3.1. Features of SERS spectrum and Normal Raman of SARS-CoV-2
The SERS technique was employed for the characterization and detection of SARS CoV-2. The average of 12 SERS spectra of SARS-CoV-2-AgNP substrate samples acquired during the period from 08–14 to 09-23-2020 are shown in Fig. 2 in perspective. The SERS spectra of SARS-CoV-2 exibits a number of marker modes spreading well all over the region between 1000 and 1700 cm− 1. Except the obvious minor differences in intensities, orientations and peak sharpness in relative band width and intensity, the SERS spectra obtained over the period of testing were identical in the spectral region 500–1700 cm− 1.The SERS spectra have a high sensitivity, a signal amplification of up to 7.0x105, and are reproducible across the period of time testing. Large enhancement factors of the electromagnetic field are only accomplished in very tiny areas of the surface of nanostructured metals, due to the increased degree of AgNP aggregation, which is critical for forming efficient "hot spots." [14, 19]. Because of the high density of the hot spots, only a tiny percentage of SARS-CoV-2 biomolecules adsorbed on junctions of two or more AgNPs resulted in a greatly increased and reproducible SERS signal [23]. SARS-CoV-2 with and without spike AgNPs was firstly tested as a proof-of-concept demonstration of the protocol developed in this study. Figure 3Aa show the representative Norma Raman (NR) spectra tests in the range of 500 to 1700 cm− 1 and and Fig. 3Ba in the spectral region of 300–3500 cm− 1. The recorded NR spectra were highly reproducible, and reveal no signal besides a weak band with maximum c.a. 1400 cm− 1 comparing to the incident beam. The Raman intensity in the NR spectra without AgNPs varies between 2 and 5 x 102. Correspondingly, the NR spectrum of clean CaF2 glass slide used as platform to spot the SARS-CoV-2 sample (Fig. 3Ab and Fig. 3Bb) exhibits no signal, possibly as a result of the SARS-CoV-2 viral suspension sample's transparency, CaF2 was utilized as the window material in order to eliminate multiple internal reflections. In contrast, the SERS spectra of SARSCoV-2 measurements in the spectral region between 1000 and 1700 cm− 1 indicate pronounced band enhancement, especially the SERS signals centered around 1000 cm− 1 (Figs. 3Ac and 3Bc), which shows highly reproducible bands with great uniformity and extraordinary sensitivity. The orientation on the surface of aggregated AgNPs could also explain the adsorption of several amino acids with cyclic R side chains, such as aromatic ring in phenylamine at 1007 cm− 1. As can be shown, our SERS-active substrate achieves a substrate with a very high enhancement magnitude, ranging from 0.2 to 1.6 x 106 (Raman Intensity). However, some bands in the SERS spectra of SARSCoV-2 show fluctuation in relative band shapes and intensities in other spectral regions between 400 and 1000 cm− 1 and 1500 to 3500 cm− 1, respectively. This is attributable to the fact that the SARS-CoV-2 biomolecules' adsorption behavior on AgNPs aggregates. The enhancement of the electromagnetic field in the slits between AgNPs aggregates has been reported to be much higher [19, 23]. Thus, before SERS measurements AgNPs are usually aggregated/agglomerated to generate such slits. Low-intensity shape bands were found, as well as a lack of high signal-to-noise ratios, implying the presence of several overlapping peaks. This could be because SARS-CoV-2 includes numerous biomolecules that all co-adsorb on the surface of AgNPs, causing peak broadening. Furthermore, the orientation of the adsorbate on the hot spots generated between the intraparticle gaps of AgNPs is likely modulated by the relative low intensity of the molecular components. In section 3.4, the SERS spectra, band intensities, and marker modes recorded in the 500–1700 and 300–3500 cm-1 regions, respectively, are examined in better detail.
