Upconversion Luminescent Humidity Sensors Based on Lanthanide-Doped MOFs

: Lanthanide-doped metal-organic frameworks (Y/Yb/Er-MOF) were synthesized by a low-cost solvothermal method. The obtained Y/Yb/Er-MOF shows the cooperative upconversion luminescence of Yb 3+ and upconversion luminescence of Er 3+ (Yb 3+ -sensitized) irradiated by a continuous wave 980 nm laser. In order to explore the potential application of Y/Yb/Er-MOF in relative humidity (RH) sensors, the RH responsiveness of Y/Yb/Er-MOF was investigated by measuring the intensity changes of upconversion luminescence. The Y/Yb/Er-MOF possesses two luminescence centers, in which Yb 3+ forms emission at 500 nm through the cooperative luminescence effect, and Er 3+ achieves 660 nm emission through excited state absorption and successive energy transfer from Yb 3+ . Hence, the ratio meter luminescence sensor for RH is constructed based on Y/Yb/Er-MOF. The results show that the response of Y/Yb/Er-MOF to RH presents a linear relationship in the range of 11–95%. The cycle stability of Y/Yb/Er-MOF responses to RH was investigated with the intensity changes of upconversion luminescence, and the recovery ratio was more than 93% each time. Therefore, the Y/Yb/Er-MOF is a humidity-sensitive material with great potential for applications such as humidity sensors.


Introduction
Humidity is a physical quantity that indicates the degree of air dryness. The less water vapor in a certain air volume at a certain temperature, the drier the air; the more water vapor, the more humid. Humidity is often expressed by relative humidity (RH), comparative humidity, mixing ratio, saturation difference, and dew point. Especially, RH is the ratio percentage of the actual water vapor pressure in the air to the saturated water vapor pressure at the current temperature, which is also the most common form of humidity. The RH of 50% air contains half as much water vapor as the saturation point at the same temperature. Air with an RH of 100% is saturated with water vapor. Water vapor in the air generally condenses out when the relative humidity exceeds 100%.
Humidity sensors are widely used in industry, agriculture, food and pharmaceutical storage, meteorology, medical health, aviation, etc. [1][2][3][4]. Due to the difference in the application environment, various types of humidity sensors have been developed to satisfy the requirements of different applications. Common humidity sensors can be divided into two main categories according to the signal used to transmit information: electronic and optical [5]. Materials used to construct humidity sensors typically include ceramics, semiconductors, and polymers, each with different advantages and limitations [6][7][8]. Opticsbased humidity sensors are generally more sensitive than electronic-based ones and can be tailored to different application environments with the well-known advantages of electromagnetic interference resistance and electrical inertia [5]. However, at present, the development of humidity sensing materials with high sensitivity to a wide range of humidities remains a major challenge.
Metal-organic framework materials (MOFs) are a type of coordination polymer that developed rapidly in the past two decades. MOFs usually possess a three-dimensional pore structure, with metal ions as the connection point and organic ligands to support to form three-dimensional spatial extension. MOFs are a type of important new porous material widely used in catalysis, energy storage, and separation. Lanthanide-doped MOFs are one of the most promising luminescence materials for humidity sensors, which possess the properties of large specific surface area and structural stability of MOFs and retain the unique luminescent properties of lanthanides [9,10]. The large specific surface area benefits from interacting more effectively with analytes (e.g., water molecules) for MOFs, thus improving the sensitivity and response speed of the sensor [11][12][13]. Lanthanide ions exhibit visible luminescence with narrow emission bands and high color purity due to their unique electronic structure, abundant electron energy levels, and long-life excited states [14,15]. Therefore, lanthanide-doped MOFs have attracted much attention as an attractive candidate material that can be used to develop humidity sensors.
Photoluminescence is a luminescence phenomenon produced by the excitation of a luminescent material with ultraviolet, visible, or near-infrared light. The lanthanide luminescence phenomenon can be divided into upconversion luminescence and downshifting luminescence depending on the difference between the excitation wavelength and the corresponding emitted light [16][17][18]. Upconversion luminescence, an anti-Stokes luminescence phenomenon, refers to the material being irradiated by low-energy light and emitting with high-energy light. Conversely, downshifting luminescence occurs [19,20]. In addition, the lanthanide luminescence is closely related to the chemical environment in which the luminescent center is located, as such the surrounding high-energy O−H, N−H, and C−H vibrations will affect the luminescence intensity [21][22][23]. Based on this phenomenon, it is possible to design and synthesize optical sensors for small molecule species (e.g., water). Currently, those reported on lanthanide-doped MOFs as humidity sensing materials are usually a downshifting luminescence process using high-energy light excitation to emit low-energy light [24,25]. In contrast, the upconversion luminescence of lanthanide-doped MOFs is rarely reported, especially for humidity sensor application.
Herein, we develop an upconversion luminescence humidity sensor based on the designed and synthesized Y/Yb/Er-MOF. Luminescence sensing over a wide RH range (11-95%) is achieved using the variation of upconversion luminescence intensity of Y/Yb/Er-MOF. The cycle stability is good based on the intensity changes of upconversion luminescence, and the recovery ratio is more than 93% each time.

