibr" rid="B36">Faber and Evans, 1983</xref>).</p>
<p>Crack bifurcation occurs at the matrix-filler interface. The primary crack runs vertically, whereas the bifurcation crack runs parallel to the matrix-filler interface. When a micro-crack forms at the end of the interface and can be deflected at 90&#xb0; to extend to the ceramic matrix, the bifurcation crack is ended, which helps stress propagation at the corner. The new fracture then spreads parallel to the primary crack (<xref ref-type="bibr" rid="B21">Cheng et&#x20;al., 2018</xref>).</p>
</sec>
<sec id="s5-5">
<title>5.5 Crack Bridging and Pull-Out</title>
<p>Take advantage of crack bridging, several types of discontinuous reinforcing fillers have been successfully applied to form toughened ceramics including second-phase whiskers (<xref ref-type="bibr" rid="B12">Becher, 1990</xref>), platelets (<xref ref-type="bibr" rid="B11">Becher, 1991</xref>), as well as elongated, plate-like, and large matrix grains (<xref ref-type="bibr" rid="B60">Himsolt et&#x20;al., 1979</xref>; <xref ref-type="bibr" rid="B105">Mussler et&#x20;al., 1982</xref>). Crack bridging happens during ceramic cracking. The two ends of the reinforcement filler link the crack surface and begin to distort as the distance between the two crack walls grows, which imposes a closure force on the crack. The two segments of fillers are tightly linked to the matrix throughout the process and consume the crack propagation energy.</p>
<p>Before reaching the reinforcement&#x2019;s deformation limit, a pull-out may occur, consuming the fracture energy, or filler-matrix debonding with crack bridging may occur. Defects in this mechanism alter the mobility of fillers, which in turn affects energy dissipation (<xref ref-type="bibr" rid="B91">Liu et&#x20;al., 2020</xref>). The extent of pullout of discontinuous reinforcement is commonly quite limited, which is due both to the short length of such phases and the fact that bonding and clamping stresses often discourage pull out. However, pullout cannot be ignored as even short pull-out lengths contribute to the toughness achieved (<xref ref-type="bibr" rid="B81">Li, 2012</xref>).</p>
</sec>
</sec>
<sec id="s6">
<title>6 Current Challenges and Future Outlook</title>
<p>Although large amount of toughening strategies have been proposed for biomedical ceramic, there still exists challenges needed to be overcome, such as biodegradability and biocompatibility, as well as trade-off between toughness and strength. These challenges indicate that there is broad developing space of ceramic toughening for biomedical use, and future outlook is put forward to shed light on this attractive research&#x20;field.</p>
<sec id="s6-1">
<title>6.1 Influence of Fracture Toughness of Ceramic on Degradability, <italic>In Vitro</italic> and <italic>In Vivo</italic> Performance</title>
<p>Biomedical applications require ceramic materials with excellent biocompatibility to ensure device acceptance and patient safety, which is the prior recommend compared with toughness. First, no short- or long-term cytotoxicity is expected for biomaterials. <xref ref-type="bibr" rid="B110">Nieto et&#x20;al. (2017)</xref> reviewed studies on graphene reinforced ceramic matrix composites (GNP-CMCs) and found all studies showed no cytotoxic effects induced by GNPs. After evaluating the long-term biocompatibility of a new ZTA, mainly in terms of DNA damage, mutagenicity and cancerogenetic potential in mammalian cells, <xref ref-type="bibr" rid="B96">Maccauro et&#x20;al. (2009)</xref> found no long-term carcinogenic effect. Besides, toughening ceramic strategies should not affect the function of cells. In <italic>in&#x20;vitro</italic> tests, the &#x3b2;-TCP-15Fe15Mg composite fabricated by <xref ref-type="bibr" rid="B134">Swain S. K et&#x20;al. (2016)</xref> was shown to support the attachment and proliferation of osteoblast and endothelial cells and the cells exhibited characteristic markers for bone formation and angiogenesis, respectively. For the second phase addition strategy, proper concentration