3.2. SERS reproducibility of SARS-CoV-2
A total of 9 SARS-CoV-2 SERS spectra were acquired from 3 random places on the same active substrate for varied concentrations to demonstrate the reproducibility of SARS-CoV-2 SERS spectra. The experiment was conducted by dilutions of inactivated SARS-CoV-2 (stock solution) from 105 vp/mL to 104, 103 and 102 (vp/mL) using ultrapure water, which served reference (Fig. 4A-D). Except for small intensity fluctuations in some bands, the SERS spectra varied with SARS-CoV-2 concentration, and the majority of the bands showed highly enhanced and reproducible SERS signals, implying the efficacy of AgNPs aggregate substrates. The excellent reproducibility could be ascribed to the virus cells’high density distribution, which indicates that most of the macromolecules of SARS-CoV-2 come into direct contact with the AgNPs’ hot spots, which possible benefit to obtain a uniform SERS signal. We observed significant SERS signal enhancement with the concentration of SARS-CoV-2. For instance, high signal enhancement ca. 6.5 x 105 times over NR scattering is achieved for 105 vp/mL of SARS-CoV-2 (Fig. 4A). In the SERS spectra, we identified the most significant bands as well as their reproducibilities reported as relative standard deviations (RSDs) at: 1007 cm-1 (4%); 1144 cm-1 (15%); and 1270 cm-1 (22%). The signal enhancement declined to ca. 3.5 x105, 1 x 105 and 4.3 x104 for SARS-CoV-2 concentrations of 104, 103 and 102 vp/mL, respectively, for each intensity, including RSDs at: 1007 cm-1, 1144 cm-1, and 1270 cm-1 detected for each intensity 1007 cm-1, 1144 cm-1, and 1270 cm-1 (Fig. 4B-D).
For SERS quantitative research, less than 20% variance in SERS intensity between different locations of the active substrate is acceptable [25], in agreement with our findings. In addition, the SERS spectra for 105 vp/mL SARS-CoV-2 concentration were recorded by mapping a small area (20 µm x 20 µm) on the slide in the range of 500 to 1700 cm-1 (Supporting material Fig. 4S). The high reproducibility in this investigation can be ascribed to a homogeneous mixing of SARS-CoV-2 viral suspension and AgNPs of the same size (60 nm) and shape (spherical).
3.3 Limit of detection (LOD) of SARS-CoV-2 based on SERS method
The LOD was explored by comparing SERS signal enhancement with SARS-CoV-2 concentration; for instance, for 105 vp/mL high signal enhancement of ca. 6.5 x 105 times over NR scattering was achieved (Fig. 5A). The signal enhancement declined to ca. 3.5 x105, 1 x 105 and 4.3 x104 7 for SARS-CoV-2 concentrations of 104, 103 and 102 vp/mL, respectively (Fig. 5B). The LOD was defined in the literature as the concentration of SARS-CoV-2 for which the strongest signal of SERS enhancement was equal to 3 times the background SERS signal intensity, with the background SERS signal intensity referring to the SERS signal from a sample with virus cells concentration of 0 [26]. In order to determine the LOD, the SERS intensities of three peaks at 1007, 1144, and 1270 cm− 1 were notably strong and the intensity of the peaks increased when the viral cell concentration of SARS-CoV-2 increased. The peak at 1007 cm− 1, on the other hand, was one of the strongest for SARS-CoV-2, and its intensity increased as the concentration of SARS-CoV-2 increased. As a result, the peak at 1007 cm− 1 was chosen as a hint vibration to estimate SARS-CoV-2 concentration and to evaluate the LOD for SARS-CoV-2 samples. The peak intensity at 1007 cm− 1 (I1007) was plotted as a function SARS-CoV-2 concentration (Fig. 5C). The lowest concentration of SARS-CoV-2 found by this approach was lower than103 vp/mL, based on the average and 3 times of the SERS signal marked as control. The peak intensity (I1007) against the concentration of SARS- CoV-2 (vp/mL) with an R2 value of 0.96 confirming that the lowest concentration of SARS-CoV-2 detected with this assay may be around 103 vp/mL.