Materials and Methods
All chemical materials and characterizations used in this work are listed in the Supporting Information.

Synthesis of Lanthanide-Doped MOFs (Denoted as Y/Yb/Er-MOF)
Y/Yb/Er-MOF was synthesized by the hydrothermal method. A mixture of 2 mmol LnCl 3 (Y 3+ :Yb 3+ :Er 3+ = 78:20:2), 1 mmol 1,3,5-benzenetricarboxylate (BTC), 16 mL dimethylformamide (DMF), and 8 mL deionized water were added to a 50 mL Teflon-lined autoclave, stirring for 2 h at room temperature. Afterward, the Teflon-lined autoclave was sealed and heated at 150 • C for 12 h and then naturally cooled down to room temperature. The resulting mixture was filtered via suction filtration and washed with DMF and ethanol, respectively, until all remaining precursors and by-products were removed. The final product was dried in a vacuum oven at 80 • C for 12 h.

Y/Yb/Er-MOF Responses to Different RH Environments
The obtained Y/Yb/Er-MOF was fully ground and placed in a sample tank of solid powder, and then the Y/Yb/Er-MOF was dried under the oven at 110 • C for 1 h. Different supersaturated aqueous solutions controlled the different RH environments at room temperature. The supersaturated aqueous solutions of LiCl, MgCl 2 , Mg(NO 3 ) 2 , NaCl, KCl, and KNO 3 at room temperature were obtained and separately kept in six closed conical flasks (250 mL). The corresponding RH was determined with a humidity meter as 11%, 33%, 54%, 75%, 85%, and 95%, respectively [26][27][28]. In order to obtain reliable RH sensing performance, Y/Yb/Er-MOF was placed directly in a flask with different RH after vacuum drying. After being kept for 30 min, it was quickly removed and placed into the spectrometer to obtain the corresponding upconversion luminescence spectrum.

Characterization of Structural Properties
The morphology of Y/Yb/Er-MOF was characterized by scanning electron microscopy (SEM) and transmission electron microscopy (TEM), as shown in Figure 1a and Figure S1, respectively. It shows that Y/Yb/Er-MOF present a rectangular prismatic morphology with an average particle size of around 20 µm. X-ray diffraction (XRD) spectra were used to analyze the crystal structure of the synthesized Y/Yb/Er-MOF. As shown in Figure 1b, the diffraction pattern of Y/Yb/Er-MOF is consistent with the previous results of Y-BTC-MOF [29], indicating that the crystal structure of BTC-MOFs matrix material is unchanged after being doped with Yb 3+ and Er 3+ . The crystal structures of Y/Yb/Er-MOF, in this case, and Y-BTC-MOF, are isomorphic and can be attributed to the tetragonal crystal system. The lanthanide ions are coordinated with O atoms from BTC. In this way, the MOFs structure is constructed [29]. In addition, energy dispersive spectroscopy (EDS) point scanning (inset of Figure 1a), as well as elemental mapping images of Y/Yb/Er-MOF (Figure 1c), were used to investigate the chemical composition and elemental distribution of Y/Yb/Er-MOF. The results provided further evidence that the elements of C, O, Y, Yb, and Er exist in Y/Yb/Er-MOF. Furthermore, the EDS (inset of Figure 1a) results showed that the elements of C, O, Y, Yb, Er, and Pt exist in the Y/Yb/Er-MOF, of which the Pt element is caused by spraying platinum during the SEM measurement process.
The resulting mixture was filtered via suction filtration and washed with DMF and ethanol, respectively, until all remaining precursors and by-products were removed. The final product was dried in a vacuum oven at 80 °C for 12 h.

