Novel Fluorescent Probe Based on Rare-Earth Doped Upconversion Nanomaterials and Its Applications in Early Cancer Detection

In this paper, a novel rare-earth-doped upconverted nanomaterial NaYF4:Yb,Tm fluorescent probe is reported, which can detect cancer-related specific miRNAs in low abundance. The detection is based on an upconversion of nanomaterials NaYF4:Yb,Tm, with emissions at 345, 362, 450, 477, 646, and 802 nm, upon excitation at 980 nm. The optimal Yb3+:Tm3+ doping ratio is 40:1, in which the NaYF4:Yb,Tm nanomaterials have the strongest fluorescence. The NaYF4:Yb, Tm nanoparticles were coated with carboxylation or carboxylated protein, in order to improve their water solubility and biocompatibility. The two commonly expressed proteins, miRNA-155 and miRNA-150, were detected by the designed fluorescent probe. The results showed that the probes can distinguish miRNA-155 well from partial and complete base mismatch miRNA-155, and can effectively distinguish miRNA-155 and miRNA-150. The preliminary results indicate that these upconverted nanomaterials have good potential for protein detection in disease diagnosis, including early cancer detection.


Introduction
MicroRNAs (miRNAs) are important regulators of cell proliferation, division, differentiation, and apoptosis. They can regulate the expression levels of various genes in DNA post-transcriptionally. The abnormal expression of miRNAs has been associated with many diseases (cancer, tumors, and diabetes) [1], and miRNAs can be obtained through blood, urine, etc. [2], which has the advantage of being non-invasive. Therefore, miRNAs are considered important biomarkers for tumors [3]. Patryk Krzeminski [4] et al. demonstrated that DNA methylation contributes to miRNA-155 expression, and the survival data of myeloma cells show a correlation between miR-155 expression and multiple myeloma outcomes. A number of studies have shown that miRNA-155 is closely related to MM, and the overexpression of miRNA 155 in blood is an important signal for the diagnosis of MM [5][6][7]. Therefore, the detection of miRNA-155 to diagnose early MM is an important and efficient method.
The concept of upconversion luminescence was first proposed by Auzel and Ovsyankin et al. [8]. The radiation process is a nonlinear anti-Stokes emission, excited by the effective absorption of two or more low-energy photons. Then, it transitions from the ground state to the excited state through a multi-step process, and finally, it returns Surface ligand exchange, surface ligand oxidation, and surface ligand assembly are common surface modification methods [47][48][49]. Jiang et al. [48] used polymeric anhydride to interact with octadecene and oleic acid ligands on the surface of nanoparticles by coordination adsorption, and then cross linked with dicyclohexanetriamine to obtain stable water-soluble upconverted nanoparticles. The effective modification of upconverted materials has become a key factor in their applications in biological detections.
In this paper, high-temperature thermal decomposition was used to prepare NaYF 4 :Yb 3+ /Tm 3+ upconverted nanoparticle materials and it was found that the optimal Yb 3+ /Tm 3+ ratio is 40:1, in terms of the luminescence efficiency. These new types of upconverted nanoparticles were modified by surface coating and tested for protein detection for the purpose of early cancer diagnosis. Instrumentation: the intelligent digital magnetic stirring electric heating mantle (ZNCL-TS-250 mL, Shanghai Anchun Instrument Co., Ltd., Shanghai, China) was used to prepare upconverted nanomaterials and carboxylated proteins. Fluorescence was measured using a fluorescence spectrometer (F-4600, Hitachi, Hitachi, Ltd., Tokyo, Japan). Phase analysis of upconverted nanomaterials was carried out by X-ray powder diffractometer (X-ray Diffraction, XRD, D8 ADVANCE, Bruker, Germany). The morphology of the upconverted nanomaterials was characterized by field emission scanning electron microscope (Scanning Electron Microscope, SEM, SU8010, Hitachi Co., Ltd., Tokyo, Japan) and scanning transmission electron microscope (Transmission Electron Microscopy, TEM, FEI TECNAI G2 F20, Hitachi Co., Ltd., Tokyo, Japan). A Fourier transform infrared spectrometer measured infrared absorption (Tensor 27, Bruker, Germany). The luminescence was measured with a 980 nm fiber laser (BOT980-5W, Xi'an Leize Electronic Technology Co., Ltd., Xi'an, China).

