An
A variety of surface plasmon resonance imaging
techniques have
been developed, which differ fundamentally in the optical configurations
used to generate images. These methods vary in how surface plasmons
are excited, how signals are collected, and how spatial information
is encoded. Scheme
summarizes the operating principles of the major SPR imaging modalities
and classifies them according to their underlying optical architectures.
The most common type is prism-coupled SPR imaging, where excited surface
plasmons propagate on a continuous metal film (Au/Ag/Al) in a Kretschmann
(prism) geometry, with reflected intensity imaged over a wide field. SPR microscopy or objective-coupled SPR, on
the other hand, uses a high-NA objective to couple light to surface
plasmons (often via the substrate side), allowing higher spatial resolution
than typical prism SPRi and more flexible imaging modes. Aside from SPRi and SPRM, there are a few other
methods that are linked to plasmonic imaging. For example, plasmonic
scattering microscopy (PSM) detects binding events by monitoring scattering
from nanostructures or surface-bound particles enhanced by near fields. Interferometric plasmonic imaging (iSPR or plasmonic
interferometry) combines a reference optical field with the SPR-modulated
field so that phase-sensitive changes (interference fringes) can be
measured, improving detectability of very small signals. Localized SPR (LSPR) imaging, a highly active
and broadly pursued research direction, uses nanoparticles or nanostructured
arrays (nanodiscs, nanoholes, nanotriangles) supporting localized
plasmons rather than propagating ones. SERS (surface-enhanced Raman scattering) imaging utilizes plasmonic
nanostructures to amplify Raman signals for chemical-fingerprint imaging.
,
Additionally, there have been reports for near-field plasmonic imaging
(NSOM-plasmonic, TERS), which uses a nanoscale probe (tip) to access
information beyond the diffraction limit of light, and waveguide-coupled plasmonic imaging, which excites
plasmons using gratings or integrated photonics (planar chips) and
images intensity/phase changes. Given
the space constraints of this review, we focus our discussion on the
SPR imaging modalities that are most commonly adopted and widely implemented.
Scheme
also illustrates
the optical configuration of a typical reflectance-based SPRi imaging
system in the Kretschmann geometry. In this system, monochromatic,
p-polarized light is employed to excite propagating surface plasmons
at the metal–dielectric interface, and imaging is performed
at a fixed incident angle selected near the plasmon resonance condition.
Binding-induced changes in the local refractive index are thus detected
as variations in reflected intensity across the sensor surface. Beyond the conventional fixed-angle, intensity-based
approach, several SPR imaging variants have been utilized that monitor
alternative resonance parameters including wavelength shifts and phase
changes associated with biomolecular interactions ( Table
).
Angle-resolved
SPR imaging enables the acquisition of reflectance images over a range
of incident angles during a single measurement. By systematically
scanning the excitation angle across the surface plasmon resonance
condition, the full angular reflectance profile can be reconstructed
for each pixel or region of interest. Since s-polarized light does not absorb, it is commonly used as
an internal reference to normalize the p-polarized response, allowing
reflectance changes to be expressed as a percentage of the maximum
reflected intensity. Imaging across multiple incident angles increases
the dimensionality of the data set and extends sensitivity to complex
surface properties, including variations in feature size, thickness,
and morphology. However, the resulting increase in data volume and
image complexity often necessitates advanced postprocessing and modeling
algorithms to accurately extract quantitative binding and structural
information.
Multiwavelength
SPR imaging varies the excitation wavelength while maintaining a fixed
incident angle. In contrast to single-wavelength,
intensity-based SPRi, multiwavelength SPRi enables visualization of
resonance shifts through full-color imaging, providing intuitive spectral
contrast across the sensor surface. By
sampling the SPR response over a range of wavelengths, this approach
offers an increased dynamic range relative to fixed-wavelength reflectivity
measurements. In practice, wavelength
interrogation may be performed either by continuously scanning across
a spectral range or by selectively monitoring multiple discrete wavelengths
within the SPR reflectivity curve. Recent dual-wavelength systems
exploit two approximately linear regions of the reflectivity spectrum,
tracking their intensity changes simultaneously. The differential intensities are computationally tracked
across regions of interest within an array, allowing faster sampling
by limiting acquisition to predefined wavelength windows rather than
the full spectrum. Multiwavelength SPRi can function either as a standalone
analytical technique or as a complementary tool for identifying optimal
operating conditions. Ongoing efforts
continue to improve wavelength interrogation strategies in SPRi systems,
and a recent study applied concepts derived from the Hadamard multiplexing
configuration to achieve a sensitivity of 3407 nm/RIU and a refractive
index resolution of 2.20 × 10 –6 RIU.
