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BY 4.0 license Open Access Published by De Gruyter Open Access March 21, 2024

Research progress on Fe3+-activated near-infrared phosphor

  • Bin Sun EMAIL logo , Huixian Zhang and Yiming Wang

Abstract

Fe3+-activated near-infrared (NIR) luminescent materials have attracted widespread attention due to their tunable emission wavelength and extensive applications in various fields such as plant growth, food analysis, biomedical imaging, and night vision. Many excellent NIR materials have been developed by introducing non-toxic and environmentally friendly Fe3+ ions into different inorganic hosts. This article elucidates the luminescent properties of Fe3+ ions by combining the Tanabe–Sugano energy level diagram and the configuration coordinate model. The latest research progress on Fe3+-doped NIR luminescent materials is outlined, summarizing the luminescent characteristics of various Fe3+-doped materials, including emission wavelength, emission bandwidth, quantum efficiency, and thermal stability. Particularly, a detailed summary and analysis of the application areas of Fe3+-doped NIR luminescent materials are provided. Finally, the future prospects and challenges faced by Fe3+-doped NIR luminescent materials are presented. This review contributes to a deeper understanding of the luminescence mechanism of Fe3+ and the research progress of iron ion-doped luminescent materials, aiming to develop advanced Fe3+-activated NIR luminescent materials with enhanced performance and explore new application fields.

1 Introduction

Near-infrared (NIR) phosphors in the NIR range have been extensively studied due to their unique properties [1,2,3,4,5,6,7,8]. With the advancement of technology, researchers have developed numerous emerging applications utilizing NIR, which has made people’s lives smarter, more convenient, and healthier [9,10,11,12]. Numerous fields benefit from the diverse applications of NIR phosphors in various industries. In the food industry, these powders play a crucial role in food inspection and quality control. They can be used to detect contaminants, monitor food freshness, and ensure compliance with safety standards. In biomedical imaging, NIR phosphors enable advanced imaging techniques, such as fluorescence microscopy and molecular imaging, allowing for enhanced visualization of tissues, cells, and biomolecules. Their use in drug delivery systems further contributes to targeted and controlled release of therapeutic agents. Beyond the realm of healthcare, NIR phosphors have proven invaluable in other industries as well. In agriculture, they facilitate plant growth monitoring by providing essential information about photosynthesis, nutrient uptake, and stress levels. In security and surveillance, these powders find application in night vision technology, enabling enhanced visibility in low-light conditions. Additionally, their unique properties are utilized in iris recognition systems, enhancing the accuracy and security of biometric identification. Furthermore, NIR phosphors have a significant impact on remote sensing technologies. They are employed in satellite imaging, allowing for the remote monitoring of environmental phenomena, weather patterns, and land use. This information aids in various fields, such as urban planning, natural resource management, and climate change studies. Figure 1 illustrates the diverse range of applications where NIR phosphors are employed, showcasing their versatility and contribution to multiple industries [13,14,15]. As research and development continue in this field, we can anticipate further advancements and the emergence of new applications, revolutionizing various sectors and improving our quality of life [16,17,18,19,20,21,22,23,24]. Trivalent rare earth ions such as Pr3+, Nd3+, Ho3+, Er3+, Tm3+, and Yb3+ are capable of NIR emission [25,26,27,28,29,30,31,32]. However, the NIR emission produced by these trivalent rare earth ions is linear, which limits their applications in food inspection, night vision illumination, NIR spectroscopy, and other technologies. Eu2+ can generate broad band emission, but the emission peak is too close to the red region and does not meet the requirements [33,34,35,36]. The potential risk of Cr3+ oxidation to Cr6+ increases the toxicity of phosphors, limiting their long-term applications in the body. In recent years, Fe3+-doped NIR phosphors for LED conversion have become one of the most promising NIR light sources, attracting widespread attention [37]. As an activator, Fe3+ has sparked wide interest among researchers. The rapid development of Fe3+-doped NIR phosphors has greatly contributed to the advancement of broadband NIR phosphor-converted LEDs and their successful applications in medical and food detection, generating significant interest among scientists [38]. However, there are still some challenges in the application of Fe3+-doped NIR phosphors, such as the need to improve the shorter emission wavelength and thermal stability. Further research is needed to develop wide-band and high-efficiency phosphors. This article provides an overview of the latest achievements in the study of Fe3+-activated NIR phosphor. We summarize the research progress on the optical properties, structural characteristics, and luminescent mechanisms of Fe3+-activated NIR phosphor [39,40,41,42,43,44,45,46].