Preparation of Upconverted Nanomaterials
Rare-earth-doped upconverted luminescent nanomaterials NaYF 4 :Yb,Tm were synthesized by high-temperature thermal decomposition. The preparation of 2 mmol NaYF 4 :20% Yb 3+ , 0.5% Tm 3+ nanomaterials was performed by first charging 1.39 mmol YCl 3 ·6H 2 O, 0.6 mmol YbCl 3 ·6H 2 O, and 0.01 mmol TmCl 3 ·6H 2 O into a three-neck round-bottom flask. Then, oleic acid (12 mL) and octadecene (30 mL) were added, and the flask flowed with nitrogen gas for 10 min to ensure no oxygen in the flask. Next, under nitrogen protection with magnetic stirring, the mixture was heated to 160 • C and reacted for 1 h to obtain a pale-yellow solution. The mixture was cooled to 50 • C and then 10 mL of a methanol solu-tion containing 8.0 mmol of ammonium fluoride and 5.0 mmol of sodium hydroxide was added dropwise to the mixture. The reaction was continuously stirred at 50 • C for 30 min to ensure a complete integration. Then, the temperature was raised to 80 • C to evaporate the methanol. During the evaporation of methanol, the solution continued to bubble, and the mixture was continuously heated to 120 • C for 30 min until no more bubbles were generated in the solution. Finally, the sample was heated to 300 • C for 90 min. After the reaction was over, the solution was naturally cooled to room temperature and cyclohexane was added to disperse the mixture. The mixture was centrifuged at 8000 rpm/min for 5 min to obtain a precipitate, which was then washed with cyclohexane. The above steps were centrifuged and washed three times, and the NaYF 4 :Yb,Tm upconverted nanomaterial finally obtained was dispersed in cyclohexane and stored. In addition, the experimental steps for the preparation of NaGdF 4 :Yb,Tm upconverted nanomaterials are the same as above. The YCl 3 ·6H 2 O in the experimental material was replaced by GdCl 3 ·6H 2 O, and the experimental steps were repeated to obtain NaGdF 4 :Yb,Tm upconverted nanomaterials.

Water-Soluble Upconverted Nanomaterials
Two mL of the cyclohexane solution of the upconverted nanomaterial prepared in the above experiment was prepared and ultrasonically dispersed for 5 min. Twenty mg of NaBF 4 was dissolved in two mL of acetonitrile solution and was added to the fully dispersed cyclohexane solution of upconverted nanomaterials by stirring at 1000 rpm/min for 30 min to obtain a mixed solution of water and oil separation. Then, the water-soluble NaYF 4 :Yb, Tm upconverted nanomaterials were obtained by centrifuging at 8000 rpm/min for 15 min.

Preparation of Carboxylated Proteins
First, we dissolved 1 g of bovine serum albumin in 20 mL of ultrapure water, then excess oxalic acid was added, and we adjusted the pH to 7-8 with an aqueous sodium carbonate solution under magnetic stirring. Then, 5 mmol of EDC was added and the mixed solution was stirred overnight. A dialysis bag with a molecular-weight cut-off of 10k-30k Da was used for dialysis. The denatured proteins were put into the dialysis bag, clamped on both sides with dialysis clips to prevent leaking, and immersed into a sodium bicarbonate aqueous solution (1000 mL, 2 mmol) leaving it in a refrigerator at 4 • C. The sodium bicarbonate aqueous solution was replaced every 4-6 h to ensure that the protein was always in a slightly alkaline environment. The protein was dialyzed and purified under this condition for at least 72 h, and the carboxylated bovine serum albumin was obtained, which was divided into centrifuge tubes and stored in a −20 • C refrigerator.

Carboxylated Protein-Modified Upconverted Nanoparticles
Next, 0.5 mL of the prepared carboxylated protein, described above, was dissolved in 2 mL of DMF solution, then water-soluble upconverted nanomaterials were added to the DMF solution and the pH was adjusted to about 8 with aqueous sodium bicarbonate solution by stirring for 2 h. After the reaction was completed, the mixed solution was centrifuged at 10,000 rpm/min for 10 min. The precipitates were washed twice with DMF centrifugation, and finally dispersed with DMF for preservation. The above operations were all carried out at room temperature.

DNA Probes Linked to Carboxylated Protein-Modified Upconverting Nanoparticles
The pH of 1 mL of the carboxylated protein-modified upconverted nanomaterials obtained in the above steps was adjusted to about 6 with 20 µmol of hydrochloric acid aqueous solution, then 5 mg EDC and 5 mg NHS were added and stirred at room temperature for 25 min to let the carboxyl groups fully react with the nanoparticles. Next, the aminated DNA probe with FAM was added to a 40 µL PBS buffer to make a concentration of 100 µmol. An appropriate amount of the solution was immediately added to the carboxylated upconverted nanomaterial solution, and then put in a shaker to react for Nanomaterials 2022, 12, 1787 5 of 17 30 min. The reaction was washed twice with PBS buffer at 10,000 rpm/min for 5 min each time, and the resulting precipitates were DNA probes with FAM linking to a carboxylated protein-modified upconverted nanomaterial fluorescent probe (DNA/dBSA /NaYF 4 :Yb, Tm).