In addition to intensity-based
detection, SPR imaging in the Kretschmann configuration can be adapted
to monitor phase changes between the incident and reflected light, with modification of the detection scheme. The phase shift of the reflected p-polarized
light is measured relative to the incident light, and the resulting
interference signal provides a sensitive readout of resonance perturbations,
which can be directly related to shifts in the effective incident
angle. Phase-based SPRi generally offers
higher intrinsic resolution than conventional intensity-based SPRi,
owing to the steep phase response near the plasmon resonance. However,
its practical sensitivity can be limited by increased susceptibility
to background noise and environmental fluctuations, as the measured
phase variations often occur on very small scales. Incorporation of tunable optical filters has enabled phase
detection over a broader wavelength range ( Figure
). An alternative
strategy for phase interrogation involves indirectly extracting phase-like
information from the SPR reflectivity curve itself. In this “quasi-phase” approach, wavelength-resolved
SPRi data are analyzed using the derivative of the SPR curve, allowing
phase-related information to be inferred without direct interferometric
detection. This method differs fundamentally from traditional phase-resolved
SPRi and offers several advantages, including a more linear relationship
between the quasi-phase signal and refractive index unit (RIU) changes.
Despite these advances, phase interrogation in SPRi remains challenged
by a limited dynamic detection range and increased instrumental complexity
relative to intensity-based methods. A
recent effort with multichannel phase-sensitive SPR imaging platforms
allowed a dynamic detection range of 3.7 × 10 –3 RIU and limit of detection (LOD) of 14.02 ng/mL for secondary antibody
binding ( Figure
).
A multiwavelength, phase-shift SPRi measurement of antibody
binding.
(A) Determination of optimal wavelengths for achieving highest phase-shift
sensitivity. (B) Images of SPRi channels with colors representing
the phase shift after sample introduction. The dashed boxes represent
the wavelengths used for the enclosed channels with red, green, and
blue corresponding to 696, 702, and 686 nm, respectively. (C) Overlayed
real-time measurements (sensorgrams) from each channel. Reproduced
with permission from ref . Copyright 2023 Elsevier.
Surface
plasmon resonance microscopy encompasses a broad class of plasmonic
imaging techniques that employ a high-numerical aperture microscope
objective, rather than a prism, to achieve total internal reflection
and excite surface plasmons.
,
Depending on the optical
configuration and detection scheme, SPRM systems can achieve spatial
resolution and sensitivity that are generally superior to conventional
SPR imaging, particularly for nanoparticle-based and single-entity
analyses.
, −
Recent advances in SPRM
have focused on improvements in optical design and signal processing.
, , ,
Parallel, postacquisition image analysis approaches, assisted by
machine learning processing and Fourier-domain transformations, have
been introduced to improve contrast, suppress noise, and extract quantitative
information from complex SPRM data sets.
,
Several emerging instrumental innovations further highlight the
expanding scope of SPRM.
,
Total internal reflection-based
SPR microscopy (TIR-SPRM) has recently been demonstrated as a means
to improve spatial resolution by combining TIR excitation with Fourier-domain
reconstruction. Terahertz (THz) microscopy
has also been integrated with SPRM imaging principals to form a THz-SPRM
platform ( Figure
). In this system, plasmon excitation is achieved
in the Otto configuration ( Figure
A), rather than the Kretschmann geometry. This configuration
permits precise control over the coupling gap between the prism/objective
and the sample surface, offering improved image quality and partially
mitigating the spatial resolution limitations imposed by long-wavelength
THz excitation. It is interesting to note that although this platform
is described as an iteration of SPR microscopy, it retains features
characteristic of SPRi, such as prism-based excitation, while omitting
elements typically associated with SPRM, i.e., the use of a high-numerical-aperture
objective. The presence of attributes from both approaches underscores
that THz sensing principles can be adapted to configurations resembling
both SPRi and SPRM. The THz-SPRM system was validated by characterizing
the semiconducting and plasmonic properties of indium antimonide (InSb)
partially covered with polypropylene or graphene ( Figure
B,D), with reflectance measured
as a function of the objective-substrate gap distance ( Figure
C).
