Abstract
Nucleic acids (deoxyribonucleic acid – DNA and ribonucleic acid – RNA) are essential components of all living organisms, with DNA encoding genetic information and RNA facilitating vital biological processes. The detection of nucleic acids having a specific sequence is crucial for identifying organisms and diagnosing genetic diseases. Because surface-enhanced Raman spectroscopy (SERS) is considered as one of the most promising analytical methods that offers important benefits such as short analysis time and exceptional sensitivity compared to other techniques, many groups are trying to apply SERS for nucleic acid detection. This review discusses how SERS spectroscopy can be used for DNA/RNA detection. Beginning with an overview of SERS theory, we delve into various SERS DNA/RNA sensors, including those based on a direct analysis of the SERS spectra of nucleic acids, and many types of sensors based on a selective hybridisation of probe and target nucleic acids. We describe how various types of sensors with increased sensitivity and reliability have evolved (from the first SERS DNA/RNA sensors described in the literature to recently developed ones). Challenges and future directions in SERS sensor development for nucleic acid detection and determination are also discussed. This comprehensive review aims to help researchers understand the field’s nuances, and to foster advancements in the use of SERS spectroscopy in the medical sector.
1 Introduction
Nucleic acids play a very important role in the functioning of all known organisms. Deoxyribonucleic acid (DNA) carries genetic instructions for the development, functioning, growth and reproduction of all organisms, whereas ribonucleic acid (RNA) is essential for most biological functions; it either performs the function itself or forms a template for the production of proteins. The detection of a nucleic acid having a given sequence may make it possible to: (i) determine the species of the organism from which it comes (to identify the organism, including microorganisms and viruses), and (ii) detect a particular gene mutation in an organism (to determine the source of a genetic disease or increased susceptibility of a given individual to a certain type of disease, including oncological diseases). Due to the great practical importance of detecting nucleic acids with a specific sequence, many analytical methods have been developed, and it is now standard for medical and biochemical laboratories to have the necessary equipment. Currently, the most popular techniques for carrying out such analyses are PCR (polymerase chain reaction) and NGS (next generation sequencing) [1], [2], [3]. However, new techniques could shorten the analysis time and increase sensitivity. Surface-enhanced Raman spectroscopy (SERS) is considered as one of the most promising analytical methods that offers important benefits such as short analysis time and exceptional sensitivity compared to other techniques. For example, Kneipp et al. showed that it is possible to detect, without any labelling, even a single DNA base molecule, based on its intrinsic surface-enhanced Raman scattering [4]. Therefore, many groups are trying to apply SERS for nucleic acid detection.
In this review, we describe various methods of detecting nucleic acids of a given sequence using SERS spectroscopy. To explain the relationship between a recorded SERS signal and the construction of a SERS sensor, we start with a brief presentation of the very basic theory of SERS spectroscopy. We then describe various types of SERS DNA/RNA sensors. To better understand how such sensors work, each type is described, starting with those that were developed first, followed by the most important breakthroughs that led to greater sensitivity and reliability. We then give some examples of SERS DNA/RNA analyses carried out recently. The article concludes with a short summary and a discussion of the challenges facing the further development of SERS sensors used to detect nucleic acids. We hope that this review will be useful for researchers starting work in this fascinating area of science and medical/biochemical technology.
2 Fundamental principles of SERS spectroscopy
As the name of this method itself suggests, in surface-enhanced Raman scattering (SERS) spectroscopy a very large increase is achieved in the efficiency of the generation of the Raman signal for molecules adsorbed on certain surfaces (or located at very close to them). The increase in the intensity of the Raman signal is explained by synergistic cooperation between two mechanisms: one due to a local increase in the intensity of the electric field in the proximity of the illuminated plasmonic structures, and the other based on chemical interactions leading to the formation, by the adsorbed molecule and the metal, of a complex having an increased Raman scattering cross-section. The first is called the electromagnetic mechanism; the second is called the chemical, or charge transfer, mechanism.
There is little point in a detailed theoretical discussion of SERS spectroscopy here, since many excellent reviews are available that explain the various mechanisms of the SERS effect [5], [6], [7]. We have chosen, therefore, to provide only very basic information about the mechanisms involved in SERS enhancement such as is necessary to understand how SERS DNA/RNA sensors operate.
In the SERS DNA/RNA sensors developed to date, the main contribution to the SERS enhancement factor comes from the electromagnetic mechanism. There is a large local increase in the intensity of the electric field of the incident radiation in close proximity to the plasmonic nanoobjects (used as typical SERS substrates in SERS DNA/RNA sensors). When using excitation radiation from the red part of the visible spectrum, the plasmonic nanoobjects are usually formed from gold, silver or copper – that is, from metals with a very small imaginary part of permittivity at the excitation frequency used. Illumination of the plasmonic nanostructures by an electromagnetic wave induces collective oscillations of the surface conduction electrons, called surface plasmons [8], [9] – see Figure 1. These excited plasmons generate an intense, localised electromagnetic field near the surface of the illuminated plasmonic objects, creating regions of high electromagnetic SERS enhancement – see Figure 2. The enhancement factor of the SERS signal is approximately proportional to the fourth power of the amplification of the electric field strength induced by the excitation of the localised surface plasmons [10] – which means that the local SERS enhancement factor can be very high, reaching values (e.g. 1010–1012) that make it possible, in some cases, to detect even a single molecule [11]. Because the SERS enhancement decreases more or less as a function of r −10 with increasing distance from a plasmonic nanoparticle, it is vital to have the electromagnetic nanoresonators located very close to the analysed molecules [12]. The largest amplification of the Raman scattering intensity is therefore observed for molecules within the first adsorbate layer.
![Figure 1:
Diagram showing excitation of surface plasmons in metallic nanoparticles under illumination at appropriate frequency. Reprinted with permission from ref. [15]. Copyright 2015 Royal Society of Chemistry.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_001.jpg)
Diagram showing excitation of surface plasmons in metallic nanoparticles under illumination at appropriate frequency. Reprinted with permission from ref. [15]. Copyright 2015 Royal Society of Chemistry.
![Figure 2:
Upper panel: transmission electron microscopic (TEM) images of some agglomerates of gold nanorods used as substrates for SERS measurements. Lower panel: maps (in the logarithmic scale) of local electromagnetic SERS enhancement factor performed using the E
4 approximation (the local electromagnetic SERS enhancement is described by the fourth power of the local electric field enhancement). Electric field enhancement factor was calculated via discrete dipole approximation simulation for aggregates of gold nanorods observed on the currently applied SERS substrate. Laser excitation radiation λ
exc = 785 nm. Reprinted from ref. [14]. CC BY license.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_002.jpg)
Upper panel: transmission electron microscopic (TEM) images of some agglomerates of gold nanorods used as substrates for SERS measurements. Lower panel: maps (in the logarithmic scale) of local electromagnetic SERS enhancement factor performed using the E 4 approximation (the local electromagnetic SERS enhancement is described by the fourth power of the local electric field enhancement). Electric field enhancement factor was calculated via discrete dipole approximation simulation for aggregates of gold nanorods observed on the currently applied SERS substrate. Laser excitation radiation λ exc = 785 nm. Reprinted from ref. [14]. CC BY license.
A very important property of the electromagnetic SERS enhancement factor is that very high values are attained in the narrow slits between the plasmonic nanoparticles (see Figure 2). High SERS enhancement factors are also achieved for molecules adsorbed on parts of the plasmonic nanostructures having high curvature, such as vertices and edges [13], [14]. Places at which a very high SERS enhancement factor is generated are known as “hot spots”.
In addition to this SERS electromagnetic enhancement mechanism, SERS chemical enhancement (or charge-transfer enhancement) also affects the intensity of the resulting SERS spectra. This mechanism resembles the ordinary resonance Raman process, and its largest values are observed when the energy of photons in the incident beam is fitted to the difference between energies of the Fermi level in the SERS substrate and an unoccupied molecular orbital of absorbed molecule or between the highest occupied molecular orbital of absorbed molecule and the Fermi level in the SERS substrate [5]. In the electrochemical systems, by the modification of the potential of the SERS substrate, it is possible to control the energy of Fermi level in substrate, and hence to influence the value of the enhancement due to the charge transfer mechanism [5]. The typical values of SERS chemical enhancements are only about 101–102 [11] and in typical SERS DNA sensors, SERS chemical enhancement is usually marginal, which is also related to the fact that the chemical mechanism of the SERS enhancement occurs only for molecules directly interacting with the surface of the substrate. However, in some cases, when DNA/RNA nitrogenous bases interact directly with the surface of the SERS substrate, the chemical contribution to the enhancement factor of the SERS spectrum can visibly affects the intensity of the measured SERS signal.
3 Detection methods based on direct analysis of SERS spectra of nucleic acids
The first SERS spectra of DNA molecules were reported as early as 1985, by Brabec and Niki [16]. Their experiments showed that the relative intensities of the nucleobase bands (the experiments were performed on DNA containing adenine) were much stronger for dissociated DNA (single-stranded DNA – ssDNA) than for standard double-stranded DNA (dsDNA). These experiments only made it possible to detect a possible dissociation of natural DNA, and so were of relatively little analytical value. It is worth emphasizing, though, that Brabec’s and Niki’s results strongly suggested that dsDNA does not become denatured or dissociated when adsorbed at a SERS-active silver surface – and this was very important in planning subsequent experiments.
Another important step in the detection of specific DNA fragments based on direct analysis of their SERS spectra was taken by Xu et al. [17]. This group managed to significantly reduce the irreproducibility of SERS spectra, which had significantly hampered reliable DNA detection. They did so by using iodide-modified Ag nanoparticles. Highly reproducible SERS signals were obtained for single- and double-strand DNA in aqueous solutions close to physiological conditions. Sample SERS spectra from a set of oligonucleotides composed of different numbers of adenine and cytosine are shown in Figure 3 [17]. As can be seen, the percentage of adenine in the oligonucleotide under study can be calculated from the relative intensity of the adenine band at 723 cm−1 [17].