Experimental Results and Discussion
3.1. The Effect of Yb 3+ Doping Concentration on the Luminescence of Upconverted Nanomaterials Figure 1 shows the energy structure and the transitions of Yb 3+ and Tm 3+ ions in the upconverting luminescence process. It can be seen that upconversion luminescence is a complex multi-photon energy transfer and conversion process. The energy level transition of 2 F 7/2 → 2 F 5/2 of the sensitizer Yb 3+ ion matches the energy of the near-infrared photon at 980 nm, so it can continuously absorb the excitation energy and then transfer it to the adjacent luminescent center Tm 3+ . The 3 H 5 , 3 F 2 ( 3 F 3 ), and 1 G 4 energy levels are from Tm 3+ ions. Among them, there are three methods for upconversion luminescence: (1) the 3 H 6 energy level absorbs three photons continuously and transitions to the 1 G 4 energy level; (2) the 3 H 6 energy first absorbs two photons continuously and then transitions to the 3 F 2 , then, through the cross-relaxation process 3 F 2,3 + 3 H 4 → 3 H 6 + 1 D 2 to the 1 D 2 ; (3) the non-radiation transitions from 1 G 4 , 1 D 2 of Tm 3+ to the lower energy levels 3 F 2,3,4 , 3 H 4,5,6 to achieve upconversion luminescence. From the emission spectra of NaYF 4 :Yb,Tm and NaGdF 4 :Yb,Tm in Figure 3b,d, it can be seen that different host materials NaY(Gd)F 4 will not affect the position of the emission peak, but the doping concentration of Yb 3+ ions affects the intensity of the emission peak. However, the change is not a simple linear increase or decrease with the increase or decrease in the doping ratio of Yb 3+ . obtained in the above steps was adjusted to about 6 with 20 μmol of hydrochloric acid aqueous solution, then 5 mg EDC and 5 mg NHS were added and stirred at room temperature for 25 min to let the carboxyl groups fully react with the nanoparticles. Next, the aminated DNA probe with FAM was added to a 40 μL PBS buffer to make a concentration of 100 μmol. An appropriate amount of the solution was immediately added to the carboxylated upconverted nanomaterial solution, and then put in a shaker to react for 30 min. The reaction was washed twice with PBS buffer at 10,000 rpm/min for 5 min each time, and the resulting precipitates were DNA probes with FAM linking to a carboxylated protein-modified upconverted nanomaterial fluorescent probe (DNA/dBSA /NaYF4:Yb,Tm). Figure 1 shows the energy structure and the transitions of Yb 3+ and Tm 3+ ions in the upconverting luminescence process. It can be seen that upconversion luminescence is a complex multi-photon energy transfer and conversion process. The energy level transition of 2 F7/2 → 2 F5/2 of the sensitizer Yb 3+ ion matches the energy of the near-infrared photon at 980 nm, so it can continuously absorb the excitation energy and then transfer it to the adjacent luminescent center Tm 3+ . The 3 H5, 3 F2 ( 3 F3), and 1 G4 energy levels are from Tm 3+ ions. Among them, there are three methods for upconversion luminescence: (1) the 3 H6 energy level absorbs three photons continuously and transitions to the 1 G4 energy level; (2) the 3 H6 energy first absorbs two photons continuously and then transitions to the 3 F2, then, through the cross-relaxation process 3 F2,3 + 3 H4 → 3 H6 + 1 D2 to the 1 D2; (3) the non-radiation transitions from 1 G4, 1 D2 of Tm 3+ to the lower energy levels 3 F2,3,4, 3 H4,5,6 to achieve upconversion luminescence. From the emission spectra of NaYF4:Yb,Tm and NaGdF4:Yb,Tm in Figure 3b,d, it can be seen that different host materials NaY(Gd)F4 will not affect the position of the emission peak, but the doping concentration of Yb 3+ ions affects the intensity of the emission peak. However, the change is not a simple linear increase or decrease with the increase or decrease in the doping ratio of Yb 3+ .

