Preparation and Photoluminescence of Transparent Poly(methyl methacrylate)-Based Nanocomposite Films with Ultra-High-Loading Pendant ZnS Quantum Dots

Transparent nanocomposite films containing quantum dots are popular because of their extensive applications. However, nanoparticles tend to aggregate, resulting in phase separation of the nanoparticles in the polymer matrix. Herein, we present a bulk thermo-curing copolymerization method to fabricate poly(methyl methacrylate)-based nanocomposite films with ultra-high-loading ZnS quantum dots (ZnS/PMMA), utilizing polymerizable group-capped ZnS and monomer of methyl methacrylate (MMA). We found that the nanocomposite film is highly transparent, although the transmittance decreases with the ZnS content, especially at the wavelength between 300 nm and 400 nm. The results from X-ray diffraction (XRD), transmission electron microscopy (TEM), and dynamic mechanical thermal analysis (DMTA) show that the ZnS quantum dots maintain their original crystal structure, and are uniformly dispersed in the nanocomposite films, even with a very high ZnS content (41 wt %, determined by thermogravimetric analysis). The thermogravimetric analysis shows that the nanocomposite films possess a better thermal stability than that of pure PMMA film. The photoluminescence measurements show that ZnS/PMMA nanocomposite films have good optical properties. The fluorescence intensity increases with the increment of free ZnS content to 30 wt %, and then decreases due to self-reabsorption at a higher ZnS content. The transparent ZnS/PMMA nanocomposite films have a potential application as photoluminescence material.


Introduction
Quantum dots (QDs) possess attractive properties, such as narrow tunable emission and a high photoluminescence quantum yield (PLQY), making them promising candidates for numerous applications, including light-emitting diodes (LEDs) [1], photodetectors [2], biological labeling and imaging [3,4], lasers [5], and energy harvesting [6]. However, quantum dots are sensitive to moisture and oxygen, and tend to aggregate as a result of their highly specific surface energies. Incorporation of quantum dots in the polymer material can improve its stability, because the aggregation can be blocked by polymers among nanoparticles, and moisture can be prevented by the polymer matrices, especially hydrophobic ones. Moreover, the incorporation of inorganic quantum dots can endow the materials' new or largely enhanced properties.
Many efforts have been made to develop QDs/polymer nanocomposite films. Quantum dots possess unique size-dependent properties; therefore, it is critical to control the nanoparticle size and size distribution, as well as the dispersion homogeneity in the polymer matrix. Two main approaches have been developed to fabricate nanocomposite films' incorporated quantum dots, including either

X-ray Diffraction
X-ray diffraction (XRD) data of ME-capped ZnS, polymerizable group-capped nanoparticles, and ZnS/PMMA nanocomposites were recorded on a Bruker AXS D8 X-ray diffractometer (Rheinstetten, Germany) with a Cu Kα (λ = 1.5406 Å) source, operated at 40 kV and 20 mA at 293 K. The 2θ scanning range was from 10 • to 90 • , with a step size of 0.02 • and at a scanning speed of 1 degree/min.

Transmission Electron Microscopy
ZnS/PMMA nanocomposite films were embedded in Epon 812 epoxy resin, and then polymerized overnight at 60 • C. Ultrathin sections were cut using a Boeckeler Power Tome XL microtome (Tucson, AZ, USA). Cross-sections of the nanocomposite films were observed and photographed using a JEM-2100 transmission electron microscope (Tokyo, Japan). ME-capped ZnS and polymerizable group-capped nanoparticles were also observed with JEM-2100.

Dynamic Mechanical Thermal Analysis
The nanocomposite films were cut into 5 × 30 mm 2 rectangular bars, and their dynamic mechanical behaviors were recorded on a Tritec 2000 (Hayward, CA USA) instrument in a single cantilever bending mode. A storage modulus (E') and tan δ were registered as a dependence on temperature ranging from 0 to 250 • C, using a 5 • C/min heating rate at a frequency of 1 Hz.

