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Heat Treatment Effect on [Eu.sup.3+] Doped Te[O.sub.2]-BaO-[Bi.sub.2][O.sub.3] Glass Systems with Ag Nanoparticles.

1. Introduction

Superior properties, for instance, mechanical and thermal stability, high devitrification resistance, and suitable infrared transparency, make tellurite glasses promising materials for variety of applications related to the field of optics, for example, light upconversion materials, lasers, solar cells, or optical amplifiers [1-6]. Additionally, these glasses are suitable for utilization as luminescent materials owing to their low phonon energy (700 [cm.sup.-1]) in comparison to other oxide glasses and wide transmission window. This property leads to minimization of the nonradiative losses. Tellurite glasses also exhibit good solubility of rare earth ions that allows for possible employment of their f-f transitions in order to obtain efficient light sources with tunable emission color [7, 8].

In recent years, glasses doped with silver gained much attention considering possibility of the localized surface plasmon resonance (LSPR) phenomenon utilization. LSPR is observed in case of nanoparticles with sizes smaller than 100 nm. Electron excitations creating charge oscillations at the metal-insulator boundary lead to large local electric field enhancement in the vicinity of nanoparticles, creating so called "hot-spots." As a result, it is possible to increase the intensity of rare earth ions emissions. Formation of silver nanoparticles is facilitated by high mobility of silver ions in tellurite glass matrix and suitable redox potential of [Ag.sup.+] [right arrow] [Ag.sup.0] reduction [9]. Silver is reduced through one-step process:

[Ag.sup.+] + 1[e.sup.-] [right arrow] [Ag.sup.0] (1)

with the reduction potential of [E.sub.0] = 0.7996 V [10]. Highly mobile silver ions are form nanoparticles by matrix-assisted reduction process, for example, by structural elements of Te[O.sub.2] matrix with uncompensated charge. Silver diffuses into tellurite glass matrix, changes its valance state, and forms nanoparticles through Ostwald ripening. Thus, it is promising to synthesize the nanoparticles inside glass matrix and in consequence achieve emission enhancement of rare earth ions with employment of metal nanoparticles.

One of the first reports on LSPR in glass medium was the work of Malta et al. [11] on borosilicate glasses. Enhancement of [Eu.sup.3+] ions emissions has been observed. Lately, numerous works concerning silver nanoparticles and emission enhancements through LSPR phenomenon have been reported in case of various glass systems [12-15]. Number of studies described the formation of silver nanoparticles in glass matrix through heat treatment approach. While in higher temperatures mobility of silver ions increases, heat treatment approach involves annealing of samples usually above glass transition temperature to introduce metallic nanoparticles [16]. That method is widely applied in order to create nanoparticles through their agglomeration and to obtain enhancement of rare earth emission intensity. Jiao et al. examined the luminescence of [Eu.sup.3+] in borate glasses after addition of silver and mechanisms of Ag ions agglomeration. In this case, enhancement of emission intensities has been detected [17]. White light emission in europium doped phosphate glasses was obtained by Fan et al. [18]. In this study, an efficient energy transfer between nanoparticles and [Eu.sup.2+] and [Eu.sup.3+] species has been detected. Moreover, a number of studies were dedicated to describe silver influence on rare earths emission intensities in matrices demonstrating lower phonon energies such as tellurite and tellurite based glasses.

Amjad et al. [19] studied the influence of silver nanoparticles on the luminescence properties of [Eu.sup.3+] in Te[O.sub.2]-ZnO glass systems and obtained increase of emission intensities of europium ions. Dousti et al. focused on the silver doped Te[O.sub.2]-PbO glasses [20]. Du et al. reported tellurite-germanate glasses for solar converters doped with Ag nanoparticles to enhance [Pr.sup.3+] emission intensity [21]. Fares et al. obtained Te[O.sub.2]-BaO-Nb2O5-Er2O3 glasses with embedded silver nanoparticles [22]. Enhancement of lifetime and emission intensities of the [Er.sup.3+] [sup.4][I.sub.13/2] [right arrow] [sup.4][I.sub.15/2] transition has been observed. Huang et al. studied [Er.sup.3+]/[Tm.sup.3+] codoped Te[O.sub.2]ZnO-[Na.sub.2]C[O.sub.3]-[Er.sub.2][O.sub.3]-[Tm.sub.2][O.sub.3]-AgN[O.sub.3] glasses doped with silver and observed 1.85 [micro]m band fluorescence enhancement mainly attributed to the intensified local field effect induced by Ag NPs [23]. Wu et al. presented study on influence of silver on [Er.sup.3+]/[Yb.sup.3+] codoped Te[O.sub.2]-[Bi.sub.2][O.sub.3]-Ti[O.sub.2] glasses [24].