of reinforcement is a critical factor to be controlled. According to the evaluation of <xref ref-type="bibr" rid="B143">Zhang et&#x20;al. (2019)</xref>, hydroxyapatite ceramic with 3&#xa0;wt% ZrO<sub>2</sub> showed good cell viability and no cytotoxicity, and the mouse bone mesenchymal stem cells continued to proliferate on the ceramic surface observed for 5&#xa0;days. <xref ref-type="bibr" rid="B130">Shuai et&#x20;al. (2016)</xref> doped ZnO whisker (ZnOw) in the ceramic matrix, and cells attachment, extension and interconnection behavior of MG63 cells were enhanced with the ZnOw increasing from 1&#xa0;wt% to 5&#xa0;wt%. However, when ZnOw were further increased to 10&#xa0;wt%, a sharp decrease of cell expansion degree was observed.</p>
<p>Biocompatibility of toughened ceramic has been studied mostly in terms of <italic>in&#x20;vitro</italic> cytocompatibility, but fewer <italic>in vivo</italic> analysis has been conducted, which is a vital process before being considered for clinical applications. <xref ref-type="bibr" rid="B114">Petre et&#x20;al. (2019)</xref> investigated the <italic>in vivo</italic> biocompatibility of both resorbable and nonresorbable PVA fiber-reinforced calcium phosphate cements. And these fibers were well dispered in the matrix without inducing inflammatory responses or other adverse reactions. Moreover, the inclusion of PVA fibers did not negatively affect the ingrowth of new bone into the PVA fiber-reinforced cements. The <italic>in vivo</italic> test of <xref ref-type="bibr" rid="B74">Kucko et&#x20;al. (2019)</xref> also showed that PVA fibers do not compromise the excellent osteocompatibility of calcium phosphate cements. Nevertheless, further <italic>in vivo</italic> studies should be performed to investigate the biocompatibility of various types of toughened ceramics in more detail.</p>
<p>Degradability is significant for biomaterials like bone substitutes, which determines the final repair effect of bio-implants; while biomaterials for other applications, such as dental restorations or artificial joint, require to be stable rather than degradable. Therefore, most degradability tests of toughened ceramic are conducted in bone substitute ceramic composites. Significantly influenced by mechanical properties of biomaterials, degradability is mostly tested by soaking materials in the simulated body fluid (SBF) (<xref ref-type="bibr" rid="B141">Xiang et&#x20;al., 2007</xref>). Toughening strategies, especially second phase addition may&#x20;change the degradation rate and degradability. <xref ref-type="bibr" rid="B83">Li et&#x20;al. (2015)</xref> found that the addition of ZnO or ZrO<sub>2</sub> decreased the&#x20;degradation rate, and improved the degradability of wollastonite. Similarly, <xref ref-type="bibr" rid="B40">Feng et&#x20;al. (2014)</xref> observed the degradation rate of calcium silicate ceramic scaffolds decreased with the increase of hydroxyapatite whisker content. Moreover, toughened bone substitute ceramic possesses the apatite-forming ability in SBF, and osteoblast-like cells spread well on the scaffolds and proliferated with increasing culture time (<xref ref-type="bibr" rid="B40">Feng et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B99">Mehrali et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B83">Li et&#x20;al., 2015</xref>). However, soaking in the SBF tests only the <italic>in&#x20;vitro</italic> bio-degradability, and <italic>in vivo</italic> degradability should also be increasingly studied in the future.</p>
</sec>
<sec id="s6-2">
<title>6.2&#x20;Trade-Off Between Toughness and Strength, as Well as Esthetic and Function</title>
