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Frequency Shifts in SERS-Based Immunoassays: Mechanistic
Insights and Application in Protein Carbonylation Detection
Hao Ma,1 Songlin Liu,1 Naiqing Zheng,2 Yawen Liu,1 Xiao Xia
Han,1 Chengyan He,3 Hui Lu4* and Bing Zhao1*
1. State Key Laboratory of Supramolecular Structure and
Materials, Jilin University, Changchun 130012, P. R. China.
2. National Engineering Laboratory for AIDS Vaccine, School of
Life Science, Jilin University, Changchun 130012, P. R. China
3. China-Japan Union Hospital of Jilin University, Changchun
130033, P. R. China.
4. School of Biological Sciences, Faculty of Biology, Medicine
and Health, The University of Manchester, Manchester M13 9PT,
UK.
ABSTRACT: Frequency-shift based surface-enhanced Raman
spectroscopy (SERS) has exhibited great potential applications in
bioanalytical chemistry and biomedicine in recent years. The basis
and the crucial factors determining frequency shifts are, however,
still unclear. Herein, we have systematically investigated how
solvents, antigens and antibodies affect the band shifts in
SERS-based immunoassays. By applying the charge transfer theory
together with Stark effect and time-dependent density functional
theory (TDDFT) calculation, mechanistic insights into the frequency
shifts in immunoreactions is proposed and discussed in details.
Accordingly, the experimental condition is further optimized and is
successfully applied for the first time to detect carbonylated
proteins, promising diagnostic biomarkers for human diseases. This
study provides theoretical guidance for designing SERS frequency
shift-based immunoassays and paves a new avenue for the further
applications of the strategy in clinical diagnosis.
PAGE 2
Surface-enhanced Raman spectroscopy (SERS) has been proved to be
a powerful tool for chemical analysis, material science and
biomedicine in recent years.1-6 As a novel readout method with
excellent spectral reproducibility, SERS frequency shifts have been
applied into immunoassays since 2012.7 Recent years, the fast
growing research field allows widespread applications in the
detection of cancer biomarkers,8, 9 DNA,10 miRNA11 and protein
self-assembles.12 On the other hand, carbonylated proteins are
promising biomarkers for human diseases (Alzhermer’s disease and
diabetes et al.) 13, 14 and have been attracting the interest of
numerous laboratories regarding detection and identification. A
fast, highly sensitive and selective assay is of great importance
for detection of these biomarkers in clinical diagnosis.
The key factors that control the frequency shifts have been
explored, but the related mechanism is poorly understood. Olive et
al. reported the vibrational frequency shifts in the
antibody-reporter complexes.7 Their theory is based on harmonic
oscillator model and it is demonstrated that this phenomenon is
influenced by pH, hydrophobic interactions between proteins and
pressure. Moreover, the changes in the polarizability of
molecule-metal complexes were found to contribute to the frequency
shifts.10, 15 Our previously studies suggested that hydrogen
binding and enzymatic reaction may cause frequency shifts of the
Raman reporters, in which the charge-transfer effect was considered
as a dominant factor.16-18
We recently reported an approach for the detection of
alpha-fetoprotein (AFP) by SERS frequency shifts of
p-mercaptobenzoic acid (MBA).19 Here, the frequency shifts were for
the first time found to be a comprehensive reflection of different
vibrational modes of MBA, named as a ratio metric method. More
recently, we found the frequency shifts are solvent dependent as
demonstrated in the related study by Zhao et al.11 Moreover, the
SERS frequencies suffer obvious shifts when the Raman reporter and
antigen are fixed and a different antibody is introduced. Thus, all
these factors may influence the frequency shifts, and a better
understanding of the mechanism is of great importance for
experimental design and improving the accuracy of SERS-based
immunoassays.
In this study, we systematically investigated the factors
(solvents, antigens and antibodies) that control the band shifts of
a Raman reporter, MBA in SERS-based immunoassays. Together with the
charge transfer theory, Stark effect and time-dependent density
functional theory (TDDFT) calculation, the mechanism of the
frequency shifts in immunoreactions is explored. Accordingly, the
experimental condition is further optimized and is successfully
applied for the first time to detect carbonylated proteins.
