1 Introduction

For the past many years, organic stabilizing agents, such as oleic acid, thioglycerol, and so on [1,2,3,4,5,6] along with other polymers and surfactants, have been utilized in the synthesis of zinc oxide (ZnO) nanoparticles (NPs), which impart the material its stability and also function as a structure modifier [7,8,9,10,11,12,13]. In recent times, stabilization of NPs using bio-capping agents, such as amino acids [14, 15], plant extracts [8, 13, 16], and so on, have attracted substantial interest since such structures are bio-compatible and therefore may be employed for biological applications including DNA or drug delivery, imaging, cosmetics, and others [17, 18]. Thus, amino acids (building blocks of protein) may be deliberated as ideal bio-compatible stabilizing agents. Based on the characteristics of their side chains, amino acids are categorized into various groups, wherein, the physical properties of the side chains may act as an influence during the interaction of amino acid residues with other compounds. Sreevalsa et al. [19] reported the synthesis of l-histidine-capped ZnO nanocrystals possesing potential bio-imaging application with regard to the intense photoluminescence (PL) emission observed at wavelength of ~ 527 nm. Another study based on the biological application of amino acid capped ZnO nanostructures (NSs) has been put forth by Ramani et al. [20]. They utilized three different types of amino acids, namely, l-alanine, l-threonine, and l-glutamine for the capping purpose of ZnO NSs, which resulted in the formation of various morphologies of ZnO. These NSs were then tested for their efficacy as anti-microbial agents against Escherichia coli, Staphylococcus aureus, Klebsiella pneumoniae, and Bacillus subtilis. They concluded the synergistic effect of the respective amino acids adsorbed at the surface of ZnO NSs toward microbial inhibition. Likewise, several reports state the bio-compatible nature of NPs when bound with amino acids [14, 20,21,22]. Moreover, amino acids perform a dual function by acting as an agglomeration controller as well as a shape modifier when used as a binder during NPs synthesis [15]. Wu et al. [15] employed a facile and bioinspired method for ZnO NSs synthesis using histidine as the structure-directing and structure-assembling agent. On varying the ratio of histidine used in their study, they obtained various ZnO hierarchical architectures, such as prism- and flower-like structures, including hollow microspheres. Thus, structure controlled synthesis of ZnO NPs is possible by adjusting the molar ratio of the bio-capping agent used in the study. In this current work, the amino acid glycine has been used as the bio-capping agent [23, 24] for the synthesis of various NSs of ZnO. Glycine is a neutral amino acid, which becomes amphoteric in aqueous medium. Therefore, the co-ordination or the capping ability of this amino acid and its influence over the structural, morphological, and optical aspects of ZnO is an interesting field to investigate (such as the formation of nano-flower buds with increased glycine concentration and nanosheets with different synthetic method).

There are several known synthesis methods of ZnO NPs in Refs. 16 and 25. An important fact that has been deduced by comparing the various synthesis methods is that they may also influence the structural formulation of the NPs, provided all the other parameters remain constant [7]. Elahe et al. [26], compared ZnO NPs based on the method of synthesis, i.e. biosynthesis and chemical synthesis. In their investigation, they found that biosynthesized ZnO NPs exhibited spherical and flower-like structures while chemical synthesis formed irregular surface morphology with much larger size, as compared to the former. Hence, morphology as well as size tuning of the NPs may be achieved by employing different synthesis approaches. However, for a method to prove effective, not only the purity of the final product is important, but also the corresponding cost-effectiveness and eco-friendliness of the method opted. Thus, simple and economical methods of glycine capped ZnO NPs (gly@ZnO NPs) have been considered in this study. In order to compare the differences in morphology, size, optical and structural properties of the as-synthesized ZnO NPs, three different methods of synthesis were considered in this study, namely, room-temperature solid state, co-precipitation and hydrothermal methods. The results exhibited interesting photophysical and morphological outcome. The choice of these synthesis techniques was based on the simplicity, economical, eco-friendly, and time saving properties. Moreover, a co-relation based on the photoluminescence (PL) (optical) and Field emission scanning electron microscopy (FESEM) (morphological) studies has also been executed.

The problem of water scarcity is accelerating day-by-day [27, 28]. The major causes attributing to this ever-rising water pollution include improperly treated organic wastes (such as drugs, dyes, and other chemicals), heavy metal ions, etc., in addition to the solid plastic wastes [29, 30]. Organic dyes [31] mostly dissipate from the textile industry [32]. They have a complex molecular structure and are highly stable under ambient condition. Dyes are toxic and known to be carcinogenic in nature [33, 34]. Therefore, proper treatment of dyes before disposal into water bodies and the removal of already disposed dyes from aquatic media are of utmost importance and should be immediately taken into consideration. In the current research, the issue of degrading an organic dye, rhodamine B (RhB), into simple, non-harmful inorganic compounds has been accounted using the as-synthesized gly@ZnO NPs through the method of photocatalysis under natural solar irradiation. It has been well established through previous studies that reactive oxidative species (ROS) are primarily responsible for the overall photocatalytic degradation phenomenon [35, 36]; therefore, herein, a study related to the role of various ROS has been carried out using complimentary radical scavengers. Additionally, the stability of the as-synthesized photocatalyst has also been tested by performing the reusability test.