3.4. SERS characterization of SARS-CoV-2
The current investigation, which took place from August to October 2020. The SERS technique was used to explore using AgNPs, SARS-CoV-2 characterisation and detection of key biomolecules such as structural proteins derived from SARS-CoV-2 composition. The average typical SERS spectra of SARS-CoV-2 mixed with aggregated AgNPs are shown in the region between 500 and 1700 cm-1 (Fig. 6A) and 300 and 3500 cm-1 (Fig. 6B), respectively. Table 1 shows the complete list of peaks wavenumber for SARS-CoV-2 as well as suitable tentative biomolecules assignments. The primary vibrational sharp and intense signals are visible in the SERS spectrum of SARS-CoV-2 at 1007, 1221, 1453 and 1270 cm-1; in the mid intense at 1095, 1144, 1580 cm-1; broad low intense at 1500 and 733 cm-1; low intense at 1405, 954, 1381, 1304 cm-1; and very low intense signals in the region between 500 and 887 cm-1. The pronounced intense band centred at 1007 cm-1, which is assigned to Phe marker, and the C-C skeletal stretching vibration of the phenylalanine ring combined with C-H in plane. Other vibrational modes of Phe located at 1001 cm-1 attributed to the symmetric ring breathing mode; 1018 and 1022 cm-1 assigned to the in-plane C-H bending, at 1032 cm-1 attributed to in-phase motion υ(C-C) and δ(C-C-H) [12]. The next intense band at 1221 cm-1 is ascribed to PO2-, NH2 markers of amide III, which result from the coupling of υ (C-N) and δ(N-H), although it has a week band in the region 300–3500 cm-1, it is discernible (Fig. 6B) and has a low signal-to-noise ratio suggesting the presence of overlapping peaks. This is because SARS-CoV-2 cells contain numerous macromolecules that likely co-adsorb on AgNPs surfaces, resulting in peak reduction and distortion. Strong bands at 1070 cm-1 attributed to (γ-C-N) also indentified in the SERS spectra of other viruses [17, 18]. Vibrational modes exist in the amide I, II and III, which are conformational sensitive. Primary C = O stretching, in-plane modes of N-H bending, and υ(C-C) vibrational modes are included in the amide groups. At 1270 cm-1 ascribed to NH2 marker, whis is very strong amide III mode for α-sheet disorder conformation. Band at 1268, 1286, and 1296 cm-1 (amide III vibration of protein α-helix structure) were identified in the SERS spectra of other viruses [17, 18]. CH(CH2) bending modes markers in proteins and nucleic acids are responsible for the next strong peak at 1453 cm-1. Amino acids and purines molecules are probably to promote adsorption on hot spot located on AgNPs’ surface, allowing for an enhancement in the vibration of these molecules at 1095 cm-1, a medium-intense band can be assignable to the complex symmetrical mode of PO2- marker, which is composed of nucleic acids (Fig. 6A). However, in the SERS spectrum of Fig.6B, this band appears to have shifted slightly to 1075 cm-1, a strong band at 1070 cm-1 attributed to (γ-C-N) also indentified in the SERS spectra of other viruses [17,18]. This spectral shift can be attributed to the molecular layers coating the AgNPs, and the relative intensity of the molecular components is modulated by the orientation of the adsorbate onto the AgNPs surfaces. The next medium-intense bands appear at 1144 cm-1 which correspond to C-N stretching proteins marker, and at 1500 cm-1, which is due to the presence of amide II υ(C=C) in benzenoid ring, indicating that SARS-CoV-2 molecules are adsorbed to AgNPs carboxyl groups and other molecules related to amino groups. The ring breathing modes in purine DNA/RNA are assigned to the low-broad intense at 733 (Fig. 6A) and 743 (Fig. 6B), probably from building blocks created during amino acid catabolism. A virion (also called a virus, or particle) is made up of DNA or RNA molecules surrounded by a protective coat of proteins [32]. Tyr, Trp, Adenine, Guanine (DNA/RNA); C=C bending mode of Phenylalanine markers, can also be ascribed to the next low-broad intensity at 1580 cm-1 [33, 