![Figure 3:
Detection of oligonucleotides based on direct analysis of their SERS spectra. (a) SERS spectra of a set of oligonucleotides composed of different numbers of adenine (A) and cytosine (C), in which A % = A/(A + C) = 1, 0.9, 0.7, 0.5, 0.3, 0.1, 0, as indicated in the figure. All the spectra were normalised to the intensity of the PO2
− band at 1,087 cm−1. (b) Plot of the normalised (1 for the pure A sequence and 0 for the pure C sequence) relative band intensity of the 723/1,087 cm−1 bands versus the real ratio value of A in these oligonucleotides. Reprinted with permission from ref. [17]. Copyright 2015 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_003.jpg)
Detection of oligonucleotides based on direct analysis of their SERS spectra. (a) SERS spectra of a set of oligonucleotides composed of different numbers of adenine (A) and cytosine (C), in which A % = A/(A + C) = 1, 0.9, 0.7, 0.5, 0.3, 0.1, 0, as indicated in the figure. All the spectra were normalised to the intensity of the PO2 − band at 1,087 cm−1. (b) Plot of the normalised (1 for the pure A sequence and 0 for the pure C sequence) relative band intensity of the 723/1,087 cm−1 bands versus the real ratio value of A in these oligonucleotides. Reprinted with permission from ref. [17]. Copyright 2015 American Chemical Society.
Direct analysis of the SERS spectra of adsorbed DNA also makes it possible to identify more complex fragments of DNA. For example, by means of statistical analysis (principal component analysis–linear discriminant analysis (PCA-LDA)) of the SERS spectra of both whole genome DNA lysed from the cell line and cell-free DNA collected from the cell culture media, Liu et al. managed to identify DNA of the wild type BRAF gene and DNA of the BRAF V600E mutant gene (see Figures 4 and 5) [18]. Before the SERS analysis, the DNA chains were multiplied by 30 polymerase chain reaction (PCR) amplification steps. As SERS substrates, Liu et al. tested various positively-charged plasmonic nanostructures, including gold/silver nanospheres, nanoshells, nanoflowers, and nanostars; among them, the gold/silver nanostars exhibited the highest SERS activity [18]. A synthetic BRAF V600E sequence with a length of 218 bp was utilized to evaluate the sensitivity of the SERS measurements amplified by nanostars. By varying the number of input copies of the DNA template, the study demonstrated continuously improved SERS signals with increasing DNA input copies, even at the lowest detectable amount of DNA (102 input copies, see Figure 5). This method successfully differentiated between wild type and mutant BRAF genes in cell line DNA and cell-free DNA, including in real plasma samples. Importantly, the technique demonstrated high sensitivity, detecting only 100 input copies of the target DNA sequences. The study suggests that this direct SERS strategy is promising for the sensitive and accurate detection of certain “actual” DNA fragments, even in clinical samples.
![Figure 4:
Scheme of steps in DNA mutation SERS detection with the use of plasmonic nanostars. Reprinted with permission from ref. [18]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_004.jpg)
Scheme of steps in DNA mutation SERS detection with the use of plasmonic nanostars. Reprinted with permission from ref. [18]. Copyright 2020 American Chemical Society.
![Figure 5:
Detection of DNA chains based on direct analysis of their SERS spectra. (a) SERS spectra of BRAF V600E amplicons adsorbed on plasmonic nanostars for various numbers of input DNA copies, (b) the averaged SERS intensities of the bands at 729 and 788 cm−1 (n = 10) plotted against the number of input copies of DNA. The gel electrophoresis image is shown in the inset. Reprinted with permission from ref. [18]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_005.jpg)
Detection of DNA chains based on direct analysis of their SERS spectra. (a) SERS spectra of BRAF V600E amplicons adsorbed on plasmonic nanostars for various numbers of input DNA copies, (b) the averaged SERS intensities of the bands at 729 and 788 cm−1 (n = 10) plotted against the number of input copies of DNA. The gel electrophoresis image is shown in the inset. Reprinted with permission from ref. [18]. Copyright 2020 American Chemical Society.
Similar direct label-free DNA detection was performed by AlSafadi et al. to detect deafness mutations associated with single and dual sites related to the GJB2 gene [19]. SERS spectra measured on plasmonic silver nanoarrays on Si of normal DNA DMF-33 (GGGGGG) as well as mutant DNA at single-site DMF-9 (GGGGG) were validated by the Raman band intensity quenching of their guanine fingerprint for mutant DNA DMF-9, at 1,366 and 1,595 cm−1, respectively [19]. The DNA detection sensitivity of the fabricated SERS DNA sensor was as low as 0.1 pg/μL, with complete reproducibility [19]. The results of these experiments suggest that, using a direct SERS strategy, certain “actual” DNA fragments can be detected sensitively and accurately, even in clinical samples.
In addition to a comparative analysis of the SERS spectra of the mutant and respective wild gene leading to the detection of mutations in DNA, it has also been shown that SERS spectroscopy can identify bacteria based on their genomic DNA composition, which acts as a sample-distinguishing marker [20]. Shvalya et al. showed that multivariate statistical principal component analysis of the SERS spectra of DNA extracted from common bacterial species (Escherichia coli, Janthinobacterium lividum, Micrococcus luteus and Staphylococcus aureus) makes it possible to determine their genomic composition (percentage of guanine-cytosine and adenine-thymine bases), which in turns permits the analyzed bacteria to be identified (see Figure 6) [20]. These researchers also pointed out that this type of measurements requires exceptionally clean, repeatable, highly-active plasmonic systems, such as gold nanoparticles synthesized through a single-step plasma reduction of an ionic gold-containing vapored precursor (see Figure 6) [20]. Moreover, it should also be remembered that nanostructures used for SERS measurements often age relatively quickly and significantly change their SERS activity [20]. Another problem is that sometimes one has to wait an even longer period of time for the SERS substrate to stabilize [20]. These are additional factors that complicate SERS measurements.
![Figure 6:
Research methodology for SERS bacterial identification based on an analysis of DNA spectra. Simplified scheme of the research steps: (1) Atmospheric pressure plasma-jet system operating on an Ar/He gas mixture used to synthesize gold nanostructures and attach them to a silicon wafer, followed by substrate sensitivity test. (2) Cultivation of bacterial strains, followed by isolation of DNA fragments. (3) SERS spectra of various samples of DNA, principal component analysis, and the genomic ratio of GC versus AT, estimated from the SERS band intensities. Reprinted from ref. [20]. CC BY license.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_006.jpg)
Research methodology for SERS bacterial identification based on an analysis of DNA spectra. Simplified scheme of the research steps: (1) Atmospheric pressure plasma-jet system operating on an Ar/He gas mixture used to synthesize gold nanostructures and attach them to a silicon wafer, followed by substrate sensitivity test. (2) Cultivation of bacterial strains, followed by isolation of DNA fragments. (3) SERS spectra of various samples of DNA, principal component analysis, and the genomic ratio of GC versus AT, estimated from the SERS band intensities. Reprinted from ref. [20]. CC BY license.
Analysing the SERS spectra of DNA can be also used to detect DNA methylation [21]. Zhang et al. showed that the addition of zirconium ions (Zr4+) to the analysed system (a solution of silver nanoparticles and DNA) is very helpful when conducting this type of analysis. Zirconium ions strongly interact with phosphate backbone of the DNA, causing the folded DNA molecules to open, enhancing the SERS signals of the four DNA bases (A, C, G, T) to be obtained, and making it possible to identify the subtle differences between normal and methylated DNA with a single base-level sensitivity (see Figure 7) [21]. Moreover, zirconium ions facilitate the removal of citrates ions (used in the synthesis of Ag nanoparticles) from the surface of Ag nanostructures because Zr4+ combines with citrate and form a zirconium citrate complex (citrates give a clearly visible SERS spectrum, which interferes with SERS spectra of DNA). Zirconium ions induce also aggregation of silver nanoparticles, creating SERS “hot spots” for enhanced detection sensitivity (see Figure 7) [21]. Identifying the subtle differences between the SERS spectra of normal and methylated DNA with a single base-level sensitivity was facilitated by combining principal component analysis with 2D correlation spectroscopy analysis [21].
![Figure 7:
Schematic of preparing a DNA sample for SERS analysis (upper panel), the process of silver nanoparticle agglomeration, and the recorded SERS spectra of methylated and normal DNA. Reprinted with permission from ref. [21]. Copyright 2022 Elsevier.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_007.jpg)
Schematic of preparing a DNA sample for SERS analysis (upper panel), the process of silver nanoparticle agglomeration, and the recorded SERS spectra of methylated and normal DNA. Reprinted with permission from ref. [21]. Copyright 2022 Elsevier.
Tip-enhanced Raman spectroscopy (TERS) is an interesting type of SERS spectroscopy that has also been tested for DNA/RNA detection. In TERS spectroscopy, the nanoresonator used to enhance the efficiency of the generation of the Raman signal takes the form of a very sharp needle, such as that typically used for STM (scanning tunnelling microscopy) or AFM (atomic force microscopy) measurements. However, it is made of (or at least covered with) a plasmonic metal (Au or Ag). After bringing the TERS needle close to the sample surface, the place where the needle tip is located is illuminated with a laser beam and the Raman signal is measured. In the place directly under the tip of the illuminated plasmonic needle, the intensity of the electric field increases significantly; an enhanced Raman spectrum (de facto SERS spectrum) arises and is measured. The area of the surface of the analysed sample from which the highly enhanced Raman signal is measured is very small (comparable to the area of the needle tip, which is many orders of magnitude smaller than the area of the surface on which the laser beam is focused). Therefore, TERS measurements have very high spatial resolution (see Figure 8 [22]), and when a DNA/RNA strand deposited on a metallic surface is scanned using a TERS microscope, differences in the Raman spectra obtained from different places on the strand can be observed, making it possible to determine the sequence of the tested DNA/RNA strand.
![Figure 8:
Schematic diagram of measuring the TERS spectrum of an RNA strand. Reprinted with permission from ref. [22]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_008.jpg)
Schematic diagram of measuring the TERS spectrum of an RNA strand. Reprinted with permission from ref. [22]. Copyright 2020 American Chemical Society.