<p>Toughness and strength are typically exclusive properties, which means the improvement of toughness usually comes with a decrease in strength (<xref ref-type="bibr" rid="B79">Launey and Ritchie, 2009</xref>). If the decrease of strength is within proper range, the toughening methods are still acceptable, because of the following reasons. On the one hand, the strength of most ceramic is high enough to satisfy clinical requirements. On the other hand, the best strength is not the highest but the strength that matches those of the human tissues. Therefore, toughening is a more essential issue than strengthening for ceramics of biomedical applications and receives extensive attentions. Toughening strategies from second phase addition, surface modification to manufacturing process improvement have been studied to solve this problem. Considering different clinical application scenarios, ceramics for biomedical applications could be classified as esthetic-demanding and non-esthetic-demanding: dental restorations are the representatives of the former type of ceramic, in which esthetic sometimes is even paid more attention than toughness; while the latter, such as dental implants and artificial joints which could not be seen, mainly requires promising mechanical properties, especially toughness. What&#x2019;s more, studies concerning esthetic, including color and translucency, are still limited. Adding reinforcing fillers as second phase to ceramic matrix is one of the most widely used strategies, and even commercial ceramic products have been fabricated based on this strategy; in contrast, surface modification strategies gain less studies and applications. Toughening based on ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> system or mica glass ceramics (<xref ref-type="bibr" rid="B47">Gali and Kumar, 2019</xref>), and using ion-exchange (chemical methods) tends to preserve excellent esthetics, while adding colorful fillers like AgNPs (<xref ref-type="bibr" rid="B45">Fujieda et&#x20;al., 2012</xref>) would affect ceramic color. For non-esthetic demanding applications, high toughness is the first consideration, which is fine achieved by fiber/whisker-shape (<xref ref-type="bibr" rid="B1">Aguilar-Elgu&#xe9;zabal and Bocanegra-Bernal, 2013</xref>) or nanocarbon adding (<xref ref-type="bibr" rid="B131">Siddiqui et&#x20;al., 2018</xref>).</p>
</sec>
<sec id="s6-3">
<title>6.3 Other Challenges</title>
<p>The ZrO<sub>2</sub>-Al<sub>2</sub>O<sub>3</sub> system is well studied and used in clinic, such as dental restorations and implants, as well as femoral heads and hip joints. Although the addition of Al<sub>2</sub>O<sub>3</sub> helps to improve the problem of low-temperature degradation (LTD) of ZrO<sub>2</sub>, it should still be paid enough attention during application, because most medical devices are applied in humid body environment which promotes degradation (<xref ref-type="bibr" rid="B109">Nguyen et&#x20;al., 2009</xref>; <xref ref-type="bibr" rid="B14">Borchers et&#x20;al., 2010</xref>). LTD refers to the t-to-m transformation of ZrO<sub>2</sub> induced by hydrothermal aging in the humid environments, and with LTD, the energy barrier for t-to-m transformation is decreased due to incorporation of water constituents into zirconia lattice (<xref ref-type="bibr" rid="B54">Guo, 2004</xref>). Non-metal materials, especially nanocarbon materials, show their potential as reinforcement fillers due to excellent mechanical properties. Nevertheless, the application of nanocarbon materials still faces some challenges. Firstly, it&#x2019;s difficult for nanocarbon to disperse in ceramic matrix due to its large specific surface area, surface energy, van der Waals forces caused by the intermolecular electrical dipole moment, and interactions between functional groups, as well as easy aggregation and entanglement properties (<xref ref-type="bibr" rid="B87">Liang et&#x20;al., 2018</xref>). Secondly, the interface invasion between nanocarbon and ceramic is regarded unsuitable due to the differences in surface tension and density. Furthermore, it is difficult to determine the temperature during sintering, because nanocarbon can be destroyed at high temperatures when interface bonding is diminished. What&#x2019;s more, measurement of ceramic matrix composites with nanocarbon is not homogeneous, for the composites are extremely anisotropic (<xref ref-type="bibr" rid="B91">Liu et&#x20;al., 2020</xref>). Therefore, combination of different types of second phase materials may be a possible approach to exert synergistic effect and, in the meantime, diminish their disadvantages.</p>