2 Experimental section

2.1 Chemical specifications

The chemicals used in this study were of analytical grade, which includes zinc acetate dihydrate (Zn(CH3COO)2·2H2O; Lobachemie make; molecular weight (MW) 219.50 g/mol), sodium hydroxide (NaOH; Lobachemie make; MW 40 g/mol), glycine (C2H5NO2; Merck made; MW 75.07 g/mol), p-benzoquinone (C6H4O2; Lobachemie; MW 108.095 g/mol), tertiary butyl alcohol (C4H10O; Merck made; MW 74.12 g/mol), ethylene diamine tetra acetate (C10H16N2O8; Merck make; MW 292.24 g/mol), methanol (CH3OH; Rankem make), and rhodamine B (C28H31ClN2O3; Lobachemie make; 479.02; absorbance maxima in water: 550–554 nm). Deionized (DI) water with resistivity: 18.5 MΩ cm was used for all analysis.

2.2 Characterization

Information related to the crystal structure of Gly@ZnO NPs was obtained through PAN Alytical Spectris technologies PW 3040/60 X-ray diffractometer with Cu Kα1 radiation (λ = 1.54056 Å), working voltage of 40 kV, and current of 30 mA. The existence of bio-capping fragments on ZnO NPs’ surface was confirmed by Fourier transform infrared spectroscopic (FTIR) spectrum obtained from IRAffinity-1S Shimadzu Fourier transform infrared spectrophotometer. Optical properties were studied using UV–visible (UV–Vis) absorption data performed on Shimadzu 1800 UV–Vis spectrophotometer and PL spectroscopy measured on Shimadzu Spectrofluorophotometer (RF-5301 PC) with excitation wavelength (λexc) of 325 nm. Nitrogen (N2) adsorption–desorption measurements were performed using Quantachrome Instruments, Autosorb-IQ volumetric adsorption analyser at −200 °C. For measurement, the samples were de-gassed at 150 °C for 4 h in a degassing port of the adsorption apparatus. The determination of specific surface area of the samples was carried out employing the adsorption data points obtained at (P/P0) between 0.4 and 1.0 using Brunauer–Emmett–Teller (BET) equation. The mean (average) pore diameter was estimated using Barrett–Joyner–Halenda (BJH) method. The electrochemical impedance spectra (EIS) were recorded by Electrochemical Analyzer CHI608E, wherein silver/silver chloride (Ag/AgCl) was used as the reference electrode, Platinum wire as the counter-electrode and a glassy carbon electrode (GCE) as the working electrode. The electrochemical experiments were performed under dark conditions at room temperature. EIS responses were acquired using a well-cleaned GCE modified with the respective gly@ZnO samples. 1 mM potassium ferricyanide (K3Fe(CN)6) in 0.1 M potassium chloride (KCl) was employed as the redox analyte. The polarization of the electrode was performed at 0.25 V against the frequency range of 1 Hz to 100 kHz. [Fe(CN)6]3−/4− couple was used as the redox probe following the work performed by Maruthupandy et al. [37]. High-resolution transmission electron microscopy (HRTEM) with LaB6 source and voltage of 200 kV equipped with an energy dispersive X-ray spectroscopy (EDS) was used for the microstructural and elemental analysis, respectively. Lux-meter (MEXTECH; model no. LX-1010B) was used to measure the solar intensity [(intensity = 1080 × 100) lx for all the photocatalytic experiments]. Morphological information was obtained using JEOL FESEM, Model: 7610F.

2.3 Synthesis

Tuning the morphology, size, microstructure, and optical properties of NPs largely depend upon their methods of synthesis and the type of capping agents used [38,39,40,41]. The use of low-temperature, top-down, and solid-state method is a highly efficient technique of preparing ZnO NPs [7, 42, 43] since this method is environmentally benign, cost-effective (requires only a simple mortar-pestle) and utilizes a minimum temperature (although high-temperature solid-state methods have also been reported, in the present study a temperature of 100 °C was employed). For identifying the morphology and size-tuning based on different synthesis methods, two bottom-up solution-phase approaches of ZnO NPs synthesis were also employed, namely, co-precipitation and hydrothermal methods. Stability of the as-synthesized NPs is another concern since the high energy NPs tend to aggregate and form bulk particles. To address this issue, the use of a bio-capping agent, glycine, was considered in this work. Figure 1 represents the different synthetic strategies and the steps involved in the respective technique of gly@ZnO NPs formation. These samples have been designated as GZ1, GZ2, GZ3, GZ4, and GZ5 throughout the manuscript based on their synthesis method as given in Fig. 1. Further, the pH values of the samples measured during their synthesis were 12, 11.8, 11.9, 12.2, and 12.2 for GZ1, GZ2, GZ3, GZ4, and GZ5, respectively. However, during the washing process, these pH values were brought to the neutral level of ~ 7.