Figure 1 
               Target applications of NIR pc-LED with different emission wavelengths (730–1,800 nm) [39,40,41,42,43,44,45,46].
Figure 1

Target applications of NIR pc-LED with different emission wavelengths (730–1,800 nm) [39,40,41,42,43,44,45,46].

2 Chemical synthesis

The crystal structure of the host lattice determines the coordination environment of the dopant ions, such as positional symmetry and interionic spacing. In this article, we provide a detailed description of the synthesis methods and experimental design used in the study. We discuss the selection of raw materials, reaction conditions, and preparation steps, and provide precise data and characterization methods for the experimental results. In terms of synthesis methods, researchers have developed various techniques for preparing Fe3+-doped NIR phosphors. Sol–gel method, co-precipitation method, and thermal decomposition method, among others, have been widely used to prepare materials with excellent properties. In addition to conventional solid-state reaction methods, some novel synthesis strategies, such as hydrothermal method and microwave-assisted method, have also been adopted to achieve controlled morphology and structure.

3 Discussion

Phosphors doped with Fe3+ exhibit excellent NIR emission performance. These materials demonstrate tunable NIR luminescent properties within the range of 700–1,100 nm, closely related to their band structures, emissive centers, and interactions with activating ions. By controlling synthesis conditions, modifying the matrix, and adjusting the doping concentration, the emission intensity and peak of fluorescent materials can be customized to achieve the desired optical performance. We have discussed the series of fluorescent powders doped with Fe3+ from the following three perspectives: 1) Why choose Fe3+ as the activator and the luminescent properties of Fe3+ ions; 2) Typical luminescent properties and research progress of Fe3+-activated NIR phosphor; 3) Some application areas and potential of Fe3+-activated NIR phosphor.

3.1 Why choose Fe3+ as the activator and the luminescent properties of Fe3+ ions?

Fe3+ is a non-rare earth element and one of the most abundant elements on Earth. The cost-effective extraction of Fe3+ from iron, along with its stable supply and wide availability of iron resources compared to other rare earth elements, makes Fe3+ more sustainable and reduces dependence on rare elements, thus saving energy. One of the important advantages of Fe3+ is its non-toxicity, which is crucial in many applications. The use of safe and non-toxic substances is particularly important in various fields, especially in medicine and biosciences, where Fe3+ dopants fulfill this requirement and are widely used in applications such as biomedical imaging, drug delivery, and biosensing. Additionally, Fe3+ possesses a unique energy level structure and tends to exhibit NIR emission in octahedral environments (which will be discussed in detail in the next section). These advantages make Fe3+ an ideal dopant for NIR applications.