The analysis is based on aforementioned solvatochromic trends of
Ag-MBA chip, a model system prepared via a self-assembled method.16
The experimental details are summarized in the supporting
information. As seen in Figure 1, the SERS spectra of MBA are
dominated by the peaks at 1075 cm-1, and 1584 cm-1, which can be
assigned to in-plane ring breathing mode coupled with C-S vibration
(1075 cm-1) and aromatic vibration (1584 cm-1) mode respectively.20
The band at 1075 cm-1 shifted to 1078.3 cm-1 in the most nonpolar
solvent (CCl4), and to 1072.2 cm-1 in the most polar solvent (H2O).
All the other bands were located between the above two wavenumbers
when the Ag-MBA chip was exposed to the solvents of C2H5OH, MeCN,
and DMSO. This tendency is attributed to the effective electric
field created by the polarization of the solvent. Interestingly,
the intensities of the bands at 998 and 1022 cm-1 ascribed to the
in-plane breathing modes (b2 modes) reveal a similar solvatochromic
effect, which increase with the polarization of the solvents. The
consistent results from frequency shifts and band intensities
suggested the mechanistic corrections between the two of them.
Moreover, as can be seen in Figure 1C, D, we also observed same
tendencies
Figure 1. Effect of solvents on the SERS spectra of the MBA. (A)
SERS spectra of the MBA-Ag films in different solvents: a. CCl4, b.
C2H5OH, c. MeCN, d. DMSO, e. H2O, f. No solvent (gas); (B)
Zoomed-in image of the dotted line in (A); (C) Zoomed-in image of
the intensity change of b2 mode (pink region) in (A); (D) SERS
spectra of antiAFP-MBA-Ag exposure to different solvents (MeCN,
DMSO, H2O); (E) SERS spectra of antiAFP conjugated with (HRP)-
MBA-Ag exposure to different solvents (MeCN, DMSO, H2O).
for MBA-antiAFP with kinds of polar solvent: MeCN, DMSO, H2O as
well, indicating the solvent effect is demonstrated in
Ag-MBA-antibody system.
We have shown that the charge transfer (CT) process would
selectively increase nontotally symmetric intensities (b1 mode),
which is a resonance Raman-like process.21, 22 As well known, MBA
can adsorb on silver surface through a Ag-S bond, and thus the
symmetry of complex is C2v if hydrogen interactions were ignored.
Noted that the CT dipole moment allowed excited states of the
complex are A1 and B2 respectively. According to Herzberg-Teller
selection rules proposed by Lombardi,23, 24 if a metal-to-molecule
CT occurs, a normal mode of b2 (A1*B2) would be allowed. Hence, in
the present system, the observed intensity changes of two bands (b2
modes) at 998 and 1022 cm-1 indicates that the metal-to-molecule CT
process occurs in the Ag-MBA complexes. To further investigate this
phenomenon, a TDDFT analysis was carried out to explore the solvent
effect on the CT process. The calculation details are provided in
the supporting information. Figure 2A shows the calculated
electronic transition states of the Ag3-MBA complex with the
hole-electron distributions, which is performed by using Multiwfn
software.25 Obviously, there is a molecule-to-metal CT process in
gas phase. When the solvents are introduced into the Ag3-MBA
system, the electric fields created by the solvent polarization
will disturb the electronic structure of the complex, inhibiting
the CT of molecule-to-metal. In another word, the introduction of
the solvents induced a metal-to-molecule CT process. Meanwhile, the
energy gap between the highest occupied molecular orbital (HOMO)
and lowest unoccupied molecular orbital (LUMO) is changed
dramatically as illustrated in Figure S1. Because of the larger
dipole moment of HOMO, the influence on the ground state of Ag3-MBA
can be neglected, which is stabilized by the solvents. On the other
hand, in the electron density point of view, a molecule-to-metal CT
process should induce a decrease of electron density (ρ) in MBA,
whereas an increase of electron density from metal-to-molecule CT
process. Hence, compared with the MBA without solvents, the
molecule with certain solvent contains higher ρ.
