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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Chem.</journal-id>
<journal-title>Frontiers in Chemistry</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Chem.</abbrev-journal-title>
<issn pub-type="epub">2296-2646</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1036715</article-id>
<article-id pub-id-type="doi">10.3389/fchem.2023.1036715</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Chemistry</subject>
<subj-group>
<subject>Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Recent advances in lanthanide-doped up-conversion probes for theranostics</article-title>
<alt-title alt-title-type="left-running-head">Xu et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fchem.2023.1036715">10.3389/fchem.2023.1036715</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Xu</surname>
<given-names>Danyang</given-names>
</name>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Chenxu</given-names>
</name>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Wenjing</given-names>
</name>
<xref ref-type="fn" rid="fn1">
<sup>&#x2020;</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1743796/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Lin</surname>
<given-names>Bi</given-names>
</name>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Lv</surname>
<given-names>Ruichan</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1058843/overview"/>
</contrib>
</contrib-group>
<aff>
<institution>Engineering Research Center of Molecular and Neuro Imaging</institution>, <institution>Ministry of Education</institution>, <institution>School of Life Science and Technology</institution>, <institution>Xidian University</institution>, <addr-line>Xi&#x2019;an</addr-line>, <addr-line>Shaanxi</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/541104/overview">Preston Todd Snee</ext-link>, University of Illinois at Chicago, United States</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/1830826/overview">Yahong Jin</ext-link>, Guangdong University of Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/570248/overview">Mikhail Zamkov</ext-link>, Bowling Green State University, United States</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Ruichan Lv, <email>rclv@xidian.edu.cn</email>
</corresp>
<fn fn-type="equal" id="fn1">
<label>
<sup>&#x2020;</sup>
</label>
<p>These authors have contributed equally to this work</p>
</fn>
<fn fn-type="other">
<p>This article was submitted to Nanoscience, a section of the journal Frontiers in Chemistry</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>09</day>
<month>02</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>11</volume>
<elocation-id>1036715</elocation-id>
<history>
<date date-type="received">
<day>05</day>
<month>09</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>31</day>
<month>01</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Xu, Li, Li, Lin and Lv.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Xu, Li, Li, Lin and Lv</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Up-conversion (or anti-Stokes) luminescence refers to the phenomenon whereby materials emit high energy, short-wavelength light upon excitation at longer wavelengths. Lanthanide-doped up-conversion nanoparticles (Ln-UCNPs) are widely used in biomedicine due to their excellent physical and chemical properties such as high penetration depth, low damage threshold and light conversion ability. Here, the latest developments in the synthesis and application of Ln-UCNPs are reviewed. First, methods used to synthesize Ln-UCNPs are introduced, and four strategies for enhancing up-conversion luminescence are analyzed, followed by an overview of the applications in phototherapy, bioimaging and biosensing. Finally, the challenges and future prospects of Ln-UCNPs are summarized.</p>
</abstract>
<kwd-group>
<kwd>lanthanide-doped</kwd>
<kwd>probes for theranostics</kwd>
<kwd>up-conversion</kwd>
<kwd>up-conversion luminescence</kwd>
<kwd>biomedicine</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Rare earth-based nanomaterials have attracted attention due to their superior fluorescence properties. Because of their dense energy levels that enable complex electronic transitions, rare Earth elements have become a treasure house of luminescence (<xref ref-type="bibr" rid="B77">Li et al., 2015a</xref>; <xref ref-type="bibr" rid="B11">Binnemans, 2015</xref>). Rare earth-based nanomaterials require specific wavelength of excitation to photoluminesce (<xref ref-type="bibr" rid="B165">Tsang et al., 2015</xref>; <xref ref-type="bibr" rid="B4">Adachi, 2018</xref>; <xref ref-type="bibr" rid="B136">Quan et al., 2018</xref>; <xref ref-type="bibr" rid="B119">Mintz et al., 2019</xref>; <xref ref-type="bibr" rid="B120">Mir et al., 2020</xref>; <xref ref-type="bibr" rid="B47">Gierschner et al., 2021</xref>). The emission can be characterized as up-conversion or downconversion luminescence (<xref ref-type="bibr" rid="B141">Reddy et al., 2018</xref>). For example, Ln- UCNPs can be excited by infrared light to emit visible light. If modified properly, they can become good candidates for tumor diagnosis and treatment.</p>
<p>Phototherapy (PT) (<xref ref-type="bibr" rid="B80">Li et al., 2018</xref>; <xref ref-type="bibr" rid="B72">Lan et al., 2019</xref>; <xref ref-type="bibr" rid="B219">Zhen et al., 2019</xref>; <xref ref-type="bibr" rid="B187">Xie et al., 2020</xref>), as a new type of treatment with good targeting and low toxicity, is often classified as photodynamic therapy (PDT) or photothermal therapy (PTT). Phototherapy is gradually becoming an important supplement for tumor treatment. Therefore, Ln-UCNPs can serve as a substrate for composition with other materials for phototherapy, to aid surgical navigation, to enhance the precision of imaging, and for efficient treatment (<xref ref-type="bibr" rid="B145">Shanmugam et al., 2014</xref>; <xref ref-type="bibr" rid="B102">Liu et al., 2019a</xref>).</p>
<p>In addition to therapy, Ln-UCNPs also have potential for use in bioimaging and biosensing (<xref ref-type="bibr" rid="B211">Zhang et al., 2016</xref>; <xref ref-type="bibr" rid="B214">Zhang et al., 2019</xref>). Functionalized Ln-UCNPs can be applied in Computed Tomography (CT) and Magnetic Resonance Imaging (MRI) among others, which adds value to the bioimaging field (<xref ref-type="bibr" rid="B210">Zhang et al., 2011</xref>; <xref ref-type="bibr" rid="B151">Sun et al., 2013</xref>; <xref ref-type="bibr" rid="B86">Li et al., 2019</xref>). Regardless, Ln-UCNP-based biological imaging has shortcomings and there is significant room for improvement. Ln-UCNPs also perform well in biosensing (<xref ref-type="bibr" rid="B50">Guo et al., 2016</xref>; <xref ref-type="bibr" rid="B116">Mahata et al., 2017</xref>). Ln-UCNPs can be used as pH and temperature sensors as well as gas and DNA sensors, to name a few, due to temperature sensitivity and other optical properties. It is foreseeable that the use of Ln-UCNPs will expand in the sensor field (<xref ref-type="bibr" rid="B173">Wang et al., 2014a</xref>; <xref ref-type="bibr" rid="B26">Cui et al., 2014</xref>; <xref ref-type="bibr" rid="B30">Dong et al., 2015</xref>; <xref ref-type="bibr" rid="B125">Pan et al., 2017</xref>).</p>
<p>This manuscript reviews research on the synthesis, luminescence modulation, and the latest achievements in phototherapy, bioimaging and biosensing of Ln-UCNPs. Synthetic methods are summarized in <xref ref-type="sec" rid="s2">Section 2</xref>, research on luminescence modulation is outlined in <xref ref-type="sec" rid="s3">Section 3</xref>, and then applications for Ln-UCNPs in phototherapy, bioimaging and biosensing are introduced in <xref ref-type="sec" rid="s4">Section 4</xref>. Finally, the current challenges of Ln-UCNPs and their prospects for the future are discussed.</p>
</sec>
<sec id="s2">
<title>2 Synthesis methods of Ln-UCNPs</title>
<p>Many challenges concerning the morphology and performance of Ln-UCNPs must be addressed for successful application in biomedicine. Fortunately, many kinds of Ln-UCNPs have been synthesized that enable the potential for applications. Rare Earth luminescent materials have attracted much attention because of their flexibility and easy modulation. Different nanoparticles can be synthesized by controlling the reaction conditions; these include the temperature, pH, precursor concentrations, etc. Researchers have successively realized several luminescence mechanisms such as excited state absorption (ESA), energy transfer up-conversion (ETU), cooperative sensitization up-conversion (CSU), photon avalanche (PA), and energy transfer-mediated up-conversion (EMU). This section introduces the most common methods, specifically thermal decomposition and hydrothermal/solvothermal, as well as several other synthetic approaches. A brief comparison of these methods is provided in <xref ref-type="table" rid="T1">Table 1</xref>.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Typical methods of Ln-UCNPs synthesis (<xref ref-type="bibr" rid="B75">Li and Lin, 2010</xref>; <xref ref-type="bibr" rid="B31">Du et al., 2011</xref>; <xref ref-type="bibr" rid="B93">Lin et al., 2012</xref>).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Method</th>
<th align="center">Morphology</th>
<th align="center">Reaction condition</th>
<th align="center">Product stability</th>
<th align="center">Synthetic cost</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">Thermal decomposition</td>
<td align="center">Controllable</td>
<td align="center">Harsh</td>
<td align="center">Stable</td>
<td align="center">Higher</td>
</tr>
<tr>
<td align="center">Hydrothermal/solvothermal</td>
<td align="center">Controllable</td>
<td align="center">Simple</td>
<td align="center">Stable</td>
<td align="center">Lower</td>
</tr>
<tr>
<td align="center">Co-precipitation</td>
<td align="center">Uncontrollable</td>
<td align="center">Simple</td>
<td align="center">Stable</td>
<td align="center">Lower</td>
</tr>
</tbody>
</table>
</table-wrap>
<sec id="s2-1">
<title>2.1 Thermal decomposition method</title>
<p>The thermal decomposition method is the most facile to create high-quality Ln-UCNPs. Thermal decomposition is the process of pyrolyzing organometallic precursors in an organic solvent under an oxygen-free environment. In general, the precursors are organic salts of rare Earth ions, such as trifluoroacetate and acetate among others. Octadecene (ODE) is the most frequently used high-boiling organic solvent. Oleic acid (OA) and oleylamine (OM) can serve dual roles as solvents and as ligands that adsorbed onto the nanoparticles to control their size and shape. It is worth noting that the crystal nucleation and growth process that control the nanoparticle uniformity can be adjusted with the temperature, heating rate, and precursor concentrations during synthesis.</p>
<p>Yan and co-authors first synthesized LaF<sub>3</sub> crystals by thermal decomposition using a single-source precursor (<xref ref-type="bibr" rid="B213">Zhang et al., 2005</xref>). Later they pioneered the use of multi-source precursors to prepare high quality nanocrystals through thermal decomposition, which greatly promoted the development of Ln-UCNPs (<xref ref-type="bibr" rid="B202">Yin et al., 2010</xref>). Murray and collaborators studied the influence of reaction time and the ratio of sodium to lanthanide precursors on the morphology of &#x3b2;-NaYF<sub>4</sub>-based Ln-UCNPs in detail, thereby obtaining beautiful rare earth-based nanocrystals (<xref ref-type="bibr" rid="B200">Ye et al., 2010</xref>). We applied LnCl<sub>3</sub> (Ln &#x3d; Y and Er) as precursors in an OA and ODE mixture that was heated to a high temperature, next NH4F and NaOH were added to obtain core nanoparticles of NaYF<sub>4</sub>:Er. Finally Lu(CF<sub>3</sub>COO)<sub>3</sub> and CF<sub>3</sub>COONa mixed with NaYF<sub>4</sub>: Er were further processed under high temperature and oxygen-free environment to obtain stable NaYF<sub>4</sub>:x%Er@NaLuF4 (<xref ref-type="bibr" rid="B38">Feng et al., 2018</xref>).</p>
<p>Ln-UCNPs synthesized using the thermal decomposition method are highly monodisperse and uniform in shape. They also display greater up-conversion emission intensity; however, the syntheses are complicated and the products are lipophilic and not stable, which limits the application of thermal decomposition in Ln-UCNPs synthesis.</p>
</sec>
<sec id="s2-2">
<title>2.2 Hydrothermal/solvothermal method</title>