<p>In addition to the type of second phase, the complex transition zone between ceramic matrix and reinforcement fillers, namely the interface, also play an important role on toughening, which is the basis of toughening mechanisms, such as pull-out and crack bridging. Proper interface strength is neither too weak nor too strong, so that the toughening mechanisms could dissipate energy during the loading process appropriately (<xref ref-type="bibr" rid="B88">Liu J et&#x20;al., 2013</xref>; <xref ref-type="bibr" rid="B119">Ramirez et&#x20;al., 2014</xref>; <xref ref-type="bibr" rid="B2">Ahmad et&#x20;al., 2015</xref>).</p>
<p>
<xref ref-type="bibr" rid="B26">De Aza et&#x20;al. (2002)</xref> pointed out that the idea of a well-defined stress limit, toughness (K<sub>IC</sub>), must incorporate the concept of a threshold (K<sub>I0</sub>) under which crack propagation does not occur. The K<sub>IC</sub> usually used only represents the resistance to fast fracture. However, ceramic materials are susceptible to slow crack propagation at K<sub>I</sub> values under K<sub>IC</sub>, which is attributed to stress assisted corrosion at the crack tip, or any pre-existing defect in ceramic. The combined effect of high stresses at the crack tip and the presence of water or body fluid induce crack propagation in a subcritial manner (<xref ref-type="bibr" rid="B23">Chevalier et&#x20;al., 1999</xref>). This slow crack propagation threshold may represent an intrinsic property of ceramic that gives information of its mechanical properties more realistic than the widely used toughenss, which represents only fast crack growth. The concept of slow crack propagation reminds us to pay attention to evaluations of mechanical properties, which may overestimate the behavior of ceramics.</p>
</sec>
<sec id="s6-4">
<title>6.4 Future Outlook</title>
<p>Microscopic building blocks, weak interfaces, and architecture are responsible for the extraordinary qualities of highly mineralized natural materials. Bio-inspired concepts could pave the way for new techniques to improve the toughness of brittle materials with enticing features but limited uses due to their brittleness (<xref ref-type="bibr" rid="B140">Wondraczek et&#x20;al., 2011</xref>). These new materials show that bio-inspired techniques can be used to achieve both strength and toughness, which are normally mutually exclusive qualities (<xref ref-type="bibr" rid="B123">Ritchie, 2011</xref>). Nature transforms brittleness into toughness through three &#x201c;overarching features&#x201d;: (I) stiff and hard construction blocks are separated by (II) weaker interfaces, which are organized in (III) specialized architectures (<xref ref-type="bibr" rid="B100">Mirkhalaf et&#x20;al., 2014</xref>). It may seem contradictory to make a material tougher by adding weak interfaces, but it appears to be a ubiquitous and powerful method in natural materials. <xref ref-type="bibr" rid="B100">Mirkhalaf et&#x20;al. (2014)</xref> used three-dimensional laser engraving to create weak interfaces inside the bulk of glass and then infiltrating the interfaces with polyurethane. The crack is channeled towards toughening configurations by the weak interfaces, which obstructs its propagation. The technology produces a bio-inspired glass that is 200&#x20;times tougher than non-engraved, &#x201c;intact&#x201d; glass (namely bulk glass, which was not engraved, but that is not devoid of the surface defects typical to glass exposed to air). Glass and ceramic are both brittle materials, therefore, above mentioned bio-inspired method could also be attempted in ceramics. These bio-inspired concepts have opened new pathways to improving the toughness of ceramics, and in the recent years, increasing numbers of synthetic composites inspired from biological materials have emerged (<xref ref-type="bibr" rid="B104">Munch et&#x20;al., 2008</xref>; <xref ref-type="bibr" rid="B33">Espinosa et&#x20;al., 2011</xref>). This is one of the development directions of the future, with still limited researches, which calls for more investigating efforts.</p>
