SUPPLEMENTARY MATERIAL Safety Concerns towards the Biomedical Application of PbS Nanoparticles: An approach through Protein-PbS Interaction and Corona Formation Amit Kumar Bhunia1, Pijus Kanti Samanta2, Satyajit Saha1, Tapanendu Kamilya3 * 1. Department of Physics & Technophysics, Vidyasagar University, Paschim Medinipur, 721102, India 2. Department of Physics, Ghatal R.S. Mahavidyalaya, Paschim Medinipur-721212, India 3. Department of Physics, Narajole Raj College, Paschim Medinipur-721211, India 1. Calculation of Fractal Dimension We have analyzed the structure of ‘PbS NPs-BSA’ corona by fractalyse software to calculate the fractal dimension. This software uses the Radial mass distribution method to calculate the fractal dimension. The Hausdorff dimension, D, is related as S∝RD, where, S is the area covered by each structure, R is the average distance from the center of mass of a structure to its perimeter. The slope of linear fit of ln(S) vs ln(R) gives the value of D and is calculated to be ~ 1.7. 2. Fluorescence Quenching Measurement SUPPLEMENTARY MATERIAL The PbS NPs-BSA binding kinetics and equilibrium as well as conformational change of BSA is also analyzed by fluorescence quenching measurements. πΉ β‘ πΉ0 = πΎππ [π] + 1 (2) F0 and F represent the steady-state fluorescence intensities of flourephore in the absence and presence of PbS NPs, respectively. KSV corresponds to the Stern-Volmer quenching constant and [Q] represents the concentration of PbS NPs. The values of KSV for 20, 30 and 40oC are summarised in Table-1. The increment of KSV with increasing temperature signifies that the quenching mechanism of BSA is a dynamic quenching process in presence of PbS NPs and the strength of interaction increases with temperature. The F0/F versus [Q] plots at different temperature are shown in Fig. 8 (a). The binding constant K along with the number of binding sites (n) between BSA and PbS NPs at different temperatures are calculated using the following equation: πΉ0 −πΉ β‘logβ‘[ πΉ0 −πΉ The plot of β‘πππβ‘[ πΉ πΉ ] = log πΎ + πβ‘πππ [π] (3) ] versus πππβ‘[π] gives a straight line and the slope determines the value of n. The intercept of the straight line on Y-axis determines the value ofβ‘πππ πΎβ‘. The values of β‘πππ πΎβ‘ at 20, 30 and 40oC are summarized in Table I, for comparison. In favour of positive cooperative reaction, n›1, reveals that once one protein molecule is bound to the NPs, its affinity for the NPs gradually increases in a super-linear fashion. However, in case of negative cooperative reaction, n‹1, the binding strength of the protein with the NPs becomes weaker as further proteins adsorb. As well as, for a non-cooperative reaction, n=1. SUPPLEMENTARY MATERIAL 3. Binding with Tryptophan The interaction PbS NPs with TRY is studied to investigate the probable binding sites of BSA with PbS NPs. The value of n in case of interaction of PbS NPs with TRY at 40oC is almost matched with the PbS NPs-BSA complex. 4. van’t Hoff equation and thermodynamic parameter calculation The thermodynamic parameters βH (change in enthalpy) as well as βS (change in entropy) for BSA and PbS NPs interaction are studied to account for the main forces contributing to the stability of BSA is determined by using the van’t Hoff equation βπ» ln πΎ = − π π + βπ π (4) K is analogous to the binding constant at corresponding temperature (T) in oC; R is the universal gas constant. The free energy change is analyzed by following relationship βG =β‘ βπ» β‘ −πβπ=−π πππ πΎ (5) In general, mainly four types of interactions occur between bare NPs and biological macromolecules: hydrogen bond, van der Waals interaction, electrostatic and hydrophobic interaction etc. According to the value of βH and βS, the model of interaction can be predicted as: i) βH > 0 and βS > 0; represent hydrophobic interaction. ii) βH < 0 and βS < 0; represent van der Waals and hydrogen bonding. iii) βH < 0 and βS > 0; represent electrostatic bonding. SUPPLEMENTARY MATERIAL 5. CD Spectroscopy CD spectroscopy is used to analyze the change of secondary structure of BSA in interaction with PbS. PbS NPs binding associated conformational change of BSA is analyzed by fitting the CD spectra with K2D3 software. The positive peak at 190 nm and two negative peaks at 208 and 222 nm state that BSA is α-helix rich protein. 