Y/Yb/Er-MOF Responses to Different RH Environments
The obtained Y/Yb/Er-MOF was fully ground and placed in a sample tank of solid powder, and then the Y/Yb/Er-MOF was dried under the oven at 110 °C for 1 h. Different supersaturated aqueous solutions controlled the different RH environments at room temperature. The supersaturated aqueous solutions of LiCl, MgCl2, Mg(NO3)2, NaCl, KCl, and KNO3 at room temperature were obtained and separately kept in six closed conical flasks (250 mL). The corresponding RH was determined with a humidity meter as 11%, 33%, 54%, 75%, 85%, and 95%, respectively [26][27][28]. In order to obtain reliable RH sensing performance, Y/Yb/Er-MOF was placed directly in a flask with different RH after vacuum drying. After being kept for 30 min, it was quickly removed and placed into the spectrometer to obtain the corresponding upconversion luminescence spectrum.

Characterization of Structural Properties
The morphology of Y/Yb/Er-MOF was characterized by scanning electron microscopy (SEM) and transmission electron microscopy (TEM), as shown in Figure 1a and Figure S1, respectively. It shows that Y/Yb/Er-MOF present a rectangular prismatic morphology with an average particle size of around 20 μm. X-ray diffraction (XRD) spectra were used to analyze the crystal structure of the synthesized Y/Yb/Er-MOF. As shown in Figure 1b, the diffraction pattern of Y/Yb/Er-MOF is consistent with the previous results of Y-BTC-MOF [29], indicating that the crystal structure of BTC-MOFs matrix material is unchanged after being doped with Yb 3+ and Er 3+ . The crystal structures of Y/Yb/Er-MOF, in this case, and Y-BTC-MOF, are isomorphic and can be attributed to the tetragonal crystal system. The lanthanide ions are coordinated with O atoms from BTC. In this way, the MOFs structure is constructed [29]. In addition, energy dispersive spectroscopy (EDS) point scanning (inset of Figure 1a), as well as elemental mapping images of Y/Yb/Er-MOF (Figure 1c), were used to investigate the chemical composition and elemental distribution of Y/Yb/Er-MOF. The results provided further evidence that the elements of C, O, Y, Yb, and Er exist in Y/Yb/Er-MOF. Furthermore, the EDS (inset of Figure 1a) results showed that the elements of C, O, Y, Yb, Er, and Pt exist in the Y/Yb/Er-MOF, of which the Pt element is caused by spraying platinum during the SEM measurement process.   Figure S2 display the Fourier transform infrared spectra (FTIR) of Y/Yb/Er-MOF and BTC. The spectrum of Y/Yb/Er-MOF shows the characteristic peaks of dimethylformamide (DMF). The peaks observed at 2960 and 2880 cm −1 can be attributed to the asymmetric stretching vibration and symmetric stretching vibration of the methyl group, respectively. Furthermore, the peak at 1640 cm −1 corresponds to the carbonyl group of DMF and BTC. The wide peak at 3450 cm −1 is attributed to the −OH vibration of H 2 O, indicating that Y/Yb/Er-MOF contains H 2 O molecules. The peak at 1100 cm −1 can be attributed to the C−C planar skeleton vibration of the aromatic ring, suggesting the presence of the BTC linker [29].