</sec>
</sec>
<sec id="s7">
<title>7 Conclusion</title>
<p>Ceramic encounters limitations during biomedical applications due to its brittleness. Various extrinsic toughening strategies have been proposed to deal with this problem, including adding reinforcing fillers as second phase, surface modification and manufacture processes optimization. Proper concentration of metal or/and non-metal components, with different shapes, could both be added in ceramic matrix to enhance toughness, which is the mainstream of ceramic toughening, especially in the biomedical area. Apart from traditional dispersed-filler composites, dual phase interpenetrating networks and bio-inspired &#x201c;block and mortar&#x201d; architectures have also been developed to achieve better toughening effects. Surface coating, chemical and thermal toughening approaches could influence some depth of superficial layer to impede ceramic breakage, but each exhibit limitations. Furthermore, preparation of raw materials and forming methods of ceramic should be improved, as well. Underlying toughening mechanisms of these approaches include fine-grained toughening, stress-induced phase transformation toughening, microcrack toughening, crack deflection and bifurcation, and crack bridging and pull-out. In the future, effective combination of several toughening strategies and mechanisms should be the potential direction to extend the application scope of ceramic in biomedicine.</p>
</sec>
</body>
<back>
<sec id="s8">
<title>Author Contributions</title>
<p>RB and QS wrote the original draft. RB, QS, YH and TY revised the manuscript. LP, YZ, LZ, WL, JD, ZZ reviewed the manuscript. YH, TY, and YW designed the work of review. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec id="s9">
<title>Funding</title>
<p>This work was funded by the National Key Research and Development Program of China (2020YFA0710401, 2021YFC2400403), the National Natural Science Foundation of China (51972005, U21A2055, 82101074, 51903003) and National Youth Top-notch Talent Support Program (QNBJ2019-3).</p>
</sec>
<sec sec-type="COI-statement" id="s10">
<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="s11">
<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>
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<sec id="s12">
<title>Glossary</title>
<def-list>
<def-item>
<term id="G1-fbioe.2022.840372">
<bold>Al</bold>
<sub>
<bold>2</bold>
</sub>
<bold>O</bold>
<sub>
<bold>3</bold>
</sub>
</term>
<def>
<p>alumina</p>
</def>
</def-item>
<def-item>
<term id="G2-fbioe.2022.840372">
<bold>AgNPs</bold>
</term>
<def>
<p>silver nanoparticles</p>
</def>
</def-item>
<def-item>
<term id="G3-fbioe.2022.840372">
<bold>&#x3b2;-TCP</bold>
</term>
<def>
<p>beta-tricalcium phosphate</p>
</def>
</def-item>
<def-item>
<term id="G4-fbioe.2022.840372">
<bold>BPO</bold>
</term>
<def>
<p>benzoyl peroxide</p>
</def>
</def-item>
<def-item>
<term id="G5-fbioe.2022.840372">
<bold>Bis-GMA</bold>
</term>
<def>
<p>Bisphenol A glycidyl dimethacrylate</p>
</def>
</def-item>
<def-item>
<term id="G6-fbioe.2022.840372">
<bold>Cs</bold>
<sub>
<bold>2</bold>
</sub>
<bold>O</bold>
</term>
<def>
<p>cesium&#x20;oxide</p>
</def>
</def-item>
<def-item>
<term id="G7-fbioe.2022.840372">
<bold>(Ce,Y)-TZP</bold>
</term>
<def>
<p>cerium oxide (CeO<sub>2</sub>) and yttrium oxide (Y<sub>2</sub>O<sub>3</sub>) stabilized zirconia (ZrO<sub>2</sub>)</p>
</def>
</def-item>
<def-item>
<term id="G8-fbioe.2022.840372">
<bold>CaSiO</bold>
<sub>
<bold>3</bold>
</sub>
</term>
<def>
<p>calcium silicate</p>
</def>
</def-item>
<def-item>
<term id="G9-fbioe.2022.840372">
<bold>CaSO</bold>
<sub>
<bold>4</bold>
</sub>
</term>
<def>
<p>calcium sulfate</p>
</def>
</def-item>
<def-item>
<term id="G10-fbioe.2022.840372">
<bold>CNT</bold>
</term>
<def>
<p>carbon nanotube</p>
</def>
</def-item>
<def-item>
<term id="G11-fbioe.2022.840372">
<bold>CPCs</bold>