6. FTIR Spectroscopy PbS NPs binding associated unfolding of BSA is analyzed by fitting the amide I band (1600-1700 cm-1) of FTIR spectrum. The unfolding, intra and intermolecular associations of protein were studied by monitoring the peak positions and width of amide bands within a fixed range by FTIR analysis. The FTIR absorption spectra of amide-I band (1600-1700 cm-1) is due to C=O stretching modes of peptide linkages of BSA. The vibrational energies of the carboxyl group depend in reality on the different conformations of the protein, such as ο‘-helix, ο’-sheet, ο’turns and intra and intermolecular aggregates. The determination and the assignment of the spectral components of the amide-I band can provide the information on the protein secondary structure. A Gaussian multiple-peak-fitting procedure has been employed to study the amide I band of FTIR spectra by using Microcal Origin 7.5 software after baseline correction. The quality of the fitting was evaluated based on the χ2 values (on the order of 10-6) and the square of the correlation coefficient (R2) values 0.999. The multiple peaks resulted from the deconvolution will provide us the conformations of BSA in different condition and to identify its component and, in particular, to determine the corresponding peak frequencies. The percentage area of the deconvoluted peaks gives the relative area of the components. It is worth noting that, in all the spectra considered in the present work, the maximum number N of the components which can be SUPPLEMENTARY MATERIAL safely identified in the deconvoluted amide I band does not exceed N=5 to have a meaningful fitting. SUPPLEMENTARY MATERIAL Figure-S1: (a) Absorption spectrum of PbS NPs, (b) PL spectrum of PbS NPs SUPPLEMENTARY MATERIAL Figure-S2: Absorption spectra: (a) pure BSA with CBSA=0.1 mg/mL, (b)- (e) represent the absorption of BSA-PbS NPs complex with CBSA=0.1 mg/mL and CPbS= 0.01 (b), 0.03 (c), 0.05 and (d) 0.09 mg/mL (e), respectively. SUPPLEMENTARY MATERIAL Figure-S3: (a): Shift of absorption wavelength (βλ) of BSA with CPbS. (b) Change of absorption intensity (βA) of BSA with CPbS. SUPPLEMENTARY MATERIAL Figure-S4: Schematic representation of interaction and corona formation of PbS NPs and BSA SUPPLEMENTARY MATERIAL SUPPLEMENTARY MATERIAL Figure-S5: Fig. S5(i): (a) represents the fluorescence spectrum of pure BSA with CBSA=0.1 mg/mL. Fig. S5(i) (b) – (e) represent the fluorescence spectra of BSA in BSA-PbS NPs complex with CBSA=0.1 mg/mL and CPbS= 0.01, 0.03, 0.05, 0. 1 mg/mL. The spectra are taken at 20oC. Fig. S5(ii): (a) represents the fluorescence spectrum of pure BSA with CBSA=0.01 mg/mL. Fig. S5(ii): (b) – (e) represent the fluorescence spectra of BSA in BSA-PbS NPs complex with CBSA=0.1 mg/mL and CPbS= 0.01, 0.03, 0.05, 0. 1 mg/mL. The spectra are taken at 30oC. Fig. S5(iii): (a) represents the fluorescence spectrum of pure BSA with CBSA=0.01 mg/mL. Fig. S5(iii): (b) –(e) represent the fluorescence spectra of BSA in BSA-PbS NPs complex with CBSA=0.1 mg/mL and CPbS= 0.01, 0.03, 0.05, 0. 1 mg/mL. The spectra are taken at 40oC. SUPPLEMENTARY MATERIAL Figure-S6: Fig. S6(a) represents the F0/F versus Q plot for PbS NPs-BSA complex. Fig. S6(b) represents the log K versus 1/T plot for PbS NPs-BSA complex. SUPPLEMENTARY MATERIAL Figure-S7: Fig. S7(a) (a) represents the fluorescence spectrum of pure TRY with CTRY=0.1 mg/mL. Fig. S7(a) (b) – (e) represent the fluorescence spectra of TRY in TRY-PbS NPs complex with CTRY=0.1 mg/mL and CPbS= 0.01, 0.03, 0.05, 0. 1 mg/mL. The spectra are taken at 40oC. Fig. S7(b) represents F0/F versus Q plot for TRY-PbS NPs complex. SUPPLEMENTARY MATERIAL Figure-S8: CD Spectra; (a) pure BSA (b) BSA-ZnO complex SUPPLEMENTARY MATERIAL Figure-S9: FTIR Spectra: (a) Amide bands of BSA-PbS NPs complex. (b) Amide-I band of BSA-PbS NPs complex. Green lines represent the curves fitted by multiple peaks fitting by Microcal Origin. SUPPLEMENTARY MATERIAL TABLE I BSA BSA BSA TRY T (K) 293 303 313 313 KSV mM-1 1.09 1.58 1.90 1.74 Log K ( µM)-1 2.348 2.564 3.708 2.950 ΔG° (kJ/mol) -5.717 -6.456 -9.646 -7.355 ΔH° (kJ/mol) ΔS° (J/mol) N -51.39 15.574 14.823 13.311 0.8086 0.9006 1.1282 1.0718 Table I: Binding parameters and thermodynamic parameters of BSA–PbS NPs TABLEII Conformers A1 ο’ ο‘ T A2 FTIR Area (%) Position (cm-1) A B A B 17.34 0.87 1605.2 1613.2 12.50 04.44 1626.3 1626.8 62.82 60.01 1650.7 1649.6 04.68 32.58 1674.2 1685.1 02.66 02.10 1688.1 1704.9 CD ο’ /ο‘ CD FTIR A B A B A B 0.13 8.65 8.34 0.12 68.13 68.04 0.198 0.074 - Table II: Fitting parameters of amide-I band for BSA A: pure BSA, B: BSA-PbS NPs complex. Area (%) = 100 represents the total area under curve.