Thermogravimetric Analysis
ME-capped ZnS, polymerizable group-capped ZnS NPs, as well as the nanocomposite films in the dry state were sealed in aluminum pans, and then thermogravimetric analysis (TGA) was performed using a SDT-Q600 TGA instrument (New Castle, DE, USA) at a heating rate of 10 • C/min in the temperature range from ambient to 600 • C in a nitrogen gas purge.
2.4.5. Light Absorption/Transmittance Spectra ME-capped and polymerizable-group-capped ZnS were dispersed in DMF under ultrasound to obtain a clear and uniform solution with a concentration of 10 mg/mL. The nanocomposite films were cut into 10 × 40 mm 2 strips and placed vertically in the light road. Transmittance and absorption of the nanocomposite films were recorded at wavelengths from 200 to 800 nm with a UV-Vis spectrophotometer (Heλios, Thermo Electro, Cambridge, UK), using the air as a reference. The transmittance and absorption of ME-capped and polymerizable group-capped ZnS were determined using DMF as a reference at the same wavelength range.

Photoluminescence Spectra
Photoluminescence (PL) spectra of ME-capped and polymerizable group-capped ZnS NPs and ZnS/PMMA nanocomposite films were measured on a VARIAN Cary Eclipse fluorescence spectrophotometer (Lake Forest, CA, USA) with an Xe-lamp as the excitation source, the tube voltage at 600 V, and excitation and emission slits of 5 nm.

Results and Discussion
The synthesis route of transparent high QD-loading nanocomposite films was shown in Scheme 1. A multi-hydroxyl group on the surface of ME-capped ZnS, from tightly absorbing mercaptoethanol, endows grafting sites for polymerizable molecule. Polymerizable group-capped ZnS was synthesized by a partial chemical graft of the hydroxyl on the surface of ZnS by 2-isocyanatoethyl methacrylate. ME-capped and polymerizable group-capped ZnS can be well-dispersed in DMF to obtain a clear solution. High-resolution transmission electron microscopy (HRTEM) photography, as shown in Figure 1, indicates that the nanoparticle diameter is about 3 nm with a uniform size distribution. The lattice fringes with a distance of 0.294 nm can be clearly observed, indicating that the grafting reaction of the polymerizable molecules on the ZnS surface do not influence the crystalline structure of ZnS NPs. This is important for the quantum dot to maintain its attractive properties, such as tunable emission, high photoluminescence quantum yield, and high refractive index. According to Rayleigh's law, light scattering of the spherical particles in the nanocomposite films leads to an intensity loss that can be calculated as follows: where I 0 and I are the intensity of the incident and transmitted light, respectively; φ is the volume fraction of the particles; l refers to the thickness of the nanocomposite film; and λ is the wavelength of the incident light. The variables n NP and n P are the refractive index of nanoparticles and the polymer matrix in the nanocomposite films, respectively. It can be concluded from Equation (1) that the size of the nanoparticles in the nanocomposite films has a much stronger effect on the transmittance than the film thickness. Generally, the upper limit of the nanoparticle size is about 40 nm for transparent It can be predicted that less than 1% of the incident light intensity will be lost because of the scattering of ZnS NPs in the nanocomposite films. Therefore, nanoparticle aggregation will be a considerable factor affecting transmittance of nanocomposite films.  The solvent of DMF was used in the preparation of the nanocomposite films, because polymerizable group-capped ZnS nanoparticles cannot disperse in the monomer of MMA. In the bulk thermo-curing copolymerization strategy, all reagents were mixed together as follows: polymerizable ZnS0.15 was dispersed in the DMF solvent, and then the monomer of MMA and initiator of AIBN were added under ultrasonic dispersion to form a clear and uniform polymerizable solution. After 12 h curing at 80 °C, the nanocomposite films were transparent, as Scheme 1. Schematic illustration of the partial chemical graft of polymerizable molecules