<p>The hydrothermal/solvothermal method is facile for synthesizing Ln-UCNPs under mild conditions at a low cost. Generally, hydrothermal syntheses are carried out in a reactor to provide a high-pressure environment. Simple rare Earth nitrates or chlorides are used as precursors for the preparation of Ln-UCNPs. The most common solvents are water, ethanol, glycol and other simple hydrophilic inorganic/organic solvents (<xref ref-type="bibr" rid="B138">Rafique et al., 2019</xref>). Li and co-workers introduced oleic acid into solvothermal synthesis. As an oleophilic organic solvent, it broadened the range of materials and structures that can be realized using this method (<xref ref-type="bibr" rid="B175">Wang et al., 2005</xref>). The selection of organic additives has a significant impact on the morphology and size of the product. Hydrophilic organic ligands that can adhere to the surface of products and inhibit particle aggregation can endow the nanocrystals with good hydrophilicity, biocompatibility, and functionalizability with biomolecules. It was reported that ethylene diamine tetra acetic acid (EDTA), polyvinyl pyrrolidone (PVP), hexadecyl trimethyl ammonium bromide (CTAB) and polyacrylic acid (PAA)/poly ethylenimine (PEI) as additives improve the morphology and dispersion of Ln-UCNPs (<xref ref-type="bibr" rid="B121">Mousavand et al., 2010</xref>; <xref ref-type="bibr" rid="B81">Li et al., 2020a</xref>). A mixed solution of Ln(NO<sub>3</sub>)<sub>3</sub>, Y:Yb:Tm &#x3d; 70:30:0.5, was used as a rare Earth precursor with EDTA as an organic additive. NaYF<sub>4</sub>: Yb<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup> were synthesized by high temperature and pressure in a reactor (<xref ref-type="bibr" rid="B188">Xu et al., 2020</xref>). The advantages of hydrothermal/solvothermal method include the potential for large-scale production. Moreover, the reaction is always carried out under closed conditions without harmful gas leakage, so it is environmentally friendly and non-toxic. However, these conditions also make it impossible to observe the crystal growth process, which impede the studies into the reaction mechanisms.</p>
</sec>
<sec id="s2-3">
<title>2.3 Co-precipitation methods</title>
<p>The products of the co-precipitation method are usually chemically homogeneous and uniformly distributed; however, the surfaces are rough and difficult to control. Coudret et al. obtained ultra-small Na(Gd-Yb)F<sub>4</sub>:Tm through an improved co-precipitation method (<xref ref-type="fig" rid="F1">Figure 1</xref>). In addition to the synthesis of specific precursors and microwave-assisted heating, the influence of oleic acid content on heating efficiency was discussed (<xref ref-type="bibr" rid="B6">Amouroux et al., 2019</xref>). In 2014, Liu and co-workers demonstrated a simpler co-precipitation method to prepare core-shell NaGdF4 nanoparticles doped with luminescent lanthanide ions that did not require precise control of the feeding rate of shell precursors. However, the large core-shell nanocrystals had a low up-conversion efficiency (<xref ref-type="bibr" rid="B170">Wang et al., 2014b</xref>). Jin and co-workers synthesized a near-infrared (NIR) fluorescence &#x201c;turn-on&#x201d; kit based on rare Earth ion-doped nanoparticles and gold nanoparticles, which created an HIV-1 based DNA detection system that was simple, homogeneous, and highly selective (<xref ref-type="bibr" rid="B224">Zhou et al., 2019</xref>). Chen and co-workers were the first to report the synthesis of CaS:Eu<sup>2&#x2b;</sup>,Sm<sup>3&#x2b;</sup> near infrared photostimulated luminescence nanocrystals by a high temperature co-precipitation method. The materials exhibited a fast response to stimuli over 800&#x2013;1,600&#xa0;nm (<xref ref-type="bibr" rid="B41">Gao et al., 2019</xref>). In conclusion, the application of the co-precipitation method creates products that have biomedical applications; however, they are limited by defects. Regardless, this simple process is conducive to industrial production.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Mixing and high-temperature heating steps are important processes in the controlled thermal coprecipitation synthesis of sub-5-nm Na(Gd&#x2212;Yb)F4:Tm. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B6">Amouroux et al., 2019</xref>) Copyright 2019: American Chemical Society].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g001.tif"/>
</fig>
</sec>
<sec id="s2-4">
<title>2.4 Other methods</title>
<p>In addition to the processes discussed previously, several novel methods have been developed for the synthesis of Ln-UCNPs. For instance, microemulsions and ionic liquids have been applied, and Ln-UCNPs have been prepared using microwave heating. The microemulsion method creates materials in droplets that contains the surfactant, cosurfactant, solvent and water. Few product nanoparticles are prepared this way; furthermore, the dispersion is poor because the growth of the particles is affected by the size of the micelle. Li and colleagues reported a method of microemulsion assisted synthesis of functionalized Ln-UCNPs. The nanoparticles was synthesized in a heterogeneous oil-water microemulsion phase, and the product had a high cross-section and adjustable pore size (<xref ref-type="bibr" rid="B27">Dai et al., 2020</xref>).</p>
<p>Microwave synthesis has unique properties, including increased speed and heating efficiency, which contributes to energy savings and environmental protection. It was reported that NaGdF<sub>4</sub>:Yb, Er can be directly synthesized using a microwave digestion/extraction system; furthermore, the produced have good biomedical application prospects (<xref ref-type="bibr" rid="B76">Li et al., 2012</xref>).</p>
</sec>
</sec>
<sec id="s3">
<title>3 Up-conversion luminescence modulation</title>
<p>Key issues concerning the optical properties of Ln-UCNPs include the small absorption cross-section, fluorescence quenching, and the electronic structure that may result in multiple emission lines despite excitation at a single wavelength. As a result, Ln-UCNPs should be classified according to the requirements of applications (<xref ref-type="bibr" rid="B84">Li et al., 2015b</xref>). In recent years, a series of Ln-UCNPs with enhanced up-conversion luminescence (UCL) have been obtained by adjusting the composition and structure. This provides a deeper understanding of the characteristics and nature of rare Earth luminescence and broadens the potential for applications (<xref ref-type="bibr" rid="B185">Wu et al., 2016</xref>; <xref ref-type="bibr" rid="B42">Garfield et al., 2018</xref>).</p>
<sec id="s3-1">
<title>3.1 Species and concentration of doping ions</title>
<p>Up-conversion is the process of converting low-energy photons into high-energy luminescence, which relies on energy transfer within the 4f electron manifold of the luminescent ions. Luminescence mechanisms include excited state absorption (ESA), energy transfer up-conversion (ETU), and cooperative sensitization up-conversion (CSU). The ESA process occurs within a single ion that continuously absorbs photons to create upconverted luminescence. The ETU process involved in a pair of neighboring rare Earth ions, a sensitizer as energy donor, and an activator as energy acceptor. After excitation, the ground state sensitizer ion becomes electronically excited, the energy from which is transmitted to activators. In turn the activator ion transitions to a higher electronic state, and then luminesces to the ground state. The CSU process requires at least three ion centers. Two of them are the same element that act as sensitizers. They can interact with activators simultaneously in the excited state, which in turn transfers energy to activators. Consequently, the doping of rare Earth ions is closely related to the up-conversion luminescence ability of the nanoparticles, and the luminescence intensity can be regulated by adjusting the species and concentration of rare Earth ions.</p>
<p>Ln-UCNPs are composed of activators and sensitizers within a matrix. For up-conversion, the matrix must have excellent optical properties and stability. The most studied are fluoride materials NaYF<sub>4</sub>, LaF<sub>3</sub>, LiYF<sub>4</sub>, and NaGdF<sub>4</sub> among others (<xref ref-type="bibr" rid="B171">Wang et al., 2011</xref>; <xref ref-type="bibr" rid="B97">Liu et al., 2012</xref>; <xref ref-type="bibr" rid="B170">Wang et al., 2014b</xref>; <xref ref-type="bibr" rid="B208">Zhang et al., 2015</xref>). To achieve up-conversion luminescence, the energy difference between at least three adjacent energy levels of the activator should be in close proximity. Therefore, Er<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup> and Ho<sup>3&#x2b;</sup> are the most important due to their step-like energy levels. Sensitizer ions are usually introduced due to the fact that the luminous efficiency of single-doped Ln-UCNPs is not high. Yb<sup>3&#x2b;</sup> has become the most common sensitizer due to its unique energy level structure (<xref ref-type="bibr" rid="B54">Han et al., 2014</xref>).</p>
<p>We synthesized highly doped Er<sup>3&#x2b;</sup> core-shell nanoparticles of NaYF<sub>4</sub>:x%Er@NaXF<sub>4</sub> (x &#x3d; 5, 25, 50, and 100; X &#x3d; Lu and Y). The effect on luminescence as a function of Er<sup>3&#x2b;</sup> concentration was studied. There was a significant enhancement of red emission at 100% Er<sup>3&#x2b;</sup> doping (<xref ref-type="bibr" rid="B38">Feng et al., 2018</xref>). In a sensitizer and activator co-doped system, the concentration of activator generally does not exceed 5% while the sensitizer concentration is relatively high, on the order of 15%&#x2013;40%. The emission of Yb<sup>3&#x2b;</sup>/Er<sup>3&#x2b;</sup> co-doped systems range from 510&#xa0;nm to 560&#xa0;nm (green) and 640&#xa0;nm&#x2013;670&#xa0;nm (red). This system can emit with multiple colors as a combination of green and red can produce yellow light. Er<sup>3&#x2b;</sup>/Yb<sup>3&#x2b;</sup> co-doped Na<sub>0.5</sub>Gd<sub>0.5</sub>Mo<sub>O4</sub> was reported to emit with characteristic peaks at 531/552/667&#xa0;nm; furthermore, the intensity of UCL increased with higher Yb<sup>3&#x2b;</sup> concentration over a certain range (<xref ref-type="bibr" rid="B34">Du et al., 2016</xref>). Similarly, the intense emission of the Yb<sup>3&#x2b;</sup>/Tm<sup>3&#x2b;</sup> co-doped system was in the blue region, while the Yb<sup>3&#x2b;</sup>/Ho<sup>3&#x2b;</sup> co-doped system mostly emitted green light with improved efficiency due to the sensitizer. Rare Earth ions have further utility. For example, multi-doped systems empower enhanced luminescence modulation. Liu et al. reported white light emission from Er<sup>3&#x2b;</sup>/Tm<sup>3&#x2b;</sup>/Yb<sup>3&#x2b;</sup> triple-doped SrLu2O4. The Yb<sup>3&#x2b;</sup> concentration and pump power can be tuned to modulate the emission color. The optimal doping ratio of 0.5% Er<sup>3&#x2b;</sup>, 0.5% Tm<sup>3&#x2b;</sup>, and 20% Yb<sup>3&#x2b;</sup> created the best balance of red, green and blue luminescence to produce bright white light emission (<xref ref-type="bibr" rid="B100">Liu et al., 2018a</xref>). Dammak and coworkers designed a white light modulation system, Yb<sup>3&#x2b;</sup>/Er<sup>3&#x2b;</sup>/Tm<sup>3&#x2b;</sup> doped GdPO<sub>4</sub> at a high concentration of Yb<sup>3&#x2b;</sup> (35%mol), which emitted white light with excitation by an appropriate laser power (<xref ref-type="bibr" rid="B56">Hassairi et al., 2018</xref>). &#x3b2;-NaYF<sub>4</sub>: Yb<sup>3&#x2b;</sup>, Ho<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup> triple-doped Ln-UCNPs can create multicolor UCL by adjusting the doping concentration and excitation power, which resulted in both white and red light output (<xref ref-type="bibr" rid="B40">Gao et al., 2017</xref>).</p>
</sec>
<sec id="s3-2">
<title>3.2 Surface plasmon resonance modulation</title>
<p>Metal nanoparticles exhibit a strong plasmon resonance intensity due to electron delocalization over a large surface area. The surface plasmon resonance (SPR) effect will occur when the frequency of the incident photon is the same as the surface plasma oscillation. At this time, a strong local electric field is generated around the metal nanostructure, which further increases the excitation and radiation decay rates of Ln-UCNPs and thus enhances the up-conversion luminescence. UCL can be enhanced by SPR (<xref ref-type="bibr" rid="B160">Thariani and Yager, 2010</xref>), which prompted us to theoretically explore the effects of metal nanoparticles on Ln-UCNPs luminescence using the Discrete Dipole Approximation (DDA). The DDA algorithm can calculate the electromagnetic properties of nanoparticles as a function of shape. We synthesized La2O3:Yb/Er@Au, the gold coating of which significantly enhanced the emission intensity of La<sub>2</sub>O<sub>3</sub>:Yb/Er@Au by 16.8 times. Experiments demonstrated that the amount of Au added affects the particle spacing and the intensity of UCL. The increase in the electric field simulated by DDA was in good agreement with the observations made in the presence of an Au coating (<xref ref-type="bibr" rid="B111">Lv et al., 2014a</xref>). Light exposure and heating of the metal were shown to result in drug release in Na<sub>5</sub>Lu<sub>9</sub>F<sub>32</sub>:Yb/Er@Au. Both DDA simulation and experimental studies of Ln-UCNPs revealed that the coating of Au enhanced the absorptivity, which in turn resulted in a temperature increase upon excitation that facilitated the release of doxorubicin (DOX). Therefore, this system can be used for controlled drug release by the photothermal effect (<xref ref-type="bibr" rid="B112">Lv et al., 2014b</xref>). In the first two systems, we only performed electromagnetic calculations on single Au nanoparticles. DDA was used for the first time to perform extinction calculations on the rare earth-metal model of Ln-UCNPs@SiO<sub>2</sub>-Au (<xref ref-type="fig" rid="F2">Figure 2A</xref>) (<xref ref-type="bibr" rid="B107">Lv et al., 2018a</xref>). The results revealed the potential to use DDA to guide the construction of rare earth-metal composite materials.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>