The first instance of TERS measurements at various places on a single RNA strand was described as early as 2008 by Bailo and Deckert (see Figure 9) [23]. They used a single-stranded RNA (ssRNA) homopolymer of cytosine, so this experiment cannot be considered RNA sequencing. The experiments in which the sequence of the adsorbed nucleic acid was actually determined were performed a decade later. For example, in 2018 He et al. determined the sequence of ssDNA from TERS measurements [24]. This group deposited model ssDNA (GTGGTTCGTTCGGTATTTTTAATG) on a gold surface and then scanned a silver tip along the ssDNA, collecting TERS signals at intervals of 0.5 nm (see Figure 10) [24]. They identified a given nitrogen base based on the appearance in the measured TERS spectrum of characteristic Raman bands: at 735–737 cm−1 and at 1,467–1,492 cm−1 for adenine (A), at 799–801 cm−1 and at 1,235–1,270 cm−1 for cytosine (C), at 954–958 cm−1 and at 1,545–1,554 cm−1 for guanine (G), and at 778–782 cm−1 and at 1,366–1,373 cm−1 for thymine (T) [24]. For the analysed ssDNA sample with 24 bases, only two errors were found, at the spot 7 (G → C) and at the spot 11 (T → C) [24]. In a similar way, this group also used TERS spectroscopy to determine the ssRNA sequence [22]. In this case, the detection of a given nucleobase was based on the appearance in the TERS spectrum of the following characteristic Raman bands: at 1,325–1,333 cm−1 and at 1,483–1,491 cm−1 for adenine, at 1,303–1,311 cm−1 and at 1,423–1,431 cm−1 for cytosine, at 1,457–1,465 cm−1 and at 1,566–1,566 cm−1 for guanine, and at 1,046–1,054 cm−1 and at 1,275–1,283 cm−1 for uracil [22]. The accuracy achieved in determining the sequence of ssRNA was 90 % [22].
![Figure 9:
TERS experiment along a single-stranded RNA homopolymer of cytosine adsorbed on a mica sheet. (a) Topography image showing seven adjacent spots corresponding to the positions of the TERS experiments and one additional spot for the reference measurement (position 8). (b) The Raman spectra at various positions shown in panel (a). Reprinted with permission from ref. [23]. Copyright 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_009.jpg)
TERS experiment along a single-stranded RNA homopolymer of cytosine adsorbed on a mica sheet. (a) Topography image showing seven adjacent spots corresponding to the positions of the TERS experiments and one additional spot for the reference measurement (position 8). (b) The Raman spectra at various positions shown in panel (a). Reprinted with permission from ref. [23]. Copyright 2008 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.
![Figure 10:
Determination of the sequence of ssDNA from TERS measurements. (a) TERS image of a single fragment of ssDNA with a step size of 0.5 nm. The plot shows the integral intensities of the spectrum in the region from 1,630 to 1,650 cm−1. The numbers marking the map indicate the order of the sequences. (b) The “on strand” TERS spectrum of the pixel 7 and the “off strand” spectrum one step above the pixel 7 in panel a. (c) Bar chart showing the probabilities of the appearance of a given nucleobase from spots 1 to 24 labelled in panel a. The most probable bases are labelled at the bottom. Compared to the real DNA sequence GTGGTTCGTTCGGTATTTTTAATG, two errors were found at spot 7 (G→ C) and at the spot 11 (T → C). (d) The probabilities of appearance of a given nucleobase from spots 25 to 31. The two strands in panel a are separated by 1 nm. The different sequences of spots 13–19 and spots 25–31 provides evidence that TERS imaging can distinguish two parallel DNA chains separated by just 1 nm. Reprinted with permission from ref. [24]. Copyright 2018 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_010.jpg)
Determination of the sequence of ssDNA from TERS measurements. (a) TERS image of a single fragment of ssDNA with a step size of 0.5 nm. The plot shows the integral intensities of the spectrum in the region from 1,630 to 1,650 cm−1. The numbers marking the map indicate the order of the sequences. (b) The “on strand” TERS spectrum of the pixel 7 and the “off strand” spectrum one step above the pixel 7 in panel a. (c) Bar chart showing the probabilities of the appearance of a given nucleobase from spots 1 to 24 labelled in panel a. The most probable bases are labelled at the bottom. Compared to the real DNA sequence GTGGTTCGTTCGGTATTTTTAATG, two errors were found at spot 7 (G→ C) and at the spot 11 (T → C). (d) The probabilities of appearance of a given nucleobase from spots 25 to 31. The two strands in panel a are separated by 1 nm. The different sequences of spots 13–19 and spots 25–31 provides evidence that TERS imaging can distinguish two parallel DNA chains separated by just 1 nm. Reprinted with permission from ref. [24]. Copyright 2018 American Chemical Society.
4 Detection methods based on direct analysis of SERS spectra of labelled nucleic acids
A very simple method for detecting various types of nucleic acids using SERS spectroscopy is a method that is a slight modification of the standard method for detecting nucleic acids using fluorescence [25], [26], [27]. The initial steps of both detection processes are identical: nucleic acids are amplified by PCR using specially designed primers (with attached a strong fluorophore tag or a Raman reporter – a moiety having an exceptionally large cross-section in Raman scattering). The presence of a nucleic acid with a given sequence in the analysed sample leads to the production of a large number of molecules of dye-labelled nucleic acid as a result of the PCR process. Once generated, PCR products were isolated from unincorporated tagged primers as they would otherwise produce false positive results. Then, the presence of the dye-labelled nucleic acid is determined not by fluorescence spectroscopy, but by SERS spectroscopy (actually by surface-enhanced resonance Raman scattering – SERRS) [25], [26], [27]. This means that obtaining a strong SERS spectrum of a given dye indicates the presence of a nucleic acid chain with a given sequence in the analysed sample. Typically, SERS has comparable sensitivity to fluorescence, but in some cases the sensitivity of the DNA detection using SERS can be up to 100 times higher than that of conventional fluorescence-based methods [28]. SERS, moreover, has a unique advantage that the recorded spectrum consists of sharp, molecular-specific vibrational bands, whereas fluorescence generates much broader bands. This means that in the SERS experiments it is much easier to eliminate band overlapping than in fluorescence, and therefore it is much easier to detect a larger number of Raman reporters (which are also usually fluorescent tags), and hence, to detect a larger number of the target DNA/RNA chains in one measurement [25], [26], [27]. Raman reporters are also generally more resistant to photobleaching during Raman measurements than fluorophores during fluorescence measurements [29], which allows for longer observation times. Another important advantage of SERS is reduced susceptibility to biological autofluorescence [30]. In fluorescence-based techniques, background autofluorescence from biological samples can interfere with signal detection and interpretation.
5 Detection methods based on selective hybridisation of probe and target ssDNA
As shown in the Section 3, it is possible to: (i) distinguish the SERS spectrum of various DNA fragments (for example, wild type BRAF gene and BRAF gene with V600E mutation), (ii) record Raman maps of DNA/RNA strands using a TERS microscope, which makes it possible to determine a DNA/RNA sequence with 90 % accuracy. However, SERS detection methods of DNA/RNA based on direct analysis of their Raman spectra are not yet suitable for reliably detecting DNA/RNA fragments having a given sequence. More reliable SERS detections of given fragments of nucleic acids are now only being made in experiments in which the biotarget nucleic acid (e.g., gene sequences, bacteria or viral DNA fragments) is selectively hybridised with “capture” single-stranded nucleic acid complementary to that of the probe single-stranded nucleic acid. In this Section, we describe the four most common types of SERS DNA sensors utilising selective DNA/RNA hybridisation: (i) sensors based on a hybridisation-induced attachment of a “Raman reporter” to the SERS-active surface, (ii) sensors based on a hybridisation-induced linking of various DNA/RNA–modified nanostructures, (iii) sensors based on a hybridisation-induced rearrangement of the linking and protecting alkanethiol chains attached to a SERS-active surface, and (iv) sensors that utilise DNA hydrogels. However, the types of SERS DNA/RNA sensors described below do not represent all the types of SERS DNA/RNA sensors utilising selective DNA/RNA hybridisation that have been developed. For example, Mahajan and co-workers immobilised “capture” ssDNA on a SERS-active surface, and in the next step they attached the analysed dye-modified ssDNA and then determined the susceptibility of the obtained system to dissociation under the influence of increased temperature or the application of very negative potential [31], [32]. If dissociation (melting) occurred at a higher temperature [31] or at a more negative potential [31], [32], the degree of complementarity of the “capture” ssDNA immobilised on the SERS-active surface and the analysed ssDNA was higher [31].
5.1 Methods based on the attachment of a Raman reporter to the SERS-active surface
The first developed group of SERS DNA/RNA detection methods utilising selective hybridisation with “capture” complementary ssDNA/RNA strands were based on hybridisation-induced placing of a Raman reporter directly on the SERS-active surface. The first example of such SERS DNA detection was described in 1994 by Vo-Dinh and co-workers [33]. This group attached a Raman reporter (cresyl violet) to the 5′ end of ssDNA strands complementary to the sought-after (target) ssDNA, and then carried out hybridisation with the analysed ssDNA adsorbed on a nitrocellulose filter [33]. After the hybridisation process, the ssDNA which had not hybridised was removed by careful washing. Then, the DNA absorbed on the nitrocellulose (both that which did not hybridise and that which hybridised with DNA complementary to the target DNA with cresyl violet attached) was desorbed from the nitrocellulose in a 0.1 M NaOH solution. After neutralisation, the desorbed DNA was deposited on a SERS-active substrate and the SERS spectrum was measured. The presence in the measured SERS spectrum of strong Raman bands of cresyl violet suggests that the analysed ssDNA contained the sought-after sequence complementary to the sequence of the ssDNA to which the Raman reporter had been attached.
This general principle of DNA detection (deposition of a Raman reporter on the SERS-active surface as a result of DNA hybridisation) has been applied in many slightly different SERS sensors. For example, in 1998, the same group developed a SERS sensor for detecting a DNA fragment from the gag gene region of HIV1 [34]. At first, the analysed DNA was multiplied in a polymerase chain reaction (PCR) in such a way that the obtained (multiplied) DNA fragments were labelled with cresyl violet. Cresyl violet was introduced to the formed DNA by using a cresyl violet-labelled oligonucleotide primer for PCR [34]. In another process, the capture probe ssDNA, which was complementary to an internal sequence of the amplified target ssDNA, was bound to a polystyrene substrate. After hybridisation of the capture probe ssDNA with the cresyl violet-labelled product ssDNA (multiplied and modified analysed ssDNA), the polystyrene wells were carefully washed to remove non-specifically bonded ssDNA. The polystyrene substrate with attached DNA was then coated via thermal evaporation with a 10 nm layer of silver. Finally, when the target ssDNA was present in the analysed sample, the SERS signals from the attached cresyl violet are detected [34].
