Transmission electron microscope (TEM) image (Fig. 1.(a)) shows the crystalline nature and morphology of S-CDs. It can be seen that particles are uniformly formed and almost spherical in shape. The histogram plotted (inset of Fig. 1.(a)) shows that particles have an average size of 3 nm. The existence of the crystalline graphite-like structure is confirmed in S-CDs from the HR-TEM image (Fig. 1.(b)). The interplanar spacing of 0.253 nm in S-CDs is due to the (100) phase of hexagonal graphite.
The Selected Area Electron Diffraction (SAED) pattern given in Fig. 2 indicates the poly-nanocrystalline nature of the S-CDs [43]. The interplanar distances calculated from the SAED pattern are found to be 0.20 nm and 0.24 nm which are associated with the (100) and (002) planes which illustrates effective formation of graphitic carbon structures.
The XRD pattern of S-CDs shown in Fig. 3. reveals that the sample has a broad diffraction peak around 2θ = 21o which corresponds to the (002) plane of graphite ((JCPDS file number: 41-1487). This peak can be attributed to the turbostratic phase of carbon present in CDs [44].
The Energy-dispersive X-ray (EDX) spectroscopy images (Fig. 4) of CDs and S-CDs was analysed to determine elements present in carbon dots. Both CDs yielded a carbon-oxygen ratio of 3:2, indicating a fairly high formation of graphitic structures in them. The combined presence of 7 wt% nitrogen and sulphur in S-CDs confirms the S-doping in a larger ratio.
From the Fourier transform infrared (FTIR) spectrum of the CDs (Fig. 5), the observed peak values are in good agreement with the reported data for carbon quantum dots. The characteristic bands observed at 3291 cm− 1 for both CDs and S-CDs can be attributed to stretching vibration of O-H groups during carbonization [45]. The dominant C = O stretching vibrations at 1737 cm− 1 is the evidence for the existence of more carboxylate groups on the surfaces of the CDs due to carbonization at high temperature [46]. A small band peaked at 1630 cm− 1 is due to C = C stretching mode [47]. A broad band peaked at 860 cm− 1 is due to C-H bending vibrations while bands in range 1000 cm− 1 to 1240 cm− 1 shows that the surface of the C-dots contains C-H and C-O-C bonds. The existence of the C-H bond [48] is indicated by the bands at 2940 cm− 1 and 2876 cm− 1. The C-O-C stretching vibrations in CDs is due to contributions from compounds such as volatile acids, sugars and amino acids present in the lemon juice [45].
The absorption spectra (Fig. 6) of carbon quantum dots in ethylene glycol consists of a broad and strong absorption in the UV-Visible region of the spectrum. S-CDs shows strong absorption at 240 nm which is due to π – π* transition of sp2 hybridised graphitic core. An absorption band between 250 nm and 300 nm wavelength present in both the CDs can be attributed to n – π* transition corresponding to edge states of the carbon dot core. These edge states are part of the interface between sp2 hybridised and sp3 hybridised carbon. This emissive centre is the reason for the bright blue luminescence of the carbon dots. The low energy absorption tail from 320–400 nm in CDs is due to the n – π* transition of the C = O bond. This is due to contributions from surface state transitions which are more prominent for CDs [49].
The emission spectra of both the quantum dots were recorded for varying excitation wavelengths. The CDs and S-CDs exhibit strong blue emission in the range of 440–470 nm upon UV excitations with maximum emission peaking at 448 nm wavelength. It can be observed that CDs (Fig. 7) and S-CDs (Fig. 8) showed a mixed nature of excitation dependence. From the normalised fluorescence spectra (inset of Fig. 7 and Fig. 8) the emission spectra of all excitations till 350 nm wavelength coincides for both QDs which suggests the excitation independent nature of fluorescence spectra of CDs. This behaviour changes to excitation dependent emission at higher excitation wavelengths with a red shift in emission wavelengths. Though the heterogeneous core-size distribution could be one of the factors responsible for red shift in PL as in many semiconductor nanodots, low synthesis temperature routes compared to other elemental quantum dots makes surface fluorescence emission a plausible explanation[50].