<bold>(A)</bold> Simulation of the electric field strength (&#x7c;E&#x7c;/&#x7c;E0&#x7c;) of Ln-UCNPs@mSiO2-Au NPs (15&#xa0;nm&#x2013;D&#x2013;5&#xa0;nm geometry) under irradiation at &#x3bb;exc &#x3d; &#x3bb;SPR and &#x3bb;exc &#x3d; 800&#xa0;nm, with different silica spacers with thickness D of 5, 15, and 30&#xa0;nm &#x7c;E&#x7c;/&#x7c;E0&#x7c; is the enhancement factor. The electric field is amplified as &#x7c;E&#x7c; &#x3e; &#x7c;E0&#x7c;. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B107">Lv et al., 2018a</xref>) Copyright 2018: <xref ref-type="bibr" rid="B107">Lv et al. (2018a)</xref>]. <bold>(B)</bold> DDSCAT simulation results. Extinction spectra of the corresponding electronic strength images of SPS@Au. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B91">Lin et al., 2020</xref>) Copyright 2020: American Chemical Society].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g002.tif"/>
</fig>
<p>Although considerable progress has been made, many issues remain to be addressed. In the simulations discussed above, gold shells were used to simulate gold coatings. To obtain more accurate results, the Au shells were replaced with randomly distributed gold spheres to simulate Ln-UCNPs@mSiO<sub>2</sub>-Au. Both DDA simulation and experiments demonstrated that the presence of 5&#xa0;nm Au spheres results in enhancements; however the experimental results on 20&#xa0;nm Au sphere were inconsistent with the DDA simulations due to insufficient uniformity and aggregation. Regardless, the overall accuracy of the model on the modulation of the luminescence was improved (<xref ref-type="bibr" rid="B110">Lv et al., 2020</xref>). Next, we synthesized Au/Ag@Ln-UCNPs, and used DDA to simulate the enhancement on UCL due to the presence of gold nanocages of different sizes and thicknesses. Optical characterizations revealed that the luminous intensity of Au/Ag@Ln-UCNPs is twice that of Ln-UCNPs alone. In addition, Au/Ag@Ln-UCNPs were also effective for PTT/PDT treatment of tumors (<xref ref-type="bibr" rid="B96">Liu et al., 2019b</xref>). Additionally, Ln-UCNPs@SiO<sub>2</sub>@Au (SPS@Au) was synthesized and coated with ZnPc (zinc phthalocyanine) to produce SPS@Au/ZnPc. DDA was used to simulate the extinction of SPS@Au/ZnPc as a function of gold particle content (<xref ref-type="fig" rid="F2">Figure 2B</xref>), the results from which revealed enhanced luminescence properties (<xref ref-type="bibr" rid="B91">Lin et al., 2020</xref>).</p>
<p>The finite difference time domain (FDTD) method can be used to simulate the enhancement of UCL due to metal SPR. Song and coworkers used FDTD to simulate NaYF<sub>4</sub>: Yb<sup>3&#x2b;</sup>, Er<sup>3&#x2b;</sup> up-conversion luminescence in the presence of a gold rod. Single-layer gold nanorod (GNRs) and Ln-UCNPs were assembled on both sides of an isolating MoO<sub>3</sub> layer to demonstrate a luminescence enhancement effect of more than 35 times (<xref ref-type="bibr" rid="B203">Yin et al., 2016</xref>). Zhou and coworkers used FDTD to model Ag@SiO<sub>2</sub> to calculate the optimal Ag particle size and silicon layer thickness. The prepared Ag@SiO<sub>2</sub>@YF<sub>3</sub>:Ho<sup>3&#x2b;</sup> nanoparticles exhibited better luminous intensity (<xref ref-type="bibr" rid="B190">Xu et al., 2019</xref>). Although enhancements are realized using the current strategy of metal modulation to enhance UCL, the effects are actually quite modest. Methods to achieve greater optical enhancements is a problem to be solved in the future.</p>
</sec>
<sec id="s3-3">
<title>3.3 Algorithm optimization</title>
<p>A large number of experiments are usually required to determine the optimal doping concentration for Ln-UCNPs.</p>
<p>However, computer technology has revolutionized the traditional screening method. Using algorithms to guide this process can greatly simplify experimental realization. The doping optimization of rare Earth luminescent powder is essentially a combination optimization problem. A product can be designed on a computer and then experimentally realized; these steps are repeated to obtain a material with the best properties. In this process, heuristic algorithms based on natural body algorithms, have been used to guide the synthesis of rare earth-doped luminescent powders with high quantum yield. Heuristic algorithms include the genetic algorithm (GA), particle swarm optimization (PSO), and simulated annealing (SA) (<xref ref-type="bibr" rid="B59">Hopper and Turton, 2001</xref>; <xref ref-type="bibr" rid="B53">Hamza et al., 2017</xref>; <xref ref-type="bibr" rid="B124">Ozdemir and Karaboga, 2019</xref>). GA is a global random search optimization algorithm that uses the &#x201c;survival of the fittest&#x201d; mechanism to derive relationships between the material properties and the mole percentage of each raw material, and is often used to guide chemical synthesis optimization problems (<xref ref-type="bibr" rid="B67">Katoch et al., 2021</xref>). PSO simulates &#x201c;bird predation.&#x201d; The algorithm is easy to understand and program, has global search ability; as a result it has been applied in the field of combinatorial chemistry. Annealing is the process in which the temperature of the system decreases with time (<xref ref-type="bibr" rid="B159">Thangaraj et al., 2011</xref>). SA continuously iterates a simulated annealing process to find a solution that meets design specifications (<xref ref-type="bibr" rid="B149">Suman and Kumar, 2006</xref>). This algorithm has not yet been applied to combinatorial chemistry problems. Therefore, the most widely used optimization algorithm is the genetic algorithm (<xref ref-type="bibr" rid="B108">Lv et al., 2018b</xref>).</p>
<p>Our group has studied the pros and cons of SA, the improved SA of harmony search, PSO, and GA for guiding the synthesis of luminescent powders (<xref ref-type="fig" rid="F3">Figure 3</xref>). The efficacy of the four algorithms were evaluated by taking the same first-generation luminescent powder as the starting point for optimization and performing 5 iterations. SA had no obvious optimization effect; however, better results were obtained when combined with the harmony search. The genetic algorithm was better than PSO; however, generational analysis found that the brightness of the luminous powders as guided by PSO was more gradual (<xref ref-type="bibr" rid="B109">Lv et al., 2019</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Comparison of SA, HSA, PSO, and GA algorithms to the final average and maximum luminescence intensity. Variance of <bold>(A)</bold> all concentrations and <bold>(B)</bold> the Ce/Tb concentrations in different generations. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B109">Lv et al., 2019</xref>) Copyright 2019: American Chemical Society].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g003.tif"/>
</fig>
<p>In recent years, it was reported that the regression equation was built through the experimental results, which showed the relationship between luminescence and doping concentration. Then genetic algorithm was used to get the doping concentration corresponding to the maximum luminescence intensity (<xref ref-type="bibr" rid="B150">Sun et al., 2015</xref>). Coincidentally, <xref ref-type="bibr" rid="B218">Zhao et al. (2019)</xref> used the genetic algorithm to modulate Er<sup>3&#x2b;</sup>/Yb<sup>3&#x2b;</sup> co-doped Ba5Gd8Zn4O21, resulting in efficient red light emission.</p>
</sec>
<sec id="s3-4">
<title>3.4 Dye sensitization</title>
<p>Ln-UCNPs are challenged with weak absorptions and narrow optical excitation regions. These issues can be addressed using the dye sensitization strategy in which organic near-infrared chromophores are coordinated to the surface of Ln-UCNPs. Examples include IR783, IR806, IR808, and indocyanine green (ICG) which act as &#x201c;antennas&#x201d; to capture photons and transfer energy to the up-conversion rare Earth particles to improve UCL (<xref ref-type="bibr" rid="B57">Hazra et al., 2018</xref>). In 2012, <xref ref-type="bibr" rid="B226">Zou et al. (2012)</xref> used IR806 to sensitize &#x3b2;-NaYF<sub>4</sub>: Yb, Er for the first time. In this study, the intensity of up-conversion luminescence <italic>via</italic> excitation with an 800&#xa0;nm laser increased by 1,100 times compared to that realized from excitation at 980&#xa0;nm. This work prompted widespread application of this strategy for up-conversion luminescence enhancement. Han and coworkers synthesized (&#x3b2;-NaYF<sub>4</sub>: 20% Yb<sup>3&#x2b;</sup>, 2% Er<sup>3&#x2b;</sup>) Ln-UCNPs without hydrophobic organic ligands, and then explored the best ratio of near-infrared dyes to Ln-UCNPs to enhance luminescence. They coordinated IR783, IR808, IR820 and IR845 to Ln-UCNPs, and found enhancements of 80, 200, 70 and 10, respectively. To explore the sensitization effect of multiple dyes, IR783 and IR845 were simultaneously coordinated to the same Ln-UCNPs. The multidye-sensitized Ln-UCNPs showed a wider wavelength range and were applied for orthogonal bioimaging (<xref ref-type="bibr" rid="B184">Wu et al., 2015</xref>). Chen et al. proposed a new concept of energy-cascaded up-conversion (ECU) through the design of an IR808-sensitized core/shell Ln-UCNPs. IR808 was coordinated to the Ln-UCNPs and acted as an antenna to collect excitation energy that was transferred to Nd<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup> and Yb<sup>3&#x2b;</sup> through a multi-step process. This approach achieved a high up-conversion quantum efficiency of 19% (<xref ref-type="bibr" rid="B18">Chen et al., 2015</xref>).</p>
<p>Although the sensitization strategy can significantly enhance UCL, the dyes are quenched in water which greatly limits potential applications. Researchers have explored the synthesis of more stable and brighter dye-sensitized Ln-UCNPs. It was reported that Ln-UCNPs sensitized with Cy7 enhanced UCL in ethanol by &#x223c;30 times, although the effect was limited in water by &#x223c;2 times. To address this problem phosphatidylcholine was introduced to improve water dispersibility, which resulted in an increase of 17 times efficiency and enabled lymphatic imaging (<xref ref-type="bibr" rid="B227">Zou et al., 2016</xref>). Liu and coworkers revealed that quenching of dye sensitized Ln-UCNPs in water is the result of dye aggregation. Generally, near-infrared dyes are coupled to Ln-UCNPs through chemical coordination; in contrast, Liu and coworkers constructed dye-sensitized systems through hydrophobic interactions. The amphiphilic molecule DSPE-PEG (1,2-distearoyl-n-glycerol-3-phosphoethanolamine-N- [(polyethyleneglycol)-methoxy]) was used to coat the dye Car-Cl. As a result, the sensitization was improved 85 times in water. Unfortunately, aggregation-induced quenching was nonetheless observed at high concentrations.</p>
<p>To further eliminate strong coordination between the dye and rare Earth ions, Liu and coworkers used two long hydrophobic alkyl chains to replace the carboxyl group of the dye Car-Cl to produce a new dye (Alk-Cl), the use of which achieved enhancement of UCL of 215 times (<xref ref-type="fig" rid="F4">Figure 4</xref>) (<xref ref-type="bibr" rid="B89">Liang et al., 2020a</xref>). In addition, NIR-II dye (IR-1061) was used to sensitize core-shell Ln-UCNPs and solve the problem of quenching in water. It was worth noting that the purpose of this research was not to enhance up-conversion, rather, to obtain a strong near-infrared signal. Application of this strategy resulted in an increase in the 800&#xa0;nm emission of Tm<sup>3&#x2b;</sup> ions by 2.83 times. Furthermore, the near-infrared emission had a deeper tissue penetration depth, which is more conducive for biological imaging compared to visible emitters (<xref ref-type="bibr" rid="B57">Hazra et al., 2018</xref>). Although Ln-UCNPs have multicolor emission, it should be noted that red light has the advantages of deep penetration depth and imparts minimal damage to tissues in biological application.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>
<bold>(A)</bold> Schematic illustration of the alleviation of Aggregation-Caused Quenching (ACQ) and promotion of dye sensitization in aqueous phase by coating with DSPE-PEG. <bold>(B)</bold> Schematic illustration of improving dye-sensitization performance through eliminating ACQ of dye molecules. <bold>(C)</bold> Schematic illustration of improving dye sensitization performance through alleviating EBT from Nd<sup>3&#x2b;</sup> to dyes. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B89">Liang et al., 2020a</xref>) Copyright 2020: John Wiley &#x26; Sons, Inc.].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g004.tif"/>
</fig>
</sec>
<sec id="s3-5">
<title>3.5 Surface modification</title>