Fig. 1
figure 1

Description of the procedures for synthesizing gly@ZnO NPs

2.4 Photocatalytic activity measurements

The photocatalytic degradation of RhB was performed under solar irradiation with the average measured intensity of (1080 × 100) lx. Figure 2 represents the stepwise procedure employed for carrying out the photocatalytic degradation studies. Also, during the photocatalytic reaction, the 5 mL solution (aliquot) was subjected to UV–Vis spectral analysis, while the whole reaction mixture was covered with aluminium foil. After analysis, the aliquot was transferred back into the reaction medium and again exposed to sunlight irradiation. Degradation efficiencies of gly@ZnO NPs were calculated in percentage of decrease in the concentration of dyes relative to the absorption measurements. For the reusability test, GZ2 was chosen in three consecutive experiments while maintaining similar reaction conditions, i.e. 0.05 g GZ2 with 50 mL of RhB solution. The interval of exposure under solar radiation was also kept constant at 60 min. After each test, the photocatalyst was recovered through centrifugation and 50 mL of RhB solution was added. Rest of the steps were followed as before.

Fig. 2
figure 2

Steps involved in the photocatalytic degradation studies of RhB by gly@ZnO NPs (*corresponds to [44])

3 Results and discussion

3.1 Characterization

3.1.1 Structural analysis

Figure 3a shows the XRD diffraction patterns of GZ1, GZ2, GZ3, GZ4, and GZ5 samples, respectively. In accordance with the JCPDS card no. for ZnO (36-1451) [7], the entire diffraction pattern corresponds to the ZnO hexagonal wurtzite structure. Additional peaks of Zn(CH3COO)2, sodium acetate, etc., or any other impurity peaks were not observed, which may be attributed to the high-purity formation of all gly@ZnO NPs. The consistency of 2θ values in case of all the samples indicates a negligible change in the ZnO lattice with insignificant microstrain effect. Employing the Debye Scherer equation [45], average crystallite sizes of gly@ZnO NPs were calculated in Table 1. Further, Table 1 provides information on the values of 2θ (peak positions), lattice constants (a and c), volume of unit cell (V), lattice (d) spacing, and full width at half maxima (FWHM) of (101) plane, respectively. From this table, it may be inferred that in case of all the samples, the lattice structure and unit cell do not exhibit a significant difference. Therefore, there is presumably no distortion in ZnO structure or changes in ZnO lattice. Additionally, not much variation in the average crystallite sizes of the as-synthesized gly@ZnO NPs may be noticed. The samples GZ1, GZ2, and GZ3 have approximately similar crystallite sizes, while GZ4 and GZ5 samples have slightly bigger crystallite sizes. This observation suggest that the structure-directing ability of glycine in the solid-state synthesis and solution-phase (i.e. co-precipitation and hydrothermal) techniques may have led to the formation of different microstructures as well as morphologies of gly@ZnO NPs.

Fig. 3
figure 3

a XRD spectra and b FTIR patterns of gly@ZnO NPs

Table 1 XRD data analysis corresponding to (101) crystal plane of gly@ZnO NPs

The capping effect of glycine on the surface of gly@ZnO NPs was confirmed on the basis of FTIR spectra as shown in Fig. 3b, recorded in the scanning range of 600–2000 cm−1. FTIR bands for free glycine are observed at 1596 cm−1 for the antisymmetric vibrational mode of COOa(COO)] and 1412 cm−1 for the symmetrical vibrational mode of COOs(COO)] [46]. In this work, shifts in the FTIR band positions were observed to 1730.61 and 1452.2 cm−1, respectively. These shifts may be ascribed to the symmetrical stretching vibrational mode of glycine indicating the co-ordination of the oxygen atom from the COO group [46]. The intensity of these peaks was observed to be the highest in case of GZ2, which may be attributed to the presence of more glycine moiety on ZnO surface. This validates the XRD analysis, wherein smaller crystallite size was observed for GZ2.

3.1.2 Morphological and elemental studies

The various properties, such as optical, surface, structural, and so on, of NPs depend greatly on the morphology of the as-formed particles [47, 48]. This means that the differences in the photophysical and catalytic properties of various samples may directly be co-related to the shape of the particles present in the respective samples. Different morphologies exhibit different surface area as well as varying degree of surface defects. Therefore, in order to fully understand and associate this fact with the present investigation, FESEM studies were performed, as provided in Fig. 4a–e. FESEM images of GZ1, GZ2, and GZ3 clearly point out the fact that the amount of capping material (glycine) during synthesis helps to regulate and modify the morphology of the NPs, which means, in this case, glycine acted as a structure-directing agent during the formation of ZnO NPs. When the amount of glycine was considered as least during synthesis (in GZ1), certain highly agglomerated structure with few ZnO nanorods was observed, as shown in Fig. 4a.