Upconversion Luminescence of Y/Yb/Er-MOF
The UV-vis absorption spectra of Y/Yb/Er-MOF and BTC are shown in Figure S3. The spectrum of Y/Yb/Er-MOF retains the same absorption peak with BTC, yet a new peak appears around 980 nm, caused by the participation of Yb 3+ and Er 3+ in forming the MOFs structure. Considering the absorption of Y/Yb/Er-MOF in the near-infrared (NIR) band, we deduce that the Y/Yb/Er-MOF can be excited by the NIR laser to obtain the corresponding upconversion luminescence spectrum. As expected, Figure 2a show the upconversion luminescence spectrum of Y/Yb/Er-MOF irradiated by a continuous wave 980 nm laser, which shows three characteristic peaks at 500 nm, 520 nm, and 660 nm of lanthanide ions, respectively.  Figure S2 display the Fourier transform infrared spectra (FTIR) of Y/Yb/Er-MOF and BTC. The spectrum of Y/Yb/Er-MOF shows the characteristic peaks of dimethylformamide (DMF). The peaks observed at 2960 and 2880 cm −1 can be attributed to the asymmetric stretching vibration and symmetric stretching vibration of the methyl group, respectively. Furthermore, the peak at 1640 cm −1 corresponds to the carbonyl group of DMF and BTC. The wide peak at 3450 cm −1 is attributed to the −OH vibration of H2O, indicating that Y/Yb/Er-MOF contains H2O molecules. The peak at 1100 cm −1 can be attributed to the C−C planar skeleton vibration of the aromatic ring, suggesting the presence of the BTC linker [29].

Upconversion Luminescence of Y/Yb/Er-MOF
The UV-vis absorption spectra of Y/Yb/Er-MOF and BTC are shown in Figure S3. The spectrum of Y/Yb/Er-MOF retains the same absorption peak with BTC, yet a new peak appears around 980 nm, caused by the participation of Yb 3+ and Er 3+ in forming the MOFs structure. Considering the absorption of Y/Yb/Er-MOF in the near-infrared (NIR) band, we deduce that the Y/Yb/Er-MOF can be excited by the NIR laser to obtain the corresponding upconversion luminescence spectrum. As expected, Figure 2a show the upconversion luminescence spectrum of Y/Yb/Er-MOF irradiated by a continuous wave 980 nm laser, which shows three characteristic peaks at 500 nm, 520 nm, and 660 nm of lanthanide ions, respectively. The emission peak is observed in the visible region with the maximum emission peak at around 500 nm, caused by the cooperative luminescence of Yb 3+ clusters. Cooperative luminescence usually describes the process by which a pair of ions emit a single photon by simultaneous reduction from its excited state. Cooperative luminescence represents a special type of electron transition that occurs in a spectral region where a single ion has no absorption or emission. Cooperative luminescence was first demonstrated in 1970 with a pair of excited Yb 3+ ions [30]. Since then, the Yb 3+ -dimers have been widely explored for applications due to their unique electron configuration, such as scintillators, solid struc- The emission peak is observed in the visible region with the maximum emission peak at around 500 nm, caused by the cooperative luminescence of Yb 3+ clusters. Cooperative luminescence usually describes the process by which a pair of ions emit a single photon by simultaneous reduction from its excited state. Cooperative luminescence represents a special type of electron transition that occurs in a spectral region where a single ion has no absorption or emission. Cooperative luminescence was first demonstrated in 1970 with a pair of excited Yb 3+ ions [30]. Since then, the Yb 3+ -dimers have been widely explored for applications due to their unique electron configuration, such as scintillators, solid structure probes, and optical bistability [31][32][33][34][35][36]. In order to determine the origin of the upconversion luminescence signal, in this case, the upconversion luminescence intensity was recorded as a function of excitation power density (Figure 3a) by a conventional Log/Log curve with a linear fit slope of 2.2 (Figure 3b), indicating a two-photon process that is expected for Yb 3+ -dimers.
Chemosensors 2022, 10, x 5 of 9 ture probes, and optical bistability [31][32][33][34][35][36]. In order to determine the origin of the upconversion luminescence signal, in this case, the upconversion luminescence intensity was recorded as a function of excitation power density (Figure 3a) by a conventional Log/Log curve with a linear fit slope of 2.2 (Figure 3b), indicating a two-photon process that is expected for Yb 3+ -dimers. In addition, the upconversion luminescence spectrum of Y/Yb/Er-MOF (Figure 2a) shows characteristic emission peaks (520 nm and 660 nm) of Er 3+ ions. As shown in Figure  2b, after being irradiated by a continuous wave 980 nm laser, Yb 3+ in Y/Yb/Er-MOF absorbs energy and occupies the excited state 2 F5/2. Subsequently, the non-radiant energy transfer occurs between the excited state of Yb 3+ and the ground state of Er 3+ ( 4 I15/2). After that, Er 3+ achieves the excited state ( 4 I15/2 → 4 I11/2), and Yb 3+ returns to the ground state ( 2 F7/2). Due to its unique outermost electron configuration, the Er 3+ ion possesses abundant energy levels corresponding to the different excited states. The excited Er 3+ can be further pumped to a higher energy level excited state through excited state absorption and successive energy transfer from Yb 3+ , thus forming emissions at 520 nm ( 2 H11/2 → 4 I15/2) and 660 nm ( 4 F9/2 → 4 I15/2). Therefore, as presented in Figure 2a, there are two luminescence centers during the upconversion luminescence process of Y/Yb/Er-MOF. One luminescence center is Yb 3+ , which forms emission at 500 nm through the cooperative luminescence effect. The other luminescence center is Er 3+ , which results in emissions at 520 and 660 nm that are sensitized by the Yb 3+ ion.