To the best of our knowledge, there are no reports on europium doped Te[O.sub.2]-BaO-[Bi.sub.2][O.sub.3]-Ag (TBBAg) systems with silver nanoparticles obtained through heat treatment process. Similar glass materials have never been studied in terms of silver incorporation and its influence on rare earth ions emission. The aim of this work is the synthesis of silver nanoparticles in tellurite glass matrix and to study the influence of silver addition on luminescence of europium ions incorporated into TBBAg glass. This novel glass matrix is promising material for [Eu.sup.3+] host with its excellent properties. Since Te[O.sub.2] is conditional glass former, BaO is introduced to stabilize the glass matrix. Heavy metal oxides such as barium oxide are proven to induce higher devitrification resistance of glasses [25]. Moreover, low phonon energy of tellurite glass promotes radiative transitions of rare earth ions. The aforementioned properties of synthesized glass matrix are the reason that it has been used in this work. Silver nanoparticles, on the other hand, are introduced to study the rare earth ions emission enhancement through LSPR phenomenon. It has never been done before in glass system of similar composition. Since this work is also focused on matrix influence on luminescence of rare earth ion, europium ions have been chosen as a luminescent center since its emission properties are well understood. Additionally, study of the LSPR as a function of different amount of silver in glass is performed. Finally, influence of heat treatment procedure on luminescent properties of obtained material is discussed. TBBAg system is promising material for color tunable phosphors that can be used in LEDs and in lighting industry.

2. Experimental

Synthesis of tellurite glass samples involved mixing and pulverizing of high purity Te[O.sub.2], BaC[O.sub.3], [Bi.sub.5]O[(OH).sub.9][(N[O.sub.3]).sub.4], Eu[(N[O.sub.3]).sub.3], and AgN[O.sub.3] raw materials in powder form. Conventional melt-quenching technique has been used to obtain amorphous glass material. Well-mixed batches were placed in porcelain crucibles and were gradually heated to 800[degrees]C in order to enhance the mixing of ingredients. After 30 minutes the temperature was reduced to 700[degrees]C for the next 30 minutes. Afterwards, obtained melt was poured onto a preheated steel plate (300[degrees]C), pressed immediately between steel plates, and then cooled down to room temperature. Each stage of this procedure was carried out in the air atmosphere. Such approach led to synthesis of homogenous, transparent samples.

Heat treatment (HT) stage involves annealing of the samples usually above glass transition temperature. In this work, heat treatment at 350[degrees]C in the air atmosphere has been applied. This has been done to initiate the migration of silver ions that would lead to formation of silver nanoparticles embedded in glass matrix. HT procedure is considered to be the method of choice in case of solid state samples since it is a simple, one-step process that allows controlling annealing parameters. Different HT times have been applied in order to study the evolution of the glass system and change of sample properties. HT parameters are presented in Table 1 in detail.