Effect of Yb 3+ Doping Concentration on Upconverted Nanomaterials
NaYF 4 :x%Yb 3+ , 0.5%Tm 3+ and NaGdF 4 :x%Yb 3+ , 0.5%Tm 3+ (x = 5, 10, 20, 50, 80) nanomaterials were synthesized by high-temperature thermal decomposition under the same experimental conditions by varying the doping molar fraction of Yb 3+ ions with a fixed Tm 3+ ions molar fraction of 0.5%. Figures 2 and 3 show the multi-directional characterization results of the prepared NaYF 4 :x%Yb 3+ , 0.5%Tm 3+ and NaGdF 4 :x%Yb 3+ , 0.5%Tm 3+ . As shown in Figures 2a-j and 3a-j, all the nanomaterials exhibit the characteristics of high size dispersion and good crystallinity. It can be seen from Figures 2k and 3k that NaYF4: 20%Yb 3+ , 0.5%Tm 3+ and NaGdF 4 :20%Yb 3+ , 0.5%Tm 3+ are uniform in morphology and size, forming a complete and regular hexagonal phase. Obviously, the doping concentration of Yb 3+ ions does not have much effect on the morphology of the upconverted nanomaterials. The nanomaterials with different Yb 3+ doping ratios can be synthesized with particle sizes between 25-38 nm, which lays a good foundation for the subsequent preparation of upconversion fluorescent probes. NaYF 4 :x%Yb 3+ , 0.5%Tm 3+ (x = 5, 10, 20, 50, 80) and NaGdF 4 :x%Yb 3+ , 0.5%Tm 3+ (x = 5, 10, 20, 50, 80) were subjected to phase analysis, as shown in Figures 2l and 3l, the XRD patterns were compared with standard card No.16-0994 (NaF 4 ), and the diffraction peaks obtained all corresponded to the standard card one by one, indicating that the samples obtained under this condition were all pure hexagonal NaYF 4 :Yb, Tm and NaGbF 4 :Yb, Tm. experimental conditions by varying the doping molar fraction of Yb ions with a fixed Tm 3+ ions molar fraction of 0.5 %. Figures 2 and 3 show the multi-directional characterization results of the prepared NaYF4:x%Yb 3+ , 0.5%Tm 3+ and NaGdF4:x%Yb 3+ , 0.5%Tm 3+ . As shown in Figures 2a-j and 3a-j, all the nanomaterials exhibit the characteristics of high size dispersion and good crystallinity. It can be seen from Figures 2k and 3k that NaYF4: 20%Yb 3+ , 0.5%Tm 3+ and NaGdF4:20%Yb 3+ , 0.5%Tm 3+ are uniform in morphology and size, forming a complete and regular hexagonal phase. Obviously, the doping concentration of Yb 3+ ions does not have much effect on the morphology of the upconverted nanomaterials. The nanomaterials with different Yb 3+ doping ratios can be synthesized with particle sizes between 25-38 nm, which lays a good foundation for the subsequent preparation of upconversion fluorescent probes. NaYF4:x%Yb 3+ , 0.5%Tm 3+ (x = 5, 10, 20, 50, 80) and NaGdF4:x%Yb 3+ , 0.5%Tm 3+ (x = 5, 10, 20, 50, 80) were subjected to phase analysis, as shown in Figures 2l and 3l, the XRD patterns were compared with standard card No.16-0994 (NaF4), and the diffraction peaks obtained all corresponded to the standard card one by one, indicating that the samples obtained under this condition were all pure hexagonal NaYF4:Yb, Tm and NaGbF4:Yb, Tm.     Figure 4 shows the fluorescence spectra of nanomaterials with different concentrations of Yb 3+ doping. It can be seen from Figure 4a,c that the emission peak position is not affected by the host material NaY(Gd)F4 or the doping concentration of Yb 3+ ions. The intensity of the emission peak changes as the doping ratio of Yb 3+ changes, but the change is not a simple linear increase or decrease with the increase or decrease in the doping ratio of Yb 3+ . As shown in Figure 4, the luminescence intensity at 450, 477 and 646 nm increased gradually with the increase in Yb 3+ concentration up to 20%, then the emission intensity is decreased with the increase in Yb 3+ concentration (Figure 4b,d).
Upon Yb 3+ doping, with the change in doping concentration, the number of photons absorbed at 980 nm increases, and the energy transferred to Tm 3+ ions increases, so that its luminescence is enhanced. When the concentration of Yb 3+ continues to increase, the photon energy absorbed by the Yb 3+ ions will pass through the "bridge" between Yb 3+ − Yb 3+ and surface defects. Through energy resonance transfer, the energy will be transferred to the surface defects and organic vibration groups, through the free radiation process. According to the experimental results, when the optimal Yb 3+ doping mole fraction is 20%, the luminescence reaches its peak. As shown in Figure 4, the luminescence intensity at 450, 477 and 646 nm incre gradually with the increase in Yb 3+ concentration up to 20%, then the emission inte is decreased with the increase in Yb 3+ concentration (Figure 4b,d).
Upon Yb 3+ doping, with the change in doping concentration, the number of pho absorbed at 980 nm increases, and the energy transferred to Tm 3+ ions increases, so its luminescence is enhanced. When the concentration of Yb 3+ continues to increase photon energy absorbed by the Yb 3+ ions will pass through the "bridge" between Y Yb 3+ and surface defects. Through energy resonance transfer, the energy will be t ferred to the surface defects and organic vibration groups, through the free radi process. According to the experimental results, when the optimal Yb 3+ doping mole tion is 20%, the luminescence reaches its peak.