As a typical ion with a 3d5 electron configuration, Fe3+ ion has five electrons in its outermost shell, with an electron configuration of 1s22s22p63s23p63d5. The 3d electrons, being in the outermost shell, are significantly influenced by the surrounding crystal field. Therefore, the choice of matrix directly affects the luminescent properties of Fe3+ ions. It is known that Fe3+ ions can achieve NIR emission in an octahedral coordination environment. The energy level splitting of Fe3+ ions in an octahedral coordination environment is shown in the Tanabe–Sugano (T–S) diagram (Figure 2): the ground state term of this configuration is 6A1 (6S), the free electron term 4G splits into 4T1 and 4T2, and the degenerate 4A1/4E and 4D splits into 4E and 4T2. The 6A1 (6S) term is a horizontal line, and the 4A1/4E and 4E terms are also horizontal, so their energy is independent of the crystal field. The transitions from the ground state to these three states should produce sharp peaks, while transitions to stronger ligand fields such as 4T1 and 4T2 will result in broader bands. Similar to the 3d3 electron configuration of Cr3+ ion, it can be observed from the T–S energy level diagram in Figure 2 that the emission wavelength of Fe3+ is strongly influenced by the crystal field strength. The values of octahedral crystal field parameters D q, Racah parameters B and C, as well as the crystal field strength D q/B, for Fe3+-doped fluorescent powders can be estimated using the following equation [47]:

(1) E ( A 1 6 ( S 6 ) T 2 4 ( D 4 ) ) = 13 B + 5 C ,

(2) E ( A 1 6 ( S 6 ) E 2 4 ( D 4 ) ) = 17 B + 5 C ,

(3) E ( A 1 6 ( S 6 ) T 1 4 ( P 4 ) ) = 18 B + 7 C ,

(4) E ( A 1 6 ( S 6 ) T 1 4 ( G 4 ) ) = 10 D q + 10 B + 6 C ( 26 B 2 / 10 D q ) ,

(5) E ( A 1 6 ( S 6 ) T 2 4 ( G 4 ) ) = 10 D q + 10 B + 6 C ( 26 B 2 / 10 D q ) .

Figure 2 
                  T–S energy-level diagram of the 3d5 electronic configuration in the octahedral field as well as the PLE and PL spectra of Fe3+ doping NIR phosphor [47].
Figure 2

T–S energy-level diagram of the 3d5 electronic configuration in the octahedral field as well as the PLE and PL spectra of Fe3+ doping NIR phosphor [47].

Generally, the excitation of Fe3+-doped NIR fluorescent powders originates from 6A1(6S) → 4E(4D), 6A1(6S) → 4T2(4D) and 6A1(6S) → 4T2(4G) transitions; the emission is due to the Fe3+ 4T1(4G) → 6A1(6S) of electronic transition. From the T–S diagram (Figure 2), it can be observed that the weaker the crystal field strength, the smaller the peak wavelength of the emitted light [47].

The d–d transitions of Fe3+ in octahedral sites are subject to the strict restriction of the Laporte selection rule. This limitation presents a challenge in achieving high luminescence efficiency for long-wavelength NIR emission in Fe3+. The Laporte selection rule is a principle used to predict the spectroscopic activity of transition metal ions. According to this rule, charge transfer transitions are forbidden when the initial and final orbitals have the same symmetry. In the case of octahedral coordination, this means that d-electrons at the center of the octahedron cannot undergo transitions between the same spin orbitals, thus limiting the spectroscopic properties of octahedral complexes. Therefore, to achieve high luminescence efficiency for long-wavelength NIR emission in Fe3+, it is necessary to modify the structure of octahedral complexes by altering the ligand environment or introducing additional modifications. This may involve selecting appropriate ligands, tuning the crystal field strength, or introducing external alkaline earth metals, among other approaches. While this task presents challenges, it also offers numerous opportunities and prospects for applications. Achieving high luminescence efficiency for long-wavelength NIR emission in Fe3+ will contribute to the development of efficient NIR emissive materials, which are of significant importance in fields such as optoelectronics, biomedical imaging, and energy conversion. Consequently, researchers have been exploring various methods to overcome the limitations imposed by the Laporte selection rule in order to achieve high luminescence efficiency for long-wavelength NIR emission in Fe3+. The outcomes of these efforts will provide us with more choices of NIR emissive materials and drive further advancements and innovations in related fields.