on the mercaptoethanol (ME)-capped ZnS surface and the bulk copolymerization process of poly(methyl methacrylate)-based nanocomposite films with ultra-high-loading ZnS quantum dots (ZnS/PMMA). IEM is an abbreviation of 2-Isocyanatoethyl methacrylate, and MMA means a monomer of methyl methacrylate. The last photograph is ZnS/PMMA nanocomposite films under UV illumination (the thickness is 0.7 mm, with a loading free ZnS 0.15 quantum dots (QDs) varying from 10 wt % to 70 wt %, at a 20 wt % increment from left to right). It can be predicted that less than 1% of the incident light intensity will be lost because of the scattering of ZnS NPs in the nanocomposite films. Therefore, nanoparticle aggregation will be a considerable factor affecting transmittance of nanocomposite films.  The solvent of DMF was used in the preparation of the nanocomposite films, because polymerizable group-capped ZnS nanoparticles cannot disperse in the monomer of MMA. In the bulk thermo-curing copolymerization strategy, all reagents were mixed together as follows: polymerizable ZnS0.15 was dispersed in the DMF solvent, and then the monomer of MMA and initiator of AIBN were added under ultrasonic dispersion to form a clear and uniform polymerizable solution. After 12 h curing at 80 °C, the nanocomposite films were transparent, as The solvent of DMF was used in the preparation of the nanocomposite films, because polymerizable group-capped ZnS nanoparticles cannot disperse in the monomer of MMA. In the bulk thermo-curing copolymerization strategy, all reagents were mixed together as follows: polymerizable ZnS 0.15 was dispersed in the DMF solvent, and then the monomer of MMA and initiator of AIBN were added under ultrasonic dispersion to form a clear and uniform polymerizable solution. After 12 h curing at 80 • C, the nanocomposite films were transparent, as shown in the inserted photograph in Figure 2. We also prepared a nanocomposite film by physically embedding ME-capped ZnS NPs, which were opaque, even decreasing the ME-capped ZnS less than 5 wt %, although the polymerizable solution was also clear and uniform. This indicates that the difference between ME-capped ZnS nanoparticles and the MMA monomers was enlarged during the polymerization of monomers into a polymer. The attachment of ZnS NPs onto the polymer backbone by copolymerization between polymerizable ZnS 0.15 and the monomer of MMA blocks the microphase separation of ZnS NPs from the PMMA matrix, to which the enlarged difference can be ascribed. shown in the inserted photograph in Figure 2. We also prepared a nanocomposite film by physically embedding ME-capped ZnS NPs, which were opaque, even decreasing the ME-capped ZnS less than 5 wt %, although the polymerizable solution was also clear and uniform. This indicates that the difference between ME-capped ZnS nanoparticles and the MMA monomers was enlarged during the polymerization of monomers into a polymer. The attachment of ZnS NPs onto the polymer backbone by copolymerization between polymerizable ZnS0.15 and the monomer of MMA blocks the microphase separation of ZnS NPs from the PMMA matrix, to which the enlarged difference can be ascribed. Pure PMMA film shows high transparency between 250 and 800 nm; while the nanocomposite films with high ZnS content are transparent, the incorporation of ZnS in the nanocomposite films decreases its transmittance, especially at the wavelength ranging from 300 nm to 400 nm, as shown in Figure 2. This indicates that the ZnS nanoparticle in the nanocomposite films has a strong absorption. The transmittance of the nanocomposite film with a free ZnS0.15 content of 10 wt %, 30 wt %, 50 wt %, or 70 wt % is respectively about 90%, 84%, 77%, or 74% at the wavelength of 555 nm, which is the most sensitive wavelength for human eye and corresponds to yellow and green light [17]. This indicates that ZnS nanoparticles disperse uniformly in the nanocomposite films. However, it seems that the transmittance is much less than that predicted by Rayleigh's law, indicating possible slight aggregation of ZnS NPs in nanocomposite film with high content of ZnS.