Differential scanning calorimetry (DSC) measurements were executed on Netzsch Simultaneous TGA-DSC, STA 449 F1, in order to determine the thermal properties of the material such as glass transition and crystallization temperature. Investigations were conducted on powder samples in platinum-rhodium crucibles with heating rate of 15[degrees]C [min.sup.-1] in the air atmosphere. Structural investigations were performed using several techniques. Examination of internal structure of prepared samples was carried out using conventional X-ray diffraction (XRD) technique. Measurements were executed on powder samples using Philips X'PERT PLUS diffractometer with Cu-Ka radiation ([lambda] = 0.154 nm). Chemical bonds existing in the structural units of the glass samples were determined using Fourier Transform Infrared (FTIR) spectroscopy results. These measurements were undertaken on Perkin-Elmer Frontier MIR/FIR spectrometer with TGS detector in the midinfrared spectral range. Examination involved creating pellet-type samples containing mixture of glass with potassium bromide (KBr) in weight ratio 1: 100. The same amount of ingredients with controlled grain size was introduced in case of all measured samples. Measurements were performed with 0.5 [cm.sup.-1] spectral resolution. X-ray photoelectron spectroscopy analysis (XPS) was carried out with the employment of X-ray photoelectron spectrometer (Omicron NanoTechnology) with 128-channel collector. Investigated samples were precleaned by Ar ion beam. XPS measurement has been done at room temperature in ultrahigh vacuum conditions, below 1.1 x [10.sup.-8] mBar. The photoelectrons were excited by an Mg-Ka X-ray source. The X-ray anode was operated at 15keV and 300 W. Omicron Argus hemispherical electron analyser with round aperture of 4 mm was used for analysing of emitted photoelectrons. The binding energies were corrected using the background C1s line (285.0 eV) as a reference. XPS spectra were analysed with Casa-XPS software using a Shirley background subtraction and Gaussian-Lorentzian curve as a fitting algorithm. For transmission electron microscopy TEM samples were placed on copper grids coated with a 2% collodion solution and carbon. Probes were examined using a Tecnai Spirit BioTwin (FEI) electron microscope at 120 kV. UV-vis spectra were collected on Perkin-Elmer Lambda 35 UV-vis spectrophotometer in the range of 350-700 nm. Measurements were conducted in the air atmosphere. Photoluminescence (PL) spectra were collected in the 430-750 nm range in case of emission spectra and 250-500 nm for excitation spectra using Perkin-Elmer LS 55 spectrofluorometer. Measurements were performed using pellet samples mixed with KBr in weight ratio of 1 : 1.

Calculations of the extinction coefficients were achieved using the multireflectance formula [27]:

T = [(1 - R).sup.2] x [e.sup.-[alpha]d]/([(1 - R).sup.2] x [e.sup.-2[alpha]d]), (2)

where [alpha] is the extinction coefficient, d is the sample thickness, R is the reflectance, and T is the transmittance. For each sample, values of reflectance and the transmittance were measured. Extinction coefficient value was calculated by subtracting the extinction coefficient of the sample without silver addition from that of the annealed samples containing silver nanoparticles.

3. Results and Discussion

3.1. Structural Studies

3.1.1. DSC. DSC curves of Ag0 and Ag1 glass samples are presented in Figure 1((a) and (b)). Glass transition temperature [T.sub.g] is located at 321 and 318[degrees]C, respectively. In case of Ag0 sample, one clear exothermic peak attributed to the crystallization process may be distinguished at 416[degrees]C. On the other hand, DSC curve of Ag1 consists of the main crystallization peak at 420[degrees] C and, additionally, another exothermal peak at 387[degrees]C. Thermal stability [28] (TS) regions have been determined and equaled 95[degrees]C in case of Ag0 and 69[degrees] C for Ag1 sample. Thermal parameters of studied samples are presented in Table 2.

These measurements have been performed mainly in order to investigate the TS region. Its range is crucial for silver nanoparticles formation process, considering the fact that their synthesis is usually performed below the temperature of the first crystallization peak but above the glass transition temperature. Above [T.sub.g], glass properties such as viscosity and ion mobility change, favoring silver nanoparticles agglomeration. Additionally, such approach prevents the crystallization of glass matrix which is the case in our work.

Therefore, synthesis of Ag nanoparticles has been performed in the range between [T.sub.g] and the onset of the first crystallization peak at 387[degrees] C. It is our consideration that used temperature range would be sufficient to initialize migration of silver ions to form silver nanoclusters. This is possible due to decrease of glass viscosity with increasing temperature.

3.1.2. XRD. XRD results were obtained for glass materials annealed for 3,6,12, and 24 hours. Amorphous halo is evident indicating that no long range order periodicity existed in the samples. It was not possible to detect any Ag nanoparticles signals, because only 1-3mol% of silver was introduced into the samples.