The Effect of Tm 3+ Doping Concentration on Upconverted Nanomaterials
NaYF4:20%Yb 3+ , x%Tm 3+ and NaGdF4:20%Yb 3+ , x%Tm 3+ were synthesized by same method and conditions by varying the concentration of Tm 3+ (x = 0.2, 0.3, 0.5 1.0) while the concentration of Tb 3+ was fixed at 20%. Figures 5 and 6 show the m directional characterization results of the prepared NaYF4:20%Yb 3+ , x%Tm 3+ NaGdF4:20%Yb 3+ , x%Tm 3+ . As can be seen in Figures 5a-j and 6a-j, all the nanomate have high dispersibility in size distribution and good crystallinity. It can be seen Figures 5k and 6k that the upconverted nanomaterials have uniform morphology size, forming a regular hexagonal phase. Similarly, by changing the doping conce

The Effect of Tm 3+ Doping Concentration on Upconverted Nanomaterials
NaYF 4 :20%Yb 3+ , x%Tm 3+ and NaGdF 4 :20%Yb 3+ , x%Tm 3+ were synthesized by the same method and conditions by varying the concentration of Tm 3+ (x = 0.2, 0.3, 0.5, 0.8, 1.0) while the concentration of Tb 3+ was fixed at 20%. Figures 5 and 6 show the multi-directional characterization results of the prepared NaYF 4 :20%Yb 3+ , x%Tm 3+ and NaGdF 4 :20%Yb 3+ , x%Tm 3+ . As can be seen in Figures 5a-j and 6a-j, all the nanomaterials have high dispersibility in size distribution and good crystallinity. It can be seen from Figures 5k and 6k that the upconverted nanomaterials have uniform morphology and size, forming a regular hexagonal phase. Similarly, by changing the doping concentration of Tm 3+ , the morphology of the upconverted nanomaterials does not change too much. The particle sizes of nanomaterials with different Tm 3+ doping ratios can be between 21-43 nm. The XRD pattern of NaGdF 4 : x%Yb 3+ , 0.5%Tm 3+ (x = 0.2, 0.3, 0.5, 0.8, 1) and NaGdF 4 : 20%Yb 3+ , x%Tm 3+ (x = 0.2, 0.3, 0.5, 0.8, 1) nanomaterials was also compared with the standard card No.27-0699 (NaGdF 4 ), NaGdF 4 : Yb, Tm is a pure hexagonal phase. As shown in Figures 5l and 6l, the diffraction peaks obtained all corresponded to the standard card, which means that the samples obtained under this condition were all pure hexagonal NaYF 4 :Yb, Tm and NaGbF 4 :Yb, Tm. tion of Tm 3+ , the morphology of the upconverted nanomaterials does not change too much. The particle sizes of nanomaterials with different Tm 3+ doping ratios can be between 21-43 nm. The XRD pattern of NaGdF4: x%Yb 3+ , 0.5%Tm 3+ (x = 0.2, 0.3, 0.5, 0.8, 1) and NaGdF4: 20%Yb 3+ , x%Tm 3+ (x = 0.2, 0.3, 0.5, 0.8, 1) nanomaterials was also compared with the standard card No.27-0699 (NaGdF4), NaGdF4: Yb, Tm is a pure hexagonal phase. As shown in Figures 5l and 6l, the diffraction peaks obtained all corresponded to the standard card, which means that the samples obtained under this condition were all pure hexagonal NaYF4:Yb, Tm and NaGbF4:Yb, Tm.  The luminescence spectra of materials with different Tm 3+ concentrations are shown in Figure 7. As the mole fraction of Tm 3+ increases from 0.2% to 0.5%, the luminescence peaks at 450, 475, and 646 nm also change. As the mole fraction of Tm 3+ increases from 0.5% to 1%, the emission intensities of these three luminescence peaks gradually decrease. When the mole fraction of Tm 3+ is 0.2%, the luminescence intensity of the nano- The luminescence spectra of materials with different Tm 3+ concentrations are shown in Figure 7. As the mole fraction of Tm 3+ increases from 0.2% to 0.5%, the luminescence peaks at 450, 475, and 646 nm also change. As the mole fraction of Tm 3+ increases from 0.5% to 1%, the emission intensities of these three luminescence peaks gradually decrease. When the mole fraction of Tm 3+ is 0.2%, the luminescence intensity of the nanomaterial is not strong because there are not enough excitable Tm 3+ ions in the nanomaterials. As the concentration of Tm 3+ increases gradually, the number of excitable Tm 3+ ions increases accordingly, and the luminescence of nanomaterials becomes stronger accordingly. When the mole fraction of Tm 3+ reaches 0.5%, the upconversion luminescence intensity reaches the maximum, and then gradually becomes weaker. This is because the increase in Tm 3+ ion concentration reduces the interionic distance and strengthens the interaction. Finally, the concentration quenching effect and cross-relaxation effect are observed, resulting in a decrease in luminescence intensity. At the same time, when the sample is excited with the same power of the 980 nm laser, since the total energy is fixed, the energy that each Tm 3+ can receive will decrease with the increase in Tm 3+ , leading to the weakening of the luminescence.