Fig. 4
figure 4

FESEM images (100 nm scale bar) of a GZ1, b GZ2, c GZ3, d GZ4, e GZ5, and f elemental information of GZ2 as obtained through EDX spectroscopic measurements

With increase in the amount of glycine to the most (in GZ2), it may be seen from Fig. 4b that 3–4 nanorods have agglomerated to form bundle-like structures which further agglomerated to ultimately form flower bud-like ZnO nanostructures. The uniformity of nanobuds in GZ2 may also be noted. In case of GZ3, the concentration of glycine was in-between that of GZ1 and GZ2, wherein ZnO nanorods arranged into bundles as shown in Fig. 4c. In this case, unlike GZ1, only agglomerated ZnO nanorods are seen, although these bundles have not inclined towards the formation of ZnO nanobuds as in the case of GZ2. Based on these results, the highest amount of glycine (as in the case of GZ2) was chosen for the synthesis of GZ4 and GZ5 but with two different synthesis approaches, so to understand the role of the synthesis procedure in altering the morphology of ZnO NPs (for synthesis information, refer Sect. 2.3). Figure 4d illustrates sheet-like structures of GZ4 intertwined with one another, while in case of GZ5 (Fig. 4e), ZnO nanosheets with thicker surfaces are visible, including very few agglomerated rod-like structures. These changes in morphologies, as evidenced for GZ2, GZ4, and GZ5, owing to the utilization of different synthesis techniques, confirm the role of various synthesis approaches for morphological tuning, when all the other experimental parameters are kept constant. In Sect. 3.2, the formation mechanism of these nanostructures of ZnO capped with glycine has been explained in detail. EDX analysis is an important tool to confirm the elemental composition of the sample. Figure 4f corresponds to the EDX spectra for GZ2, representing the presence of zinc, oxygen, and carbon in the sample. The presence of carbon is attributed to the carbon grid used as a sample holder during analysis. The corresponding weight and atomic percentages of elements present in GZ2 are also shown, which are in accordance with the expected values.

3.1.3 Optical analysis

The gly@ZnO NPs were ultra-sonically dispersed in DI water and their UV–Vis absorbance recorded in the scanning range of 300–450 nm; the corresponding results are shown in Fig. 5a. The spectra were corrected for water contribution.

Fig. 5
figure 5

a Absorbance spectra of gly@ZnO NPs with inset figure corresponding to the Tauc plots and b absorbance spectra of undried GZ2, GZ4 and GZ5

It may be observed that the representative absorption peaks of all the samples are slightly blue shifted with reference to the absorbance maximum of bulk ZnO (~ 380 nm).This ascertains the presence of smaller particles as compared to that in bulk ZnO [49, 50]. The narrow absorbance peaks may be accredited to the intrinsic band gap absorption of ZnO NPs arising from the electronic transitions, i.e. O2p valence band (VB) → Zn3d conduction band (CB) [51, 52]. The absorbance maxima of the samples are approximately at analogous positions which means that the particles have almost similar sizes. The inset of Fig. 5b depicts the estimation of direct optical band gap energies (Eg) of the respective gly@ZnO samples, which were calculated employing Tauc equation [53]. The values of the band gap energies of gly@ZnO NPs (2.98 ± 0.07 eV) are lower than that of bulk ZnO (~ 3.3 eV) [54]. A reasonable justification to this observation may be the existence of various surface defects, such as valence-band donor level overlap of the surface states, defect levels within the band gap, and so on [55,56,57]. These defects may be identified through PL spectroscopic technique [58]. Further, in order to justify the formation of ZnO nuclei prior to heat treatment, the UV–Vis absorbance measurements of the undried GZ2, GZ4, and GZ5 were performed (similarly as before) which is shown in Fig. 5b. This graph clearly shows the absorbance peaks of ZnO with minor shifts in the peak positions relative to those of the corresponding dried gly@ZnO NPs. The probable reason for this observation may be the presence of zinc-hydroxyl groups, which are the ZnO growth species. It is well known that heat treatment increases the size of the particles via agglomeration [59, 60]; therefore, the hypsochromic shifts in the absorbance bands of undried samples as compared to dried ones may be as a result of their comparatively larger size than undried gly@ZnO NPs.