On the other hand, in case of nanoparticles one can observe widening of diffraction peaks and due to nanoscale size such peak can overlap with wide amorphous halo. Exemplary result of AgEu1 sample heat-treated for 6 hours is presented in Figure 2.

3.1.3. FTIR. FTIR technique was employed to reveal any structural alterations induced by heat treatment procedure or by the change of composition. Moreover, basic structural elements of the matrix were also revealed. Tellurite glasses are usually composed of Te[O.sub.3] pyramids and Te[O.sub.4] trigonal bipyramids. Obtained measurement results of as-prepared and heat-treated Ag1 samples are presented in Figure 3. To examine heat treatment induced changes in tellurite glass matrix two samples have been chosen for measurement: as prepared and heat-treated for 96 hours. Main feature is the wide band visible in the 530-850 [cm.sup.-1] range. This band can be deconvoluted into two signals positioned at 650 [cm.sup.-1] and 730 [cm.sup.-1]. The first one (pink curve) at 650 [cm.sup.-1] came from Te-O stretching vibrations of TeO4 trigonal bipyramids [29-31]. The second one (green curve) at approximately 730 [cm.sup.-1] is associated with oscillations of Te-O in Te[O.sub.3] trigonal pyramids [30, 31]. Te[O.sub.4] derived signal is stronger in both cases. This might indicate that more Te[O.sub.4] species exist in obtained material.

Intensities of the aforementioned bands varied slightly as a function of annealing time. Heat treatment for 96 h resulted in increased intensity of these two peaks. However, observed changes of FTIR spectra are minor. Ratio between intensities of Te[O.sub.4] and Te[O.sub.3] derived bands remained approximately constant. Therefore, it is concluded that glass matrix is resistant to heat treatment procedure and stays unchanged even when long annealing times have been applied. It is consistent with XRD results that indicated no crystallization of glass matrix after HT process.

3.1.4. XPS. XPS experiment has been performed to provide insight on valance state of silver in tellurite glass matrix. Exemplary spectra of as-prepared Ag1 sample, Ag1, and Ag3 samples crystallized for 6h are presented in Figure 4(a). [Ag3d.sub.5/2] and [Ag3d.sub.3/2] photoelectron peaks of silver have been observed at 368 and 374 eV, respectively. Spin orbit components in all cases were separated by distance of 6 eV which is characteristic of silver. Shape of obtained spectra is comparable to others published before [32]. However, it is difficult to distinguish between different silver state components of [3d.sub.5/2] peak. Therefore, definition of silver oxidation state on the basis of XPS measurements is challenging and sometimes impossible. Consequently, modified Auger parameter ([alpha]') had to be calculated. In order to acquire it, kinetic energy values of silver M4VV Auger lines are determined (presented in Figure 4(b)). Their positions equaled 355.6 eV, 357.3 eV, and 357.6 eV in case of Ag1 (HT = 0 h), Ag1 (HT = 6 h), and Ag3 (HT = 6h) samples, respectively. Parameter has been calculated according to the following equation:

[alpha]' = BE ([Ag3d.sub.5/2]) + KE (Ag M4VV), (3)

where BE([Ag3d.sub.5/2]) is the binding energy of [Ag3d.sub.5/2] peak and KE(Ag M4VV) is kinetic energy of M4VV Auger line peak. Parameter a for metallic silver equals 726 eV [26]. Calculated results are presented in Table 3.

As-prepared Ag1 sample possessed lowest modified Auger parameter which suggests that in case of Ag1 specimen most of silver exists in ionic form. It is indicative that mixture of metallic and ionic silver exists in both heat-treated samples since obtained results are in the range between parameters characteristic to AgO species and metallic silver.

However, some portion of silver ions changed their valance state and formed [Ag.sup.0] species. For heat-treated Ag1 sample parameter [alpha]' equaled 725.4 eV which means that mixture of Ag oxidation states existed with the great majority of [Ag.sup.0] species. Moreover, parameter of Ag3 sample is even higher and equals 725.6 which confirms that most of silver exists in [Ag.sup.0] form. Since the value of parameter for Ag3 sample is close to that of metallic silver, it is concluded that ratio of [Ag.sup.0] to other Ag species in that specimen is the highest of all samples.