3.2 Typical luminescent properties and research progress of Fe3+-activated NIR phosphor

Recently reported Fe3+-doped phosphors have emission wavelengths exceeding 800 nm. They have great potential for various applications, such as CaAl12O19:Fe3+ (808 nm) [48], SrAl12O19:Fe3+ (811 nm) [48], and CaGa2O4:Fe3+ (809 nm) [49]. It offers a flexible design for new Fe3+-doped NIR persistent phosphors through cation substitution and local crystal field modification. Table 1 summarizes some NIR phosphors doped with Fe3+. In 2022, Wang reported unprecedented long-wavelength NIR emission phosphors of Fe3+-activated Sr2−y Ca y (InSb)1−z Sn2z O6 [50]. Overall emission tuning from 885 to 1,005 nm and full-width at half-maximum (FWHM) broadening from 108 to 146 nm were achieved through crystallographic site engineering strategies. NIR emission was significantly enhanced after complete Ca2+ incorporation due to the reduced symmetry induced by substitution. Ca2InSbO6:Fe3+ phosphor exhibited a peak at 935 nm with an ultra-high internal quantum efficiencies (IQE) of 87%. The synthesized tunable emission phosphors showed enormous potential for NIR spectral detection. This work initiated the development of efficient Fe3+-activated broadband NIR emission phosphors and opened up a new pathway for the design of NIR emitting phosphor materials. In 2022, Zhang et al. successfully synthesized Fe3+-activated NaScSi2O6 phosphor [51]. Upon excitation at 300 nm UV light, a wide NIR emission band at 900 nm with an FWHM of 135 nm and an IQE of 13.3% was observed. The luminescence was related to the 3d–3d transitions of Fe3+ in octahedral coordination, confirming the effectiveness of Fe3+ activators in achieving efficient NIR emission. In 2022, Xiang et al. reported a series of environmentally friendly and low-cost Fe3+-activated ZnGa2O4 phosphors [52]. The Fe3+-doped phosphors exhibited a broad emission range from 650 to 850 nm, with a maximum emission peak at 720 nm and an FWHM of 70 nm. The emission intensity remained at 71% even at an elevated temperature of 423 K. The NIR pc-LED made of this phosphor exhibited strong NIR emission. In 2023, Li et al. reported a novel Fe3+-activated NIR persistent phosphor composed of Mg2SnO4 [53]. Fe3+ ions occupied both tetrahedral and octahedral sites, and due to the energy level alignment, electrons released from traps preferentially returned to the excited energy level of Fe3+ in the tetrahedral sites via tunneling, resulting in efficient NIR persistent emission at a peak wavelength of 789 nm with an FWHM of 140 nm. This phosphor demonstrated a record-breaking persistence duration of over 31 h in Fe3+-based phosphors for night vision applications, serving as a self-sustainable light source. This work not only provided a new type of efficient Fe3+-doped NIR persistent phosphor for technological applications but also established practical guidelines for the rational tuning of persistent emission. Based on the