<p>During the synthesis of nanoparticles, long-chain polymers like oleic acid always were wrapped on the surface of Ln-UCNPs. In this way, the stability and luminescence intensity in aqueous are decreased compared with organic solvents, which limits the application in organisms. The following methods are usually used to deal with synthesized Ln-UCNPs. 1) Acid or excess ethanol was added. The ligands on the surface of Ln-UCNPs can be removed under the ultrasound. Capobianco and co-workers successfully removed the oleic acid ligands on the surface of NaGdF<sub>4</sub>: Yb<sup>3&#x2b;</sup>,Er<sup>3&#x2b;</sup> by the means of acid treatment (<xref ref-type="bibr" rid="B13">Bogdan et al., 2011</xref>) 2). The hydrophobic ligands were replaced by hydrophilic ligands, such as PEI, PAMAM, and PAA, to increase the water solubility of the nanoparticles. (<xref ref-type="bibr" rid="B69">Kovalenko et al., 2009</xref>; <xref ref-type="bibr" rid="B70">Kovalenko et al., 2010</xref>; <xref ref-type="bibr" rid="B156">Tangirala et al., 2010</xref>) 3) Inorganic material shells were coated on the surface of Ln-UCNPs, such as SiO<sub>2.</sub> This method can improve the water solubility of the nanoparticles effectively. It is worth noting that, thickness of the SiO<sub>2</sub> needs to be determined by multiple experiments. Since too thick or too thin SiO<sub>2</sub> layers may affect the luminescence intensity of Ln-UCNPs and make the synthesis process more difficult. (<xref ref-type="bibr" rid="B88">Li and Zhang, 2006</xref>)</p>
</sec>
</sec>
<sec id="s4">
<title>4 Ln-UCNPs-based theranostics</title>
<p>The traditional treatment for tumors, chemotherapy and surgical resection, have disadvantages that must be addressed. Several new therapies have attracted recent attention (<xref ref-type="bibr" rid="B9">Atmaca et al., 2021</xref>; <xref ref-type="bibr" rid="B68">Kobayashi et al., 2021</xref>; <xref ref-type="bibr" rid="B103">Lu et al., 2021</xref>; <xref ref-type="bibr" rid="B128">Pedziwiatr-Werbicka et al., 2021</xref>; <xref ref-type="bibr" rid="B225">Zhu et al., 2021</xref>). PT mainly includes photodynamic therapy and photothermal therapy. In PDT, irradiating a photosensitizer produces reactive oxygen species (ROS) that cause oxidative damage to cells (<xref ref-type="bibr" rid="B193">Yan et al., 2021a</xref>). In PTT, light-induced heating damages cancer cells (<xref ref-type="bibr" rid="B147">Shi et al., 2021</xref>). Combining photosensitizer or photothermal agent with Ln-UCNPs can achieve PT with near-infrared light.</p>
<sec id="s4-1">
<title>4.1 Ln-UCNPs-based drug delivery</title>
<p>Drug delivery is an important part of cancer treatment. Generally, Ln-UCNPs can be used as a vehicle for drug delivery to achieve a specific therapy. Mechanisms for drug delivery using Ln-UCNPs include passive, active, and physical targeting. In the passive targeting strategy, drugs are combined with Ln-UCNPs to achieve targeted therapy with the help of the enhanced permeability and retention (EPR) effect. In the active targeting strategy, drugs are combined with Ln-UCNPs, and the interaction between a ligand and receptor, or antigen and antibody, is used to specifically recognize cells to achieve the targeted delivery of drugs. <xref ref-type="bibr" rid="B23">Chen et al. (2017)</xref> designed Tm<sup>3&#x2b;</sup>-doped UCNPs and combined them with light-activated Ru complexes, so that enzyme inhibitors can be released by NIR excitation. In the physical targeting strategy, designer nanoparticles can be used to release drugs in specific locations by external environmental stimulus, such as changes in pH or temperature, photoexcitation, or magnetic targeting. Lin and coworkers designed Ln-UCNPs doped with Yb<sup>3&#x2b;</sup> and Tm<sup>3&#x2b;</sup> with additional modification of hydrazine monohydrate on the surface. In an acidic environment, the hydrogen bonds in the nanoparticles dissociate, enabling drug release (<xref ref-type="bibr" rid="B197">Yang et al., 2014</xref>). <xref ref-type="bibr" rid="B123">Mykhaylyk et al. (2001)</xref> designed magnetic nanoparticles that can deliver drugs to penetrate the blood-brain barrier and enter the mouse brain (<xref ref-type="bibr" rid="B123">Mykhaylyk et al., 2001</xref>). De et al. designed a polyelectrolyte complex based on Yb<sup>3&#x2b;</sup> and Er<sup>3&#x2b;</sup> to deliver pharmaceutical grade protein (<xref ref-type="bibr" rid="B28">De et al., 2022</xref>). The modified nanosystem overcame the problem of protein aggregation in the cell membrane and protected the protein drugs from destruction by proteases and the action of heat. At the same time, the nanoscale drug carrier system responded to the 980-nm NIR light, and realized the imaging of the protein delivery process.</p>
</sec>
<sec id="s4-2">
<title>4.2 Ln-UCNPs-based phototherapy</title>
<p>PDT has been clinically applied as a supplement to traditional therapy. Porphyrin is the first photosensitizer approved for this purpose (<xref ref-type="bibr" rid="B161">Tian et al., 2020</xref>), and mTHPC (meso-tetra hydroxy phenyl chlorin), a second generation photosensitizer, has shown many excellent characteristics in photodynamic therapy (<xref ref-type="bibr" rid="B131">Pinto et al., 2021</xref>; <xref ref-type="bibr" rid="B191">Yakavets et al., 2021</xref>; <xref ref-type="bibr" rid="B206">Yuan et al., 2021</xref>). In addition, chlorin dihydrogen E6 (Chlorin e6, Ce6), ZnPc and other photosensitizers have been widely used in scientific research although they have not been clinically approved (<xref ref-type="bibr" rid="B19">Chen et al., 2021a</xref>; <xref ref-type="bibr" rid="B215">Zhang et al., 2021a</xref>; <xref ref-type="bibr" rid="B21">Chen et al., 2021b</xref>; <xref ref-type="bibr" rid="B61">Hu et al., 2021</xref>; <xref ref-type="bibr" rid="B74">Lee et al., 2021</xref>; <xref ref-type="bibr" rid="B146">Shen et al., 2021</xref>; <xref ref-type="bibr" rid="B221">Zheng et al., 2021</xref>). Most photosensitizers are hydrophobic and easily aggregate in solution, which introduces practical difficulties (<xref ref-type="bibr" rid="B101">Liu et al., 2021a</xref>; <xref ref-type="bibr" rid="B94">Lin et al., 2021</xref>; <xref ref-type="bibr" rid="B178">Wei et al., 2021</xref>; <xref ref-type="bibr" rid="B182">Wu et al., 2021</xref>). Compared with PDT, there are less examples of the clinical application of PTT for tumor treatment. ICG is a dye that has been widely used in clinical diagnosis (<xref ref-type="bibr" rid="B106">Lutken et al., 2021</xref>; <xref ref-type="bibr" rid="B158">Teng et al., 2021</xref>). It can absorb in the near-infrared (600&#x2013;900&#xa0;nm) which enhances tissue penetration. In addition to its use in imaging and diagnosis, ICG has high photothermal conversion efficiency for photothermal therapy which is helpful for follow-up treatment of tumors (<xref ref-type="bibr" rid="B140">Ravichandran et al., 2020</xref>; <xref ref-type="bibr" rid="B209">Zhang et al., 2021b</xref>).</p>
<p>Currently, most of the photothermal agents are still applied in preclinical or early clinical research due to the fact that photothermal reaction cannot not completely eradicate a tumor; furthermore, there are additional risks due to overheating caused by laser ablation (<xref ref-type="bibr" rid="B39">Gao et al., 2020</xref>; <xref ref-type="bibr" rid="B51">Guo et al., 2021</xref>; <xref ref-type="bibr" rid="B87">Li et al., 2021</xref>; <xref ref-type="bibr" rid="B126">Pang et al., 2021</xref>; <xref ref-type="bibr" rid="B217">Zhao et al., 2021</xref>).</p>
<p>Ln-UCNPs are candidates for phototherapy due to their low toxicity and ability to be excited by near-infrared light. Ln-UCNPs are often used to deliver other molecules or add modifiers, for which the ability to upconvert expands the range of usable therapeutic agents making it more suitable for cancer phototherapy. In most cases, PDT and PTT effects exist simultaneously (<xref ref-type="bibr" rid="B195">Yang et al., 2021a</xref>; <xref ref-type="bibr" rid="B10">Bian et al., 2021</xref>; <xref ref-type="bibr" rid="B196">Yang et al., 2021b</xref>).</p>
<p>Generally, Ln-UCNPs is used in phototherapy to convert near infrared into visible light to trigger a photodynamic response. Guang and co-workers synthesized BiNS@NaLnF<sub>4</sub>(Ln &#x3d; Gd) using a solvothermal method (<xref ref-type="fig" rid="F5">Figure 5A</xref>). Specifically, NaGdF4 was loaded onto Bi ultra-thin nanosheets, and up-conversion was observed under 980&#xa0;nm laser irradiation to stimulate ROS generation. NaLnF<sub>4</sub> has a light-to-heat conversion efficiency of 35.3% (<xref ref-type="bibr" rid="B114">Ma et al., 2021a</xref>). Ln-UCNPs can also be used as a light energy converter to participate in the reconstruction of a tumor&#x2019;s microenvironment (<xref ref-type="fig" rid="F5">Figure 5B</xref>). The emitted light of a Ln-UCNPs can activate a photoacid to release H<sup>&#x2b;</sup>, which reduced the pH value of the tumor environment and improved the release of ROS in the cell in response to acid environment (<xref ref-type="bibr" rid="B169">Wang et al., 2020</xref>). <xref ref-type="bibr" rid="B95">Liu et al. (2020)</xref> synthesized an injectable DNA-Ln-UCNPs-Au hydrogel, which enhanced the aggregation of Ln-UCNPs-Au through electrostatically complexed DNA strands and achieved a photothermal conversion efficiency of 42.7% (<xref ref-type="fig" rid="F5">Figure 5C</xref>). In <italic>in vivo</italic> experiments, DNA-Ln-UCNPs-Au showed good stability and anti-cancer activity. In these preclinical studies, Ln-UCNPs have played an important role for tumor treatment. Since the excitation wavelength is in near-infrared band, phototherapy based on Ln-UCNPs can avoid the self-absorption problem of biological tissues and increase the penetration depth.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>
<bold>(A)</bold> <italic>In vitro</italic> PTT confocal images of ECA109 cells treated with PBS and BiNS@NaLnF4, with or without NIR irradiation. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B114">Ma et al., 2021a</xref>) Copyright 2021: Royal Society of Chemistry]. <bold>(B)</bold> Images of tumor after treatment. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B169">Wang et al., 2020</xref>) Copyright 2020: Royal Society of Chemistry]. <bold>(C)</bold> Photographs of female BALB/c nude mice bearing T24 tumors when treated with DNA&#x2013;Ln-UCNPs-Au hydrogel, Ln-UCNPs-Au, and PBS samples over a period of 21&#xa0;days after NIR irradiation in 3&#xa0;min (1&#xa0;W&#xa0;cm<sup>&#x2212;2</sup>); s.c., subcutaneous injection. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B95">Liu et al., 2020</xref>) Copyright 2020: John Wiley &#x26; Sons, Inc.].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g005.tif"/>
</fig>
</sec>
<sec id="s4-3">
<title>4.3 Ln-UCNPs-based phototherapy with chemotherapy</title>
<p>Chemotherapy can address the shortcomings of phototherapy, while phototherapy can more accurately target tumors and can be used to visually monitor drug release when combined with bioimaging (<xref ref-type="bibr" rid="B7">Andre et al., 2020</xref>; <xref ref-type="bibr" rid="B12">Birtle et al., 2020</xref>; <xref ref-type="bibr" rid="B220">Zheng and Xu, 2020</xref>; <xref ref-type="bibr" rid="B192">Yan et al., 2021b</xref>). A Ln-UCNPs-based multifunctional platform, Ln-UCNPs@PDA@Cy3-pep, that has treatment and real-time monitoring functions was reported (<xref ref-type="bibr" rid="B98">Liu et al., 2021b</xref>). The Ln-UCNPs comprised the core, while the chemotherapeutic drug staurosporine (STS) was loaded on the polydopamine (PDA) shell. The complex was shown to be effective for both photothermal therapy and chemotherapy under near infrared light irradiation. The quenching and restoration of Cy3 fluorescence was used to monitor the anti-cancer efficiency of the complex in real time (<xref ref-type="bibr" rid="B98">Liu et al., 2021b</xref>). Ju and coworkers reported a combination of chemical-photodynamic therapy based on a dual emitting Ln-UCNPs that was functionalized with a photosensitizer and the prodrug camptothecin. The surface was modified to enhance water solubility and targeting. Near-infrared excitation resulted in ultraviolet emission that activated the toxicity of CPT, and additional blue emission activated the photosensitizer to produce singlet oxygen to kill cancer cells (<xref ref-type="bibr" rid="B58">He et al., 2021</xref>). Huang and coworkers modified the photosensitizer to the surface of Ln-UCNPs to obtain Ln-UCNPs@PFNS. AQ4N, a hypoxia-activated prodrug that displays high toxicity selectively to hypoxic environment, was added to the pH-sensitive surface coating for chemotherapy (<xref ref-type="fig" rid="F6">Figure 6</xref>). The surface coating decomposed at the tumor site due to the acidic environment, resulting in exposure of AQ4N and the photosensitizer. Under near-infrared excitation the photosensitizer generated ROS and aggravated the hypoxia at the tumor site which enhanced the therapeutic effect of hypoxia-activated AQ4N (<xref ref-type="bibr" rid="B64">Ji et al., 2019</xref>). It is promising to actively explore therapies that can assist chemotherapy given its role as the dominant cancer treatment. It is foreseeable that the structure and optical properties of Ln-UCNPs will add value in chemotherapeutic approaches to treat cancer more effectively (<xref ref-type="bibr" rid="B90">Liang et al., 2020b</xref>).</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>