Additional study has been performed on Ag1 sample heat-treated for 6 hours in order to describe bismuth ions valance state. There was a possibility of bismuth reduction and nucleation since heat treatment process created environment propitious for metallic nanoparticles formation. No evidence for bismuth nucleation has been obtained since bismuth Bi4f signals observed (Figure 5) are characteristic to bismuth in oxide state. Peaks possess symmetric shape and are positioned at 159.6 and 164.9 eV (for [Bi4f.sub.7/2] and [Bi4f.sub.5/2], resp.). Thus, it can be concluded that only [Bi.sup.3+] ions exist in glass matrix. This is consistent with the fact that [Bi.sub.2][O.sub.3] is conditional glass former and probably is one of the components creating the amorphous matrix.

3.1.5. TEM. In order to observe the silver nanoparticles embedded in tellurite glass material, TEM measurement has been performed. Samples with Ag1, Ag2, and Ag3 designations annealed for 6 hours has been chosen for measurement. Exemplary TEM images have been presented in Figures 6(a), 6(b), and 6(c). As it can be noticed, nanoparticles are indeed synthesized within amorphous tellurite glass matrix. The shape of nanoparticles is spherical. However, nanoparticles of different size have been obtained in different samples. Increase of dimensions with increasing amount of introduced silver can be observed. In case of Ag1 samples nanoparticles size does not exceed 30 nm whereas in Ag2 and Ag3 sample sizes exceed 30 nm and 40 nm, respectively.

TEM measurements are strongly supported with the aforementioned XPS results which indicated that majority of silver is in metallic form in Ag3 sample. Increased number of Ag species resulted in formation of larger agglomerates.

In Figure 7 exemplary TEM images of Ag1 samples heat-treated for 3, 6, and 12 hours have been presented. It is worth noticing that with changing heat treatment time diameter of observed nanoparticles increases with heat treatment duration. In samples heat-treated for 3 hours nanoparticles are not exceeding 20 nm in diameter. On the other hand in sample heat-treated for 12 hours nanoparticles of 30-40 nm have been observed. It can be thus concluded that change of heat treatment parameters influences the size of silver nanoparticles embedded in tellurite glass matrix.

3.2. Optical Studies

3.2.1. UV-vis. UV-vis spectrum of AgEu1 sample is shown in Figure 8. It can be noticed that absorption signals characteristic to [Eu.sup.3+] were present. Peaks at 465 and 532 nm due to [sup.7][F.sub.0] - [sup.5][D.sub.2] and [sup.7][F.sub.0]-[sup.5][D.sub.1] transitions have been observed and assigned on the basis of the energy levels reported in [33].

To observe the influence of Ag quantity on silver nanoparticles formation samples without europium addition have been measured first. In Figures 9(a), 9(b), and 9(c) extinction coefficient in function of wavelength has been presented for obtained series. Through application of different HT conditions, it is possible to obtain tunable LSPR peak depending on silver content. Position and intensity of LSPR band varied slightly with different HT time applied. Samples heat-treated for 6, 24, and 48 hours are shown. Moreover, amount of incorporated silver is also a factor influencing the LSPR band intensity and position. It might indicate that silver nanoparticles size can be altered through change of silver content and performing different HT procedure. However, due to the fact that observed LSPR bands are very wide and amount of introduced silver is small it is difficult to accurately calculate exact shift value of LSPR bands caused by the changes of nanoparticle sizes.

Surface plasmonband is visible in Figures 9(a), 9(b), and 9(c) in the range of 500-550 nm. Silver LSPR peak has been observed above 500 nm in [22, 34]. In tellurite matrix with its refractive index of approximately 2, LSPR band shifts to higher wave lengths in comparison to silicate glasses [20]. This is consistent with the following equation [35]:

[[lambda].sup.2.sub.m] = 2[pi]cm[Ne.sup.2] ([[epsilon].sub.[infinity]] + 2[n.sup.2])/[[epsilon].sub.0], (4)

where N is the concentration of free electrons, [[epsilon].sub.[infinity]] is the metal optical dielectric function, [[epsilon].sub.0] is the permeability of free space, n is the refractive index of glass host, and c and m are speed of light and electron effective mass, respectively. One can find that wavelength of LSPR depends on refractive index of glass matrix. Thus, LSPR is red shifted in case of matrices with higher refractive indices [36].