PL studies were performed in the wavelength range of 340–600 nm. Figure 6 represents the PL spectra of all the as-synthesized gly@ZnO NPs. It is highly interesting to note that although most of the emission peaks are common in the as-synthesized samples (as shown in Fig. 6), the nature of green emission peak is similar for GZ1 and GZ2 and different for the rest, a broad green emission peak in GZ3 and GZ4 (both dried and undried), and no green emission in GZ5 (both dried and undried). This difference in the PL spectra may be co-related to their corresponding morphologies. The morphology of GZ1 depicts an agglomerated structure with few nanorods, while that of GZ2 is nanobundles, which have agglomerated into nanobuds-like structure. The agglomeration of individual particles is the highest in these two structures as compared to that in nanorods of GZ3 or nanosheets as in the case of GZ4 and GZ5. Therefore, agglomeration may have been the main reason for inducing green emission defect (of similar type) in these two samples. For comparison, PL was performed for GZ2, GZ4, and GZ5 samples before and after the heat treatment. In the PL spectra of undried GZ2, the green emission peak is broad and non-intense. This leads to the inference that in this sample, the heat treatment was basically the main factor which induced more defect states arising from green emission. In GZ4, although the PL spectra for dried and undried samples have the same nature, the intensity of the bands is opposite to each other, wherein up to blue-emitting region, the intensity is higher for dried sample and after that the intensity is relatively lower than that for undried GZ4, as observed in Fig. 6d. The nature of the PL spectra for both undried GZ5 and dried GZ5 is the same (Fig. 6e). Further, no green emission has been observed in this case, which leads to the conclusion that visible region-related defect states are not present in these samples. This means that the defect emission states corresponding to green emission are suppressed during the hydrothermal synthesis. The differences in intensity (as has been encountered in all the gly@ZnO NPs) may be attributed to the increase in the magnitude of the defect states pertaining to the visible region for the dried and undried samples.

Fig. 6
figure 6

PL spectra of a GZ1 with the inset figure depicting the deconvoluted spectra for the peak centred at 545 nm, b GZ2 and undried GZ2, with inset representing the deconvolution of the peak located at 545 nm of GZ2, c GZ3 and undried GZ3, d GZ4, e GZ5 and undried GZ5

Figure 6 displays the appearance of various emission peaks, which are explained as follows: (i) the near band-edge emission (NBE) (at 362 nm and 361 nm) for GZ1, GZ2 and GZ4, respectively, is due to exciton recombination; (ii) the blue emission band ranging from 450–495 nm is the characteristic band of ZnO, which may be attributed to the electron–hole pair recombination between singly ionized Zn interstitial state (I*Zn) and the valence band [61]; and (iii) the green emission bands appearing for GZ1, GZ2, and GZ4, respectively, may be ascribed to the recombination of electrons arising from the deep level isolated singly ionized oxygen centres with the photo-produced holes [61]. Therefore, it may be inferred that the PL spectra of the samples may be manipulated or controlled by tuning the morphology and phase structures.

3.1.4 Specific surface area analysis

In order to determine the specific surface area and the porous nature of the as-synthesized gly@ZnO NPs, N2 adsorption–desorption isotherms and Barret–Joyner–Halenda (BJH) pore size distribution curves of GZ2, GZ3, and GZ4 were studied, respectively, and have been presented in Fig. 7a–c.

Fig. 7
figure 7

ac N2 adsorption–desorption isotherm (BET) and BJH pore size distribution (inset) and d corresponding specific surface area and average pore diameters of GZ2, GZ4, and GZ5, respectively

The obtained isotherms of these samples belong to type-IV N2 adsorption–desorption isotherm with an H1 hysteresis loop at relative pressure (P/Po) ranging from 0.4 to 1.0. The insets of Fig. 7a–c represent the corresponding curves of the BJH pore size distribution. The BJH pore size distribution of GZ2 and GZ5 reveals the mesoporous nature of these samples, while that of GZ4 exhibits its macroporous nature [62,63,64]. The average pore diameters of GZ2, GZ4, and GZ5 are given in Fig. 7d along with their BET-specific surface areas. The highest BET-specific surface area has been obtained for GZ2, which may be attributed to its 3D-flower bud-like morphology as obtained from FESEM image.

3.1.5 Electrochemical impedance spectral (EIS) analysis

The PL analyses of the samples provided an insight into the presence of defect states in the samples. These defects may strongly influence the electrical properties of the samples as well as their photocatalytic activities. In this regard, EIS analyses were performed since it is a powerful technique to probe into the electrical characteristics of the as-prepared ZnO semiconductor nanomaterials [65].

Fig. 8
figure 8

Electrical impedance spectra: Nyquist plot of gly@ZnO samples under dark conditions

Figure 8 represents the Nyquist plots of all the gly@ZnO samples. As may be observed, there is only one semi-circle arc in the Nyquist plots of all the samples. These semi-circle arcs represent the recombination resistance, which in turn is related to the electronic recombination at the interface. Further, the radius of the arc signifies the recombination resistance [66, 67], whose value is inversely proportional to the values of the recombination rate and density of electrons in the material. In this case, the recombination resistance of GZ1 and GZ2 is relatively much higher as compared to other samples. Since larger recombination resistance corresponds to lower rates of recombination, comparatively greater electron transfer occurs in these samples. This explanation ultimately implies the higher rates of electron transfer in GZ1 and GZ2 as compared to other samples.