Optical configuration
and imaging data of an InSb terahertz SPRM
sensor. (A) Instrumental design for terahertz SPR microscopy in the
Otto configuration utilizing an InSb sensor chip. (B) Images of InSb
chip partially obscured by a 35 nm thin film of graphene at variable
distances of objective from substrate. (C) A graph of reflectance
vs distance from objective to substrate for 35 nm graphene thin film.
(D) Images of InSb chip partially obscured by a 20 μm film of
polypropylene at variable distances of objective from substrate. Reproduced
with permission from ref . Copyright 2023 MDPI.
Beyond the common plasmonic imaging methods like SPRi and SPRM, an
emerging suite of lesser-explored techniques has been growing, including
methods such as interferometric plasmonic microscopy, plasmonic scattering
microscopy, and waveguide-coupled SPR. These iterative techniques
build on the core principles of SPRi and SPRM, offering improvements
in sensitivity, resolution, and the ability to extract complementary
information that adds greater dimensionality to existing plasmonic
imaging approaches. These methods highlight promising innovations
with the potential to expand sensing capabilities into new regimes.
It is known that the reliance on reflected light in SPRM limits
achievable image contrast, and by extension, sensing resolution.
,
Further, analyte scattering patterns resulting from interference
between the analyte and the surface plasmon wave produces a visual
tailing effect, limiting resolution and analysis of heterogeneous
samples, especially in the absence of corrective models to compensate.
,
While the plasmonic scattering has typically been considered an
undesirable byproduct, it can serve as measurable optical signal that
forms the basis of more sensitive techniques such as interferometric
plasmonic imaging, plasmonic scattering microscopy, and near-field
plasmonic imaging. Interferometric plasmonic microscopy (iPM) utilizes
common-path interferometry, producing images from the interference
between reflected light and the near-field scattering interaction
of surface plasmons with surface nanostructures. Although the scattering produces relatively small intensity
variations, which are particularly difficult to elucidate among the
parabolic patterning in unprocessed images, recent advances in holographical
image reconstruction and convolutional neural network (CNN) processing
have aided in extracting high quality amplitude and phase information
from iPM images.
,
The ability of iPM to image individual
particles has been utilized to characterize gold nanostructure surfaces as well as the surface absorption, liposome
fusion, and antibody capture of exosomes. Image reconstruction drastically increased the working resolution
of iPM images, but the technique is still bottlenecked by the need
for standalone postprocessing procedure.
Plasmonic scattering
microscopy (PSM) utilizes the scattering interactions
between analytes and the surface plasmon wave by selectively monitoring
the out-of-plane interference patterns, which are detectable in the
far-field. By not relying on reflected
light, contrast is significantly improved, enabling higher brightness
and improved spatiotemporal resolution necessary for analyzing individual
surface structures and their binding events in heterogeneous samples.
Since PSM sensing can be achieved with an objective above the sensing
surface, it is technically compatible with both prism-coupled SPRi
and SPRM while retaining their respective sensing capabilities.
,
Recent work of PSM includes protein-antibody kinetic analysis, antibodies and small molecules binding to cellular
membranes, as well as exosome immobilization
and surface protein characterization for biomarker analysis. Further, the incorporation of an interferometric
phase parameter in PSM data processing yields material-specific parameters,
such as nanoparticles’ refractive index, which can enable nanoparticle differentiation in complex
samples. Therefore, interference-coupled
PSM could be a potential platform for drug delivery studies using
nanoparticles as recognition tags. It is worth noting that by relying
on scattered light instead of reflected light, PSM could be considered
an application of interferometric scattering microscopy (iSCAT) instead
of SPRi or SPRM. While scattering techniques such as iSCAT possess
enhanced imaging resolution relative to SPRi and SPRM due to not being
diffraction-limited,
,
they usually lack the sensitivity,
kinetic resolution, and multiplex capabilities of plasmonic imagining,
−
while PSM possesses both enhanced sensitivity and resolution relative
to standard SPRM again.