<bold>(A)</bold> Transmission electron microscope (TEM) images of Ln-UCNPs (a), Ln-UCNPs@PFNS (b), Ln-UCNPs@PFNS@MnCaP (c) and (Ln-UCNPs@PFNS/AQ4N) @MnCaP (d). <bold>(B)</bold> Schematic of the treatment of mice with intravenously injected (Ln-UCNPs@PFNS/AQ4N)@MnCaP and treatment by illumination. <bold>(C)</bold> The tumor growth curves for different treatments. Error bars indicate SD (<italic>n</italic> &#x3d; 6). [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B64">Ji et al., 2019</xref>) Copyright 2019: Elsevier].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g006.tif"/>
</fig>
</sec>
<sec id="s4-4">
<title>4.4 Ln-UCNPs-based phototherapy with immunotherapy</title>
<p>In recent years, immunotherapy has attracted attention due to the targeting capability and increased safety. Tumor immunotherapy does not reply on external stimuli, rather, it activates the immune response and cultivates immune cells to attack cancer cells (<xref ref-type="bibr" rid="B155">Tan et al., 2020a</xref>). Unlike traditional therapies, cancer cells can be removed continuously and quickly. Due to the efficacious anti-cancer effects of anti-CTLA-4 and anti-PD-1 antibodies, immunotherapy has the potential to revolutionize tumor treatment (<xref ref-type="bibr" rid="B66">Kamata-Sakurai et al., 2021</xref>; <xref ref-type="bibr" rid="B157">Tay et al., 2021</xref>). Many studies have demonstrated the potential for immunotherapy to improve the survival rate of patients and improving quality of life (<xref ref-type="bibr" rid="B14">Borcoman et al., 2019</xref>; <xref ref-type="bibr" rid="B168">Wallis et al., 2019</xref>; <xref ref-type="bibr" rid="B122">Mpekris et al., 2020</xref>). The combination of Ln-UCNPs-based phototherapy and immunotherapy may augment each other&#x2019;s therapeutic effects. Liu et al. prepared a core-shell structure with a core PDA, a NaGdF<sub>4</sub>:Yb/Er shell, and modified it with the photosensitizer Ce6 (<xref ref-type="fig" rid="F7">Figure 7A</xref>). When irradiated with a 980&#xa0;nm laser, the PDA component of the PDA@Ln-UCNPs-PEG/Ce6 acted as a photothermal agent while the Ce6 functioned as a photodynamic therapy agent. Phototherapy stimulated the body to produce an immune response, activated T lymphocytes and T memory cells, and helped to inhibit tumor metastasis and recurrence. However, it did not protect the mice from death threats caused by cancer. When combined with the immunosuppressant PD-1, the survival rate of mice was significantly improved to 77.8%, demonstrating the advantages of immunotherapy in long-term survival (<xref ref-type="bibr" rid="B194">Yan et al., 2019</xref>). Similarly, Chen and co-authors constructed a Ln-UCNPs/ICG/rose bengal (RB-mal) system (<xref ref-type="fig" rid="F7">Figure 7B</xref>) that triggered enhanced phototherapy by ICG under near-infrared irradiation. Tumor-derived protein antigen was captured by the nano-platform and kept in place to trigger a systemic anti-tumor immune response. Experiments in mice proved that Ln-UCNPs/ICG/RB-mal can not only cure tumors <italic>in situ</italic>, but also inhibits the growth of distant tumors, illustrating the generation of a tumor-specific immune response (<xref ref-type="bibr" rid="B172">Wang et al., 2019a</xref>). In addition, Ln-UCNPs can stimulate the immune response. Li and co-workers combined Ln-UCNPs with PCpG for immunotherapy (<xref ref-type="fig" rid="F7">Figure 7C</xref>). The core-shell nanoparticles NaGdF<sub>4</sub>:70%Yb, 1%Tm@NaGdF<sub>4</sub> emitted at 313, 363, 453 and 478&#xa0;nm under 980&#xa0;nm laser excitation. The UV light activated PCpG to release the immunotherapy agent CpG. In mouse experiments, it was worth noting that the CpG/UCs conjugate proved more effective compared to PCpG/UCs &#x2b; NIR; however, the former caused severe systemic toxicity which reveals the advantages of using Ln-UCNPs in this process (<xref ref-type="bibr" rid="B24">Chu et al., 2019</xref>).</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>
<bold>(A)</bold> Scheme of synergistic phototherapy for augmentation of antitumor immunity. Upon laser irradiation, nanoparticles ablate the primary tumor through phototherapy. (Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B194">Yan et al., 2019</xref>) Copyright 2019: John Wiley &#x26; Sons, Inc.). <bold>(B)</bold> Schematic depiction of the experimental approach for the evaluation of the abscopal effects induced by Ln-UCNPs/ICG/RB-mal based phototherapy. (Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B172">Wang et al., 2019a</xref>) Copyright 2019: John Wiley &#x26; Sons, Inc.). <bold>(C)</bold> Schematic of the design of a photoactivatable immunodevice through the integration of Ln-UCNPs with the UV light-responsive photoactivatable CpG (PCpG). Ln-UCNPs act as transducer to upconvert NIR light into UV light locally, thus liberate CpG oligonucleotides (ODN) from PCpG to achieve refined temporal control on its immunoactivity. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B24">Chu et al., 2019</xref>) Copyright 2019: Nature Publishing Group].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g007.tif"/>
</fig>
<p>When combining phototherapy with immunotherapy, both the near-infrared irradiation and phototherapy reagents elicit the body&#x2019;s immune response (<xref ref-type="bibr" rid="B60">Hou et al., 2018</xref>; <xref ref-type="bibr" rid="B27">Dai et al., 2020</xref>; <xref ref-type="bibr" rid="B153">Sun et al., 2020</xref>). However, the process is not clear, and as such exploring complex systems that can cause an immune response is still an urgent issue to be solved.</p>
</sec>
</sec>
<sec id="s5">
<title>5 Ln-UCNPs-based bioimaging</title>
<p>Recent research in biological imaging has centered on the design of new optical molecular probes (<xref ref-type="bibr" rid="B199">Yao et al., 2020</xref>).</p>
<p>Since biological tissue is a high-scattering medium, current imaging technology has disadvantages such as low penetration depth, interference from biological autofluorescence, and may cause tissue damage which greatly limits the application of biological imaging (<xref ref-type="bibr" rid="B65">Jia et al., 2020</xref>). Ln-UCNPs have a strong anti-Stokes shift, and the ability to absorb near-infrared light helps avoid biological background fluorescence interference (<xref ref-type="bibr" rid="B29">Dhal et al., 2020</xref>). Furthermore, near-infrared light has a deep tissue penetration depth. However, Ln-UCNPs cannot be directly applied to biological imaging due to fluorescence quenching, hydrophobicity, biological toxicity and other problems. Addressing these issues requires modification to their structure (<xref ref-type="bibr" rid="B223">Zhou et al., 2020</xref>).</p>
<sec id="s5-1">
<title>5.1 Ln-UCNPs-based fluorescence imaging</title>
<p>Fluorescence imaging generally uses photoluminescence probes, for which Ln-UCNPs are excellent candidates as their application does not result in tissue damage (<xref ref-type="bibr" rid="B62">Hu et al., 2020</xref>; <xref ref-type="bibr" rid="B212">Zhang et al., 2020</xref>). Recently, Hao and co-workers synthesized polyacrylic acid-modified NaLnF4: 40Gd/20Yb/2Er, (Ln &#x3d; Y, Yb, Lu, PAA-Ln-NRs). PAA-Ln-NRs with bright NIR II emission were injected into the tail vein of mice, and under excitation from a 980&#xa0;nm laser they achieved high-precision imaging of small tumors and metastases that enabled early cancer diagnosis (<xref ref-type="bibr" rid="B181">Wu et al., 2019</xref>). Liu et al. synthesized dye-sensitized Ln-UCNPs with a reduced propensity for aggregation in water through hydrophobic coordination. Issues with the quenching of Ln-UCNPs luminescence in water was addressed by adjusting the dye absorption band (<xref ref-type="bibr" rid="B89">Liang et al., 2020a</xref>). Chen et al. designed an ingenious NaYF<sub>4</sub>@NaYbF<sub>4</sub>@NaYF<sub>4</sub>:Yb<sup>3&#x2b;</sup>/Tm<sup>3&#x2b;</sup>@NaYF<sub>4</sub> structure for multi-channel fluorescence imaging. After intravenous and subcutaneous injection of the Ln-UCNPs, clear <italic>in vivo</italic> color imaging was obtained (<xref ref-type="bibr" rid="B78">Li et al., 2020b</xref>). The Fuyou group (<xref ref-type="bibr" rid="B134">Qiu et al., 2017</xref>; <xref ref-type="bibr" rid="B99">Liu et al., 2018b</xref>; <xref ref-type="bibr" rid="B127">Park et al., 2018</xref>) recently synthesized a rare-earth probe with NIR-II imaging capability. Ce<sup>3&#x2b;</sup> doping significantly increased the intensity of NIR-II luminescence, resulting a higher resolution in <italic>in vivo</italic> tumor imaging (<xref ref-type="bibr" rid="B15">Cao et al., 2020</xref>).</p>
<p>There are some interesting new studies for Ln-UCNPs outside <italic>in vivo</italic> imaging. Giri et al. coated Ln-UCNPs with oleylamine to obtain OA-Ln-UCNPs, and then further processed it to make a Ln-UCNPs oleogel with better skin permeability. The loading of Ln-UCNPs in the oleogels was varied to study the relationship between concentration and fluorescence intensity. For <italic>in vitro</italic> experiments, the Ln-UCNPs oleogel could penetrate the skin more deeply than free OA-Ln-UCNPs and be used as a skin tissue imaging agent under near-infrared excitation. Xu and co-workers reported the application of Ln-UCNPs in plant cell imaging, whereby LiErF4:1%Tm<sup>3&#x2b;</sup>@LiYF4 with a core-shell structure could enter the cell membrane easily and emit bright red light (<xref ref-type="bibr" rid="B133">Qiao et al., 2021</xref>).</p>
</sec>
<sec id="s5-2">
<title>5.2 Ln-UCNPs-based computed tomography</title>
<p>Computed tomography (CT) is based on the difference in the absorption and transmittance of X-rays among various tissues of the human body. The data is scanned by an instrument and processed to determine the pathological condition (<xref ref-type="bibr" rid="B130">Pfeiffer, 2018</xref>). Lanthanides have high X-ray attenuation coefficients (<xref ref-type="bibr" rid="B63">Issa et al., 2018</xref>), for example, the atomic number and electron density of Lu and Yb are greater than iodine which is currently used in CT. Du et al. reported the synthesis of core-shell nanoparticles NaYF<sub>4</sub>:Yb/Er@NaLuF<sub>4</sub>:Nd/Yb@NaLuF<sub>4</sub> and surface modification of chitosan. Next, Ag<sub>2</sub>Se was grown <italic>in situ</italic> to form NaYF<sub>4</sub>:Yb/Er@NaLuF<sub>4</sub>:Nd/Yb@NaLuF<sub>4</sub>@CS@Ag<sub>2</sub>Se. <italic>In vivo</italic> imaging experiments with these agents demonstrated potential for clinical CT (<xref ref-type="bibr" rid="B32">Du et al., 2020</xref>). Bismuth doping of materials significantly improves CT imaging as Bi has better X-ray attenuation ability compared to lanthanides. You et al. reported the synthesis of a porous BiF3:Yb, Er nanomaterial that generated an <italic>in vivo</italic> CT signal as demonstrated with concentration dependence. The CT value curve showed that the Hounsfield unit (HU) value of the sample was higher than observed in commercial Iohexol (<xref ref-type="bibr" rid="B216">Zhao et al., 2020</xref>). Gao and co-workers reported the synthesis of BaYF5 with different bismuth doping ratios: Yb, Er, Bi-x (x &#x3d; 0&#x2013;3). Under the excitation of a 980&#xa0;nm laser, the up-conversion luminescence was enhanced with increasing Bi content, reaching a maximum at x &#x3d; 2.5. Then Ln-UCNPs was coated with citrate for biological imaging. Both <italic>in vitro</italic> and <italic>in vivo</italic> experiments demonstrated that the Ln-UCNPs can be successfully used in X-ray CT imaging by accumulating at the tumor site (<xref ref-type="bibr" rid="B105">Luo et al., 2020</xref>).</p>
</sec>
<sec id="s5-3">
<title>5.3 Ln-UCNPs-based magnetic resonance imaging</title>