3.1.6 Microstructural studies

To determine the microstructure of GZ2, HRTEM characterization was carried out as depicted in Fig. 9a–c, respectively. As may be observed from Fig. 9a, b, hexagonal particles are present in the microstructure of GZ2. This corresponds to the fact that hexagonal particles formed bundles, which later agglomerated to form a flower bud-like GZ2 nanostructures. The average length and breadth of the particles were calculated to be in the range of 10–12 nm and 25–30 nm, respectively.  Figure 9c represents the HRTEM image of GZ2 sample. The value of d-spacing, as calculated from this image, was found to be 2.09 Å for (101) plane, which is consistent with the value as obtained from the XRD analysis (2.48 Å), as reported in Table 1. Figure 9d represents the selected area electron diffraction (SAED) pattern of GZ2 sample, which indicated the polycrystalline nature of the sample. For other samples also, similar crystalline nature was observed.

Fig. 9
figure 9

TEM images of GZ2 at a magnification of 10 nm, b magnification of 5 nm, c HRTEM image displaying the lattice fringes, and d SAED pattern

3.2 Formation mechanism of various morphologies of gly@ZnO NPs

Based on the aforementioned results, the probable formation mechanism of various morphologies of gly@ZnO NPs has been discussed in this section. It has been established that hydroxyl ions and amino acid molecules, in this case glycine molecule, act as competitive ligands toward Zn2+ owing to the various rates of formation constants of the complex [15, 68]. In case of GZ1 and GZ3, the ratio of glycine/Zn2+/NaOH was maintained at 0.5:1:5 and 1:1:5, respectively. Thus, OH must have played a vital role in directing the structure of the as-formed NPs. Since the concentration of glycine was much lesser than that of the hydroxide precursor, formation of Zn(OH)n complex may have been greater than Zn(glycine)n complex, and this must have been the reason for the formation of rod-like nanostructures, wherein elongation of the c-axis was predominant [7]. It is also to be noted that in case of GZ1, the amount of glycine was insufficient in exhibiting its potential capping application, whereas in case of GZ3, as the amount of glycine was doubled, agglomeration-controlled synthesis of ZnO NPs was observed with the overall conversion of particles into rod-like structures. In case of GZ2, the ratio of the precursors used was 2:1:5. This increased concentration of glycine led to its adsorption on the surface of ZnO nuclei (analogous to FTIR result) and as a consequence, nanobuds-like structure resulted from the agglomeration of nanobundles. It is evident from the structures of GZ4 and GZ5 that unlike in the previous cases, herein, the formation of nanosheets has taken place. The most important distinction between GZ1, GZ2, GZ3, GZ4, and GZ5 is their method of synthesis, respectively.

Fig. 10
figure 10

Pictorial representation of gly@ZnO NPs formation mechanism

The former were prepared through the grinding process in the solid-state phase, while the latter were prepared via solution-based systems. Further, the contact time of the reacting molecules was longer in the latter as compared to the former. Through this discussion, it may be concluded that the solution-based synthesis methods favour the formation of nanosheets when glycine is used as a capping agent under parameters as described in Fig. 1. The mechanism of nanosheets formation (GZ4) may be explained as the mixing of the precursors led to the formation of ZnO nuclei, which then grew into nanoclusters. Further, ZnO growth species, i.e. Zn(OH)n, favourably adsorbed onto the surface of ZnO nuclei and consequently, assisted the growth along c-axis in order to reduce the energy otherwise required for hexagonal crystal structure [69,70,71]. Thereafter, ZnO NPs underwent oriented coalescence leading to the formation of nanosheets-like structure. The formation of thicker nanosheets, as in the case of GZ5, relies on the defect states available in nanosheets (as in GZ4). Since the synthesis procedures of GZ4 and GZ5 are similar up to the stirring step after the mixing of precursors, it may be assumed that during this time interval, thinner nanosheets as in GZ4 were already formed. The defects available in these nanosheets must have acted as nucleation sites during the hydrothermal process that the growth of secondary nanosheets occurred [71] and thereby resulted in the formation of thicker nanosheets. A schematic has been presented in Fig. 10 to pictorially describe these explanations.

3.3 Application: rhodamine B degradation studies

The toxicity of RhB for marine as well as terrestrial species has been previously discussed in Refs. 72,73,74. Pertaining to the fatal effects of this harmful dye, the present investigation has attempted to degrade the complex molecular structure of the RhB organic dye into simple, non-harmful inorganic compounds.