analysis and summary of the above literature, it can be observed that a disadvantage of Fe3+-doped NIR phosphors is the inability to be efficiently excited by blue light, which limits their applications to some extent. In 2023, Cheng et al. synthesized Fe3+-activated NaAl5O8 NIR phosphors [54]. Under excitation at 346 nm, NaAl5O8:Fe3+ phosphors exhibited NIR emission with a main peak at 754 nm. Emission spectra were measured in the temperature range of 303–463 K, revealing that the emission intensity at 423 K remained at 83.1% of that at 303 K, indicating excellent thermal stability of the sample. The luminescent behavior of the sample was studied after immersing it in deionized water for 0–10 h. These findings suggest that NaAl5O8:Fe3+ samples hold promise for applications in high-temperature or humid environments. Furthermore, the use of NaAl5O8:Fe3+ in the preparation of anti-counterfeit ink demonstrated its potential in the field of anti-counterfeiting. In 2023, Yang et al. synthesized Fe3+-activated Li2ZnAO4 (A = Si, Ge) phosphors through solid-state reactions, with Fe3+ occupying the tetrahedral sites of Zn2+ [38]. Under excitation by 300 nm ultraviolet light, broad NIR emission bands were observed at 750 nm (Li2ZnSiO4:Fe3+) and 777 nm (Li2ZnGeO4:Fe3+), with IQE of 62.70% (Li2ZnSiO4:Fe3+) and 30.57% (Li2ZnGeO4:Fe3+). The thermal stability at 373 K was improved from 35.43 to 49.79% through cation tuning. The combination of activation energy, electron-phonon coupling, and Debye temperature explained the enhanced thermal stability of Li2ZnGeO4:Fe3+ phosphors. Additionally, the synthesized phosphors exhibited sensitive and selective detection of Cu2+ ions. In 2023, the research team led by Quanlin Liu utilized the structural confinement effect in Sr9Ga(PO4)7 (SGP) to selectively control energy transfer pathways, suppressing luminescence concentration and thermal quenching effects. They found that in Fe3+-doped SGP compounds, the relatively large Fe3+-Fe3+ distances hindered energy transfer between Fe3+ ions, resulting in weakened concentration quenching. The Sr9Ga0.8(PO4)7:0.2Fe3+ (SGP:0.2Fe3+) phosphor exhibited the highest NIR luminescence intensity. Additionally, they introduced trivalent Yb3+ to investigate its influence on the luminescence of Fe3+-doped phosphor systems. Co-doping Yb3+ into SGP:0.2Fe3+ resulted in much shorter Fe3+–Yb3+ distances compared to Fe3+–Fe3+, facilitating rapid energy transfer from the quenching center Fe3+ to the thermally stable center Yb3+. The thermal stability of SGP:0.2Fe3+ ,0.07Yb3+ was greatly enhanced compared to SGP:0.2Fe3+. This study provided a method to enhance NIR luminescence by utilizing structural confinement to control energy transfer pathways and suppress concentration and thermal quenching effects. Finally, they demonstrated the potential applications of SGP:0.2Fe3+ and SGP:0.2Fe3+ ,0.07Yb3+ phosphors in the fields of night vision and optical thermometry [47].