<p>Magnetic resonance imaging is a technique in which radio frequency pulses are applied to generate structural information (<xref ref-type="bibr" rid="B163">Tirotta et al., 2015</xref>; <xref ref-type="bibr" rid="B25">Clough et al., 2019</xref>). The signal is generated from relaxation of nuclei from the excited state to equilibrium over the relaxation time. There are two relaxation times, labeled T1 and T2, where T1 is the spin-lattice or longitudinal relaxation time and T2 is the spin-spin or transverse relaxation time. Therefore, MRI is divided into T1 MRI and T2 MRI. The lanthanide gadolinium is the main contrast agent for T1 MRI due to its paramagnetic properties (<xref ref-type="bibr" rid="B79">Li et al., 2014</xref>; <xref ref-type="bibr" rid="B198">Yang et al., 2016</xref>; <xref ref-type="bibr" rid="B166">Tse et al., 2019</xref>). Liu et al. reported a T1-weighted nanocontrast agent with smart MRI switch based on NaGdF<sub>4</sub>. Ultra-small NaGdF<sub>4</sub> and pH-sensitive CaCO<sub>3</sub> generated self-assembled bare self-assembled nanoparticles (BSNPs) in organic solvents (<xref ref-type="fig" rid="F8">Figure 8</xref>). The addition of a tumor targeting coating on the surface effectively guided the BNSPs to the tumor location, and then CaCO<sub>3</sub> reacted with the acidic environment to release NaGdF<sub>4</sub> to achieve MRI with 60 times higher contrast compared to the commercial contrast agent Magnevist (<xref ref-type="bibr" rid="B201">Yi et al., 2019</xref>). Superparamagnetic Fe<sub>3</sub>O<sub>4</sub> nanoparticles combined with Ln-UCNPs are often used in T2 MRI. Li et al. synthesized Fe<sub>3</sub>O<sub>4</sub>@NaGdF<sub>4</sub>:Yb:Er-HMME with a core-shell structure, which was used for both treatment and imaging. The super paramagnetism of the sample was first confirmed, and its T2-weighted MRI performance was studied. Compared with the commercial T2 contrast agent Feridex, the samples performed better, and were effective for use in <italic>in vivo</italic> T2 MRI (<xref ref-type="bibr" rid="B176">Wang et al., 2019b</xref>).</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Positive contrast enhancement evaluation <italic>in vivo</italic>. <bold>(A, B)</bold> T1-weighted MRI and corresponding pseudocolor images of tumor-bearing mice after intravenous injection of cell membrane coated-BSNPs (MSNPs) <bold>(A)</bold> and Magnevist <bold>(B)</bold> with the same dosage (2.5&#xa0;&#x3bc;mol of Gd<sup>3&#x2b;</sup> for each mouse). Images were captured before and at different time points after the administration of contrast agents. The time points were collected at the midpoint of the time interval during each imaging acquisition. The dotted circles represent the regions of interest: 1) tumor, 2) muscle, 3) background, and 4) bladder. Scale bars are 5&#xa0;mm for all images. The small spots on the corners are from the circulation apparatus in the MRI scanner. <bold>(C, D)</bold> Tumor-to-background (T/B) and tumor-to-muscle (T/M) contrast ratios based on the corresponding MRI images. Values represented as means &#xb1; s.d. (<italic>n</italic> &#x3d; 3). [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B201">Yi et al., 2019</xref>) Copyright 2019: John Wiley &#x26; Sons, Inc.].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g008.tif"/>
</fig>
</sec>
<sec id="s5-4">
<title>5.4 Other imaging based on Ln-UCNPs</title>
<p>Single-Photon Emission Computed Tomography (SPECT) and Positron Emission Tomography (PET) are two techniques in nuclear medicine. PET is the only imaging technique that can interrogate biomolecular metabolism, receptors, and neuromediator activity <italic>in vivo</italic>. Generally, substances necessary for metabolism, such as glucose, are labeled with short-lived radionuclides such as <sup>18</sup>F and <sup>11</sup>C. After injection into the human body, metabolic activities are reflected by the accumulation of the radiolabeled probes to enable diagnosis. <xref ref-type="bibr" rid="B36">Fang et al. (2020)</xref> used cancer cell membrane-modified NaGdF<sub>4</sub>:Yb,Tm@NaGdF<sub>4</sub> for UCL/MRI/PET trimodal tumor imaging and successfully differentiated triple-negative breast cancer subtypes MDA-MB-231 and MCF-7. <xref ref-type="bibr" rid="B152">Sun et al. (2011)</xref> used an efficient strategy for labeling Ln-UCNPs with <sup>18</sup>F, and successfully applied the materials in sentinel lymph nodes mapping with PET imaging and detection. The materials were realized by the reaction between rare Earth cations and fluoride ions. The process was simple, fast, and efficient as no organic reagents were applied.</p>
<p>The principle of SPECT is to label probes with short half-life nuclides and inject them intravenously. The nuclides emit &#x3b3;-rays through decay, and the &#x3b3;-rays are then converted into electrical signals and input into a computer for tomography reconstruction. A cross-section or three-dimensional image reflecting the physiological condition of organs in the human body can be obtained. <xref ref-type="bibr" rid="B78">Li et al. (2020b)</xref> prepared radioactive PEG-modified NaYF<sub>4</sub>:Yb, Er, Sm. These 10-nm nanoparticles were detected in kidney and urine by SPECT imaging and gamma counter analysis, confirming the potential for these probes as a biodistribution markers (<xref ref-type="bibr" rid="B16">Cao et al., 2013</xref>). <xref ref-type="bibr" rid="B115">Ma et al. (2021b)</xref> prepared a platelet membrane-coated nanostructure (PM-PAAO-Ln-UCNPs) containing Ln-UCNPs and Ce6 photosensitizer (PAAO &#x3d; poly(noctylamine) acrylate), and injected them into mice models. SPECT/CT dual-mode imaging was performed and the precise location of an atherosclerotic plaque was demonstrated.</p>
</sec>
</sec>
<sec id="s6">
<title>6 Ln-UCNPs-based biosensing</title>
<p>The unique optical properties of Ln-UCNPs make them effective for biological analysis and sensing. First, they are easily incorporated into a fluorescence analysis scheme due to their robust emission properties and high chemical stability. Second, the near-infrared excitation of Ln-UCNPs can effectively avoids autofluorescence of biological tissues. The use of Ln-UCNPs as fluorescent sensors has been extensively studied (<xref ref-type="bibr" rid="B73">Laurenti et al., 2016</xref>; <xref ref-type="bibr" rid="B45">Gerelkhuu et al., 2019</xref>; <xref ref-type="bibr" rid="B205">Yuan et al., 2019</xref>; <xref ref-type="bibr" rid="B148">Su et al., 2020</xref>; <xref ref-type="bibr" rid="B49">Gu et al., 2021</xref>). This section introduces the application of Ln-UCNPs-based pH and temperature sensors, as well as gas and ion sensors and some other platforms. And the typical cases of Ln-UCNPs for sensing are shown in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Typical cases of Ln-UCNPs for sensing.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">No</th>
<th align="center">Sensor system</th>
<th align="center">Excitation (nm)</th>
<th align="center">Emission</th>
<th align="center">Sensor type</th>
<th align="center">Recent advances</th>
<th align="center">References</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">1</td>
<td align="center">NaYF<sub>4</sub>:Yb,Tm-T (Thymine)</td>
<td align="center">980</td>
<td align="center">475&#xa0;nm</td>
<td align="center">ECL sensor</td>
<td align="left">In the presence of Hg<sup>2&#x2b;</sup>, the T monolayer-modified Au electrode (AuE/T) absorbed Hg<sup>2&#x2b;</sup>and T-Ln-UCNPs by T-Hg<sup>2&#x2b;</sup>-T matching. Surface-tethered T-Ln-UCNPs further recruited more Hg<sup>2&#x2b;</sup>, as well as T-Ln-UCNPs, thus forming a Ln-UCNPs-T-Hg<sup>2&#x2b;</sup>-T-Ln-UCNPs reticular architecture on the surface of the electrode</td>
<td align="center">
<xref ref-type="bibr" rid="B29">Dhal et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">2</td>
<td align="center">ssDNA-NaYF<sub>4</sub>:Yb,Er@SiO<sub>2</sub>
</td>
<td align="center">980</td>
<td align="center">549, 654&#xa0;nm</td>
<td align="center">miRNA sensor</td>
<td align="left">In the absence of complementary miRNA sequences, the ssDNA functionalized particles interact with the GQD leading to an enhancement of the up-conversion emission. In the presence of the target miRNA sequences, the hybridization process yields dsDNA on the surface of the Ln-UCNPs that hinders the interaction with GQD and reduces the up-conversion fluorescence enhancement.</td>
<td align="center">
<xref ref-type="bibr" rid="B223">Zhou et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">3</td>
<td align="center">NaLuGdF<sub>4</sub>:Yb,Er-Fe<sup>3&#x2b;</sup>, C u<sup>2&#x2b;</sup>, and Li<sup>&#x2b;</sup>
</td>
<td align="center">980</td>
<td align="center">543&#xa0;nm</td>
<td align="center">CAs sensor</td>
<td align="left">It was found that catecholamines could be more effectively detected in the presence of Ln-UCNPs-Fe<sup>3&#x2b;</sup>, whereas, dopamine and epinephrine were detected selectively using Ln-UCNPs-Li<sup>&#x2b;</sup> and Ln-UCNPs-Cu<sup>2&#x2b;</sup> sensors.</td>
<td align="center">
<xref ref-type="bibr" rid="B62">Hu et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">4</td>
<td align="center">APTEs-NaYF4:Yb,Er-Pt</td>
<td align="center">980</td>
<td align="center">543&#xa0;nm</td>
<td align="center">TNT sensor</td>
<td align="left">The Janus capsule motors were fabricated by layer-by-layer assembly of Ln-UCNPs-functionalized polyelectrolyte microcapsules, followed by sputtering of a platinum layer onto one half of the capsule.</td>
<td align="center">
<xref ref-type="bibr" rid="B212">Zhang et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">5</td>
<td align="center">NaGdF<sub>4</sub>:Yb,Er@SiO<sub>2</sub>&#x2013;Spiropyran</td>
<td align="center">980</td>
<td align="center">540&#xa0;nm</td>
<td align="center">HIS fluorescent nanosensor</td>
<td align="left">HIS could specifically bind to SP, which could cause the isomerization of SP. His will lead to fluorescence quenching of the sensor based on inner filter effects (IFE)</td>
<td align="center">
<xref ref-type="bibr" rid="B181">Wu et al. (2019)</xref>
</td>
</tr>
<tr>
<td align="center">6</td>
<td align="center">NaYF<sub>4</sub>:Yb,Er-pHrodo</td>
<td align="center">980</td>
<td align="center">550, 590&#xa0;nm</td>
<td align="center">pH sensor</td>
<td align="left">A nanosensor based on up-conversion resonance energy transfer (UC-RET) between an upconverting nanoparticle (Ln-UCNPs) and a fluorogenic pH-dependent dye PHrodo &#x2122; Red that was covalently bound to the aminosilane surface of the nanoparticles. The sensitized fluorescence of the pHrodo&#x2122; Red dye increases strongly with decreasing PH.</td>
<td align="center">
<xref ref-type="bibr" rid="B99">Liu et al. (2018b)</xref>
</td>
</tr>
<tr>
<td align="center">7</td>
<td align="center">NaYF<sub>4</sub>:Yb,Tm-BODIPY</td>
<td align="center">980</td>
<td align="center">451, 475, 64 8&#xa0;nm</td>
<td align="center">pH sensor</td>
<td align="left">The blue UCL of NaYF4:Yb<sup>3&#x2b;</sup>,Tm<sup>3&#x2b;</sup>Ln-UCNPs excited at 980&#xa0;nm, that overlaps with the absorption of the pH-sensitive fluorophore, provides reabsorption based excitation of the dye, the spectrally distinguishable green fluorescence of which is switched ON upon protonation, preventing photoinduced electron transfer within the dye moiety, and the pH-inert red UCL act as reference.</td>
<td align="center">
<xref ref-type="bibr" rid="B127">Park et al. (2018)</xref>
</td>
</tr>
<tr>
<td align="center">8</td>
<td align="center">NaGdF4:Yb,Er-mOrange</td>
<td align="center">980</td>
<td align="center">540&#xa0;nm</td>
<td align="center">pH sensor</td>
<td align="left">The Ln-UCNPs-mOrange nanoprobe could be fluorescently imaged with 980&#xa0;nm excitation, having deep penetration depth, by a fluorescence microscope on a coverslip, or uptaken in a single HeLa cell. Nigericin mediated intracellular pH (3.0, 5.0, and 7.0) could be accurately estimated from the CLSM derived FRET ratio.</td>
<td align="center">
<xref ref-type="bibr" rid="B134">Qiu et al. (2017)</xref>
</td>
</tr>
<tr>
<td align="center">9</td>
<td align="center">La<sub>2</sub>MoO<sub>6</sub>:Er</td>
<td align="center">379</td>
<td align="center">555&#xa0;nm</td>
<td align="center">Temperature Sensor</td>
<td align="left">By means of a fluorescence intensity ratio (FIR) technique, the temperature sensing performances in the temperature range of 303&#x2013;463&#xa0;K were investigated based on thermally coupled levels, <sup>2</sup>H11/2 and <sup>4</sup>S3/2, of Er<sup>3&#x2b;</sup> ions. The sensor sensitivity of Er<sup>3&#x2b;</sup>-activated La<sub>2</sub>MoO<sub>6</sub> nanoparticles can be greatly affected by the doping concentration and the maximum sensor sensitivity was determined to be about 0.0097&#xa0;K<sup>&#x2212;1</sup> at 463&#xa0;K.</td>
<td align="center">
<xref ref-type="bibr" rid="B32">Du et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">10</td>
<td align="center">NaGdF<sub>4</sub>:1%Tm/49%Yb@NaGdF<sub>4</sub> :15%Tb/1.5%Eu</td>
<td align="center">980</td>
<td align="center">545&#xa0;nm</td>
<td align="center">Temperature sensor</td>
<td align="left">The large difference in energy between the emission of Tb<sup>3&#x2b;</sup>and Eu<sup>3&#x2b;</sup>made the spectra easier to be detected and calculated based on relative intensity measurement compared to single-ion based systems.</td>
<td align="center">
<xref ref-type="bibr" rid="B216">Zhao et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">11</td>
<td align="center">NaLuF<sub>4</sub>:Mn,Ln-PNIPAM-Au</td>
<td align="center">980</td>
<td align="center">544, 660,</td>
<td align="center">Temperature sensor</td>
<td align="left">By utilizing red/near-infrared dual emitting NaLuF4:Mn<sup>2&#x2b;</sup>,Ln<sup>3&#x2b;</sup>(Ln<sup>3&#x2b;</sup> &#x3d; Yb<sup>3&#x2b;</sup>, Er<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup>) Ln-UCNPs as the energy donor and Au nanoparticles as the acceptor, the temperature resolution of the Ln-UCNPs is significantly increased from 3.1&#xb0;C to 0.9&#xb0;C in the physiological temperature range.</td>
<td align="center">
<xref ref-type="bibr" rid="B105">Luo et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="center">12</td>
<td align="center">NaY(WO<sub>4</sub>)<sub>2</sub>:Er,Yb</td>
<td align="center">980</td>
<td align="center">552, 655&#xa0;nm</td>
<td align="center">Temperature sensor</td>