A significantly simpler SERS DNA sensor which utilises hybridisation-induced placing of a Raman reporter on the SERS-active substrate was achieved by immobilising capture ssDNA (complementary to the target ssDNA) on a SERS-active substrate [35]. Then, after proper modification of the analysed ssDNA (by attaching to it chains of, for example, rhodamine B), hybridisation with the immobilised capture ssDNA was carried out and the SERS signal measured. If the target ssDNA was present in the analysed sample, rhodamine B was attached to the SERS-active substrate and a strong SERS spectrum of this Raman reporter was measured [35]. Using such an approach, Allain et al. detected a fragment of the BRCA1 breast cancer susceptibility gen [35], [36]. Barhoumi and Halas noticed that, because the Raman scattering cross-section of adenine is so large, when the probe DNA sequence was adenine-free, adenine could be used as a Raman reporter [37]. Therefore, in this type of approach, there is no need to use any Raman reporter. To form an adenine-free probe ssDNA sequence general enough to detect any target ssDNA sequence, adenine was replaced in the probe ssDNA by 2–aminopurine [37]. This substitution preserved the same hybridisation characteristics of the substituted sequence [37]. Using such adenine-free probe ssDNA sequences, any adenine-containing DNA target oligonucleotide can be easily detected using SERS, due to the presence of the characteristic Raman band of adenine at 736 cm−1 (see Figure 11) [37].
![Figure 11:
Schemes showing DNA hybridisation between the thiolated probe DNA, with 2–aminopurine substituted for adenine, and the unlabelled target DNA; any adenine-containing DNA target oligonucleotide leads to the appearance in the measured SERS spectrum of a characteristic band of adenine at 736 cm−1. Reprinted with permission from ref. [37]. Copyright 2010 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_011.jpg)
Schemes showing DNA hybridisation between the thiolated probe DNA, with 2–aminopurine substituted for adenine, and the unlabelled target DNA; any adenine-containing DNA target oligonucleotide leads to the appearance in the measured SERS spectrum of a characteristic band of adenine at 736 cm−1. Reprinted with permission from ref. [37]. Copyright 2010 American Chemical Society.
The next significant improvement of SERS DNA sensors based on the hybridisation-induced placing of a Raman reporter on a SERS-active surface was achieved by eliminating the need to modify the analysed DNA. In created what is known as a “sandwich-type” SERS DNA sensor, two strands of ssDNA complementary to two different fragments of the target ssDNA are used. One ssDNA, complementary to one fragment of the target DNA, (known as the capture DNA) is immobilised on the SERS-active substrate [38], [39]. Then, hybridizations with the analysed ssDNA and the reporter ssDNA (which is also complementary to a fragment of the target ssDNA and has a Raman reporter attached to it) are carried out. When the analysed sample contains the target ssDNA, the reporter ssDNA with the attached Raman reporter is immobilised on the SERS-active substrate (see Figure 12), which means that the Raman reporter is located in close proximity to the SERS-active substrate, and hence a strong SERS spectrum of the Raman reporter is observed [38], [39]. Such SERS DNA sensors can detect a remarkably low DNA concentration at ∼1 fM [38]. Analysis of how changing various construction details of such a sensor affects the intensity of the generated Raman signal showed that, although in general there is an increase in the intensity of the SERS signal when the distance between the Raman scatterer and the SERS-active surface decreases, for this type of sensor a greater intensity of the measured Raman signal is usually observed when the Raman reporter is farther away from the plasmonic substrate (see Figure 12) [40]. This is probably caused by a significant change in the hybridisation efficiency for the different structures of the sensor analysed, due to some steric hindrances [49].
![Figure 12:
Scheme of sandwich-type SERS DNA sensors utilising capture DNA (complementary to one fragment of the target DNA) immobilised on a SERS-active substrate and reporter ssDNA (which is also complementary to a fragment of the target ssDNA and has a Raman reporter attached). Sensor in configuration A (Raman reporter “outside” the double-stranded DNA) and in configuration B (Raman reporter “inside” the double-stranded DNA). Reprinted from ref. [40]. CC BY license.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_012.jpg)
Scheme of sandwich-type SERS DNA sensors utilising capture DNA (complementary to one fragment of the target DNA) immobilised on a SERS-active substrate and reporter ssDNA (which is also complementary to a fragment of the target ssDNA and has a Raman reporter attached). Sensor in configuration A (Raman reporter “outside” the double-stranded DNA) and in configuration B (Raman reporter “inside” the double-stranded DNA). Reprinted from ref. [40]. CC BY license.
It should be emphasized that analogous sandwich-type sensors for DNA detection can also be based on fluorescence spectra [41], [42]. As mentioned above, the main advantage of SERS-based sensors over fluorescence-based sensors is that the recorded SERS spectrum consists of sharp bands, while fluorescence generates much broader bands. Therefore, it is much easier to eliminate band overlap in SERS experiments than in fluorescence experiments and to detect more target DNA/RNA strands in one SERS measurement than in one fluorescence measurement.
An interesting observation was made by Guselnikova et al. who, using principal component analysis, showed that it is possible to distinguish the SERS spectrum of capture ssDNA adsorbed on a SERS-active gold substrate from the SERS spectrum of dsDNA formed on a SERS substrate as a result of the hybridization of complementary capture and target ssDNAs [43]. This means that, in principle, the classical so-called sandwich-type SERS DNA sensors described above can be constructed without the use of a Raman reporter. This group also showed that it is possible to distinguish structures formed by two, not completely complementary ssDNA strands based on the obtained SERS spectra.
A very interesting type of SERS DNA/RNA sensors, whose operation is based on changing the distance between the Raman reporter and the surface of the SERS substrate, is what is known as hairpin sensors. Hairpin sensors are divided into two groups: on-off [44], [45], [46] and off-on [47], [48]. In the on-off hairpin sensors, developed first, the DNA probe sequence consists of a middle section that contains a sequence complementary to the target sequence to be detected, as well as two arms that have complementary sequences and thus form a hairpin loop configuration under normal conditions (see Figure 13) [44], [45], [46]. The hairpin loop configuration is designed such that the Raman reporter is in contact or close proximity (<1 nm) to the SERS-active surface, which makes it possible to induce a strong SERS effect of the Raman reporter (see Figure 13). Hybridisation with a complementary target ssDNA opens the hairpin loop and physically separates the Raman reporter from the SERS-active substrate. Since, as mentioned in Section 2, the SERS enhancement factor depends strongly on the distance, d, between the Raman reporter and the SERS-active surface (as d −10 [12]), the hybridisation process leads to a strong decrease in the SERS effect and causes a quenching of the measured SERS signal after hybridisation [44], [45], [46]. Using this approach, Vo-Dinh et al. detected the gag gene sequence of the human immunodeficiency virus type 1 (HIV-1) [44] and single-nucleotide polymorphisms in breast cancer BRCA1 gene [46], Sha et al. detected RNA of the Hepatitis C virus (HCV) [45], whereas Kang et al. quantitatively determined let-7a miRNA in MCF-7 cell derived exosomes [49]. As a very active substrate in SERS spectroscopy, this last group used a close-packed and ordered array of gold octahedral nanoparticles; they achieved a broad linear range for this let-7a miRNA sensor (from 10 aM to 10 nM) and a low detection limit (5.3 aM), without using any signal amplification strategy [49].

Schematic diagram of the concept of a hairpin on-off SERS sensor. (a) A SERS signal is observed when the hairpin is in the closed-state conformation, but diminishes in the open-state conformation. (b, c) SERS spectra from a plasmonics nanoprobe in the absence (b) and in the presence (c) of the target ssDNA.
A few years after developing the hairpin on-off SERS sensor, Vo-Dinh and co-workers developed a hairpin sensor having an off-on structure [47], [48]. In this approach, ssDNA (from which the “stem-loop” is formed) with an attached a Raman reporter at one end and a thiol moiety at the other end is immobilised onto a SERS-active substrate via a metal-sulphur bond. ssDNA serving as a “placeholder” strand is partially hybridised with ssDNA immobilised at the metal surface with an attached Raman reporter, keeping the Raman reporter away from the SERS-active surface (see Figure 14). In this configuration (i.e. in the absence of target ssDNA), the probe ssDNA is “open” and the sensor generates a very low SERS signal (the sensor is “off”). Upon exposure to the target ssDNA, the placeholder ssDNA strand leaves the SERS-active surface; this allows the stem-loop structure to “close” and moves the Raman reporter onto the SERS-active surface, yielding a strong SERS signal (the sensor is “on”). Using hairpin off-on SERS sensors, Vo-Dinh et al. detected the RSAD2 human gene [47] and a fragment of DNA formed from DENV 4 RNA of the dengue virus [48]. In both cases, a cyanine5 moiety was used as the Raman reporter [47], [48].
![Figure 14:
Schematic diagram of the concept of a hairpin off-on SERS sensor. Reprinted with permission from ref. [47]. Copyright 2015 Elsevier Inc.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_014.jpg)
Schematic diagram of the concept of a hairpin off-on SERS sensor. Reprinted with permission from ref. [47]. Copyright 2015 Elsevier Inc.
Some increase in the usability of a hairpin SERS DNA sensor is achieved by introducing magnetic properties into it. Lu et al. formed hairpin on-off SERS sensor by immobilizing ssDNA in a folded hairpin structure on core-satellite Fe3O4@SiO2–Au nanostructures (see Figure 15) [50]. The ssDNA fragment used in this sensor contained a 23-base loop sequence to specifically capture the target tetracycline resistance gene (tetA) and a 7-base stem sequence on either side to keep the probe DNA in a hairpin structure at room temperature (see Figure 15) [50]. The detection limit of tetA in environmental samples was calculated to be 25 copies μL−1 [50]. This limit of detection is comparable to that of the conventional, quantitative PCR technique, which was 15.8 copies μL−1 in detecting Mycobacterium tuberculosis-specific DNA [50].
![Figure 15:
Schematic illustration of the concept of a hairpin on-off SERS sensor having magnetic properties. DNA hairpin structures were immobilized on core-satellite Fe3O4@SiO2–Au nanostructures. Reprinted with permission from ref. [50]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_015.jpg)
Schematic illustration of the concept of a hairpin on-off SERS sensor having magnetic properties. DNA hairpin structures were immobilized on core-satellite Fe3O4@SiO2–Au nanostructures. Reprinted with permission from ref. [50]. Copyright 2020 American Chemical Society.
The hairpin type strategy is also used to construct DNA sensors based on the measurement of the fluorescence spectrum [51], [52]. Similar to other SERS and fluorescence sensors with an analogous structure, sensors based on the measurement of SERS spectrum allow for better elimination of band overlap and thus allow for the detection of a larger number of target DNA/RNA strands in a single measurement.