UV-vis results are consistent with XPS and TEM measurements presented in previous section. Observation suggests the successful nanoparticles formation.

3.2.2. Photoluminescence. In case of excitation spectrum monitored at 615 nm, several bands corresponding to the 4f-4f transitions of [Eu.sup.3+] are apparent. They were assigned to [sup.7][F.sub.0]-[sup.5][D.sub.4] (362nm), [sup.7][F.sub.0]-[sup.5][L.sub.7] (382nm), [sup.7][F.sub.0]-[sup.5][L.sub.6] (395nm), [sup.7][F.sub.1]- [sup.5][D.sub.3] (415nm), and [sup.7][F.sub.0]-[sup.5][D.sub.2] (465nm) transitions [19,37]. Spectrum of AgEu1 sample is presented in Figure 10.

In case of 395 nm excitation, number of peaks due to transitions of [Eu.sup.3+] was observed. Starting with low wavelengths, signals at 536 and 557 nm (as a result of [sup.5][D.sub.1]-[sup.7][F.sub.1] and [sup.5][D.sub.1]-[sup.7][F.sub.2], transitions) and peaks at 588, 615, 654, and 703 nm ([sup.5][D.sub.0]-[sup.7][F.sub.1], [sup.7][F.sub.2], [sup.7][F.sub.3], and [sup.7][F.sub.4] transitions) can be noticed [37-40]. Additionally, matrix spectrum (Ag0 sample) has been obtained as a reference which is included in presented emission spectra.

The same excitation has been used for samples with silver nanoparticles generated through heat treatment process. Results are presented in Figures 11(a), 11(b), and 11(c). For AgEu1 sample annealed for 3, 6, and 12 hours increase of [Eu.sup.3+] emission intensities was observed. Maximum of [sup.5][D.sub.0]-[sup.7][F.sub.2] band intensity (615 nm) was detected for 6 hours of HT time. This can be explained by LSPR which enhances europium ions transitions. [Eu.sup.3+] ions lying near silver nanoparticles are influenced by increased local field around AgNPs. Radiative transition of [sup.5][D.sub.0]-[sup.7][F.sub.2] is electric-dipole transition [41]. It is hypersensitive to local environment change and modification of local symmetry. Considering this, increase of its intensity may indicate influence of silver nanoparticles. Ratio between intensities of 5D0-7F2 peak and [sup.5][D.sub.0]-[sup.7][F.sub.2] magneticdipole transition (588 nm) allows evaluating if the intensity change of [sup.5][D.sub.0]-[sup.7][F.sub.2] transition has the origin in electric field enhancement. This parameter reached the maximum of its value after HT of 6 hours. This is indicative for local electric field influence of AgNPs. To visualize interaction between rare earth ions and silver nanoparticles energy level diagram of [Eu.sup.3+] has been presented in Figure 12.

However, when longer heat treatment times have been applied, quenching of europium transitions was noticed. It is apparent in case of emission spectrum of the AgEu1 sample annealed for 24 hours. This is most likely caused by [Eu.sup.3+]-AgNP energy transfer processes that hinder the radiative transitions promote nonradiative relaxations.

Additionally, growth of silver nanoparticles could lead to decrease of [Eu.sup.3+]-AgNP distance that enhances energy transfer processes [42]. At shorter [Eu.sup.3+]-AgNP distance dipole-dipole interactions become significant resulting in decrease of europium ions luminescence intensity [43,44]. Quenching can also have its origin in increased absorbance of silver nanoparticles grown for longer time periods.

For AgEu2 and AgEu3 glass samples, enhancement of europium emission bands is not observed. The reason is probably an excessive amount of silver added to glass sample. Quenching can occur when ratio of RE ions to silver is below one. Energy transfer mechanisms such as [Eu.sup.3+] [right arrow] AgNP transfer takes place which ultimately prevents the increase of europium ions emission intensities [9,45]. It should be noted that relative position between AgNPs and [Eu.sup.3+] ions is crucial since dipole interactions dominate over local field enhancement when distance separating them becomes shorter. Due to possible small separation between ions and nanoparticles this quenching mechanism cannot be neglected.