Response of Y/Yb/Er-MOF to Relative Humidity (RH)
As mentioned above, the three emission peaks of the upconversion luminescence of Y/Yb/Er-MOF are composed by the cooperative luminescence effect of Yb 3+ (500 nm) and the upconversion luminescence of Er 3+ center (520 and 620 nm), respectively. Therefore, it can be deduced that the luminescence process can be divided into two stages. The first stage is from the ground state ( 2 F7/2) to the excited state ( 2 F5/2) of Yb 3+ after irradiation by a 980 nm laser. The second stage is that the excited state ( 2 F5/2) of Yb 3+ transmits the energy to realize its own cooperative luminescence and sensitizes the upconversion luminescence of Er 3+ . The surrounding chemical environment of the luminescence centers will affect the energy transfer process during the second stage. If there are water molecules around Yb 3+ , the vibration of −OH with high energy will absorb part of the energy transferred from the excited state of Yb 3+ , which will quench the upconversion luminescence of Y/Yb/Er-MOF. In addition, the upconversion luminescence spectrum of Y/Yb/Er-MOF (Figure 2a) shows characteristic emission peaks (520 nm and 660 nm) of Er 3+ ions. As shown in Figure 2b, after being irradiated by a continuous wave 980 nm laser, Yb 3+ in Y/Yb/Er-MOF absorbs energy and occupies the excited state 2 F 5/2 . Subsequently, the non-radiant energy transfer occurs between the excited state of Yb 3+ and the ground state of Er 3+ ( 4 I 15/2 ). After that, Er 3+ achieves the excited state ( 4 I 15/2 → 4 I 11/2 ), and Yb 3+ returns to the ground state ( 2 F 7/2 ). Due to its unique outermost electron configuration, the Er 3+ ion possesses abundant energy levels corresponding to the different excited states. The excited Er 3+ can be further pumped to a higher energy level excited state through excited state absorption and successive energy transfer from Yb 3+ , thus forming emissions at 520 nm ( 2 H 11/2 → 4 I 15/2 ) and 660 nm ( 4 F 9/2 → 4 I 15/2 ). Therefore, as presented in Figure 2a, there are two luminescence centers during the upconversion luminescence process of Y/Yb/Er-MOF. One luminescence center is Yb 3+ , which forms emission at 500 nm through the cooperative luminescence effect. The other luminescence center is Er 3+ , which results in emissions at 520 and 660 nm that are sensitized by the Yb 3+ ion.