Moreover, in order to compare the CT contribution from different
assemblies more directly and accurately, we applied the concept
Figure 2. The solvent effect on different assembles. (A)
Hole-electron distribution for Ag3-MBA complex with consideration
of the solvent effect. The blue and red isosurfaces represent the
hole and electron distributions, respectively. The isosurface value
is taken as 0.002; (B) ρCT and (C) frequency shifts of the four
assemblies in different solvents of H2O, DMSO, MeCN, C2H5OH and
CCl4.
of the ‘degree of CT (ρCT)’ proposed by Lombardi et al.23 Based
on our previous work, (k) of a k-band can be expressed as following
equation:
(1)
where Ik(CT) is the intensity of a band which is ascribed to
SERS intensity by CT resonance. Also, it is crucial to choose a
reference band without CT contribution to SERS intensity, the line
of Ik(CT), which originated from SPR. Mostly, Ik(SPR) is very small
or zero when the CT vibrations are nontotally symmtric. In this
case, we selected the ring breathing A1 mode at 1075 cm-1 as the
peak of I0(SPR), which is enhanced in the whole spectrum. As for
Ik(CT), we selected the in-plane vibration band at 992 cm-1 (B2
mode) for investigating CT of metal-to-molecule. Thus, Eq. 1 can be
expressed as follows:
(2)
Clearly, compared with the frequency shifts of the four
assemblies shown in Figure 2C, a similar trend is observed.
Therefore, it is deduced that there is an intrinsic correction
between these two SERS transformations. The perturbation of
vibrational spectra by electromagnetic fields has been known for
many years, which is predicted to be promising to explain various
results observed in SERS.26 The effect of an electric field on the
frequency splitting of a molecule vibration (Stark effect) has been
studied in different systems.27-30 As it has been well established
by Boxer and coworkers,26 the expansions of field-induced Stark
shift can be expressed as the following equation:
(3)
Here represents the difference in the dipole moment, and
represents the polarizability difference. F is the electric field.
Here, we use this theory to interpret the SERS transformation
together with the general expression for the polarizability
tensor.23, 28, 31, 32 In the present system Eq. 3 can be expressed
as:
+
(4)
Briefly, two CT processes are involved in the present system: B
tensor (molecule-to-metal CT process) and C tensor
(metal-to-molecule CT process). Where is the electronic transition
from HOMO to LUMO in MBA. is the electronic transition from HOMO to
the Fermi level of silver. represents the electronic transition
from Fermi level to LUMO. As discussed above, the molecule-to-metal
CT is largely inhibited. The polarizability tensor is mainly
affected by the metal-to-molecule CT process. Assuming the electric
field is the same, this CT contribution is directly proportional to
the frequency shift. Thus, it is reasonable for the observed
similar trend of CT and the frequency shift. Furthermore, we
observed a similar tendency in a Au-MBA system as discussed in
Figure S2, which suggested that the metals affect more remarkably
the ρCT than the electric field.
However, it is obvious that the solvent effect is not the only
factor that influences the frequency shifts of Raman probe. The
diversity of the antibodies and antigens will also affect to some
extent the SERS band shifts. As shown in Figure 2, the antibodies
(antiAFP and conjugated antiAFP) display different ρCT and the
frequency shifts. Moreover, the similar results were observed when
introducing different antigens (data not shown). To further explore
these controlling factors, we designed a SERS-based imunoassay for
carbonylated proteins. In the present study, there are two antigens
(DNPH and DNP-BSA) and two antibodies (IgG and IgE). As illustrated
in Figure 3A and Figure S3, when introducing DNPH into the proposed
Ag-MBA-antibody chip, the frequency shifts of MBA with IgG and IgE
are almost the same, indicating that such small molecule cannot
induce deformation or change of the polarizability of MBA. In
contrast, when the DNP-BSA bound into the Ag-MBA-IgG chip, an
upshifted (2 cm-1) band was observed as referred to the case of
DNPH. Therefore, we deduced that the BSA with high molecule weight
may induce a deformation of MBA (Figure 3B). A similar frequency
shift was observed for the characteristic peak located at 1111
cm-1.
Figure 3. Effect of antigen and antibody on the SERS spectra of
the MBA. (A) SERS spectra for proposed chips with IgG and different
antigens; (B) schematic diagram of the MBA deformation with
different antigens; (C) the ρCT versus different antibodies; (D)
DFT calculation of Ag3-MBA with consideration of the isotype
effect.