Observed lack of enhancement in case of Ag2 and Ag3 series is consistent with TEM results. At higher concentrations silver creates larger agglomerates which could be observed in Figure 6. In case of those samples size of the nanoparticles is not optimal for emission enhancement of rare earth ions. At this point, energy transfer mechanisms become dominant. Moreover, absorption of silver nanoparticles may have increased with size and as a result intensity of rare earth ions emission is decreased. In our system, silver nanoparticles of sizes exceeding approximately 30 nm resulted in lack of [Eu.sup.3+] luminescence enhancement. It is thus concluded that dimensions of silver nanoparticles should be strictly controlled in order to avoid quenching in compositions with higher silver content. This could be done with introduction of appropriate silver amount and heat treatment time. In case of this work, best results were obtained in samples with silver nanoparticles of sizes below 30 nm. Such nanoparticles have been synthesized in AgEu1 series heat-treated for 6 hours.

Exemplary CIE diagrams of Ag1, Ag2, and Ag3 samples heat-treated for 6 hours are presented in Figure 13. Excitation with 395 nm wavelength resulted in reddish-orange emission in case of all samples. Silver amount did not influence the emission color significantly. For simplicity, only samples annealed for 6 hours are presented since all obtained samples emitted similar red to orange color

4. Conclusions

Presented XRD results have shown that amorphous material of 73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]-2[Eu.sub.2][O.sub.3]-xAg (where x = 1,2, and 3) composition has been successfully obtained. No crystallization of glass matrix is detected in the as-prepared samples due to correct conditions of melt-quenching process. DSC study revealed that glass transition temperature and thermal stability TS changes only slightly with introduction of silver ions. For Te[O.sub.2]-BaO-[Bi.sub.2][O.sub.3] glass matrix and Te[O.sub.2]-BaO-[Bi.sub.2][O.sub.3]-Ag sample [T.sub.g] was determined as 321 and 318[degrees] C, respectively. Thermal stability parameter was slightly decreased after silver addition. This is caused by introduction of some nonbridging oxygen in glass matrix which would lead to slight decrease of glass transition temperature. Thus, obtained material is considered to be thermally stable. FTIR results presented that after exposure to heat treatment for excessive time ratio of signal intensities due to Te[O.sub.3] and Te[O.sub.4] species does not change significantly. This in fact confirms that glass matrix is not influenced by HT process and its structure is heat resistant. XPS measurement indicated that in case of Ag1 and Ag3 glass samples annealed for 6 hours most of silver changed its valance state to [Ag.sup.0]. Shape, position, and distance between Ag3d doublet also corresponds to metallic silver. Highest amount of [Ag.sup.0] has been determined in case of Ag3 series probably due to higher silver content. With the employment of TEM imaging technique, round-shaped silver nanoparticles have been observed in case of samples with different silver content and heat treatment time. More importantly, silver nanoparticles increase their sizes with increasing silver content. Nanoparticles diameters were in the range of 20-50 nm. UV-vis absorption results additionally proved that silver nanoparticles have been obtained. It is concluded that change of the silver content together with modification of heat treatment time can result in tunable LSPR band and silver nanoparticles dimensions. It is promising to further study the influence of HT process on silver nanoparticles properties. Photoluminescence measurements presented the enhancement of [Eu.sup.3+] emission bands in case of AgEu1 sample. Enhancement is observed until 6 hours of annealing is applied. Then, for 12 and 24 hours of heat treatment, decrease of intensity is observed probably due to [Eu.sup.3+]-AgNP energy transfer. Obtained materials could find application in tunable red to yellow-white light emitters.