Analysis of Fluorescence Characteristics Based on NaYF4:Yb 3+ , Tm 3+ Biological Probes
After the carboxylated bovine serum albumin was added to the upconverted nanomaterial sample for reaction treatment, we carried out repeated centrifugal washing on the sample to remove the carboxylated bovine serum albumin, and then measured the infrared absorption spectrum of the remaining samples, as shown in Figure 9a (the red line). As shown in Figure 9a, the broad infrared (IR) absorption peak at 3295.86 cm −1 represents the stretching vibration peak of OH in the carboxyl functional group; the sharp IR absorption peak at 1650.82 cm −1 represents the C=O formed after the reaction between the carboxylated protein and NH2-PEG group stretching vibration peak; 1024.05 cm −1 represents the stretching vibration absorption peak of -O-in PEG; 700.06 cm −1 broad absorption peak represents the out-of-plane rocking vibration absorption peak of NH in bovine serum albumin and NH2-PEG. Repeated centrifugal washing can completely remove the free carboxylated bovine serum albumin in the solution, and the upconversion material is inorganic and will not absorb at these positions. Therefore, it is considered that the new characteristic peaks belonging to organic functional groups can only come from carboxylated bovine serum proteins that have been attached to the surface of upconverted nanomaterials, which cannot be washed away. The above results prove that the surface of NaYF4:Yb 3+ , Tm 3+ nanomaterials contains many carboxyl functional groups, and the carboxylated bovine serum albumin has been successfully modified the surface of water-soluble nanomaterials. Figure 9b shows the excitation and emission spectra of DNA/dBSA/NaYF4:Yb,Tm excited at 480 nm. The excitation spectrum is from 450 nm to 490 nm, and the emission spectrum is from 510 nm to 530 nm, which is mainly the contribution of FAM. As described in Section 2.6, we carried out repeated centrifugal washing to fully wash the excess DNA, and then obtained the fluorescence spectrum in Figure 9c. As shown in Figure 9c, when the DNA/dBSA/NaYF4:Yb,Tm fluorescent probes were excited at 480 nm, a strong emission