To verify our hypothesis, the density functional theory was
performed to identify the expected vibrations. All the calculations
were under M062X/6-311+G*/LanL2DZ level. With the consideration of
the isotope effect, we tried to figure out the effect of antigen
weight to the vibrations. As shown in Figure 3D, we found that the
attached antigen indeed can induce frequency shift up to 2 cm-1,
which is consistent with the observed experimental result in Figure
3A. In addition, we found that different antibodies induced
different frequency shifts when introducing DNP-BSA as well as the
ρCT (Figure 3C). As for the IgG, the upshifts were attributed to
the attractive hydrophobic interactions between IgG molecules,
which thereby causing the relaxing of the deformed MBA and thus in
turn change the polarizability and the ρCT. The reason why the SERS
frequency in the IgE-DNP-BSA chip appeared a downshift is probably
the lack of intermolecular interactions, which further induced
deformation of the MBA. As a result, we find that the theory of
Olive definitely makes sense. However, to a large extent, it
depends on the type of antibodies and antigens.
Carbonylation of proteins is an irreversible oxidative damage,
which is associated with a large number of diseases. Currently,
most of the assays for detecting protein carbonylation involve
deriving carbonyl groups with 2,4-dinitrophenylhydrazine(DNPH),
which can subsequently be detected by the enzyme-linked
immunosorbent assay (ELISA) or Western blotting. However, these
methods usually lead to false-positive or false-negative results,
because it is challenging to remove unreacted DNPH fully and DNPH
can also act as an antigen. Moreover, the current and traditional
assays for carbonylated protein detection always require large
amount of protein samples with many washing steps or suffer bad
quantitative ability.
As illustrated in Figure 4A-C, given the fact that the SERS
method is simple and fast without the interference from DNP, it is
expected to establish a novel analytical method for carbonylated
proteins based on SERS frequency shifts. To this end, we optimized
the experimental condition and introduced IgG as the capture
antibody. As shown in Figure 4E, it was feasible to detect
carbonylated proteins at the concentrations ranging from 0.18 to 9
nmol/mL. We found the detection curve became saturated at the
concentration of 9 nmol/mL, a threshold value. According to the
results, the proposed SERS-based method is more sensitive than
other related assays with wider dynamic range (Table S2), thus it
may be applied to analyze clinic samples.
Figure 4. Assays for protein carbonylation: (A) a colormetric
approach, (B) Western blotting, and (C) the proposed SERS
frequency-shift method. (D) DNP-BSA-dependent SERS spectra of the
Ag-MBA-IgG chip: a. blank; b, 0.18 nmol/mL; c, 0.9 nmol/mL, d, 2.25
nmol/mL, e, 9 nmol/mL, f, 18 nmol/mL DNP-BSA; (E) frequency shifts
of the peak at 1075 cm-1 versus the carbonyl content. Each data
point represents an average of five measurements and the error bars
indicate standard derivation.
In summary, we performed a systematic analysis of transformation
of the Raman probe MBA in SERS-based immunoassays. By combination
of the CT and Stark theories, we inferred that both of the
metal-to-molecule and molecule-to-metal CT processes can induce
frequency shifts by changing the polarizability of MBA. Moreover,
with the aid of DFT theory, we demonstrated that the factors
controlling frequency shifts are not only related to the solvent
effect and CT but also involved in the isotype effect,
intermolecular interaction and types of antigens and antibodies.
Our study has clarified some fundamental questions of the
immunoreaction induced SERS transformation, and paves a new avenue
for the further applications of frequency shift-based immunoassays
in clinical diagnosis.
ASSOCIATED CONTENT
Supporting Information
Detailed information of preparation of self-assemble chips;
preparation and determination of the carbonyl proteins;
computational details; energy gaps in different solvant; comparison
of relevant assays; SERS spectra of the Au-MBA with different
solvents and the Ag-MBA-IgE with different antigens; UV-Vis spectra
of the DNP-BSA.
The Supporting Information is available free of charge on the
ACS Publications website.
AUTHOR INFORMATION
Corresponding Author
* [email protected] (H.L.); [email protected] (B.Z.)
Author Contributions
The manuscript was written through contributions of all authors.
/ All authors have given approval to the final version of the
manuscript.
NotesThe authors declare no competing financial interest.
ACKNOWLEDGMENT
This work was supported by the National Natural Science
Foundation (Grant Nos. 81572082, 21773080, 21711540292 and
21773079) of P. R. China; Project for Science & Technology
Development of Jilin Province (20180101201JC, 20190201215JC and
20190701003GH). It was also supported by the Royal Society
(IE150835 to HL).
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