5.2 Methods based on agglomeration of nanoparticles or their selective deposition via the links formed by nucleic acids
Another group of commonly used SERS sensors for the detection of nucleic acids having a given sequence are sensors where the selective hybridisation of the probe (capture) nucleic acid and the target nucleic acids leads to the formation of bonds (via double-stranded chains) that connect the nanoparticles to each other or bind the plasmonic nanoparticles to a macroscopic plasmonic substrate. Bringing plasmonic systems very close each other creates sites, in the narrow slits between the plasmonic structures, that are particularly active in SERS spectroscopy, and when such a phenomenon occurs, we observe a very strong SERS signal.
In the first developed SERS DNA sensor utilising DNA links between plasmonic structures, silver nanoparticles with a diameter of about 15 nm were attached to a smooth silver film (practically inactive in SERS spectroscopy) [53]. Linking DNA chains were seen to form between the silver film and the silver nanoparticles when the probe ssDNA was present in the analysed sample. The deposition of Ag nanoparticles on the Ag film resulted in the formation of a very SERS-active structure, and hence in a very large increase in the intensity of the SERS signal generated by the Raman reporter being used (5-((2-(and-3)-S-(acetylmercapto)succinoyl)amino) fluorescein), which had been deposited previously on the silver substrate (see Figure 16) [53]. A diagram of such a sensor is shown in Figure 16 [53]. A model 24-mer oligonucleotide was used as the target ssDNA [53]. The silver nanoparticles were functionalised with ssDNA complementary to one-half of the target ssDNA (shown in blue in Figure 16A), whereas the smooth SERS-inactive silver film was modified with ssDNA complementary to the remaining part of the target ssDNA sentence (shown in red in Figure 16A) [53]. The Ag-film modified with one capture ssDNA and the Raman reporter was then incubated with the target ssDNA and a sol of silver nanoparticles modified with the second capture ssDNA strand [53]. When both the capture ssDNA strands are complementary to the respective parts of target ssDNA, a sandwich structure is formed through sequence-selective hybridisation, and plasmonic coupling occurs between the silver nanoparticles and the silver film, creating electromagnetic SERS hot spots and a strong SERS Raman reporter signal [53]. When a non-complementary DNA strand was used, featureless spectra were obtained, which shows that the proposed method makes it possible to confirm the presence of DNA of a given sequence in the analysed sample [53].
![Figure 16:
Detection of ssDNA based on selective deposition of plasmonic nanoparticles on a plasmonic substrate. (A) Schematic illustration of the SERS detection of ssDNA utilising the creation of DNA links between silver nanoparticles and a smooth silver film (virtually inactive in SERS spectroscopy). A target ssDNA strand (a′b′) is captured by the respective ssDNA fragments attached to the silver nanoparticles (probe-a) and the silver film (probe-b), resulting in the creation of a highly SERS-active structure. Target ssDNA detection is confirmed by recording a strong SERS signal from the surface-bound Raman reporter, F. (B) SERS spectra (vertically offset for clarity) obtained from: (a) an Ag film modified with a Raman reporter, probe-b ssDNA and a′b′ target ssDNA, (b) an Ag film modified with a Raman reporter, probe-b ssDNA, a′b′ target ssDNA and silver nanoparticles with attached probe-a ssDNA, and (c) an Ag film prepared as in (b) except for using a non-complementary target sequence in place of a′b′. (C) Representative AFM images of the surface of the sensor after the attachment of Ag nanoparticles: (a) 5 × 5 μm and (b) 1 × 1 μm. Arrows point to silver nanoparticles on the surface. Reprinted with permission from ref. [53]. Copyright 2007 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_016.jpg)
Detection of ssDNA based on selective deposition of plasmonic nanoparticles on a plasmonic substrate. (A) Schematic illustration of the SERS detection of ssDNA utilising the creation of DNA links between silver nanoparticles and a smooth silver film (virtually inactive in SERS spectroscopy). A target ssDNA strand (a′b′) is captured by the respective ssDNA fragments attached to the silver nanoparticles (probe-a) and the silver film (probe-b), resulting in the creation of a highly SERS-active structure. Target ssDNA detection is confirmed by recording a strong SERS signal from the surface-bound Raman reporter, F. (B) SERS spectra (vertically offset for clarity) obtained from: (a) an Ag film modified with a Raman reporter, probe-b ssDNA and a′b′ target ssDNA, (b) an Ag film modified with a Raman reporter, probe-b ssDNA, a′b′ target ssDNA and silver nanoparticles with attached probe-a ssDNA, and (c) an Ag film prepared as in (b) except for using a non-complementary target sequence in place of a′b′. (C) Representative AFM images of the surface of the sensor after the attachment of Ag nanoparticles: (a) 5 × 5 μm and (b) 1 × 1 μm. Arrows point to silver nanoparticles on the surface. Reprinted with permission from ref. [53]. Copyright 2007 American Chemical Society.
A SERS DNA sensor quite similar to the one described above, but based on the formation of aggregates of plasmonic nanoparticles in solution, was described by Qian et al. [54]. In this approach, two types of gold nanoparticles with an attached Raman reporter (such as malachite green) were used. One portion of gold nanoparticles was functionalised with capure-1 ssDNA complementary to one part of the target ssDNA, whereas the second part of the gold nanoparticles was modified with capture-2 ssDNA complementary to the remaining part of the target ssDNA strand [54]. Adding target ssDNA to the mixture of gold nanoparticles modified with capture-1 and capture-2 ssDNA caused an agglomeration of gold nanoparticles (see Figure 17). This led to a coupling of plasmons, the formation of electromagnetic SERS hot spots in the slits between gold nanostructures, and a strong SERS signal of the Raman reporter (in this case, malachite green) [54].
![Figure 17:
Schematic illustration of the DNA-induced agglomeration of colloidal gold nanoparticles. The agglomeration permits long-range plasmonic coupling and a large increase in the SERS-activity of the nanostructure formed. Reprinted with permission from ref. [54]. Copyright 2008 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_017.jpg)
Schematic illustration of the DNA-induced agglomeration of colloidal gold nanoparticles. The agglomeration permits long-range plasmonic coupling and a large increase in the SERS-activity of the nanostructure formed. Reprinted with permission from ref. [54]. Copyright 2008 American Chemical Society.
When different Raman reporters are used (or the constructed sensor contains well-defined and easily distinguishable places where the generated analytical signal indicates the presence of a specific ssDNA fragment), it is possible to detect various ssDNA fragments using just one sensor. For example, using a SERS DNA sensor of gold nanoparticles on a gold nanowire (a scheme of which is shown in Figure 18), Kang et al. managed to detect multiple target DNAs (DNA from Enterococcus faecium, Staphylococcus aureus, Stenotrophomonas maltophilia, and Vibrio vulnificus) in a single assay [55]. These groups formed gold nanowires on a c-sapphire substrate using a vapour transport method. The formed gold nanowires with a diameter of ca. 150 nm and a length of several dozen micrometers are highly single-crystalline without twins and have atomically smooth surfaces. Therefore, the observed SERS enhancement factor is very uniform along the whole Au nanorod. The surfaces of gold nanowires were modified with the thiolated probe ssDNAs and then were transferred using a nanomanipulator to a silicon substrate. Since the created nanorods are easily visible under an optical microscope, it is relatively easy to determine which nanorod (modified with ssDNA probe complementary to a given fragment of the DNA being searched for) is located and, in this way, using a Raman microscope the analytical signal characteristic of a given fragment of the DNA being sought can be selectively measured. In order to be able to detect four different ssDNA fragments, Kang et al. used gold nanorods modified with two different probe ssDNAs (see Figure 18) and gold nanoparticles modified with two different reporter ssDNAs (see Figure 18), with two different Raman reporters attached (TAMRA and cyanine 5 dyes) [55]. It should be emphasized that the sensor created by Kang et al. cannot be classified as a sensor that could play a useful practical role in its current form. In addition to the relatively complicated procedure of identifying different Au nanowires, the target DNA was amplified by PCR with universal and species-specific primers. PCR amplicons were then purified using a PCR purification kit.
![Figure 18:
Detection of ssDNA based selective deposition of gold nanoparticles on gold nanowires. (a) Schematic illustration of a SERS DNA sensor based on what is known as a gold nanoparticle on a gold nanowire system. (b) SERS spectra obtained using such a sensor after DNA hybridisation with the complementary target ssDNA (blue spectrum), and prepared when the non-complementary target ssDNA is used in place of complementary target ssDNA (magenta spectrum). The inset shows UV–vis absorption spectra of the Au nanoparticles (green spectrum), Au nanowires (magenta spectrum), and gold nanoparticle on gold nanowire systems (blue spectrum). (c) SEM image of a typical gold nanoparticle on gold nanowire structure constructed by adding complementary target ssDNA (top) and a clean gold nanowire after the addition of non-complementary target ssDNA (bottom). Reprinted with permission from ref. [55]. Copyright 2010 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_018.jpg)
Detection of ssDNA based selective deposition of gold nanoparticles on gold nanowires. (a) Schematic illustration of a SERS DNA sensor based on what is known as a gold nanoparticle on a gold nanowire system. (b) SERS spectra obtained using such a sensor after DNA hybridisation with the complementary target ssDNA (blue spectrum), and prepared when the non-complementary target ssDNA is used in place of complementary target ssDNA (magenta spectrum). The inset shows UV–vis absorption spectra of the Au nanoparticles (green spectrum), Au nanowires (magenta spectrum), and gold nanoparticle on gold nanowire systems (blue spectrum). (c) SEM image of a typical gold nanoparticle on gold nanowire structure constructed by adding complementary target ssDNA (top) and a clean gold nanowire after the addition of non-complementary target ssDNA (bottom). Reprinted with permission from ref. [55]. Copyright 2010 American Chemical Society.
When the Raman reporters are properly selected (so as to provide non-overlapping spectra), the number of Raman reporters used in one experiment can be increased. For example, Li et al. constructed a SERS DNA sensor in which four Raman reporters (4-aminothiophenol, 4-chlorothiophenol, 4-hydroxythiophenol, and 5,5′-dithiolbis(2-nitrobenzoic acid)) were used simultaneously [56].