Table 1

Luminescence properties and related parameters of partial Fe3+-activated NIR phosphor

Phosphor PLE, PL (nm) FWHM (nm) IQE I(%)@Temp. Refs
Sr2InSbO6:Fe3+ 340, 885 108 48% / [55]
Ca2InSbO6:Fe3+ 340, 935 146 87% / [55]
NaScSi2O6:Fe3+ 300, 900 135 13.3% / [51]
ZnGa2O4:Fe3+ 344, 720 70 / 71%@423 K [56]
Mg2SnO4:Fe3+ 308, 789 140 / / [57]
NaAl5O8:Fe3+ 346, 754 / / 83.1%423 K [54]
Li2ZnSiO4:Fe3+ 300, 750 / 62.7% 35.43%@373 K [58]
Li2ZnGeO4:Fe3+ 300, 777 / 30.57% 49.79%@373 K [58]
Sr9Ga(PO4)7:Fe3+ 330, 915 155 6.6% 50%@260 K [47]

3.3 Some application areas and potential of Fe3+-activated NIR phosphor

The phosphor activated by Fe3+ ions distinguishes itself through its superior optical properties, which significantly amplify its application potential across diverse fields. These properties, encompassing high luminescence efficiency and exceptional stability, pave the way for its use in advanced imaging, plant growth, food analysis, biomedical imaging, and night vision. Next, let’s take the application in the field of anti-counterfeiting as an example to demonstrate. In 2023, Cheng et al. presented their findings on Fe3+-activated NaAl5O8 NIR phosphor, examining its phase and luminescent properties [54]. It was observed that the optical bandgap narrows as the Fe3+ doping concentration increases. The sample’s thermal stability was confirmed by maintaining 83.1% emission intensity at 423 K compared to 303 K, as measured across an emission spectrum range of 303–463 K. These research results not only demonstrate the potential applications of NaAl5O8:Fe3+ samples in high temperature or humid environments but also highlight their significance in the field of anti-counterfeiting, particularly in the context of anti-counterfeiting inks. Anti-counterfeiting inks are widely used in the protection of important documents such as currency, identification cards, and labels to prevent forgery and fraud. By utilizing NaAl5O8:Fe3+ as a phosphor material in anti-counterfeiting inks, enhanced anti-counterfeiting effects can be achieved. There are several advantages of incorporating NaAl5O8:Fe3+ in anti-counterfeiting inks. First, NaAl5O8:Fe3+ phosphor exhibits high stability and is resistant to high temperatures, allowing it to maintain its luminescent properties in environments with elevated temperatures. This is crucial during the manufacturing process of anti-counterfeiting inks, which often involves heating and curing. Second, NaAl5O8:Fe3+ phosphor demonstrates good stability in humid environments, preventing performance degradation associated with humidity and ensuring the ink’s reliability and durability in such conditions. Furthermore, the successful application of NaAl5O8:Fe3+ in anti-counterfeiting has been verified. Figure 3 illustrates the remarkable efficacy of NaAl5O8:Fe3+ when utilized as an anti-counterfeiting ink. The phosphor’s luminescent qualities are uniquely tailored, exhibiting distinct spectral features that can be precisely identified and authenticated. These tailored characteristics render the ink exceptionally conspicuous and swiftly verifiable, ensuring its integrity is effortlessly ascertainable with the employment of specialized detection apparatus or analytical instruments. This not only underscores the ink’s suitability for high-security applications but also enhances its practicality for widespread use in safeguarding valuable items from counterfeiting attempts. Hence, the successful utilization of NaAl5O8:Fe3+ phosphor as a constituent in anti-counterfeiting inks not only underscores its significance in the realm of anti-counterfeiting but also serves as a pivotal tool in the ongoing battle against counterfeit currency and forged identification cards. Furthermore, its implementation plays a crucial role in safeguarding brand integrity, fortifying fraud deterrents, and upholding consumer trust. These groundbreaking research findings provide compelling evidence to propel the advancement of anti-counterfeiting technologies, paving the way for new avenues of innovation and progress in combating counterfeit practices [54].

Figure 3 
                  Security inks (a) and the patterns written on (b) stainless steel, (c) glass, (d) plastic, and (e) paper under room light and UV light [54].
Figure 3

Security inks (a) and the patterns written on (b) stainless steel, (c) glass, (d) plastic, and (e) paper under room light and UV light [54].

Moreover, apart from its applications in anti-counterfeiting technology, NIR phosphors doped with Fe3+ have also demonstrated remarkable potential in the field of night vision. In 2023, Li et al. reported that Fe3+-doped NIR phosphor demonstrated a record-breaking duration of over 31 h, making it a self-sustainable light source for night vision applications, as shown in Figure 4 [57].

Figure 4 
                  Schematic (a) and experimental setup (b) for the self-sustainable night vision imaging. (c) Photos of a toy car taken in the dark with and without NIR PersL illumination by visible and NIR cameras [57].
Figure 4

Schematic (a) and experimental setup (b) for the self-sustainable night vision imaging. (c) Photos of a toy car taken in the dark with and without NIR PersL illumination by visible and NIR cameras [57].