Fig. 11
figure 11

a UV–Vis absorbance spectra illustrating decrease in the absorbance maxima of RhB with time of sunlight irradiation, b adsorption spectra (under dark condition) of RhB by gly@ZnO samples, c percentage of photocatalytic degradation of RhB by gly@ZnO samples, and d radical scavenging experiment depicting the role of ROS in the photocatalytic degradation process by GZ2

The UV–Vis absorption maximum of this dye in aqueous medium is at 554 nm due to the n → π* transition from C=N, C=O groups present in the dye structure [75]. The decrease in this absorbance maximum was used to estimate the decolourization level.

Fig. 12
figure 12

a Kinetics of photocatalytic RhB degradation by gly@ZnO NPs, b reusability test of GZ2 against three consecutive cycles, and c schematic representation of the degradation mechanism

Figure 11a represents the ongoing temporal absorption of RhB solution during natural solar irradiation by the respective gly@ZnO samples. Photolysis of RhB solution was also conducted under identical conditions for comparison. It may be observed that negligible reduction of ~ 17% in the absorbance maximum of RhB solution occurred upon photolysis, indicating the stability of RhB under sunlight illumination. Upon addition of the respective gly@ZnO samples (procedure given in Sect. 2.4), sharp decrease in the absorbance corresponding to > 90% was noticed. After 60 min of experimentation, the bright pink colour of RhB solution completely vanished and turned colourless. This decrease in the absorbance peak to minimum (~ 0) may be attributed to the breakdown of both the chromophoric group and the dye dimer of RhB [7]. Therefore, enhanced acceleration in the degradation process was possible due to the presence of the photocatalysts (i.e. gly@ZnO NPs). Further, the decomposition of RhB takes place via two mechanisms, i.e. (i) the destruction of conjugated structure and (ii) N-de-ethylation [76,77,78]. This means that RhB may directly break down to its photo-degraded end products like CO2, NO3 or NOx or through the stepwise N-de-ethylation process, respectively. The dominance of N-de-ethylation may be specified by a blue shift in the absorbance maxima of RhB accompanied by its decrease in intensity. As is clear from Fig. 11a, no blue shift in the peak at 554 nm was observed upon degradation. Therefore, in this case, the photocatalytic degradation of RhB was pre-dominated by the process of conjugated structure breakdown.

Figure 11b represents the adsorption spectra after 60 min of mixing RhB solution with the respective gly@ZnO samples under dark conditions. It may be observed from this graph that the maximum adsorption efficiency was 21% exhibited by GZ2 as compared to other samples. Also, from Fig. 11a, the degradation percentage of photolysis was only 17%. These results signify that both photocatalyst and photons are imperative for the complete removal of RhB dye from aqueous medium. Further, when the RhB and GZ2 reaction mixture was directly exposed to sunlight, without performing the adsorption experiment, a relatively lower photocatalytic degradation efficiency was acquired (~ 15%) than that obtained following the adsorption studies. This experiment, therefore, proves the synergistic role of adsorption and photodegradation mechanisms for the removal of RhB dye from aqueous medium. Figure 11c shows the percentage of RhB degradation with respect to specific time of irradiation. It may be noticed that under 15 min of natural solar irradiation, ~ 80% of RhB solution was degraded by GZ2, while the other samples degraded less than ~ 50%. This analysis indicates the highly proficient photodegradation property of GZ2 as compared to other samples under study. The activity of reactive oxidative species (ROS) in the reaction medium, particularly, hydroxyl radicals (OH·), superoxide radicals (O2·) and holes (h+), is responsible for the photocatalytic degradation process. These ROS undergo redox reactions with the dye molecules adsorbed at the surface of the photocatalyst and form the degradation products like carbon dioxide (CO2), water (H2O) and simple inorganic compounds [44]. In this work, due to the higher degradation efficiency of GZ2 towards RhB, the radical scavenging experiment was performed in case of GZ2 and the results are depicted in Fig. 11d. The radical scavengers used were 15 mM t-BA for ·OH, 15 mM p-BQ for O2· and 15 mM EDTA for trapping h+. Maximum degradation occurred in the absence of any quenching agent while the percentage of degradation quickly reduced upon their addition. This result indicates that all ROS are important for efficient photocatalytic degradation of RhB. On the other hand, minimum degradations were observed with EDTA and t-BA, indicating that the complimentary radicals, namely, h+ and OH·, respectively, were contributing more toward the photocatalytic degradation mechanism of RhB as compared to O2·.

The photocatalytic activity of the as-prepared gly@ZnO NPs was studied more precisely based on their RhB degradation kinetics. The linear fitting of natural logarithm for the concentration of RhB at different irradiation time fitted well by an exponential decay curve signifying pseudo-first-order kinetics as shown in Fig. 12a. The corresponding rate constant (k) values were calculated using Eq. 1 given below

$$\ln\frac{C_{\textrm{t}}}{C_{0}}=- kt$$
(1)

where C0 and Ct are the initial and final RhB concentrations at time t and k is the pseudo-first-order rate constant.