Conflicts of Interest

The authors declare that they have no conflicts of interest. References

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Tomasz Lewandowski, (1) Michal Dembski, (1) Michalina Walas, (1) Marcin Lapinski, (1) Magdalena Narajczyk, (2) Wojciech Sadowski, (1) and Barbara Koscielska (1)

(1) Department of Solid State Physics, Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Gabriela Narutowicza 11/12, 80-233 Gdansk, Poland

(2) Laboratory of Electron Microscopy, Faculty of Biology, University of Gdansk, ul. Wita Stwosza 57/246, 80-952 Gdansk, Poland

Correspondence should be addressed to Tomasz Lewandowski;

Received 28 July 2017; Accepted 1 October 2017; Published 30 October 2017

Academic Editor: Xuping Sun

Caption: FIGURE 1: DSC spectrum of Ag0 (a) and Ag1 (b) glass samples.

Caption: FIGURE 2: XRD result of AgEu1 glass sample annealed for 6 hours.

Caption: FIGURE 3: FTIR spectrum of Ag1 sample noncrystallized (dotted line) and heat-treated for 96 h (solid line). The pink curve refers to signal due to vibrations in Te[O.sub.4] elements while the green one refers to vibration signal in Te[O.sub.3].

Caption: FIGURE 4: Ag3d photoelectron peaks (a) and Auger lines (b) of Ag1 and Ag3 heat-treated samples and noncrystallized (NC) Ag1 sample.

Caption: FIGURE 5: Bi4f photoelectron peaks in Ag1 sample heat-treated for 6 h.

Caption: FIGURE 6: TEM images of Ag1, Ag2, and Ag3 samples heat-treated for 6 hours ((a), (b), and (c), resp.).

Caption: FIGURE 7: TEM images of Ag1 samples heat-treated for 3, 6, and 12 hours ((a), (b), and (c), resp.).

Caption: FIGURE 8: UV-vis transmittance spectrum of AgEu1 sample.

Caption: FIGURE 9

Caption: FIGURE 10: Excitation spectrum of AgEu1 glass sample with [[lambda].sub.em] = 615 nm.

Caption: FIGURE 11

Caption: FIGURE 12: Energy level diagram of [Eu.sup.3+] ions. Observed emissions represented by lines of different colors.

Caption: FIGURE 13: CIE chromaticity diagram of AgEu1 (diamond), AgEu2 (circle), and AgEu3 (triangle) samples heat-treated for 6 hours.
TABLE 1: Parameters of heat treatment performed on obtained samples.

Sample series            Composition (molar ratio)

Ag0               73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]
Ag1             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]-1Ag
Ag2             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]-2Ag
Ag3             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]-3Ag
AgEu1             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]
AgEu2             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]
AgEu3             73Te[O.sub.2]-4BaO-3[Bi.sub.2][O.sub.3]

Sample series           HT (h)            T ([degrees]C)

Ag0                       --                    --
Ag1             0, 3, 6, 12, 24, 48, 96
Ag2             0, 3, 6,12, 24, 48, 96
Ag3             0, 3, 6, 12, 24, 48, 96         350
AgEu1               0, 3, 6,12, 24

AgEu2               0, 3, 6, 12, 24

AgEu3               0, 3, 6, 12, 24

TABLE 2: Thermal parameters of Ag0 and Ag1 glass samples.

Sample   [T.sub.g] ([degrees]C)   [T.sub.c1] ([degrees]C)

Ag0               321                       --
Ag1               318                       387

Sample   [T.sub.c2] ([degrees]C)   TS ([degrees]C)

Ag0                416                   95
Ag1                420                   69

TABLE 3: Results of XPS measurement performed on Ag1 and Ag3 glass

Sample   HT    [Ag3d.sub.5/2]   [Ag3d.sub.3/2]   M4VV   [alpha]'
         (h)        (eV)             (eV)        (eV)     (eV)

Ag1       0        368.0            374.2        355.6   723.6
Ag1       6        368.1            373.9        357.3   725.4
Ag3       6        368.0            374.0        357.6   725.6

Value of Augerparameter of metallic silver [26]:         726.0
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Title Annotation:Research Article
Author:Lewandowski, Tomasz; Dembski, Michal; Walas, Michalina; Lapinski, Marcin; Narajczyk, Magdalena; Sado
Publication:Journal of Nanomaterials
Date:Jan 1, 2017
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