Phosphors doped with Fe3+ ions have broad prospects in applications such as luminescence thermometry and NIR stickers. In 2022, Zhang et al. conducted a study on Fe3+-activated NaScSi2O6 phosphor [51]. In their research, they excited the sample with 300 nm ultraviolet light and observed a broad NIR emission band at 900 nm, with an FWHM of 135 nm and an IQE of 13.3%. This emission behavior is closely related to the 3d–3d transitions of Fe3+ ions in octahedral sites, validating the effectiveness of Fe3+ as an activator for achieving efficient NIR emission. The research results also showed that the emission intensity of Fe3+ exhibited a linear quenching trend within the temperature range of 293–433 K. This indicates that Fe3+-doped phosphor can serve as a sensitive luminescent temperature sensing material, and the changes in its emission intensity can be used for real-time temperature measurement and monitoring. In addition, the feasibility of the synthesized phosphor material was also investigated in applications such as NIR luminescence thermometry and NIR stickers, as shown in Figure 5. This implies that Fe3+-doped phosphor has potential applications in non-contact temperature measurement technologies and patch-type infrared sensors. These applications contribute to achieving high-precision, high-sensitivity, and long-distance temperature measurements, providing more possibilities for industries such as industrial production, energy utilization, and medical diagnostics. In summary, Fe3+-doped phosphor exhibits tremendous potential in applications such as luminescence thermometry and NIR stickers. The compelling research findings surrounding Fe3+-doped phosphor offer robust evidence, bolstering the case for its continued development and expanded utilization within the realm of infrared luminescence. The intrinsic properties of this material, such as its efficient infrared emission and stable luminescent behavior under varying conditions, lay a solid foundation for breakthroughs in technological innovation. Moreover, these findings illuminate a path forward for application development in fields including, but not limited to, bioimaging, security, and optical communications. The promising results obtained thus far herald a new era of advancements, underscoring the transformative potential of Fe3+-doped phosphor in driving forward the frontiers of infrared luminescent applications [51].

Figure 5 
                  (a) Scheme of the fabrication of an IR patch by the screen printing method. Photographs under natural light captured using a visible camera (b, left) and in the dark captured using a NIR camera under UV excitation light when it is off (c, middle) and on (d, right) [51].
Figure 5

(a) Scheme of the fabrication of an IR patch by the screen printing method. Photographs under natural light captured using a visible camera (b, left) and in the dark captured using a NIR camera under UV excitation light when it is off (c, middle) and on (d, right) [51].

Research has found that the majority of Fe3+-doped NIR fluorescent materials exhibit lower IQE values. It is noteworthy that Fe3+-doped NIR fluorescent materials have broad absorption bands. This broad band feature allows them to absorb more light energy, thereby enhancing the efficiency of light excitation. This is crucial for applications such as bioimaging and photovoltaics, as it can provide stronger excitation signals or higher energy conversion efficiency. Additionally, Fe3+-doped NIR fluorescent materials have relatively long lifetimes. The lifetime of fluorescent materials is critical for the stability and optical performance of fluorescent probes. A longer lifetime can reduce background noise in fluorescence bioimaging, improve imaging clarity and signal-to-noise ratio, and also benefit the stability and long-term use of photovoltaic devices.

Unfortunately, the understanding of the luminescence mechanism and certain related luminescent properties of Fe3+-doped NIR phosphors is not yet sufficiently deep. Although some studies have revealed key luminescence mechanisms and band structures, further research is still needed to address some of the complexities involved. Second, the stability of Fe3+-doped NIR fluorescent materials needs to be improved. Some studies indicate that certain fluorescent materials undergo degradation or irreversible deactivation of fluorescence intensity under prolonged excitation or high-temperature environments. This instability limits the further promotion and application scope of the materials in practical use. Additionally, the selection of matrix materials and optimization of structural design remain challenging. The choice of matrix and novel structural design significantly impact the improvement of optical performance. It is necessary to consider the balance of ion concentration with fluorescence efficiency, lifetime, and light absorption intensity to obtain better optical performance.

In conclusion, Fe3+-doped NIR fluorescent materials have a wide range of optical performance advantages, including broad emission wavelength range, high fluorescence quantum yield, wide light absorption band, and relatively long lifetime. However, challenges regarding understanding the mechanism, stability, and structural design still need to be addressed. Future research will focus on overcoming these challenges and further improving and optimizing the optical performance of Fe3+-doped NIR fluorescent materials to achieve their widespread application in fields such as biomedical imaging and optoelectronics.