Analysis of Fluorescence Characteristics Based on NaYF 4 :Yb 3+ , Tm 3+ Biological Probes
After the carboxylated bovine serum albumin was added to the upconverted nanomaterial sample for reaction treatment, we carried out repeated centrifugal washing on the sample to remove the carboxylated bovine serum albumin, and then measured the infrared absorption spectrum of the remaining samples, as shown in Figure 9a (the red line). As shown in Figure 9a, the broad infrared (IR) absorption peak at 3295.86 cm −1 represents the stretching vibration peak of OH in the carboxyl functional group; the sharp IR absorption peak at 1650.82 cm −1 represents the C=O formed after the reaction between the carboxylated protein and NH 2 -PEG group stretching vibration peak; 1024.05 cm −1 represents the stretching vibration absorption peak of -O-in PEG; 700.06 cm −1 broad absorption peak represents the out-of-plane rocking vibration absorption peak of NH in bovine serum albumin and NH 2 -PEG. Repeated centrifugal washing can completely remove the free carboxylated bovine serum albumin in the solution, and the upconversion material is inorganic and will not absorb at these positions. Therefore, it is considered that the new characteristic peaks belonging to organic functional groups can only come from carboxylated bovine serum proteins that have been attached to the surface of upconverted nanomaterials, which cannot be washed away. The above results prove that the surface of NaYF 4 :Yb 3+ , Tm 3+ nanomaterials contains many carboxyl functional groups, and the carboxylated bovine serum albumin has been successfully modified the surface of water-soluble nanomaterials. Figure 9b shows the excitation and emission spectra of DNA/dBSA/NaYF 4 :Yb,Tm excited at 480 nm. The excitation spectrum is from 450 nm to 490 nm, and the emission spectrum is from 510 nm to 530 nm, which is mainly the contribution of FAM. As described in Section 2.6, we carried out repeated centrifugal washing to fully wash the excess DNA, and then obtained the fluorescence spectrum in Figure 9c. As shown in Figure 9c, when the DNA/dBSA/NaYF 4 :Yb,Tm fluorescent probes were excited at 480 nm, a strong emission peak is observed at 520 nm, which is consistent with the FAM fluorescence peak. It indicates that some DNA strands were not washed away due to their attachment to the carboxylated protein-modified upconversion material, namely DNA was attached successfully to the surfaces of UCNP via a protein and a FAM was added to the UCNP/DNA complex. Similarly, NaYF 4 :Yb,Tm and DNA/dBSA/NaYF 4 :Yb,Tm was excited at 980 nm, and the upconversion intensity of the luminescence is quite strong, as shown in Figure 9d. These nanocomposites have strong upconversion luminescence with good water solubility and biocompatibility, making them a new type of fluorescent probe.

Fluorescent Probes for the Detection of Different Proteins
To test the detection of these upconverted nanomaterials for protein detection, 100 pM solutions of miRNA-155, single-base mismatch of miRNA-155, double-base mismatch of miRNA-155, complete-base mismatch of miRNA-155 and miRNA-150 solution with the same concentration of 100 pM were prepared, respectively. The prepared nucleotide sequences of miRNAs and fluorescent probes are shown in Table 1. The prepared fluorescent probes of upconverted nanomaterials were tested with different miR-NAs and mismatched miRNAs, and the samples were excited by a fiber laser with a wavelength of 980 nm and their fluorescence spectra were measured.

Fluorescent Probes for the Detection of Different Proteins
To test the detection of these upconverted nanomaterials for protein detection, 100 pM solutions of miRNA-155, single-base mismatch of miRNA-155, double-base mismatch of miRNA-155, complete-base mismatch of miRNA-155 and miRNA-150 solution with the same concentration of 100 pM were prepared, respectively. The prepared nucleotide sequences of miRNAs and fluorescent probes are shown in Table 1. The prepared fluorescent probes of upconverted nanomaterials were tested with different miRNAs and mismatched miRNAs, and the samples were excited by a fiber laser with a wavelength of 980 nm and their fluorescence spectra were measured. As shown in Figure 10, the fluorescence spectrum of the fluorescent probe after connecting different miRNA-155 changed significantly. In general, the fluorescence spectra of the four groups were very similar, and the fluorescence intensity decreased significantly (compared with Figure 9d). The sample added with miRNA-155 had the strongest fluorescence intensity. The more mismatched bases, the more obvious fluorescence quenching and the smaller spectral intensity. It is worth noting that the fluorescence quenching at 345 nm, 362 nm, 450 nm, 477 nm and 646 nm is more obvious than that at 802 nm.
Nanomaterials 2022, 12, x FOR PEER REVIEW 1 As shown in Figure 10, the fluorescence spectrum of the fluorescent probe connecting different miRNA-155 changed significantly. In general, the fluorescence tra of the four groups were very similar, and the fluorescence intensity decreased s icantly (compared with Figure 9d). The sample added with miRNA-155 had the st est fluorescence intensity. The more mismatched bases, the more obvious fluores quenching and the smaller spectral intensity. It is worth noting that the fluores quenching at 345 nm, 362 nm, 450 nm, 477 nm and 646 nm is more obvious than th 802 nm. We divided the peak intensity at 802 nm (I802) by the peak intensity at 345 nm 362 nm (I362), 450 nm (I450), 477 nm (I477) and 646 nm (I646) to calculate a group of flu cence peak ratios for further analysis of the differences in fluorescence spectra of ples with different miRNA-155s. The results are shown in Table 2. As can be seen i ble 2, the five peak ratios of the fluorescent probes are very close to those of the u verted nanomaterials; then, the value of the completely mismatched miRNA155 is tively close to that of the upconverted nanomaterials, and intact miRNA-155 ha greatest effect on all five peak ratios. It seems that the completely mismatched miR 155 has little effect on the peak ratios, and the intact miRNA-155 has the greatest on the peak ratios. This result may be that miRNAs with different sequences have d ent effects on different molecular bonds of upconverted nanomaterials. It is believed these peak ratios can be used for specific recognition of miRNA-155. For fluore probes with multiple emission peaks, in addition to identifying the target substan simply comparing the changes in peak intensity, the ratios between peaks can al used for substance-specific identification. The fluorescence probe with multiple emi peaks provides more abundant optical information for the study of the characte changes of the detected object and has great application potential.  We divided the peak intensity at 802 nm (I 802 ) by the peak intensity at 345 nm (I 345 ), 362 nm (I 362 ), 450 nm (I 450 ), 477 nm (I 477 ) and 646 nm (I 646 ) to calculate a group of fluorescence peak ratios for further analysis of the differences in fluorescence spectra of samples with different miRNA-155s. The results are shown in Table 2. As can be seen in Table 2, the five peak ratios of the fluorescent probes are very close to those of the upconverted nanomaterials; then, the value of the completely mismatched miRNA155 is relatively close to that of the upconverted nanomaterials, and intact miRNA-155 had the greatest effect on all five peak ratios. It seems that the completely mismatched miRNA-155 has little effect on the peak ratios, and the intact miRNA-155 has the greatest effect on the peak ratios. This result may be that miRNAs with different sequences have different effects on different molecular bonds of upconverted nanomaterials. It is believed that these peak ratios can be used for specific recognition of miRNA-155. For fluorescent probes with multiple emission peaks, in addition to identifying the target substance by simply comparing the changes in peak intensity, the ratios between peaks can also be used for substance-specific identification. The fluorescence probe with multiple emission peaks provides more abundant optical information for the study of the characteristic changes of the detected object and has great application potential. As shown in Figure 11, when the fluorescent probes were connected to miRNA-155 and miRNA-150, respectively, the fluorescence intensity of miRNA-155 was higher than that of miRNA-150. The experimental results show that the fluorescent probe can effectively distinguish different types of miRNAs. As shown in Figure 11, when the fluorescent probes were connected to miRNAand miRNA-150, respectively, the fluorescence intensity of miRNA-155 was higher th that of miRNA-150. The experimental results show that the fluorescent probe can ef tively distinguish different types of miRNAs.