To get further information on the dispersibility of ZnS NPs in the nanocomposites, the ultrathin sections of the nanocomposite films were observed using transmission electron microscopy (TEM). The nanocomposite film embedded in physically ME-capped ZnS NPs clearly exhibits serious particle aggregation, resulting in irregular phase separation, as shown in Figure 3A. Phase separation will cause optical scattering and reduce transmittance, in good agreement with the opaque appearance of ME-capped ZnS embedded physically in nanocomposite film. The TEM photographs of the nanocomposite films from copolymerization between 10-70 wt % polymerizable group-capped ZnS0.15 and the monomer of MMA were shown in Figure 3B-E. Although no obvious ZnS NP was observed in the nanocomposite film with 10 wt % ZnS0.15, ZnS NPs can be clearly observed when the free ZnS0.15 content increased to 30 wt %. It can be seen that the nanocomposite films copolymerized from ZnS0.15 and the monomer of MMA can remarkably block ZnS aggregation in resulting nanocomposites. However, slight aggregation of ZnS NPs can still observed, resulting from the phase domain (about 6 nm) that is larger than the size of ZnS quantum dot, as shown in Figure 3C. Figure 3D-E shows a higher nanoparticle content, and the phase domain from Pure PMMA film shows high transparency between 250 and 800 nm; while the nanocomposite films with high ZnS content are transparent, the incorporation of ZnS in the nanocomposite films decreases its transmittance, especially at the wavelength ranging from 300 nm to 400 nm, as shown in Figure 2. This indicates that the ZnS nanoparticle in the nanocomposite films has a strong absorption. The transmittance of the nanocomposite film with a free ZnS 0.15 content of 10 wt %, 30 wt %, 50 wt %, or 70 wt % is respectively about 90%, 84%, 77%, or 74% at the wavelength of 555 nm, which is the most sensitive wavelength for human eye and corresponds to yellow and green light [17]. This indicates that ZnS nanoparticles disperse uniformly in the nanocomposite films. However, it seems that the transmittance is much less than that predicted by Rayleigh's law, indicating possible slight aggregation of ZnS NPs in nanocomposite film with high content of ZnS.
To get further information on the dispersibility of ZnS NPs in the nanocomposites, the ultrathin sections of the nanocomposite films were observed using transmission electron microscopy (TEM). The nanocomposite film embedded in physically ME-capped ZnS NPs clearly exhibits serious particle aggregation, resulting in irregular phase separation, as shown in Figure 3A. Phase separation will cause optical scattering and reduce transmittance, in good agreement with the opaque appearance of ME-capped ZnS embedded physically in nanocomposite film. The TEM photographs of the nanocomposite films from copolymerization between 10-70 wt % polymerizable group-capped ZnS 0.15 and the monomer of MMA were shown in Figure 3B-E. Although no obvious ZnS NP was observed in the nanocomposite film with 10 wt % ZnS 0.15 , ZnS NPs can be clearly observed when the free ZnS 0.15 content increased to 30 wt %. It can be seen that the nanocomposite films copolymerized from ZnS 0.15 and the monomer of MMA can remarkably block ZnS aggregation in resulting nanocomposites. However, slight aggregation of ZnS NPs can still observed, resulting from the phase domain (about 6 nm) that is larger than the size of ZnS quantum dot, as shown in Figure 3C. Figure 3D-E shows a higher nanoparticle content, and the phase domain from aggregation seems to be bigger as the ZnS Polymers 2018, 10, 1217 7 of 13 content increases in the nanocomposite films. This can be seen clearly in Figure 3E, in good agreement with the decreased transmittance shown in Figure 2.