,
Plasmonic scattering
also opens the doors for further iterations of scattering-based analysis,
including methods like evanescent scattering microscopy (ESM), which
shows promise in alternative surface materials and greater compatibility
with fluorescent emission.
While
surface optimizations in film thickness tuning, materials, and
3D functionalization have improved the
sensitivity in SPR methods, novel approaches to the fundamental physical
design of the sensor can also offer sensitivity enhancements. Waveguide-coupled
SPR (WCSPR) utilizes a metal–dielectric-metal surface configuration
rather than the metal–dielectric configuration in conventional
SPR. This allows for the excitation of SPs at both the lower metal–dielectric
interface and the upper metal-waveguide layer, resulting in greater
sensitivity and sharper reflectivity curves compared to normal SPR. These principles also apply to waveguide-coupled
SPR imaging, which retains the strong sensitivity improvements and
high-throughput microarray compatibility while requiring minimal modifications
to existing SPRi hardware. While few
studies have implemented waveguides in SPR imaging, recent works have
demonstrated its biosensing capabilities by analyzing protein A-antibody
interactions, as well as single-cell
tracking of wheat-germ agglutinin ligand binding events on HeLa cells. The potential ease in incorporating waveguide-coupled
surfaces into existing SPRi hardware warrants further exploration
as a viable sensitivity enhancement method.
New
While an ideal SPR imaging or microscopic sensorgram
exhibits well-defined
phases of association, equilibrium, and dissociation, experimental
noise frequently obscures these features and complicates reliable
identification of binding events. Sources of noise, including bulk
refractive index shifts, nonspecific interactions, cross-reactivity,
and weak optical signals, are often intrinsic to the instrumentation
and become increasingly pronounced as sample matrices grow more complex.
Measurements performed in biologically relevant media such as patient
serum or urine are particularly challenging, as additional matrix
components introduce background fluctuations and confounding signals
that mask true surface-binding responses. Though incremental improvements
can be achieved through optimization of optical alignment, illumination
stability, and flow control, such hardware-based approaches alone
are often insufficient to fully resolve these issues. Consequently,
a growing array of computational and machine learning-assisted analysis
strategies has been introduced into SPR imaging and microscopy workflows
to enhance signal extraction, suppress noise, and enable more robust
interpretation of complex plasmonic data sets.
Common approaches for SPR
imaging data cleanup rely on mathematical
models that facilitate identification of the resonance angle or reduce
noise in sensorgram traces. Widely used strategies include fitting
reflectance curves with analytical functions such as sigmoid or asymmetric
models, which can be combined to more accurately locate the SPR minimum
in noisy data sets. As an alternative,
centroid-based algorithms estimate the resonance condition by comparing
pixel-wise reflectance values to a defined baseline, which may be
fixed or dynamically updated depending on the implementation. Polynomial fitting represents another commonly
employed strategy, in which averaged subsets of reflectance data are
used to generate simplified polynomial representations of the sensorgram.
,
This approach was demonstrated using Horner’s polynomial
fitting method to extract average reflectance values on a row-by-row
basis across an SPRi microarray, enabling reconstruction of smoothed
reflectance curves from subdivided spatial data. Such methods can accommodate the inherent asymmetry of
SPR dips, an important consideration given that conventional polynomial
fitting often performs poorly in regions immediately surrounding the
reflectance minimum. While centroid algorithms
and polynomial fitting substantially simplify SPR image analysis and
enable rapid extraction of resonance parameters, their capacity to
resolve highly complex or low-signal data sets is limited. More advanced
modeling approaches therefore offer improved fitting accuracy and
enhanced discrimination of weak or convoluted binding signals. In
addition, postprocessing strategies can be applied following data
acquisition, spanning from relatively simple mathematical treatments
for kinetic analysis to sophisticated
machine-learning-based frameworks designed to handle large, multidimensional
SPR imaging data sets.