<td align="left">The maximum relative sensitivity (Srel) and absolute sensitivity (Sabs) were determined to be &#x223c;1.2% K<sup>&#x2212;1</sup> at 293&#xa0;K and &#x223c;0.9% K<sup>&#x2212;1</sup> at 503&#xa0;K, respectively. The excellent repeatability of fluorescence intensity ration (FIR) and low temperature uncertainty &#x394;Tmin of &#x223c;0.4&#xa0;K at 293&#xa0;K make this optical nanothermometry cover a wide temperature range of 293&#x2013;503&#xa0;K.</td>
<td align="center">
<xref ref-type="bibr" rid="B79">Li et al. (2014)</xref>
</td>
</tr>
<tr>
<td align="center">13</td>
<td align="center">Bi<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub>:Yb,Ho</td>
<td align="center">980</td>
<td align="center">550,665,750&#xa0;nm</td>
<td align="center">Temperature sensor</td>
<td align="left">The maximum relative sensitivity is calculated to be 2.44% at 498&#xa0;K, obtained from the temperature-dependent spectra by recording in the range of 298&#x2013;498&#xa0;K. The samples also provide excellent repeatability and chromaticity stability.</td>
<td align="center">
<xref ref-type="bibr" rid="B166">Tse et al. (2019)</xref>
</td>
</tr>
<tr>
<td align="center">14</td>
<td align="center">NaYF<sub>4</sub>:Yb,Er</td>
<td align="center">980</td>
<td align="center">525,548&#xa0;nm</td>
<td align="center">Temperature sensor</td>
<td align="left">The spider silks were drawn directly from Araneus ventricosus and were decorated with core&#x2212;shell Ln-UCNPs <italic>via</italic> a photophoretic effect. By measuring the fluorescence spectra of the Ln-UCNPs on the spider silks, the membrane temperature of a single breast cancer cell was obtained with absolute and relative sensitivities ranging from 3.3 to 4.5 &#xd7; 10<sup>&#x2212;3</sup>K<sup>&#x2212;1</sup>and 0.2&#x2013;0.8% K<sup>&#x2212;1.</sup>
</td>
<td align="center">
<xref ref-type="bibr" rid="B198">Yang et al. (2016)</xref>
</td>
</tr>
<tr>
<td align="center">15</td>
<td align="center">NaYF<sub>4</sub>:Yb,Er-polystyrene</td>
<td align="center">980</td>
<td align="center">542,657&#xa0;nm</td>
<td align="center">Gas sensor</td>
<td align="left">PS is chosen as a matrix because it displays permeation selectivity for CO<sub>2</sub> and rejects protons. The luminescence intensities of the Ln-UCNPs at 542 and 657&#xa0;nm increase with increasing concentration of CO<sub>2</sub>, and the detection limit is 0.11% of CO<sub>2</sub>.</td>
<td align="center">
<xref ref-type="bibr" rid="B16">Cao et al. (2013)</xref>
</td>
</tr>
<tr>
<td align="center">16</td>
<td align="center">NaYF<sub>4</sub>:Yb,Tm@PEP</td>
<td align="center">980</td>
<td align="center">474&#xa0;nm</td>
<td align="center">Fe<sup>3&#x2b;</sup> sensor</td>
<td align="left">Limit of detections (LOD) of 0.2&#xa0;&#x3bc;M and recoveries of 94.5&#x2013;102.5%, Ln-UCNPs@PEP was shown to have low cytotoxicity and was used for monitoring Fe<sup>3&#x2b;</sup> in HeLa cells by fluorescence microscopy.</td>
<td align="center">
<xref ref-type="bibr" rid="B45">Gerelkhuu et al. (2019)</xref>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<sec id="s6-1">
<title>6.1 Ln-UCNPs-based pH sensors</title>
<p>The pH of the cell can reflect its condition; for example, abnormal cells are acidic. Furthermore, as some viruses and germs are most active under acidic conditions, (<xref ref-type="bibr" rid="B179">White et al., 2017</xref>) it is important to monitor intracellular pH. Ratiometric (dual color) Ln-UCNPs-based pH ratiometric sensors can be prepared by first analyzing the emission spectrum of Ln-UCNPs to ensure that it has a pH-insensitive component to serve as a reference, and then coupling it to a fluorescent pH indicator. Proper spectral matching results in fluorescence resonance energy transfer that can generate pH-dependent emission. The Schaferling group coupled Ln-UCNPs to a fluorescent pH-dependent dye pHrodoTM Red. The NaYF<sub>4</sub>:Yb<sup>3&#x2b;</sup>, Er<sup>3&#x2b;</sup> material emits at 550 and 660&#xa0;nm under laser excitation at 980&#xa0;nm. As the emission peak at 550&#xa0;nm was found to be invariant to changes in pH, it was used as a reference signal. The dye pHrodoTM Red emitted at 590&#xa0;nm with an intensity that is dependent on pH. As a result, the combination of the two chromophores created a ratiometric fluorescence probe that displayed a linear response to pH over the range 3&#x2013;6.7 (<xref ref-type="bibr" rid="B8">Arppe et al., 2014</xref>). Likewise Resch-Genger et al. combined NaYF4:Yb<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup> with a pH-sensitive BODIPY dye to create a ratiometric pH sensor (<xref ref-type="fig" rid="F9">Figure 9</xref>). Excitation at 980&#xa0;nm resulted in 475&#xa0;nm emission of Tm<sup>3&#x2b;</sup> that was absorbed by the dye, while the pH-insensitive 648&#xa0;nm emission of Tm<sup>3&#x2b;</sup> was used as a calibrant against the 528&#xa0;nm emission of BODIPY. This two-component sensor was successfully applied for pH monitoring in <italic>Escherichia coli</italic> (<xref ref-type="bibr" rid="B137">Radunz et al., 2019</xref>). Ln-UCNPs can also be coupled to pH-dependent fluorescent proteins to create ratiometric sensors. Recently, it was reported that Ln-UCNPs were combined with mOrange fluorescent protein. Excitation at 980&#xa0;nm resulted in UCL green emission by the Ln-UCNPs, which subsequently excited the mOrange fluorescent protein. The ratio of the pH independent Ln-UCNPs emission at 655&#xa0;nm to the pH- dependent emission of mOrange fluorescent protein was a quantifiable metric that was shown to have good stability and reversibility (<xref ref-type="bibr" rid="B46">Ghosh et al., 2020</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>
<bold>(A)</bold> Simple self-referenced luminescent pH sensors based on up-conversion nanocrystals and pH-sensitive fluorescent BODIPY dyes. <bold>(B)</bold> Time-dependent changes of the G/R ratio of the pH sensor layers treated with a suspension of E. coli with D-glucose and a suspension of E. coli without D-glucose or pure buffer. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B137">Radunz et al., 2019</xref>) Copyright 2019: American Chemical Society].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g009.tif"/>
</fig>
</sec>
<sec id="s6-2">
<title>6.2 Ln-UCNPs-based temperature sensors</title>
<p>Sensitive, convenient, and biocompatible temperature sensors are needed for biological studies (<xref ref-type="bibr" rid="B164">Tran Quang et al., 2016</xref>; <xref ref-type="bibr" rid="B43">Ge et al., 2020</xref>). Some rare Earth particles have temperature sensitive luminescence properties, which makes them good candidates for biological thermal sensing (<xref ref-type="bibr" rid="B33">Du et al., 2014</xref>; <xref ref-type="bibr" rid="B222">Zheng et al., 2014</xref>; <xref ref-type="bibr" rid="B174">Wang et al., 2015</xref>; <xref ref-type="bibr" rid="B35">Du and Yu, 2017</xref>). Lin et al. synthesized doubly-doped NaLuF4:Mn<sup>2&#x2b;</sup>, Ln<sup>3&#x2b;</sup>(Ln<sup>3&#x2b;</sup> &#x3d; Yb<sup>3&#x2b;</sup>, Er<sup>3&#x2b;</sup>, Tm<sup>3&#x2b;</sup>), which have red/NIR dual emission that can be enhanced by the SPR effect of proximal Au nanoparticles. Embedding both these materials into the thermoresponsive polymer poly(N-isopropylacrylamide) (PNIPAM) resulted in a temperature dependent modulation of the Ln-UCNPs and Au nanoparticle distance. The effect was to modulate the red to NIR emission ratio, which was the metric of the temperature-sensitive sensor that had a resolution of 0.9&#xb0;C (<xref ref-type="bibr" rid="B186">Xiao et al., 2014</xref>). <xref ref-type="bibr" rid="B143">Shahzad et al. (2019)</xref> co-doped microfibers with LiYF<sub>4</sub>:Yb<sup>3&#x2b;</sup>/Er<sup>3&#x2b;</sup>, polymethyl methacrylate, and silver to create temperature sensors. The temperature dependent ratio of the emission intensity at 522&#xa0;nm and 541&#xa0;nm of the Ln-UCNPs was quantified over the range of 303&#x2013;348&#xa0;K. Doping with Ag was shown to significantly improve the photostability and temperature response of the composite (<xref ref-type="bibr" rid="B143">Shahzad et al., 2019</xref>). A study on the temperature sensitivity of ZnO:Yb<sup>3&#x2b;</sup>/Tm<sup>3&#x2b;</sup> has been reported. The Ln-UCNPs was excited using a 980&#xa0;nm laser to produce blue and red UCL emission. The UCL decreased at lower temperatures in the range of 300&#xb0;C&#x2013;780&#xb0;C. The ratio of the intensities of the blue and red emission was modulated by 2.1% K<sup>&#x2212;1</sup> at 293&#xa0;K (<xref ref-type="bibr" rid="B85">Li et al., 2017a</xref>). Zhong et al. synthesized a new type of 8.5&#xa0;nm &#xd7; 12.5&#xa0;nm nanoparticle of NaY(WO4)2:Er<sup>3&#x2b;</sup>, Yb<sup>3&#x2b;</sup> that were shown to be temperature sensitive over the range 293&#xa0;K&#x2013;503&#xa0;K (<xref ref-type="bibr" rid="B92">Lin et al., 2019</xref>). In addition to explore the relationship between luminescence of Ln-UCNPs and temperature, researchers have combined various fiber optic probes and temperature-sensitive Ln-UCNPs. Kumar et al. designed Ln-UCNPs coated with polydimethylsiloxane (PDMS) to obtain better fluorescence emission. The pure Ln-UCNPs and Ln-UCNPs-PDMS composite materials were coated on optical fibers for temperature sensing. The sensor coated with composite material displayed a linear response from 295 to 473&#xa0;K (<xref ref-type="bibr" rid="B71">Kumar et al., 2020</xref>). A recent report demonstrated the coating of a temperature-dependent Ln-UCNPs onto the surface of spider silk, a natural optical fiber, to construct a temperature sensor with good biocompatibility. The change in fluorescence intensity of Ln-UCNPs reflected the temperature change of cancer cells. In addition, the sensor successfully detected temperature changes during apoptosis (<xref ref-type="bibr" rid="B48">Gong et al., 2021</xref>). Meiling et al. designed a lanthanide nanoscale temperature measurement system that can be used for the diagnosis of <italic>in vivo</italic> inflammation. The structure included an inert core, an active shell and an inert shell. The thermosensitive lanthanide elements were localized in the intermediate shell to shield from interference of the bioactive environment. This ternary structure enabled nanothermometers to continuously measure temperature changes of up to 4&#xa0;mm depth in biological tissues, with high temperature sensitivity over a physiological temperature range of 10&#xb0;C&#x2013;64&#xb0;C (<xref ref-type="bibr" rid="B154">Tan et al., 2020b</xref>). Although Ln-UCNPs are not the only material used for temperature sensors, their use imparts unique advantages. Ln-UCNPs have adjustable excitation wavelengths and can be excited by near-infrared light, making such temperature sensors beneficial for <italic>in vivo</italic> applications. Additionally, Ln-UCNPs have multi-color luminescence, which enables a wide selection of emission for construction of a temperature sensor.</p>
</sec>
<sec id="s6-3">
<title>6.3 Ln-UCNPs-based gas sensors</title>
<p>Gas molecules are of great significance in many biological processes. For example, O<sub>2</sub> is important for maintaining metabolism (<xref ref-type="bibr" rid="B118">Mates et al., 2012</xref>). CO<sub>2</sub> can regulate breathing and the acid-base balance in the body. NO regulates cardiovascular function and improves the immunity of white blood cells (<xref ref-type="bibr" rid="B17">Carpenter and Schoenfisch, 2012</xref>; <xref ref-type="bibr" rid="B104">Lundberg et al., 2015</xref>; <xref ref-type="bibr" rid="B37">Farah et al., 2018</xref>). As a result, the sensing of gas molecules can elucidate the internal physiological behaviors of organisms. In 2010, <xref ref-type="bibr" rid="B3">Achatz et al. (2011)</xref> reported a CO<sub>2</sub> gas sensor based on Ln-UCNPs for the first time. In their system bromothymol blue was used as the luminescence intensity modifier of Ln-UCNPs on polystyrene. Specifically, bromothymol blue the absorption of bromothymol blue quenched the emission of the Ln-UCNPs; however, the presence of acidic CO<sub>2</sub> changed the pH which instigated a color change. Thus, when the CO<sub>2</sub> concentration increased, the absorption of bromothymol blue was minimized which resulted in higher intensity Ln-UCNPs fluorescence that enabled a quantitative detection of CO<sub>2</sub> with a detection limit of 0.11% (<xref ref-type="bibr" rid="B5">Ali et al., 2010</xref>). The same group created other gas sensors using Ln-UCNPs. They reported the first application of NaYF<sub>4</sub>:Yb, Tm excited by near-infrared light as an O<sub>2</sub> sensor. First, an iridium (III) oxygen probe, Ln-UCNPs, and ethyl cellulose were dissolved in tetrahydrofuran. The solvent was evaporated to yield a sensor film. The Ln-UCNPs was excited by a 980&#xa0;nm laser and emitted at 455&#xa0;nm and 475&#xa0;nm. These two emission peaks overlapped the absorption of the iridium complex at 468&#xa0;nm. Therefore, Ln-UCNPs acted as a nanolamp in the sensor. The fact that the iridium complex&#x2019;s emission at 568&#xa0;nm is quenched by O<sub>2</sub> enabled quantitatively oxygen detection (<xref ref-type="bibr" rid="B3">Achatz et al., 2011</xref>).</p>