Using the “connection mechanism” described above, Li et al. constructed a sensor which permits the simultaneous acquisition of two different analytical signals: an SPR (surface plasmon resonance) signal and a SERS signal [57]. In this sensor, gold nanoparticles functionalised with a Raman reporter and ssDNA complementary to one part of the target micro-RNA were captured onto a smooth gold film – also used as an active part of the SPR sensor – functionalised with ssDNA complementary to another part of the target micro-RNA. This sensor was used to detect three micro-RNA (miRNA) fragments that are typical cervical cancer markers: miRNA21, miRNA124 and miRNA143 [57]. The attached gold nanoparticles greatly improved the SPR response due to the mass increase and larger refractive index changes. Moreover, attaching many Au nanoparticles to the gold surface of the SPR sensor also makes it possible to obtain a strong SERS signal. Three miRNA fragments were detected simultaneously in serum to verify the practicality, selectivity and sensitivity of the sensor. From an analysis of the SPR signals, all three miRNA could be detected simultaneously, with limits of detection (LODs) of 6.3 fM for miRNA21, 5.3 fM for miRNA124, and 4.6 fM for miRNA143, and with a wide dynamic response range of 500 pM-10 nM [57]. Based on the analysis of the SERS signal, higher sensitivity could be achieved with LODs as low as 1 fM for miRNA21, 0.8 fM for miRNA124 and 1.2 fM for miRNA143 [57].
An interesting type of SERS DNA sensor that uses both the hairpin-structured DNA sequences described in detail in the previous Section and plasmonic nanoparticles attached via the DNA chain formed is the sensor developed by Si et al. (see Figure 19) [58]. In the first stage of its construction, four thiolated hairpin-structured DNA sequences 1 (hp1-SH) having fragments complementary to four different cancer-associated miRNAs (marked in Figure 19 by: miR-21, miR-221, miR-133a and miR-1246) were attached onto one of the four Au/Ag alloy nanoparticles, which were immobilized on four different locations on a quartz sheet, thus forming a SERS sensor array with four sensing units (sensing unit for: miR-21, miR-221, miR-133a, and miR-1246). As mentioned above, detecting low expression levels of miRNA is extremely challenging, but is very important because miRNAs are biomarkers of various cancers. When the target miRNA is present in the analyzed sample, the hybridization between the related hairpin-structured 1 (hp1) and the target miRNA exposed the hidden toehold in the stem of the hp1, which allowed the corresponding SERS tags to be recognized. The SERS tags were prepared by modifying the Au/Ag alloy nanoparticles with 4−mercaptobenzonitrile (a Raman reporter) and with thiolated hairpin-structured DNA sequences 2 (hp2-SH) complementary to the four hp1 sentences used. These SERS tags with adsorbed hp2-SH displaced the target miRNA from the hp1 to form a stable hp1/hp2 duplex (see Figure 19). The released target miRNA induced the next cycle, which ultimately led to more SERS tags becoming anchored on the sensor array chip; they formed more SERS hot-spots, producing a strong SERS signal [58]. This SERS DNA sensor array offers a versatile and efficient platform for the simultaneous detection of multiple cancer-associated miRNAs with a detection limit of 0.15 pM.
![Figure 19:
Scheme of a SERS DNA sensor developed by Si et al. that uses both hairpin-structured DNA sequences and the attachment of plasmonic nanoparticles via the DNA chain formed. Reprinted with permission from ref. [58]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_019.jpg)
Scheme of a SERS DNA sensor developed by Si et al. that uses both hairpin-structured DNA sequences and the attachment of plasmonic nanoparticles via the DNA chain formed. Reprinted with permission from ref. [58]. Copyright 2020 American Chemical Society.
A SERS DNA sensor that uses two response amplification mechanisms was designed by Liu et al. [59]. One mechanism for increasing the sensor’s selectivity is nicking endonuclease amplification [59]. The enzyme used for this amplification (Nt.BstNBI) can recognize the ssDNA sequence of 5′-GAGTC-3′ in dsDNA, and cleave only one DNA strand at 4 bases away from the 3′-end of its recognition site; thus, it has very high specificity, since it requires a specific recognition site [59]. The second response amplification mechanism consists of silver nanocubes (such nanoparticles, which have sharp edges and corners, provide high-quality SERS hot spots, making it possible to obtain a stronger SERS signal) [59]. The biosensor developed demonstrated an impressive limit of detection of 3.1 fM for DNA species related to oral cancer (the ORAOV1 gene) [59]. Additionally, the platform exhibited high specificity, even against single-base mismatches, making it promising for early clinical diagnosis of oral cancer [49].
In general, the detection of nucleic acids by SERS measurements using the strategy described above, that is, linking various plasmonic nanostructures to plasmonic or non-plasmonic substrates by creating DNA strands as a result of hybridization, can be modified in many various ways. For example, the substrate to which the plasmonic nanoparticles are attached can be made of: gold nanoparticles on a porous anodic aluminum oxide [60], a film of gold nanoparticles on the surface of flat silica [61], or even TiO2 nanoparticles [62]. The plasmonic nanoparticles attached by creating DNA strands can consist of, for example: gold nanoparticles modified by 4-mercaptobenzoic acid (MBA) and then covered with silver (AuMBA@Ag) [60], silver nanoparticles modified by MBA and then covered with gold (AgMBA@Au) [61], or silver nanocubes [59], [62]. In order to increase sensitivity, various recycle amplification strategies for the target nucleic acid can also be applied [60], [61], [62]; for example, catalytic hairpin assembly amplification technology by means of rehybridization with thousands of hairpin probes to trigger amplification cycles [61], [62].
By using an RNA-induced aggregation of gold nanoparticles modified with the right capture ssDNA, Tan et al. were able to image miRNA-21 and tumor tissues in vivo in a mouse [63]. The distribution of a given miRNA can even be mapped in situ inside individual cells using a hybridization-induced agglomeration of modified plasmonic nanoparticles introduced to the cells (see Figure 20) [64]. The plasmonic nanoparticles were modified with molecules of the Raman reporter and with capture nucleic acids complementary to the target miRNA. The SERS detection of miRNA in different subtypes of breast cancer cells, SK-BR-3 and MCF-7 showed that the expression level of the target miRNA in the SK-BR-3 cells was five times higher than in the MCF-7 cells, which was confirmed by the result of a gene analysis [64].

Schematic diagram for the: (a) hybridisation-induced conjugation of SERS-active gold nanoparticles modified with a Raman reporter and with ssDNA complementary to the target miRNA, and (b) cellular uptaking of miRANs, the formation of nanoclusters inside the cells, and the detection of miRNA expression level based on SERS mapping.
Also Wang et al. developed a SERS methodology for detecting miRNA inside cells [65]. In their approach, modified gold nanoparticles were self-assembled into trimers under the presence of target miRNA (miR-21), which generated a stable, enhanced electric field due to the coupling of the plasmons. The enhancement of the intensity of the electric field led to the formation of SERS hot spots, and increased the efficiency of the fluorescence, enabling the sensor to use two different analytical signals (SERS and fluorescence). Wang et al. used adenine as a reporter molecule, which simplified the labelling process [65]. This strategy successfully achieved accurate tracking and quantification of miR-21 in cancer cells, and showed good stability within the cells. The limit of detection values of the dual spectra were 3.58 pM (for the SERS signal) and 11.8 pM (for the fluorescence signal), with a relative standard deviation of less than 2.7 %.
It is also worth mentioning that the above-described aggregation of plasmonic nanoparticles induced by the created DNA strands can be used to detect more than nucleic acids. It can be also used, for example, to detect the caspase-3 protein [66], certain environmentally relevant biomolecules [67], or even molecules of individual proteins [68].
Techniques using DNA hybridization-induced formation of plasmonic nanoparticles aggregates are based on the creation of SERS hot spots in narrow gaps between plasmonic nanoobjects after aggregation and, consequently, the appearance of a strong SERS spectrum after DNA hybridization. As far as we know, the longest fragments of nucleic acids analysed by this SERS technique were from a dozen to several dozen nucleotides in length. Studying much longer nucleic acid fragments using these SERS techniques would generate problems with generated SERS enhancement factors. The optimal gap distance for the highest SERS enhancement is approximately 1 nm [69], [70], [71]. Gaps of a few nanometers are also very efficient in enhancing Raman scattering [69], [70], [71]. However, a further increase in the width of the gap leads to a significant reduction in the generated SERS signal [69], [70], [71] – therefore, in this technique, there is a limit to the thickness of the nucleic acid layer creating a “connection” between the plasmonic nanoparticles.
In addition to detection methods based on the agglomeration of plasmonic nanoparticles only, the agglomeration of plasmonic and magnetic nanoparticles can be also used to construct SERS DNA sensors. In these methods, SERS hot spots are created by bringing plasmonic nanoparticles very close each other (achieving plasmonic coupling); moreover, the magnetic-plasmonic aggregates that form can be concentrated by applying a permanent magnet to the sample being analysed. For example, Zhang et al. detected DNA derived from the West Nile virus by carrying out an agglomeration of silica shell-coated magnetic nanoparticles conjugated with capture oligonucleotides complementary to one part of the target DNA and gold nanoparticles conjugated with the Raman reporter (5,5′-dithiobis(succinimidy-2-nitrobenzoate)), as well as capture oligonucleotides (marked in Figure 21 as reporter oligonucleotides) complementary to another part of the target DNA (see Figure 21) [72]. The DNA hybridisation was conducted at pH = 7.4 by adding the target and control DNA sequences in a phosphate-buffered saline to a mixture of modified gold (plasmonic) and iron oxide (magnetic) nanoparticles [72]. After hybridisation, the agglomerates formed were precipitated from the solution using a small external magnet, and the SERS spectra of the precipitate were then measured. Zhang et al. found that the intensity of the strongest SERS band of the Raman reporter at 1,330 cm−1 was proportional to the logarithm of the concentration of the target DNA sequence in the analysed sample [72].
![Figure 21:
Schematic illustration of West Nile virus DNA capture and detection using silica shell-coated iron oxide magnetic nanoparticles (MNPs) conjugated with capture oligonucleotides complementary to one part of the target West Nile virus DNA and gold nanoparticles (GNPs) conjugated with a Raman label (5,5′-dithiobis(succinimidy-2-nitrobenzoate)) and reporter oligonucleotides complementary to another part of the target West Nile virus DNA. Reprinted with permission from ref. [72]. Copyright 2010 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_021.jpg)
Schematic illustration of West Nile virus DNA capture and detection using silica shell-coated iron oxide magnetic nanoparticles (MNPs) conjugated with capture oligonucleotides complementary to one part of the target West Nile virus DNA and gold nanoparticles (GNPs) conjugated with a Raman label (5,5′-dithiobis(succinimidy-2-nitrobenzoate)) and reporter oligonucleotides complementary to another part of the target West Nile virus DNA. Reprinted with permission from ref. [72]. Copyright 2010 American Chemical Society.