SPRi data sets are often challenging
to analyze due to weak analyte responses superimposed on background
fluctuations arising from bulk refractive index shifts. Fitting such
complex data sets to analytical curves is further complicated by the
rapid growth in data volume, as the number of collected points increases
inversely with experiment runtime and proportionally with the computational
resources required for polynomial fitting. This challenge is worsened
in SPRi configurations that acquire multidimensional data such as
angle- or wavelength-resolved SPRi, where a full sensorgram may be
generated at each iteration of the scanned parameter, leading to rapid
data accumulation. One strategy to reduce data complexity involves
sampling a limited subset of wavelengths in multiwavelength SPRi experiments,
thereby simplifying analysis and reducing acquisition time. However, this approach is only effective when
the optimal wavelength range can be accurately predicted a priori.
Alternatively, it has been demonstrated that an initial, coarse polynomial
fit to spectral reflectance curves can be refined through postprocessing
to improve resonance peak identification and suppress background noise. This refinement employs independent longitudinal
and transverse scaling and translation parameters to iteratively correct
the initial polynomial approximation. By reducing the total number
of data points required for accurate curve reconstruction, the approach
introduced by Wang et al. enables shorter
acquisition times and increased experimental throughput. Notably,
this method was shown to enhance resolution in the vicinity of the
SPR dip, where conventional fitting routines typically exhibit the
greatest uncertainty.
Common statistical modeling approaches
have been successfully applied
to SPR imaging data to elucidate binding events and enable analyte
identification in complex media. Principal component analysis (PCA),
for example, has been used to differentiate SPRi responses arising
from antibody interactions with fluid-specific biomarkers in blood,
semen, saliva, urine, and sweat. Because
each biological fluid produced a distinct SPRi response pattern, PCA
clustering enabled correct identification of 62.5% of unknown samples
containing one of the five fluids. The unidentified samples were appropriately
labeled as inconclusive rather than being misidentified, demonstrating
the robustness of this approach. Partial least-squares-discriminant
analysis (PLS-DA) represents a complementary statistical approach
that can be targeted to specific regions of sensorgrams corresponding
to known binding events, enabling predictive identification of molecular
interactions. In studies of biomarker cross-reactivity associated
with multiple sclerosis (MS), PLS-DA analysis of sensorgrams collected
from three MS-related antibodies achieved improved differentiation
of ganglioside-antibody interactions compared to PCA alone. While effective at resolving subtle binding
differences, both PCA and PLS-DA remain limited in their ability to
compare across large or heterogeneous data sets, as they are typically
applied to individual experiments or narrowly defined data subsets.
More broadly, the performance of statistical models in SPR imaging
is constrained by the dimensionality of the input data. Excessive
data points can lead to overparameterization and increased computational
burden, whereas overly sparse data sets risk oversimplification and
loss of critical binding information. These trade-offs motivate the
growing integration of advanced computational and machine-learning
strategies to more effectively manage high-dimensional SPR imaging
data sets.
The integration of machine learning (ML) into SPR
imaging has emerged
as a powerful strategy for improving method development, system simulation,
and analyte discrimination in complex media. ML-based approaches have
been shown to enhance the differentiation of closely related targets
and biomarkers in data sets where conventional fitting or statistical
models struggle to resolve subtle signal features. Because surface
plasmon polaritons are well described by Fresnel-based electromagnetic
models, SPR system responses can be accurately simulated in silico.
,
These physics-based simulations provide high-quality training data
for deep learning models, which can subsequently be applied to experimental
SPR data sets to improve resonance identification and signal interpretation. In this framework, simulated reflectance curves
effectively serve as labeled ground truth, enabling supervised learning
without the need for extensive experimental calibration data sets.
It has been demonstrated that incorporating realistic noise profiles
into training simulations, by randomly introducing variations that
mimic experimental bulk shifts, baseline drift, and optical instability,
can significantly improve model robustness.
In addition to physics-based synthetic data sets, experimentally
acquired SPR imaging data can serve as valuable training inputs for
both supervised and unsupervised machine-learning algorithms. Machine
learning algorithms such as neural networks, k-nearest neighbor (k-NN),
support vector machines (SVM), and principal component analysis are
effective tools for analyzing the large data sets generated by arrayed
and multiplexed SPR imaging platforms.
,
In addition
to downstream image analysis, advanced models can be applied during
image preprocessing to improve data quality, reproducibility, and
robustness. Convolutional neural networks,
including architectures such as U-Net image transformation models
and generative adversarial networks (GAN) for signal recovery from
noisy or suboptimal data, offer computational approaches that in certain
cases can reduce or replace the need for dedicated optical or electronic
hardware.