CDs and S-CDs were synthesised at 150oC resulting in effective carbonization and pyrolysis which in turn lead to the presence of surface states along with molecular states in CDs. Surface of CDs is often composed of many small organic fluorescence moieties. They are attached with many functional groups like –OH,-COOH, -CO or even thiol groups. These groups are randomly linked to the dots with no well defined structural order and are often responsible for weak electronic transitions. The photoluminescence properties observed are attributed to the result of the synergistic contribution of these optically active centres in the core, molecular and surface states of the dots [51]. Thus CDs with excitation independent emission in aqueous medium changes into wavelength specific PL emitting CD in a less protic solvent like ethylene glycol.
The mixed nature of wavelength dependence in our CDs can be intelligibly understood from the plot of emission peak wavelength for increasing excitation wavelength (Fig. 9). Both the CDs have almost constant PL peak wavelength till 350 nm excitations which are red shifted for higher excitations.
The short termin vitro cytotoxicity studies were done on rat spleen cells (RSC) by comparing the cell toxicity with the addition of varying volumes of CDs using trypan dye. Dead cells take up the blue colour of the dye while live cells don’t acquire the colour. So, live cells are counted to evaluate % Cell viability. A similar trypan blue exclusion method was opted to find anticancer activity of dots towards Dalton’s lymphoma ascites(DLA) cells. In this case, dead cells are counted separately to evaluate the % Cell death.
It can be observed that (Fig. 10) both CDs and S-CDs showed negligible cell killing effects on RSC and there is higher survival of these normal cells even at higher concentration. Though cell viability of normal cells remains almost constant even at all concentrations, it is evident that anticancer activity of both CDs increases with concentration. Compared to S-CDs, the undoped counterpart exhibits higher DLA tumour cell deaths at higher concentration. Absence of dopant chemicals and reduced surface functionalization in CDs also makes them more anti-cancer efficient compared to S-CDs. These dots are hence biocompatible with immense potential for application in the field of therapeutic treatment.
To further investigate the H2O2 sensing ability, emission spectra of S-CDs with various concentrations of MnO2 are examined (Fig. 11.a). It can be observed that emission intensity is quenched upon addition of MnO2. This can be well explained from the spectral overlap observed between UV-visible absorption spectrum of MnO2 and emission spectrum of S-CDs (Fig. 11.b). The broad absorption band ranging from 350 nm to 550 nm that overlaps with blue emissions of S-CDs makes MnO2 nanosheets the perfect candidate for H2O2 assay [52]. Ultrasound sonication of the MnO2 nanosheet powder with S-CDs alters the surface features of dots. Nanosheets will mask the CDs and turn OFF its ability to emit radiation. These nanosheets act as an efficient quenching agent for luminescence by covering the surface of nanoparticles [42].
From Fig. 12.a it can be inferred that fluorescence intensity of S-CDs are regained after addition of different concentrations of H2O2. The fluorescence regaining efficiency of MnO2 modified S-CDs is linearly correlated with H2O2 concentration from 0.06 mM to 1 mM (Fig. 12.b). Thus the sensor exhibits a linear response to hydrogen peroxide concentration with a detection limit of 0.49 mM.On the addition of hydrogen peroxide solutions of various concentrations, the MnO2 nanosheet modified dots will start deteriorating. Luminescence by CDs is gradually recovered on adding higher concentrations of H2O2 solution. At a particularly higher concentration of H2O2 the nanosheet will be completely decomposed and all CDs will show fluorescence. This recovery of luminescence can be attributed to reduction of MnO2 to Mn2+ mediated by H2O2. This reduction reaction can be represented as [52, 53, 54].
MnO 2 + H2O2 + 2H+ → Mn2+ + 2H2O + O2
Thus, by measuring the intensity of radiation emitted by MnO2 modified carbon dots, we can even quantify the amount of H2O2 added. The real images of fluorescence under 370 nm excitation wavelength, observed from MnO2 modified carbon dots after addition of different concentrations of H2O2 is shown in Fig. 13. The biofriendly S-CDs can be effectively utilised for designing a fluorescent probe for sensitive determination of H2O2.