When using Raman reporters that generate clearly different SERS spectra, a method based on an agglomeration of magnetic and plasmonic nanoparticles due to the creation of linking DNA chains can be also used to simultaneously detect many different fragments of nucleic acids (see Figure 22). For example, Wu et al. constructed a magnetically-assisted, SERS-based biosensor for the ultrasensitive, multiplex detection of three hepatocellular carcinoma-related miRNA biomarkers: miRNA-122, miRNA-223, and miRNA-21 [73]. The biosensor contained two types of nanoparticles: DNA-engineered fractal gold nanoparticles and Ag-coated Fe3O4 nanoparticles (Fe3O4@Ag) – see Figure 22. Wu et al. used three different DNA-engineered fractal gold nanoparticles containing three different Raman reporters: rhodamine 6G, crystal violet, and 4-aminothiophenol. Each type of gold nanoparticle containing a different type of a Raman reporter was modified with a different type of capture ssDNA, complementary to a part of the chain of three target miRNA (miRNA-122, miRNA-223, and miRNA-21). The Fe3O4@Ag nanoparticles were modified with three different ssDNAs complementary to three other fragments of the target miRNA chains – in this way, in one the multiplexed capture Fe3O4@Ag nanoparticle, three different capture ssDNA fragments were formed – see Figure 22 [73].
![Figure 22:
Schematic illustration of a magnetically assisted SERS-based biosensor for multiplex detection of three miRNA biomarkers: miRNA-122, miRNA-223, and miRNA-21. (a) Schematic processes of synthesizing rhodamine 6G, crystal violet and 4-aminothiophenol encoded fractal Au nanoparticles, used as SERS tags. (b) Design and synthesis of the capture magnetic Fe3O4@Ag substrate. (c) Procedure for detecting the multiple miRNAs, based on linking magnetic and plasmonic nanoparticles. Reprinted with permission from ref. [73]. Copyright 2021 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_022.jpg)
Schematic illustration of a magnetically assisted SERS-based biosensor for multiplex detection of three miRNA biomarkers: miRNA-122, miRNA-223, and miRNA-21. (a) Schematic processes of synthesizing rhodamine 6G, crystal violet and 4-aminothiophenol encoded fractal Au nanoparticles, used as SERS tags. (b) Design and synthesis of the capture magnetic Fe3O4@Ag substrate. (c) Procedure for detecting the multiple miRNAs, based on linking magnetic and plasmonic nanoparticles. Reprinted with permission from ref. [73]. Copyright 2021 American Chemical Society.
The miRNA detection using the sensor developed by Wu et al. was performed in the following steps – see Figure 22 [73]. Firstly, Fe3O4@Ag nanoparticles functionalised with three different capture ssDNAs were cultured with a complex sample that contained the target miRNAs, irrelevant miRNAs, and other interferences. During this stage, the target miRNAs were specifically bound to capture ssDNA-modified Fe3O4@Ag nanoparticles due to the hybridization combination. Subsequently, the Fe3O4@Ag nanoparticles with attached target miRNA were magnetically separated from the complex sample. Next, three different fractal gold nanoparticles incorporating three different Raman reporters corresponding to different target miRNAs were added, and after subsequent hybridization, the modified Au nanoparticles were attached to the modified Fe3O4@Ag nanoparticles. Finally, after another magnetic separation, the SERS signal of the resulting agglomerates was measured. The limits of detection of these three miRNAs in human serum were 349 aM for miRNA-122, 374 aM for miRNA-223, and 311 aM for miRNA-21 [73].
Magnetic separation has been also applied in many other SERS sensors designed to detect nucleic acids. To detect, for example: (i) miRNA-122, with a wide linear range of from 10 aM to 10 pM and a low detection limit of 6.82 aM [74]; (ii) microRNA-155 (which regulates a variety of biological processes, including promoting the miRNA inhibition of breast cancer invasion and metastasis), with a detection limit of 36.7 fM [75] or even 1.45 fM [76] and a wide linear range (100 fM–5 nM) [75], [76]; and (iii) circulating miRNAs (such as miRNA-499), with a detection limit of 0.37 fM and a linear range of between 1 fM and 10 nM [77].
A similar SERS DNA sensor for detecting the ssDNA associated with the BRAF V600E mutation was constructed from gold-coated magnetic nanoparticles with attached 6-mercaptopyridine-3-carboxylic acid (MPCA) as an internal reference and silver nanoparticles with an attached Raman reporter (4-mercaptobenzonic acid, 4-MBA) [78]. The gold-coated magnetic nanoparticles were modified with ssDNA complementary to one part of the target ssDNA, whereas the silver nanoparticles were functionalised with ssDNA complementary to another part of the target ssDNA. The main difference between this sensor and the standard one described above was the addition of a ligase enzyme (DNA ligase can join together two fragments of nucleic acids by forming phosphodiester bonds) (see Figure 23) [78]. In the presence of the proper BRAF mutation DNA, the ligase enzyme induced the formation of a respective chemical bond, and these two nanoparticles are covalently linked, which brought the silver nanoparticle close to the surface of the magnetic particle (see Figure 23). Due to the aggregation of nanoparticles, the intensity ratio of the 4-MBA/MPCA increased linearly in the 1–100 fmol range of the matched DNA (BRAF gene with V600E mutation). Different ratios of matched DNA in the background of a large number of the single-base mismatched DNA (BRAF normal) were used to mimic real samples, and the intensity ratios of the 4-MBA/MPCA were linear in the 0.02–1 % range of the matched DNA/mismatched DNA [78].
![Figure 23:
Schematic graph showing the process of hybridisation of DNA in a SERS DNA sensor with two different Raman reporters. The ligase enzyme leads to the formation of a chemical bond between the BRAF probes 1 and 2 chains in the presence of the target DNA. Reprinted with permission from ref. [78]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_023.jpg)
Schematic graph showing the process of hybridisation of DNA in a SERS DNA sensor with two different Raman reporters. The ligase enzyme leads to the formation of a chemical bond between the BRAF probes 1 and 2 chains in the presence of the target DNA. Reprinted with permission from ref. [78]. Copyright 2020 American Chemical Society.
5.3 Methods based on hybridisation-induced rearrangement of linking and protecting alkanethiol chains attached to SERS-active surfaces
In addition to the above approaches to DNA/RNA detection using SERS spectroscopy, whose principals were developed over a decade ago and are currently only being further developed, in 2019 Kowalczyk et al. proposed a completely new approach to DNA detection based on SERS measurements [79]. When determining the structure of various layers formed on SERS-active metals from capture ssDNA and 6-mercaptohexan-1-ol (such modified SERS substrates are often used in standard SERS DNA sensors), this group observed that hybridisation with target ssDNA complementary to the immobilised capture ssDNA induces a significant change in the conformation of chains of chemisorbed ω-substituted alkanetiols (6-mercaptohexan-1-ol and the alkanethiol linking moiety through which the capture ssDNA is attached to the metal surface) (see Figure 24) [79]. These structural changes can be easily determined from the respective SERS spectra, especially when there are no adenine moieties in a close proximity to the metal surface (see Figure 25) [79], and therefore, Kowalczyk et al. decided to attempt to detect circulating tumor DNA fragments characteristic for the BRAF mutation (c.1799T>A) using this type of SERS DNA sensor [79]. The detection was based on the conformation change of the chemisorbed ω-substituted alkanetiols (gauche → trans transformation) during the DNA hybridisation [79]. This SERS DNA sensor has been tested on clinical samples (from patients with melanoma or thyroid cancer who have the BRAF mutation, and from patients without the BRAF mutation). It was shown that this SERS DNA sensor is characterised by a low detection limit, at a level of pg μL−1, a wide analytical range from 6.75 pg μL−1 to 67.5 ng μL−1, and high selectivity [79]. It should be emphasized, however, that these analyses were not carried out using directly tissues obtained from oncological patients during standard therapies, but DNA isolated from such tissues using respective DNA purification kits. Further experiments (using only DNA samples obtained from commercial suppliers) showed that SERS-active silver substrates are significantly more promising for the SERS observation of such hybridisation-induced rearrangements than the gold substrates originally used [80].
![Figure 24:
Scheme of the rearrangement of chemisorbed 6-mercaptohexan-1-ol and an alkanethiolate linking moiety via which the capture ssDNA is attached to the SERS-active surface due to DNA hybridisation. Reprinted from ref. [80]. CC BY-NC-ND license.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_024.jpg)
Scheme of the rearrangement of chemisorbed 6-mercaptohexan-1-ol and an alkanethiolate linking moiety via which the capture ssDNA is attached to the SERS-active surface due to DNA hybridisation. Reprinted from ref. [80]. CC BY-NC-ND license.
![Figure 25:
Detection of ssDNA based on DNA hybridisation-induced rearrangement of linking and protecting alkanethiol chains. (A) Scheme of a SERS sensor based on spectral changes of the linking layer and 6-mercaptohexan-1-ol (marked as MCH in the drawing) induced by DNA hybridisation. (B) Possible structures of Au–S–C–C chain: trans (T) conformation and gauche (G) conformation. Reprinted with permission from ref. [79]. Copyright 2019 Elsevier.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_025.jpg)
Detection of ssDNA based on DNA hybridisation-induced rearrangement of linking and protecting alkanethiol chains. (A) Scheme of a SERS sensor based on spectral changes of the linking layer and 6-mercaptohexan-1-ol (marked as MCH in the drawing) induced by DNA hybridisation. (B) Possible structures of Au–S–C–C chain: trans (T) conformation and gauche (G) conformation. Reprinted with permission from ref. [79]. Copyright 2019 Elsevier.
The DNA identification based on DNA hybridization-induced rearrangement described above and some other SERS measurements described in the previous parts of this work were performed on nanostructured plasmonic surfaces (either nanostructured surfaces of plasmonic metals or nanostructured surfaces of other materials coated with a layer of a plasmonic metal) – example SEM image of a surface of such SERS substrate is shown in Figure 26. As already shown for this type of SERS substrates, the dominant part of the SERS signal comes from molecules adsorbed on SERS hot spots [81], [82]. However, if very large molecules are adsorbed, they are not able to occupy all SERS hot spots – the larger the molecule is adsorbed, the smaller the ratio of SERS hot spots is occupied [83]. This effect will undoubtedly make the study of very long chains of nucleic acid very difficult.
![Figure 26:
SEM image of a hetero-epitaxial GaN layer after photoetching and subsequent sputtering of silver – an example SERS substrate used for DNA hybridisation-induced rearrangement SERS measurements. Reprinted from ref. [80]. CC BY-NC-ND license.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_026.jpg)
SEM image of a hetero-epitaxial GaN layer after photoetching and subsequent sputtering of silver – an example SERS substrate used for DNA hybridisation-induced rearrangement SERS measurements. Reprinted from ref. [80]. CC BY-NC-ND license.