</sec>
<sec id="s6-4">
<title>6.4 Ln-UCNPs-based ion sensors</title>
<p>Although the content of metal ions in organisms is small, they play an important role in maintaining the acid-base balance of cells and organisms and other metabolic activities, and are components of many complex biological compounds. The luminescence properties of Ln-UCNPs show great advantages for metal ion detection. Many studies have demonstrated that ion sensors based on Ln-UCNPs have high sensitivity and selectivity, the results from which can be visualized for convenient operation. Iron directly participates in the transport and storage of oxygen. It is a component of hemoglobin, myoglobin and cytochrome, and is necessary for many metabolic processes (<xref ref-type="bibr" rid="B1">Abbaspour et al., 2014</xref>; <xref ref-type="bibr" rid="B142">Sangkhae and Nemeth, 2017</xref>). The Lee group reported that adrenaline-modified NaYF<sub>4</sub>:Yb, Tm was used for intracellular Fe<sup>3&#x2b;</sup> detection. PEP can complex with Fe<sup>3&#x2b;</sup>, and the energy transfer with the Ln-UCNPs occurred through non-radiative electron transfer and energy return (EBT), resulting in reduced Ln-UCNPs emission at 474&#xa0;nm. The detection limit of the Fe<sup>3&#x2b;</sup> sensor was 0.2&#xa0;&#x3bc;M over a range of 1&#x2013;10&#xa0;&#x3bc;M (<xref ref-type="bibr" rid="B44">Gerelkhuu et al., 2021</xref>). The content of zinc in the human body can affect the activity of many enzymes, and as a result Zn<sup>2&#x2b;</sup> has an important role in human health (<xref ref-type="bibr" rid="B117">Maret, 2013</xref>). Chang et al. synthesized a Zn<sup>2&#x2b;</sup> sensor composed of a Ln-UCNPs and a Zn<sup>2&#x2b;</sup> sensitive dye.</p>
<p>NaYF<sub>4</sub>:Yb/Tm@NaYF<sub>4</sub> has a multi-peak emission; the blue component at 475&#xa0;nm was within in the absorption range of the dye while the 654&#xa0;nm emission was not affected. When Zn<sup>2&#x2b;</sup> was added, the absorption of the dye shifted to 360&#xa0;nm, which led to an increase in the ratio of I475&#xa0;nm/I654&#xa0;nm. The sensor successfully detected Zn<sup>2&#x2b;</sup> in a live animal model of zebrafish (<xref ref-type="bibr" rid="B129">Peng et al., 2015</xref>).</p>
<p>Copper is an indispensable component in blood and participates in hematopoietic process and iron metabolism. It was reported that core-shell Ln-UCNPs were electrostatically adsorbed onto flexible carbon fiber cloth (CFC) to create Cu<sup>2&#x2b;</sup> sensors (<xref ref-type="fig" rid="F10">Figure 10</xref>). The absorption of Cu<sup>&#x2b;</sup> and Cu<sup>2&#x2b;</sup> coincided with the emission of Ln-UCNPs, which is a sensing mechanism. It was the first time that electrochemical technology was used to improve the sensing performance. Cu<sup>2&#x2b;</sup> accumulated when a voltage of 0.3&#xa0;eV was applied. CFC reduced the quenching of Ln-UCNPs in water. The synergy of the electrochemical technology and the CFC protective layer resulted in a detection limit of 82&#xa0;ppb (<xref ref-type="bibr" rid="B180">Wong et al., 2019</xref>). Trace fluoride can promote the normal development of teeth and bones, but excessive fluoride causes dental and skeletal fluorosis. Dual-functional gallic acid-Fe(III) modified Ln-UCNPs was reported with a 654&#xa0;nm emission that was quenched by the Fe-complex. The presence of F<sup>&#x2212;</sup> destroyed the Fe-complex, which imparted a sensing mechanism between the UCL and F<sup>&#x2212;</sup> ion analyte (<xref ref-type="bibr" rid="B113">Ma et al., 2017</xref>).</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>A schematic diagram showing the CFC-Ln-UCNPs probe for Cu<sup>2&#x2b;</sup> ion sensing with electrochemical assistance. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B180">Wong et al., 2019</xref>) Copyright 2019: Royal Society of Chemistry].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g010.tif"/>
</fig>
</sec>
<sec id="s6-5">
<title>6.5 Other new sensors</title>
<p>Recently there have been many reports on the use of Ln-UCNPs for the detection of miRNA and other biologically active molecules (<xref ref-type="bibr" rid="B204">Yuan et al., 2015</xref>; <xref ref-type="bibr" rid="B83">Li et al., 2016</xref>). Trypsin is an activating enzyme that plays an important role in food digestion and has anti-inflammatory and swelling functions (<xref ref-type="bibr" rid="B132">Plattner and Noe, 2015</xref>; <xref ref-type="bibr" rid="B177">Wattanasiritham et al., 2016</xref>). Guo et al. synthesized Ln-UCNPs-peptide-AuNP for the detection of trypsin and its inhibitors. The peptide, DDDDARC, is sensitive to trypsin. In the initial state, the emission of UCL was quenched by the Au NP due to F&#xf6;rster Resonance Energy Transfer (FRET) energy transfer. After adding trypsin the peptide was cleaved and UCL was restored. The detection limit of the trypsin sensor was 4.15&#xa0;ng/mL (<xref ref-type="bibr" rid="B183">Wu et al., 2017</xref>). Cytochromes are involved in cell redox reactions and take part in cell energy transfer (<xref ref-type="bibr" rid="B207">Zanger and Schwab, 2013</xref>). Wang et al. attached a Cy3-labeled aptamer to the surface of a Ln-UCNPs wrapped with PDA (<xref ref-type="fig" rid="F11">Figure 11</xref>). The aptamer responded to cytochrome c to trigger changes in the fluorescence intensity of Cy3, and the internal UCL served as a reference signal. The sensor reflected the level of Cytc through a ratiometric fluorescence signal, with a detection limit of 20&#xa0;nM over a range of 50&#xa0;nM to 10&#xa0;&#x3bc;M (<xref ref-type="bibr" rid="B113">Ma et al., 2017</xref>).</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Illustration of the Ln-UCNPs@PDA@AP application for sensing intracellular Cyt c. The illustration is not drawn to scale. [Reprinted with permission from Ref. (<xref ref-type="bibr" rid="B113">Ma et al., 2017</xref>) Copyright 2017: Elsevier].</p>
</caption>
<graphic xlink:href="fchem-11-1036715-g011.tif"/>
</fig>
<p>Recent studies have demonstrated that a single sensor can be used for the simultaneous detection multiple biomolecules. Xu et al. developed an Au-Au-Ln-UCNPs with an aptamer with sensitivity for both alpha-fetoprotein (AFP) and mucin 1. The sensor generated both Raman and fluorescence signals. Mucin 1 concentration was detected through the change of surface enhanced Raman scattering intensity, and AFP was sensed by the change of fluorescence intensity. The detection limits of both proteins were at an attomolar level (<xref ref-type="bibr" rid="B135">Qu et al., 2017</xref>).</p>
<p>Thrombin acts on the last step of the blood coagulation process. It can be used to stop bleeding and is a relevant marker for tumor diagnosis. Prostate-specific antigens are abundantly present in prostate tissue and semen, with extremely high tissue organ specificity, and are currently the first-choice marker for the diagnosis of prostate cancer. Kuang et al. used a Raman signal and fluorescence of Au-Ln-UCNPs in conjunction with aptamers to respond to thrombin and prostate specific antigen (PSA). The signal intensity of SERS was affected by the concentration of thrombin. The fluorescence signal was affected by PSA, and the detection limit was 3.2 &#xd7; 10<sup>&#x2212;20</sup>&#xa0;M (<xref ref-type="bibr" rid="B55">Hao et al., 2017</xref>).</p>
</sec>
</sec>
<sec id="s7">
<title>7 Biological toxicity of Ln-UCNPs</title>
<p>Despite the great potential in applications such as biotherapy, biological imaging and biosensing, the biotoxicity remains a major problem hindering the clinical application of Ln-UCNP. Most of the current studies on <italic>in vivo</italic> toxicity of Ln-UCNPs focus on mice. Ln-UCNPs enter mice in tail vein injection and reach the whole body by blood circulation. Due to the high permeability effect of capillaries to nanoparticles, the liver and spleen become the main aggregate organs of Ln-UCNPs (<xref ref-type="bibr" rid="B82">Li et al., 2017b</xref>; <xref ref-type="bibr" rid="B2">Abualrejal et al., 2019</xref>; <xref ref-type="bibr" rid="B22">Chen et al., 2019</xref>; <xref ref-type="bibr" rid="B52">Guryev et al., 2019</xref>; <xref ref-type="bibr" rid="B144">Shan et al., 2020</xref>). Chen and co-workers designed targeted contrast agents modified by PEI and FA (<xref ref-type="bibr" rid="B22">Chen et al., 2019</xref>). At 24&#xa0;h and 18&#xa0;days after the injection, the aggregation of nanoions in liver was higher than that in other tissues. Ln-UCNPs injected into the body can be eliminated by the hepatobiliary and renal metabolic systems. Tian and co-workers (<xref ref-type="bibr" rid="B162">Tian et al., 2019</xref>) found that the rate of excretion of Ln-UCNPs is independent of the modified groups. Other studies have shown that the modified group species can influence the toxicity of Ln-UCNPs. Chen and co-workers (<xref ref-type="bibr" rid="B20">Chen et al., 2018</xref>) designed a kind of unmodified nanoparticles (NaYF<sub>4</sub>:Er and NaGdF<sub>4</sub>:Yb,Er), which caused mild liver toxicity and nephritis. This can be considered as the unmodified Ln-UCNPs would release rare Earth ions under biological conditions, which will react with the phosphate group of ATP, cause ATP inactivation and tissue damage. Vedunova and co-workers (<xref ref-type="bibr" rid="B167">Vedunova et al., 2016</xref>) polymaleic anhydride octadecene, PEI, tetramethyl ammonium hydroxide modified Ln-UCNPs (NaYF<sub>4</sub>:Yb,Tm@NaYF<sub>4</sub>) respectively. The nanoparticles caused the morphological changes of the hippocampal cells, reduction in Ca<sup>2&#x2b;</sup> activity and cellular damage. Moreover, the nanoparticle size, concentration, and treatment time can also affect the biotoxicity of Ln-UCNPs (<xref ref-type="bibr" rid="B189">Xu et al., 2016</xref>; <xref ref-type="bibr" rid="B20">Chen et al., 2018</xref>; <xref ref-type="bibr" rid="B139">Rafique et al., 2018</xref>).</p>
</sec>
<sec id="s8">
<title>8 Conclusion and future prospects</title>
<p>In this review, we summarize the latest progress in the synthesis, optimization and application (especially for therapy) of Ln-UCNPs. The high-temperature pyrolysis method and hydrothermal/solvothermal procedure are still the most widespread protocols for their syntheses. In terms of improving up-conversion emission, through algorithm optimization, dye sensitization and other methods, the up-conversion emission intensity can be increased by multiple orders of magnitude. The fluorescent properties of lanthanide upconverting nanoparticles have also advanced the field of biomedicine. Near-infrared excitation addresses the limitations of ultraviolet to visible light excitation, penetrates deeper into tissue, and makes nanotherapeutic materials with light as the main excitation source a strong competitor for clinical drugs. Although lanthanide up-conversion has advanced significantly, there are still a large number of obstacles to address. We posit that the future direction of Ln-UCNPs research in the field of biology consists of: 1) Existing luminescence enhancement strategies are either ineffective or easily quenched when exposed to water. Better results may be obtained starting from the principle of up-conversion luminescence to explore optimization methods. 2) Cancer treatment drugs based on Ln-UCNPs have not been reported clinically, which may be related to long term toxicity in the body. It may be possible to extend the <italic>in vivo</italic> experiment period and minimize other factors that affect drug metabolism to simulate the therapeutic effects to the greatest extent. 3) Although the synthesis technology of Ln-UCNPs is very mature, the products are often hydrophobic. Surface modification for <italic>in vivo</italic> application will improve biocompatibility; however, this process will affect the luminescence efficiency. Finding the balance between biocompatibility and luminescence is a difficult problem. 4) Ln-UCNPs-based biosensors have been developed. However, few studies have evaluated the sensitivity and stability of Ln-UCNPs sensors for <italic>in vivo</italic> sensing. The <italic>in vivo</italic> environment is complex, and how to accurately deliver nanosensors to the detected cellular locations is also a major challenge.</p>
</sec>
</body>
<back>
<sec id="s9">
<title>Author contributions</title>
<p>RL, DX, and BL contributed to conception and design of the study. DX organized the database. CL performed the statistical analysis. DX wrote the first draft of the manuscript. BL, CL, and WL wrote sections of the manuscript. All authors contributed to manuscript revision, read, and approved the submitted version.</p>
</sec>
<sec id="s10">
<title>Funding</title>
<p>This work was supported by the Natural Science Foundation of China (NSFC Nos. 81801744 and 91859202), the National Key R&#x26;D Program of China Grant (No. 2017YFA0205202) and the Fundamental Research Funds for the Central Universities.</p>
</sec>
<sec sec-type="COI-statement" id="s11">
<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="s12">
<title>Publisher&#x2019;s note</title>
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