Response of Y/Yb/Er-MOF to Relative Humidity (RH)
As mentioned above, the three emission peaks of the upconversion luminescence of Y/Yb/Er-MOF are composed by the cooperative luminescence effect of Yb 3+ (500 nm) and the upconversion luminescence of Er 3+ center (520 and 620 nm), respectively. Therefore, it can be deduced that the luminescence process can be divided into two stages. The first stage is from the ground state ( 2 F 7/2 ) to the excited state ( 2 F 5/2 ) of Yb 3+ after irradiation by a 980 nm laser. The second stage is that the excited state ( 2 F 5/2 ) of Yb 3+ transmits the energy to realize its own cooperative luminescence and sensitizes the upconversion luminescence of Er 3+ . The surrounding chemical environment of the luminescence centers will affect the energy transfer process during the second stage. If there are water molecules around Yb 3+ , the vibration of −OH with high energy will absorb part of the energy transferred from the excited state of Yb 3+ , which will quench the upconversion luminescence of Y/Yb/Er-MOF.
Moreover, the three-dimensional pore structure of the MOFs can allow the water molecules to enter the pore and uniform the distribution of water molecules around the lanthanide ions. Thus, based on the above analysis, an optical humidity sensor can be constructed using the Y/Yb/Er-MOF.
Then, the response of Y/Yb/Er-MOF to RH was investigated by measuring the upconversion luminescence spectra of Y/Yb/Er-MOF in different RH environments. Figure 4a show the real-time response of the spectra of Y/Yb/Er-MOF with different RH environments. The emission intensity at 500 and 660 nm gradually decreases with the rise of RH, which is displayed in a linear dose-dependent manner (Figure 4b,c). It can be deduced that the Y/Yb/Er-MOF can respond to different RH environments in the RH range of 11-95%.
Chemosensors 2022, 10, x 6 of 9 Moreover, the three-dimensional pore structure of the MOFs can allow the water molecules to enter the pore and uniform the distribution of water molecules around the lanthanide ions. Thus, based on the above analysis, an optical humidity sensor can be constructed using the Y/Yb/Er-MOF. Then, the response of Y/Yb/Er-MOF to RH was investigated by measuring the upconversion luminescence spectra of Y/Yb/Er-MOF in different RH environments. Figure  4a show the real-time response of the spectra of Y/Yb/Er-MOF with different RH environments. The emission intensity at 500 and 660 nm gradually decreases with the rise of RH, which is displayed in a linear dose-dependent manner (Figure 4b,c). It can be deduced that the Y/Yb/Er-MOF can respond to different RH environments in the RH range of 11-95%. The slopes of the linear relationship are different with the recorded upconversion luminescence intensity at 500 and 660 nm, respectively, indicating that the intensity at 660 nm is more sensitive to RH than that at 500 nm, which is consistent with the discussion of the Er 3+ luminescence mechanism. As mentioned above, the upconversion luminescence at 660 nm is the characteristic emission of Er 3+ ions, and the upconversion process is sensitized by Yb 3+ . Thus, based on the different slopes, the linear relationship between different RH and corresponding luminescence intensity ratios of I500/I660 is plotted (Figure 4d). The slopes of the linear relationship are different with the recorded upconversion luminescence intensity at 500 and 660 nm, respectively, indicating that the intensity at 660 nm is more sensitive to RH than that at 500 nm, which is consistent with the discussion of the Er 3+ luminescence mechanism. As mentioned above, the upconversion luminescence at 660 nm is the characteristic emission of Er 3+ ions, and the upconversion process is sensitized by Yb 3+ . Thus, based on the different slopes, the linear relationship between different RH and corresponding luminescence intensity ratios of I 500 /I 660 is plotted (Figure 4d).
The result shows that the Y/Yb/Er-MOF constructs a ratio meter sensor for RH based on upconversion luminescence. Furthermore, the cycle stability of Y/Yb/Er-MOF was investigated by measuring the upconversion luminescence spectra of Y/Yb/Er-MOF with and without the 95% RH environment, respectively. With 95% RH, the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was kept in a 95% RH environment for 30 min. Without 95% RH denotes that the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was dried under the oven at 110 • C for 1 h. This kind of cycle was repeated 10 times, as shown in Figure 5, and recorded for the luminescence intensity at both 500 nm and 660 nm. The recovery ratio of each cycle is more than 93% each time.
The results indicate that the cycle stability of the Y/Yb/Er-MOF response to RH is excellent. Thus, Y/Yb/Er-MOF can be a desirable candidate for luminescence materials for humidity sensors. The result shows that the Y/Yb/Er-MOF constructs a ratio meter sensor for RH based on upconversion luminescence. Furthermore, the cycle stability of Y/Yb/Er-MOF was investigated by measuring the upconversion luminescence spectra of Y/Yb/Er-MOF with and without the 95% RH environment, respectively. With 95% RH, the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was kept in a 95% RH environment for 30 min. Without 95% RH denotes that the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was dried under the oven at 110 °C for 1 h. This kind of cycle was repeated 10 times, as shown in Figure 5, and recorded for the luminescence intensity at both 500 nm and 660 nm. The recovery ratio of each cycle is more than 93% each time. The results indicate that the cycle stability of the Y/Yb/Er-MOF response to RH is excellent. Thus, Y/Yb/Er-MOF can be a desirable candidate for luminescence materials for humidity sensors. Figure 5. The cycle stability of Y/Yb/Er-MOF responds to relative humidity (RH). With 95% RH, the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was kept in a 95% RH environment for 30 min. Without 95% RH means the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was dried under the oven at 110 °C for 1 h. The upconversion luminescence intensities were recorded at 500 nm (a) and 660 nm (b) for ten cycles, respectively.