Polymers 2017, 9, x FOR PEER REVIEW 7 of 13 aggregation seems to be bigger as the ZnS content increases in the nanocomposite films. This can be seen clearly in Figure 3E, in good agreement with the decreased transmittance shown in Figure 2. The X-ray diffraction (XRD) patterns of polymerizable ZnS0.15 and the nanocomposite film with different content ZnS0.15 are shown in Figure 4. It can be seen that three diffraction peaks are observed at 28.5°, 47.6°, and 56.4°, corresponding to the (111), (220), and (311) planes of ZnS with a zinc blend structure [18]. This indicates that the crystal structure and crystallinity are not affected by the grafting reaction of polymerizable molecules on the surface of ME-capped ZnS NP and the copolymerization reaction between polymerizable ZnS0.15 and the MMA monomer. The size of the ZnS nanoparticle in the nanocomposite film is also about 3.0 nm, calculated by Scherrer's formula (d = kλ/βcosθ) based on the (111) peak, in good agreement with the nanoparticle size observed from TEM. Moreover, the nanocomposite films show another broad peak at 13° from PMMA matrices, and the peak intensity rapidly decreases with improved ZnS content in the nanocomposites.  Figure 4. It can be seen that three diffraction peaks are observed at 28.5 • , 47.6 • , and 56.4 • , corresponding to the (111), (220), and (311) planes of ZnS with a zinc blend structure [18]. This indicates that the crystal structure and crystallinity are not affected by the grafting reaction of polymerizable molecules on the surface of ME-capped ZnS NP and the copolymerization reaction between polymerizable ZnS 0.15 and the MMA monomer. The size of the ZnS nanoparticle in the nanocomposite film is also about 3.0 nm, calculated by Scherrer's formula (d = kλ/βcosθ) based on the (111) peak, in good agreement with the nanoparticle size observed from TEM. Moreover, the nanocomposite films show another broad peak at 13 • from PMMA matrices, and the peak intensity rapidly decreases with improved ZnS content in the nanocomposites.  To determine the actual content of pure inorganic ZnS and the thermal stability of ZnS/PMMA nanocomposite films, thermogravimetric analysis of nanocomposite films with different ZnS0.15 content was carried out, compared with the pure PMMA polymer, as well as the ME-capped and ZnS0.15 NPs. TGA curves are shown in Figure 5, and the weight loss at each decomposition step and the residue at 600 °C are listed in Table 2. Pure PMMA polymer shows a single degradation step at the temperature range of 260-415 °C, owing to the thermo-decomposition of the PMMA polymer, while the ZnS/PMMA nanocomposite films show two obvious degradation steps corresponding to temperature ranges 250-330 °C and 360-470 °C, respectively. ME-capped ZnS and polymerizable ZnS0.15 show a weight loss at the temperature range of 250-330 °C, similar to the first decomposition temperature range of the nanocomposites, due to the decomposition of the ME molecule on ZnS surfaces. Therefore, the second temperature range of weight loss should be ascribed to the decomposition of the PMMA component in the nanocomposite films, indicating improved stability of ZnS/PMMA nanocomposite films. This may be explained in that the interaction between the ZnS nanoparticle and the PMMA polymer matrix is so strong that the thermal degradation of the PMMA polymer is more difficult [19]. The content of pure inorganic ZnS in ME-capped and polymerizable ZnS0.15 quantum dots is 62.8 wt % and 63.6 wt %, respectively, indicating the presence of many capping molecules of mercaptoethanol on the nanoparticle surface; only a small number of capping molecules were grafted by the polymerizable molecule. The residue of the nanocomposite films (pure ZnS) with free ZnS0.15 content of 10 wt %, 30 wt %, 50 wt %, and 70 wt % is respectively about 13 wt %, 28.7 wt %, 35.2 wt %, and 41 wt %, in good accordance with the calculated values based on the TGA results of the ZnS0.15 nanoparticle.  To determine the actual content of pure inorganic ZnS and the thermal stability of ZnS/PMMA nanocomposite films, thermogravimetric analysis of nanocomposite films with different ZnS 0.15 content was carried out, compared with the pure PMMA polymer, as well as the ME-capped and ZnS 0.15 NPs. TGA curves are shown in Figure 5, and the weight loss at each decomposition step and the residue at 600 • C are listed in Table 2. Pure PMMA polymer shows a single degradation step at the temperature range of 260-415 • C, owing to the thermo-decomposition of the PMMA polymer, while the ZnS/PMMA nanocomposite films show two obvious degradation steps corresponding to temperature ranges 250-330 • C and 360-470 • C, respectively. ME-capped ZnS and polymerizable ZnS 0.15 show a