34]. Low intensity band at 1405 cm-1 in the 1300- 1650 cm-1 region attributable to CH2 scissoring, shifted to 1430 cm-1, attributed to adenine or guanine, the band at 1606 cm-1 from the phenyl ring bond-stretching vibrations, assigned to in-phase motion of υ(Cδ-Cε). Low-intensity bands at 1304, 1352, and 1381 cm-1 (Fig. 6A) were ascribed to Amide III (protein) cytosine, purines (T,A,G), and tryptophan.. The next low intensity bands are seen at 954 and 915 cm-1 which correspond to the proteins υ(C-O) and C-N and υ (C-COO-). Interestingly, too weak bands (low intensities) at 887, 834, 857, and 781 cm-1 are due to phosphodiester, (O-P-O) stretching of thymine and RNA moieties in the deoxyribose molecule. Other low weak intensity bands at 577, 612, 677 and 680 cm-1 were attributed C-C twisting mode of phenylalanine and adenine, purines. Furthermore, we discovered a peak at 517 cm-1, which is assigned to the protein’s S-S stretching modes of cysteine residues in proteins, the band at 612 cm-1 appears in the Raman spectra of proteins as Phe ring breathing vibration corresponding to a homothetic motion of the ring breathing atoms C-C twist. Finally, the remaining two bands the first at 457 cm-1 assigned to amino acids with a cyclic R side, such as Phe or Trp, suggesting that the carboxyl groups-r(COO-) are chemically adsorbed to AgNPs [19, 17]. The appearance of the band at 2100 cm-1 in our samples is most likely due to dehydration of the peptide bond, which results in results in υ(C≡C) or υ(C≡N) due to degradation (peptide and protein residues) caused by laser power. The last band at 2935 cm-1 can be assigned to asymmetric and symmetric CH3 stretching vibrations of the methyl end groups of membrane lipids as well as the methyl side groups in cellular proteins. These molecules are most likely derived from E and S SARS-CoV-2 proteins associated with glycoproteins, which includes a bilayer lipid envelope outside the protein coat. (Fig. 6B, and Table 1). Using highly SERS active aggregated AgNPs substrate to identify SARS-CoV-samples, adsorption of biomolecules including proteins, peptides of SARS-CoV-2 onto the surface of AgNPs depends on the chemical origin of the biomolecules and SERS enhanced mechanism, which entails changes in frequency and intensity that are primarily related to the distance between AgNPs colloids and groups of SARS-CoV-2 biomolecules.
TABLE 1 Tentative SERS bands assignments of SARS-CoV-2 main Raman shift vibrational modes
Range (cm-1)
|
Tentative AssignmentsϮ
|
500-1700 300-3500
|
|
=
|
457
|
r (COO-)ϯ; Phe, Tyr
|
517
|
=
|
υ(S-S) disulfide (amino acid cysteine) ϯ
|
557
|
557
|
C-C twist mode of Phe (proteins)
|
612
|
612
|
C-C twist mode of Phe; δ(COO-)
|
677
|
680
|
Tyr
|
733
|
743
|
A,U, T, C, ring breathing modes in the DNA/RNA
|
781
|
=
|
υ(O-P-O) RNA
|
834
|
857
|
υs(O-P-O) str, T
|
887
|
887
|
DNA/RNA, phosphodiester, deoxyribose
|
915
|
=
|
υ(C-COO-)
|
954
|
=
|
υ(C-O) and C-N of proteins
|
1007
|
1007
|
δ(C-C) aromatic ring in Phe
|
1095
|
1095
|
υ(C-N), υ(PO2-) nucleic acid,
|
1144
|
1144
|
C-N streching in proteins, t(NH2)
|
1221
|
1221
|
Amide III, υ as (PO2-), δ(NH2)
|
1270
|
1270
|
Amide III , δ(NH2)
|
1304
|
1305
|
Amide I, C-H def
|
1352
|
1352
|
A,G C-H def
|
|
|
υs(COO-)
|
1381
|
1381
|
ρ(C-H)
|
1405
|
1405
|
CH2 sciss, G,A
|
1453
|
1453
|
δ(CHCH2), proteins and lipids
|
1500
|
1500
|
δ(C=C) in benzenoid ring, amide II
|
1580
|
1580
|
A,G (DNA/RNA), C=C bending mode of Phe
|
|
|
υs(COO-), Tyr, Trp
|
1606
|
1606
|
Phe ring bond vibration, in-phase motion of υ(Cδ-Cε)
|
=
|
2100
|
υ(C≡C), υ(C≡N), peptides residues
|
=
|
2935
|
υ(C-H), υ(C-H3) membrane of lipids
|
Ϯ All the assignments are from references [18, 27, 28, 29,30, 31]
ϯ υ, stretching; δ, bending; ρ, rocking; τ, torsion; wagg, wagging; twist, twisting,; sciss, scissoring; def, deformation; as, asymmetric; s, symmetric; C, cytosine; T, thymine; Aadenine; G, guanine; U, uracil; Phe, phenylalanine; Tyr, tyrosine, Trp, tryptophan.