5.4 Methods utilising DNA hydrogels
Interesting materials that significantly change their properties in the presence of certain nucleic acids are DNA hydrogels. After the introduction of the proper target nucleic acid, the DNA hydrogel disintegrates, and then, for example, certain nanostructures are able to easily penetrate through it. Using this approach, Si et al. developed arrays of miRNA-responsive DNA hydrogel-based SERS sensors, for nine miRNA markers of various cancers: miR-21 (breast, pancreatic, lung, ovarian and liver cancers, and leukemia), miR-221 (pancreatic, liver and thyroid cancers, and glioblastoma), miR-224 (liver cancer), miR-205 (lung cancer), miR-155 (breast and pancreatic cancers, and leukemia), miR-141 (ovarian cancer), miR-25 (colon and ovarian cancers), miR-18 (liver cancer), and miR-183 (colon cancer) [84]. At first, in the layer of the plasmonic AuAg alloy nanoparticles immobilised at the surface of the sensor, streptavidin was attached. The layer of the AuAg nanoparticles with attached streptavidin was then protected with a thin layer of DNA hydrogel (see Figure 27). Next, the plasmonic nanoparticles (and in this case the AuAg alloy nanoparticles as well) modified with biotin and a Raman reporter (4-mercaptobenzonitrile) were deposited on the DNA hydrogel [84]. The plasmonic nanoparticles could not pass through the hydrogel and bound with the streptavidin-modified sensor surface, so at this stage only a very weak SERS signals was observed. After the introduction of the target miRNA, the DNA hydrogel was disintegrated so that the plasmonic nanoparticles modified with the Raman reporter were able to pass through the hydrogel and to be captured on the streptavidin-modified detection surface. This resulted in strong SERS signals and the detection of the target miRNA [84].
![Figure 27:
Schematic illustration of preparing and applying a target miRNA-responsive DNA hydrogel-based SERS sensor. The array formed makes it possible to measure multiple target miRNAs in one sample. Reprinted with permission from ref. [84]. Copyright 2020 American Chemical Society.](/document/doi/10.1515/nanoph-2024-0230/asset/graphic/j_nanoph-2024-0230_fig_027.jpg)
Schematic illustration of preparing and applying a target miRNA-responsive DNA hydrogel-based SERS sensor. The array formed makes it possible to measure multiple target miRNAs in one sample. Reprinted with permission from ref. [84]. Copyright 2020 American Chemical Society.
6 Conclusions and outlook
Due to the very high sensitivity of surface enhanced Raman scattering (SERS) measurements (it is possible to obtain a good quality SERS spectrum from even a single molecule), SERS spectroscopy is tested as a tool to analyse samples of nucleic acids without previous multiplication. If efficient SERS tests could be developed to detect DNA/RNA with a given sequence, SERS would find even wider application in medical diagnostics, environmental monitoring and forensic analysis, because the analysis time can be significantly shortened.
The sequence of a strand of nucleic acid can be determined by measuring the Raman map of the immobilised DNA/RNA strand with very high resolution (much higher than that obtained in optical microscopes). To obtain a Raman map useful for such an analysis, it is necessary to couple the Raman spectrometer with an AFM or STM microscope, to scan the surface under examination with a plasmonic nanoresonator, and then to measure the spectral distribution map (de facto SERS spectrum) at nanometer-scale resolution. However, this type of technique does not seem promising for the construction of DNA/RNA sensors of practical use. Another method involves amplification of target nucleic acids by PCR using specially designed primers (with an attached Raman reporter). The presence of a nucleic acid with a given sequence in the analysed sample causes the production of a large number of dye-labelled nucleic acid molecules as a result of the PCR process, and thus the observation of strong Raman reporter bands in the SERS spectrum of the PCR products.
Much more promising would seem to be sensors in which the spectral SERS changes caused by the selective hybridisation of target nucleic acid with an appropriately prepared capture nucleic acid (leading, for example, to Raman reporters becoming attached to the SERS-active surface or leading to an agglomeration of plasmonic nanostructures and the appearance of strong plasmon coupling). These types of sensors have counterparts based on the measurement of the fluorescence signal. Typically, SERS has comparable sensitivity to fluorescence, but in some cases the sensitivity of the DNA detection using SERS can be up to 100 times higher than that of conventional fluorescence-based methods. Moreover, SERS has a unique advantage that the recorded spectrum consists of sharp, molecular-specific vibrational bands, whereas fluorescence generates much broader bands. Therefore, in the SERS experiments it is much easier to eliminate band overlapping and to detect a larger number of the target DNA/RNA chains in one measurement. Raman reporters are also generally more resistant to photobleaching during Raman measurements than fluorophores during fluorescence measurements.
Using the SERS techniques developed so far, which involve selective hybridization of the target nucleic acid with an appropriately prepared capture nucleic acid, only relatively short fragments of nucleic acids were detected (to our knowledge, the longest DNA/RNA fragments analysed by SERS spectroscopy are from a dozen to several dozen nucleotides in length). Studying nucleic acid fragments of much longer length using currently used SERS techniques would generate additional problems. In the case of techniques based on DNA hybridization-induced formation of aggregates of plasmonic nanostructures with nucleic acids located in the created gaps, a significant increase in the thickness of the nucleic acid layer forming a “link” between the plasmonic nanoparticles would result in a significant increase in the width of the created gaps and, consequently, a significant decrease in the generated SERS enhancement factor. When nanostructured plasmonic surfaces are used as SERS substrates, the larger the adsorbed molecule, the smaller the number of SERS hot spots that can be occupied by this molecule, and consequently, the measured SERS signal is weakened.
Although sensitive and selective sensors for the simultaneous detection of even several strands of different nucleic acids have already been developed, many elements of SERS DNA and RNA sensors can still be significantly improved. A lot of effort is being put into obtaining materials that generate higher SERS enhancement factors and are more chemically resistant. A compromise must be found between a material’s activity in SERS spectroscopy and its stability during storage and measurements (for example, nanostructured silver generally generates higher SERS enhancement factors than nanostructured gold, but is much less stable chemically). It is also important to have ready-to-use SERS sensors which can be stored for a long time, or which at least can be made quickly from components that can be stored for a long time (even at a significantly lower temperature). Ideal SERS substrates should also be homogeneous and can be easily produced in a reproducible manner. Since the production of appropriate substrates for SERS measurements is a very complex problem and its description would require the preparation of an extensive review, these issues are not discussed in this work, and the interested reader is referred to the relevant review articles: [85], [86], [87].
A very interesting problem is the construction of sensors for which the analytical signals are collected in various ways; for example, by means of SERS and surface plasmon resonance (SPR) measurements or by SERS and fluorescence measurements. When different techniques (e.g. SERS and SPR) provide the most “linear responses” in different ranges of the analyte concentration, such a sensor can be used over a very wide concentration range. Additionally, the analytical signal obtained from two different sources increases the reliability of the results. It is also important to further increase the number of DNA/RNA sequences that can be simultaneously detected by a SERS DNA/RNA sensor.
Ongoing innovations and interdisciplinary collaborations in the field of SERS-based nucleic acid detection and determination offer exciting opportunities to address significant challenges in healthcare, biotechnology and environmental science. In the future, further developments of SERS technology can be expected, including the development of novel plasmonic nanomaterials with optimised properties, and portable, inexpensive Raman spectrometers for SERS measurements. Thus, the SERS technique holds great promise in terms of revolutionising the detection and analysis of nucleic acids.
Funding source: Narodowe Centrum Nauki
Award Identifier / Grant number: 2019/35/B/ST4/02752
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Research funding: This work was financed by the National Science Centre, Poland, project No. 2019/35/B/ST4/02752.
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Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.
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Conflict of interest: Authors state no conflicts of interest.
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Informed consent: Informed consent was obtained from all individuals included in this study.
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Ethical approval: The conducted research is not related to either human or animals use.
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Data availability: Data sharing is not applicable to this article as no datasets were generated or analyzed during the current study.
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© 2024 the author(s), published by De Gruyter, Berlin/Boston
This work is licensed under the Creative Commons Attribution 4.0 International License.
Articles in the same Issue
- Frontmatter
- Editorial
- Current trends in nanophotonics
- Review
- Applications of surface enhanced Raman scattering (SERS) spectroscopy for detection of nucleic acids
- Research Articles
- Design of optical Kerr effect in multilayer hyperbolic metamaterials
- A tiny Drude scatterer can accurately model a coherent emitter in nanophotonics
- Strong coupling spontaneous emission interference near a graphene nanodisk
- Long-range molecular energy transfer mediated by strong coupling to plasmonic topological edge states
- Thermal radiation forces on planar structures with asymmetric optical response
- Molecular surface coverage standards by reference-free GIXRF supporting SERS and SEIRA substrate benchmarking
- Effect of magnesium doping on NiO hole injection layer in quantum dot light-emitting diodes
- Anomalous reflection for highly efficient subwavelength light concentration and extraction with photonic funnels
- Nanometric probing with a femtosecond, intra-cavity standing wave
- Considerations for electromagnetic simulations for a quantitative correlation of optical spectroscopy and electron tomography of plasmonic nanoparticles
- Free-electron coupling to surface polaritons mediated by small scatterers
Articles in the same Issue
- Frontmatter
- Editorial
- Current trends in nanophotonics
- Review
- Applications of surface enhanced Raman scattering (SERS) spectroscopy for detection of nucleic acids
- Research Articles
- Design of optical Kerr effect in multilayer hyperbolic metamaterials
- A tiny Drude scatterer can accurately model a coherent emitter in nanophotonics
- Strong coupling spontaneous emission interference near a graphene nanodisk
- Long-range molecular energy transfer mediated by strong coupling to plasmonic topological edge states
- Thermal radiation forces on planar structures with asymmetric optical response
- Molecular surface coverage standards by reference-free GIXRF supporting SERS and SEIRA substrate benchmarking
- Effect of magnesium doping on NiO hole injection layer in quantum dot light-emitting diodes
- Anomalous reflection for highly efficient subwavelength light concentration and extraction with photonic funnels
- Nanometric probing with a femtosecond, intra-cavity standing wave
- Considerations for electromagnetic simulations for a quantitative correlation of optical spectroscopy and electron tomography of plasmonic nanoparticles
- Free-electron coupling to surface polaritons mediated by small scatterers