</term>
<def>
<p>calcium phosphate cements</p>
</def>
</def-item>
<def-item>
<term id="G12-fbioe.2022.840372">
<bold>GNP</bold>
</term>
<def>
<p>graphene nanoplatelets</p>
</def>
</def-item>
<def-item>
<term id="G13-fbioe.2022.840372">
<bold>GO</bold>
</term>
<def>
<p>graphene&#x20;oxide</p>
</def>
</def-item>
<def-item>
<term id="G14-fbioe.2022.840372">
<bold>GPL</bold>
</term>
<def>
<p>graphene platelet</p>
</def>
</def-item>
<def-item>
<term id="G15-fbioe.2022.840372">
<bold>HA</bold>
</term>
<def>
<p>hydroxyapatite</p>
</def>
</def-item>
<def-item>
<term id="G16-fbioe.2022.840372">
<bold>HIP</bold>
</term>
<def>
<p>hot isostatic pressing</p>
</def>
</def-item>
<def-item>
<term id="G17-fbioe.2022.840372">
<bold>IF</bold>
</term>
<def>
<p>indentation fracture method</p>
</def>
</def-item>
<def-item>
<term id="G18-fbioe.2022.840372">
<bold>K</bold>
<sub>
<bold>lc</bold>
</sub>
</term>
<def>
<p>fracture toughness</p>
</def>
</def-item>
<def-item>
<term id="G19-fbioe.2022.840372">
<bold>L-(&#x2b;)-Tar</bold>
</term>
<def>
<p>homochiral L-(&#x2b;)-tartaric&#x20;acid</p>
</def>
</def-item>
<def-item>
<term id="G20-fbioe.2022.840372">
<bold>NS</bold>
</term>
<def>
<p>Noritake Super Porcelain AAA (Noritake Dental Supply Co., Nagoya, Japan)</p>
</def>
</def-item>
<def-item>
<term id="G21-fbioe.2022.840372">
<bold>PtNPs</bold>
</term>
<def>
<p>platinum nanoparticles</p>
</def>
</def-item>
<def-item>
<term id="G22-fbioe.2022.840372">
<bold>PVA</bold>
</term>
<def>
<p>poly (vinyl alcohol)</p>
</def>
</def-item>
<def-item>
<term id="G23-fbioe.2022.840372">
<bold>PBS</bold>
</term>
<def>
<p>phosphate-buffered saline solution</p>
</def>
</def-item>
<def-item>
<term id="G24-fbioe.2022.840372">
<bold>PNIPAM</bold>
</term>
<def>
<p>poly(N-isopropylacrylamide)</p>
</def>
</def-item>
<def-item>
<term id="G25-fbioe.2022.840372">
<bold>PICN</bold>
</term>
<def>
<p>polymer infiltrated ceramic network</p>
</def>
</def-item>
<def-item>
<term id="G26-fbioe.2022.840372">
<bold>SPS</bold>
</term>
<def>
<p>spark plasma sintering</p>
</def>
</def-item>
<def-item>
<term id="G27-fbioe.2022.840372">
<bold>SA6</bold>
</term>
<def>
<p>strontium hexaaluminate</p>
</def>
</def-item>
<def-item>
<term id="G28-fbioe.2022.840372">
<bold>SLS</bold>
</term>
<def>
<p>selective laser sintering</p>
</def>
</def-item>
<def-item>
<term id="G29-fbioe.2022.840372">
<bold>SENB</bold>
</term>
<def>
<p>single-edge notched&#x20;beam</p>
</def>
</def-item>
<def-item>
<term id="G30-fbioe.2022.840372">
<bold>Si</bold>
<sub>
<bold>3</bold>
</sub>
<bold>N</bold>
<sub>
<bold>4</bold>
</sub>
</term>
<def>
<p>silicon nitride</p>
</def>
</def-item>
<def-item>
<term id="G31-fbioe.2022.840372">
<bold>SEVNB</bold>
</term>
<def>
<p>single-edge V-notched&#x20;beam</p>
</def>
</def-item>
<def-item>
<term id="G320-fbioe.2022.840372">
<bold>SEPB</bold>
</term>
<def>
<p>single-edge precracked beam</p>
</def>
</def-item>
<def-item>
<term id="G32-fbioe.2022.840372">
<bold>MgO</bold>
</term>
<def>
<p>magnesium&#x20;oxide</p>
</def>
</def-item>
<def-item>
<term id="G33-fbioe.2022.840372">
<bold>TEGDMA</bold>
</term>
<def>
<p>Tri(ethyleneglycol) dimethacrylate</p>
</def>
</def-item>
<def-item>
<term id="G34-fbioe.2022.840372">
<bold>WOF</bold>
</term>
<def>
<p>work of fracture</p>
</def>
</def-item>
<def-item>
<term id="G35-fbioe.2022.840372">
<bold>3Y-TZP</bold>
</term>
<def>
<p>3&#xa0;mol% yttria stabilized zirconia</p>
</def>
</def-item>
<def-item>
<term id="G36-fbioe.2022.840372">
<bold>1Y6Ce-TZP</bold>
</term>
<def>
<p>1&#xa0;mol% Y<sub>2</sub>O<sub>3</sub> &#x2b; 6&#xa0;mol% CeO<sub>2</sub> stabilized&#x20;ZrO<sub>2</sub>
</p>
</def>
</def-item>
<def-item>
<term id="G37-fbioe.2022.840372">
<bold>ZnOw</bold>
</term>
<def>
<p>zinc oxide whisker</p>
</def>
</def-item>
<def-item>
<term id="G38-fbioe.2022.840372">
<bold>ZTA</bold>
</term>
<def>
<p>zirconia-toughened alumina</p>
</def>
</def-item>
<def-item>
<term id="G371-fbioe.2022.840372">
<bold>ZrO</bold>
<sub>
<bold>2</bold>
</sub>
</term>
<def>
<p>zirconia</p>
</def>
</def-item>
</def-list>
</sec>
</back>
</article>