weight loss at the temperature range of 250-330 • C, similar to the first decomposition temperature range of the nanocomposites, due to the decomposition of the ME molecule on ZnS surfaces. Therefore, the second temperature range of weight loss should be ascribed to the decomposition of the PMMA component in the nanocomposite films, indicating improved stability of ZnS/PMMA nanocomposite films. This may be explained in that the interaction between the ZnS nanoparticle and the PMMA polymer matrix is so strong that the thermal degradation of the PMMA polymer is more difficult [19]. The content of pure inorganic ZnS in ME-capped and polymerizable ZnS 0.15 quantum dots is 62.8 wt % and 63.6 wt %, respectively, indicating the presence of many capping molecules of mercaptoethanol on the nanoparticle surface; only a small number of capping molecules were grafted by the polymerizable molecule. The residue of the nanocomposite films (pure ZnS) with free ZnS 0.15 content of 10 wt %, 30 wt %, 50 wt %, and 70 wt % is respectively about 13 wt %, 28.7 wt %, 35.2 wt %, and 41 wt %, in good accordance with the calculated values based on the TGA results of the ZnS 0.15 nanoparticle.  The storage modulus (E) and the loss factor (tan δ) of ZnS/PMMA nanocomposite films with different ZnS content were recorded as a function of temperature. From the viscoelastic curves shown in Figure 6, it can be seen that storage modulus of pure PMMA film is about 2000 MPa. Incorporation of a ZnS nanoparticle into PMMA film greatly increases its storage modulus-e.g., increasing to 3165 MPa as ZnS content increases to 70 wt %. However, pure PMMA film shows the highest amplitude of the damping peak ((tan δ)max) that decreases to 0.62 as the ZnS content increases to 70 wt %. Moreover, the glass transition temperature (Tg), corresponding to the temperature of the maximum of tag δ, increases from 114 °C to 134 °C. These observations can be explained by improved cross-link density, indicating that more than one hydroxyl on the ZnS surface is grafted with polymerizable molecule, and polymerizable ZnS0.15 NPs act as a cross-linker in the nanocomposite films.
The loss spectra (tan δ versus temperature) of the ZnS/PMMA nanocomposite films decreases with improved ZnS content, and all the maximum of tan δ are less than 1, differing from pure PMMA film (the maximum of tag δ is about 1.48). This indicates that the distance between cross-link sites decreases [20], and that nanocomposite films have a higher storage modulus than loss modulus. The widths at the half-height on the relaxation peak are sensitive to the homogeneity of the networks. In Figure 6, it is clear that the nanocomposite films exhibited a single glass transition peak, indicating further uniform dispersion of ZnS in the nanocomposite films as expected.  The storage modulus (E) and the loss factor (tan δ) of ZnS/PMMA nanocomposite films with different ZnS content were recorded as a function of temperature. From the viscoelastic curves shown in Figure 6, it can be seen that storage modulus of pure PMMA film is about 2000 MPa. Incorporation of a ZnS nanoparticle into PMMA film greatly increases its storage modulus-e.g., increasing to 3165 MPa as ZnS content increases to 70 wt %. However, pure PMMA film shows the highest amplitude of the damping peak ((tan δ) max ) that decreases to 0.62 as the ZnS content increases to 70 wt %. Moreover, the glass transition temperature (T g ), corresponding to the temperature of the maximum of tag δ, increases from 114 • C to 134 • C. These observations can be explained by improved cross-link density, indicating that more than one hydroxyl on the ZnS surface is grafted with polymerizable molecule, and polymerizable ZnS 0.15 NPs act as a cross-linker in the nanocomposite films. The storage modulus (E) and the loss factor (tan δ) of ZnS/PMMA nanocomposite films with different ZnS content were recorded as a function of temperature. From the viscoelastic curves shown in Figure 6, it can be seen that storage modulus of pure PMMA film is about 2000 MPa. Incorporation of a ZnS nanoparticle into PMMA film greatly increases its storage modulus-e.g., increasing to 3165 MPa as ZnS content increases to 70 wt %. However, pure PMMA film shows the highest amplitude of the damping peak ((tan δ)max) that decreases to 0.62 as the ZnS content increases to 70 wt %. Moreover, the glass transition temperature (Tg), corresponding to the temperature of the maximum of tag δ, increases from 114 °C to 134 °C. These observations can be explained by improved cross-link density, indicating that more than one hydroxyl on the ZnS surface is grafted with polymerizable molecule, and polymerizable ZnS0.15 NPs act as a cross-linker in the nanocomposite films.