Conclusions
In this paper, a novel NaYF4:Yb,Tm surface-functionalized fluorescent probe w proposed based on upconverted nanomaterials. Quantitative analysis of the effects Yb 3+ and Tm 3+ ion concentrations on the morphology, size, and luminescence proper of NaYF4:Yb,Tm and NaGdF4:Yb,Tm indicated that the optimal doping concentration tio of Yb 3+ :Tm 3+ is 40: 1. In the study, by comparing the fluorescence emission of NaY 20% Yb, 0.5% Tm and NaGdF4: 20% Yb, 0.5% Tm, upconverted nanomaterials with b ter luminescence properties were obtained. A novel fluorescent probe was designed the surface carboxylation of NaYF4:Yb,Tm and the connection with amino group a DNA. The probe can be used for the detection of different specific biological miRN When the fluorescent probes are used to detect different miRNAs, they can distingu different miRNAs, especially miRNAs with base mismatches, from non-specific R molecular analytes. The preliminary studies indicate that the upconverted probes hav good potential for protein detection in early cancer diagnosis.
Author Contributions: Conceptualization, Instruction, Funding and Writing: Y.L., L.Z. and W Experimental design and processing: Z.D.; Material Characterization, data analysis and sim

Conclusions
In this paper, a novel NaYF 4 :Yb,Tm surface-functionalized fluorescent probe was proposed based on upconverted nanomaterials. Quantitative analysis of the effects of Yb 3+ and Tm 3+ ion concentrations on the morphology, size, and luminescence properties of NaYF 4 :Yb,Tm and NaGdF 4 :Yb,Tm indicated that the optimal doping concentration ratio of Yb 3+ :Tm 3+ is 40:1. In the study, by comparing the fluorescence emission of NaYF 4 : 20% Yb, 0.5% Tm and NaGdF 4 : 20% Yb, 0.5% Tm, upconverted nanomaterials with better luminescence properties were obtained. A novel fluorescent probe was designed for the surface carboxylation of NaYF 4 :Yb,Tm and the connection with amino group and DNA. The probe can be used for the detection of different specific biological miRNAs. When the fluorescent probes are used to detect different miRNAs, they can distinguish different miRNAs, especially miRNAs with base mismatches, from non-specific RNA molecular analytes. The preliminary studies indicate that the upconverted probes have a good potential for protein detection in early cancer diagnosis.