Table 2 Rate constant values of gly@ZnO NPs for RhB degradation and their corresponding degradation percentages

The calculated values of rate constants for the photocatalytic degradation of RhB by the as-prepared gly@ZnO NPs are given in Table 2 along with their corresponding degradation percentages. It is evident from Table 2 that the sample GZ2 has the highest value of the rate constant indicating the highest photocatalytic degradation efficiency amongst the other gly@ZnO NPs. Further, photostability of the catalyst is of paramount importance to carry out a low-cost process. In this regard, the reusability test of GZ2 was performed over three successive cycles, depicted in Fig. 12b. It was observed that negligible change in the degradation efficiencies was observed, indicating the stability of GZ2 sample. Hence, GZ2 may prove to act as an industrially viable photocatalyst.

The reason for the higher photocatalytic degradation efficiency of GZ2 as compared to other samples may be attributed to relatively higher surface area of GZ2 due to morphology as well as greater magnitude of visible light defect states. It has been reported in literature that the 3-D flower-like morphology has more surface area as compared to 2-D nanorods or nanosheets [79]. In this study also, a similar trend was observed, wherein the ZnO with 3D nano-flower bud-like morphology exhibited a higher specific surface area as compared to those with 2D nanosheets-like morphology, as confirmed through N2 adsorption–desorption analysis. As was observed through PL studies, the intensity of visible light defect emission was the highest in case of GZ2. It has been well established that the higher magnitude of defect states increase the lifetime of electron or hole as well as the effective surface area of the particles. This higher recombination resistance of GZ2 was recognized through EIS analysis. Therefore, greater adsorption of the dye by GZ2 was possible through increased surface area, while higher rates of electron transfer accelerated the photodegradation of RhB molecules by GZ2. Since the defect states increases the lifetime of electron or hole as well as the effective surface area of the particles, greater adsorption and thereby degradation of RhB molecules were possible with this sample.

Table 3 Comparison of photocatalytic dye degradation efficiencies of ZnO nanostructures synthesized using different capping agents

The possible mechanism during the interaction of photons with dye molecules and photocatalyst has been reported elsewhere by the Authors for other samples [7, 13, 16] and is schematically presented in Fig. 12c for the present study. The probable products of degraded RhB molecules, as mentioned in this figure, are based on previous studies [62, 90]. Table 3 represents the comparison between the photocatalytic dye degradation efficiencies of ZnO nanostructures as collected from previous literature with the current study. It may be seen from this table that the current work is amongst the samples exhibiting the highest degradation efficiencies.

4 Conclusions

In this study, glycine was used as a structure modifier and an agglomeration controller of the as-synthesized particles. Three different methods of synthesis were compared on the basis of their properties and photocatalytic performance, i.e. solid state, co-precipitation, and hydrothermal methods. Based on the overall results, the following conclusions have been drawn:

  1. 1

    In solid-state synthesis, the amount of glycine determined the structural orientations of the particles, as was observed from GZ1, GZ2, and GZ3 samples. With an increase in the glycine amount, the agglomerated particles first orientated into rod-like structures, while further increase led to the arrangement of these rods into flower-like morphology. These results confirmed the requirement for the optimum usage of capping agent for structural modification of the NPs.

  2. 2

    On changing the synthetic process to solution phase, the formation of nanosheet-like structures occurred. This result clearly proves the alteration in the physical form of the NPs upon the utilization of varying synthetic processes.

  3. 3

    After analysing the PL data of all the samples, it was observed that the nature of the PL curve was strongly co-related to the morphology of the as-synthesized ZnO NPs.

  4. 4

    Further, higher magnitude of visible region defect levels corresponded to the effective surface area of the as-synthesized particles and consequently resulted in higher photocatalytic activity.

  5. 5

    The optical band gap energy was found to exhibit hypsochromic shift as compared to that of bulk ZnO due to the presence of various defect states in the samples.

  6. 6

    The specific surface area of gly@ZnO NPs greatly dependent upon their morphology, wherein nano-flower buds-like ZnO exhibited the highest surface area as compared to other structures which may be attributed to its 3D structure and higher magnitude of surface defects.

  7. 7

    Through EIS analyses of all the samples, the greater recombination retardation was observed in case of GZ1 and GZ2 samples, indicating the relatively higher electron transfer in these samples amongst others.

  8. 8

    RhB degradation was observed to be relatively maximum in case of GZ2 owing to its 3D flower bud-like structure possessing comparatively higher surface area due to a greater magnitude of the defect states as well as lower recombination rates corresponding to higher electron transfer.

  9. 9

    GZ2 exhibited excellent stability as a photocatalyst making it a potential candidate for industrial usage.

Therefore, the morphology and the corresponding properties of the NPs may be tuned employing different synthetic processes.