The loss spectra (tan δ versus temperature) of the ZnS/PMMA nanocomposite films decreases with improved ZnS content, and all the maximum of tan δ are less than 1, differing from pure PMMA film (the maximum of tag δ is about 1.48). This indicates that the distance between cross-link sites decreases [20], and that nanocomposite films have a higher storage modulus than loss modulus. The widths at the half-height on the relaxation peak are sensitive to the homogeneity of the networks. In Figure 6, it is clear that the nanocomposite films exhibited a single glass transition peak, indicating further uniform dispersion of ZnS in the nanocomposite films as expected.  The loss spectra (tan δ versus temperature) of the ZnS/PMMA nanocomposite films decreases with improved ZnS content, and all the maximum of tan δ are less than 1, differing from pure PMMA film (the maximum of tag δ is about 1.48). This indicates that the distance between cross-link sites decreases [20], and that nanocomposite films have a higher storage modulus than loss modulus. The widths at the half-height on the relaxation peak are sensitive to the homogeneity of the networks.
In Figure 6, it is clear that the nanocomposite films exhibited a single glass transition peak, indicating further uniform dispersion of ZnS in the nanocomposite films as expected.
The UV absorption of ME-capped ZnS, polymerizable ZnS 0.15 , and the nanocomposite films with different ZnS content is shown in Figure 7. It can be seen that ME-capped ZnS and polymerizable ZnS 0.15 show a similar absorption spectrum, with a maximum absorption centre at 277 nm (4.47 eV), corresponding to a calculated ZnS nanoparticle diameter of about 3 nm, according to Brus's model [14]. This value is similar to the particle size observed directly from TEM images shown in Figure 1. The excited state energy (4.47 eV) is larger than a band gap bulk value of 3.66 eV for ZnS. Such a strong and narrow absorption peak at 277 nm is known to arise from quantum confinement effect, which occurs when the particle size of nanocrystals is comparable with the Bohr radius. Polymerizable ZnS 0.15 and ZnS/PMMA nanocomposite films show further absorption at 340 nm (3.66 eV), corresponding to the characteristic absorption peak of ZnS bulk material, and the intensity of the absorption increases as ZnS content in the nanocomposite film improves. This indicates that part of ZnS NPs may lose their quantum effect due to aggregation. The exited energy of the quantum dot is inversely related to its particle size [21]. The nanocomposite film with 10 wt % ZnS 0.15 shows a slight blue shift compared to ME-capped ZnS and polymerizable ZnS 0. 15 . This indicates that the incorporation of ZnS in the polymer by copolymerization stabilizes nanoparticle size by blocking the aggregation. The luminescent efficiency of the quantum dots increases with decreasing particle size, exhibiting better luminescent properties with smaller QD particle sizes [22]. The maximum absorption wavelength shows a slight redshift with ZnS 0.15 increasing content in the nanocomposite films. This indicates that the particle size increases when high ZnS content is incorporated into the nanocomposite films.    No obvious fluorescence was observed for pure PMMA film at an excitation wavelength of 365 nm. However, as a typical semiconductor, ZnS quantum dots possess interesting fluorescent characteristics that are preserved in the nanocomposite films as expected; the fluorescence intensity seemed to increase when the ZnS 0.15 content increases from 0 to 50 wt %. In addition, we found that ZnS quantum dots are unstable, and their fluorescent intensity decreases greatly after one-day displacement away from light. However, no obvious decrease was observed for the fluorescent intensity of PMMA-based nanocomposite films. This indicates that ZnS is more stable in PMMA-based matrices than in DMF