4 Outlook and challenges

4.1 Outlook

Looking ahead, with the increasing demand for NIR fluorescent materials, Fe3+-doped NIR fluorescent materials are expected to find more applications in a wider range of fields. In the field of biomedical imaging, Fe3+-doped NIR fluorescent materials have great potential in tumor labeling, early cancer detection, and photodynamic therapy due to the deep penetration ability of NIR light and low tissue autofluorescence interference. In the field of biosensors, Fe3+-doped NIR fluorescent materials have high sensitivity and selectivity, enabling efficient, rapid, and accurate detection of biomolecules, providing strong support for disease diagnosis and drug screening. Additionally, Fe3+-doped NIR fluorescent materials have a wide range of application prospects in the field of photovoltaics, which can improve photovoltaic conversion efficiency and energy output, providing new possibilities for the development and utilization of renewable energy. In summary, significant progress has been made in the research of Fe3+-doped NIR phosphors due to their tunable luminescent properties and potential applications in the NIR spectral range, making them a hot research topic. Further research will help to understand its luminescence mechanism, improve its luminescence efficiency and stability, and expand its application prospects in the fields of biomedical imaging and optoelectronics.

4.2 Challenges

Although in recent years, Fe3+-doped NIR fluorescent materials have been widely studied and received extensive attention due to their unique optical properties and potential applications, significant progress has already been made in the fields of biomedical imaging, biosensors, and photovoltaics. However, there are still challenges that need to be addressed in current research. For example, some Fe3+-doped NIR phosphors still exhibit issues with long-term excitation and stability, which limits their further advancement in practical applications. Additionally, further research is needed to deepen our understanding of the Fe3+ doping mechanism and luminescent properties.

First, in the realm of preparation and synthesis, it is crucial to embark on further exploration and refinement of suitable synthesis methods and process conditions. As the current preparation methods possess certain complexities and challenges in controlling material parameters, it is imperative to undertake more research to discover efficient, controllable, and reproducible preparation techniques. Additionally, to bolster the efficiency and stability of fluorescence, a more comprehensive understanding of the Fe3+ doping mechanism and luminescent properties becomes indispensable in facilitating enhanced material design and synthesis.

Second, emphasis should be placed on material stability and long-term reliability. The challenges lie in mitigating light attenuation and degradation, which can adversely impact luminescence performance in prolonged excitation and high-temperature environments. To tackle this predicament, it is imperative to develop more robust materials, including enhancing the light damage threshold and augmenting their optical durability. These advancements will enhance stability and render them more suitable for practical applications.

Additionally, to further enhance luminescent performance, structural design improvements, crystal structure enhancement, and doping methods can be implemented. In particular, optimizing the doping concentration and dopants is an important research direction with the potential to achieve optimal control of material properties and luminescence efficiency. Furthermore, exploring novel synthesis techniques and the influence of external factors, such as temperature and pressure, on luminescent properties may offer additional avenues for improving material performance.

In summary, Fe3+-doped NIR fluorescent materials hold immense promise and potential for applications in biomedical imaging, biosensors, and photovoltaics. Nevertheless, certain challenges persist in terms of preparation methods, stability, and luminescent performance. Future research efforts will be directed toward overcoming these challenges, enhancing the performance and stability of Fe3+-doped NIR fluorescent materials, expanding their application prospects, and expediting their translation and utilization in the fields of biomedical imaging and optoelectronics.

Acknowledgments

This work was supported by the “Kunlun Talents - High-level Innovation and Entrepreneurial Talents” project (Elite Talents Project) in Qinghai Province. The work was finished with the help of Huixian Zhang and Yiming Wang.

  1. Funding information: This work was supported by the “Kunlun Talents - High-level Innovation and Entrepreneurial Talents” project (Elite Talents Project) in Qinghai Province.

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

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Received: 2023-09-18
Revised: 2023-11-06
Accepted: 2023-12-07
Published Online: 2024-03-21

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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