Conclusions
In summary, we have demonstrated a luminescence humidity sensor based on lanthanide-doped MOFs using upconversion luminescence signals in response to relative humidity changes. The Y/Yb/Er-MOF was synthesized by the solvothermal method. With the two luminescence centers (Yb 3+ and Er 3+ ) during the upconversion process, a ratio meter luminescence sensor for RH is constructed based on Y/Yb/Er-MOF. An analysis of the upconversion luminescence spectra shows that Y/Yb/Er-MOF is able to respond linearly to RH in the range of 11-95% with wonderful cycle stability. The recovery ratio of each cycle is more than 93% each time. The excellent humidity sensing performance of Y/Yb/Er-MOF is caused by the framework structure of MOFs and the sensitivity of lanthanide luminescence to the environment. Therefore, this work makes lanthanide-doped Y/Yb/Er-MOF attractive as an effective optical humidity sensor for humidity detection, which will broaden the applications of lanthanide-doped MOFs materials.
Supplementary Materials: The followings are available online at www.mdpi.com/xxx/s1, Figure  S1: Transmission electron microscopy images of Y/Yb/Er-MOF with different magnifications; Figure  S2: Fourier transform infrared spectroscopy spectra of Y/Yb/Er-MOF and BTC; Figure S3: The UVvisible absorption spectra of Y/Yb/Er-MOF and BTC. Figure 5. The cycle stability of Y/Yb/Er-MOF responds to relative humidity (RH). With 95% RH, the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was kept in a 95% RH environment for 30 min. Without 95% RH means the upconversion luminescence intensity was recorded after the Y/Yb/Er-MOF was dried under the oven at 110 • C for 1 h. The upconversion luminescence intensities were recorded at 500 nm (a) and 660 nm (b) for ten cycles, respectively.

Conclusions
In summary, we have demonstrated a luminescence humidity sensor based on lanthanidedoped MOFs using upconversion luminescence signals in response to relative humidity changes. The Y/Yb/Er-MOF was synthesized by the solvothermal method. With the two luminescence centers (Yb 3+ and Er 3+ ) during the upconversion process, a ratio meter luminescence sensor for RH is constructed based on Y/Yb/Er-MOF. An analysis of the upconversion luminescence spectra shows that Y/Yb/Er-MOF is able to respond linearly to RH in the range of 11-95% with wonderful cycle stability. The recovery ratio of each cycle is more than 93% each time. The excellent humidity sensing performance of Y/Yb/Er-MOF is caused by the framework structure of MOFs and the sensitivity of lanthanide luminescence to the environment. Therefore, this work makes lanthanide-doped Y/Yb/Er-MOF attractive as an effective optical humidity sensor for humidity detection, which will broaden the applications of lanthanide-doped MOFs materials.