solution. The emission spectra of ME-capped ZnS and polymerizable ZnS 0.15 dispersed in DMF with a concentration 10 mg/mL are shown as the insert in Figure 9. Usually, redshift in the peak emission wavelength occurs as the concentration of QDs increases due to self-reabsorption and Förster resonance energy transfer (FRET) among neighboring QDs, and becomes more significant as the interparticle distance decreases [23]. The peak emission wavelength (λ m ax) redshifts from 390 nm of ME-capped ZnS to 430 nm of polymerizable ZnS 0.15 , and polymerizable ZnS 0.15 has higher fluorescence intensity than that of ME-capped ZnS. The mission behavior exhibits a well-defined excitonic emission feature, consistent with the results for highly luminescent ZnS NPs [24]. The redshift of the peak emission wavelength indicates that polymerizable ZnS 0.15 is prone to self-reabsorption and FRET among the QDs, probably because of its different surface ligand. The greater fluorescent intensity of polymerizable ZnS 0.15 may be from the annealing effect of the thermal grafting reaction of the polymerizable molecule on an ME-capped ZnS surface, as well as the coverage of surface defects with polymerizable molecule chains [25]. Figure 9 shows the fluorescence emission spectra of the ZnS/PMMA nanocomposite film with excitation at 365 nm. The peak wavelength of characteristic emissions at about 413 nm is observed for ZnS/PMMA nanocomposite films with 10 and 30 wt %, indicating a minor hypsochromic shift compared with polymerizable ZnS 0.15 in DMF. This shift can be explained by an increase in the refractive index of the surrounding matrix [26]. ZnS/PMMA nanocomposite film with 30 wt % ZnS 0.15 shows a higher emission intensity than that with 10 wt % ZnS 0.15 ; the emission intensity then drops as the ZnS 0.15 content increases-e.g., at 50 wt % and 70 wt %. Moreover, two emission peaks were observed upon the nanocomposite with 50 and 70 wt %, indicating that self-absorption happens at a high ZnS content.

Conclusions
ME-capped ZnS quantum dots were synthesized, after which a polymerizable molecule of 2-isocyanatoethyl methacrylate (IEM) was chemically grafted onto the ZnS surface, in order to synthesize polymerizable group-capped ZnS. Furthermore, transparent nanocomposite films with

Conclusions
ME-capped ZnS quantum dots were synthesized, after which a polymerizable molecule of 2-isocyanatoethyl methacrylate (IEM) was chemically grafted onto the ZnS surface, in order to synthesize polymerizable group-capped ZnS. Furthermore, transparent nanocomposite films with

Conclusions
ME-capped ZnS quantum dots were synthesized, after which a polymerizable molecule of 2-isocyanatoethyl methacrylate (IEM) was chemically grafted onto the ZnS surface, in order to synthesize polymerizable group-capped ZnS. Furthermore, transparent nanocomposite films with ultra-high-loading ZnS nanoparticles (up to 41 wt %, determined by TGA) were successfully fabricated by bulk thermo-curing copolymerization between the polymerizable group-capped ZnS and the monomer of MMA. TEM and XRD analysis indicate that ZnS NP dispersed uniformly in the nanocomposite films and remains in its original crystalline structure of ME and polymerizable group-capped ZnS. The TGA measurement displays that ZnS/PMMA nanocomposite films possess better thermal stability than a pure PMMA polymer. The UV absorption and transmittance measurement showed that the incorporation of ZnS in the nanocomposite films slightly decreased its transmittance. However, all nanocomposite films possess strong absorption when the wavelength is between 300 and 400 nm. Luminescent photographs show that ZnS/PMMA nanocomposite films exhibit good optical properties. The fluorescence intensity under UV irradiation increased as ZnS increased in increments to 30 wt %, and then decreased as the ZnC increased further to 70 wt % due to self-reabsorption.