By incorporating features derived from association,
steady-state,
and dissociation regimes of analyte–surface interactions, ML
models can be trained to predict and differentiate binding behaviors
with high specificity ( Figure
). Beyond temporal sensorgram
features, spatial analysis of signal homogeneity and relative feature
positioning across SPRi arrays provides additional insight into analyte
binding dynamics. This approach has been demonstrated using both convolutional
neural networks (CNNs) and k-NN classifiers, which showed marked improvements
in distinguishing closely related analytes compared to conventional
statistical methods. Additionally, matrix components can be explicitly
incorporated into the training process, enabling ML models to differentiate
true binding events from bulk refractive index shifts and nonspecific
background responses ( Figure
). In neural-network implementations, raw sensorgram data
can be introduced at the input layer, while weighted statistical descriptors
are incorporated into hidden layers to establish relative relationships
among data points. These architectures enable computation of performance
metrics, including accuracy, precision, sensitivity, and specificity,
associated with identified resonance features. In addition, some models
generate self-evaluating error metrics (e.g., false-negative indicators,
FN), allowing bidirectional or iterative architectures to flag uncertain
classifications and trigger additional processing steps when needed. A notable advantage of neural-network-based
approaches is their adaptability: models can be incrementally retrained
as new experimental data sets become available, facilitating continuous
performance improvement and enabling seamless redeployment in future
SPRi experiments without complete model reconstruction.
Schematic representation
and resulting data of machine learning-assisted
multiple sclerosis detection using fixed-angle SPR imaging. (A) Graphical
representation of autoimmune attack in MS, involving antibodies targeting
gangliosides located in the myelin sheath. (B) Schematic of the utilized
SPRi methodology for this work, with different gangliosides captured
on microarray spots followed by interaction with their respective
antibodies. (C) 3D bar plot showing the response of 25 ng/mL of each
antibody in serum over each ganglioside-functionalized surface, illustrating
a lack of strong specificity for the interactions. (D) PCA analysis
is able to reliably determine antibody identity based on response
across the entire ganglioside array. (E) Including concentrations
below 25 ng/mL negatively affects identification and more advanced
statistical methods (machine learning) is needed. (F) Nnet of 10 ng/mL
anti-GT 1b over the three ganglioside surfaces (top) showing
model predicted ganglioside based on response at different time points.
A confusion matrix (bottom) shows the ability of the model to accurately
classify the interactions occurring. (G) kNN generated using the same
data as the neural net of 10 ng/mL anti-GT 1b . This model
worked well during steady state and after dissociation, achieving
96% accuracy at classification. Reproduced with permission from ref . Copyright 2022 Elsevier.
An example
of applying neural network machine learning
to biosensor
development can be best seen in an inflammation sensor developed during
the 2019 SARS-CoV2-Pandemic. A 6 ×
8 SPRi array with 6 repeats each was used to produce 288 sensorgrams
in 100 min of antibody capture for six cytokines in blood serum (see Table
). To increase data
processing throughput and accuracy, a neural network was utilized
to distinguish binding events from background noise. The data was
preprocessed using dark-field image processing to reduce nose and
enhance contrast, then a CNN model using 6 layers of downsampling
and 5 layers of upsampling was utilized to quantify binding signals.
Standards of each cytokine were individually spiked into serum and
calibration curves were obtained and utilized to determine levels
of each cytokine in 40 patients with COVID-19 to determine which patients
were at risk of dangerous immune responses. Besides disease applications,
Thadson et al. demonstrated the capabilities of CNN ML to build a
phase retrieval algorithm capable of extracting phase and reflectivity
information directly from single-shot SPRM images, aiming to replace
dedicated SPRM hardware interferometers ( Figure
). Their
model utilized a context aggregation network (CAN) trained on Fresnel
simulations, which incorporated reflection and transmission coefficients,
gold thickness, as well as sample and substrate refractive index to
extract phase and reflectivity profiles from SPRM back focal plane
(BFP) images. Additionally, the model could simulate and account for
simpler sources of shot noise to reduce artifacts. This deep learning
model showed marked agreement of both the extracted phase and reflectivity
profiles between simulated and experimental images ( Figure
), yielding a 3.5× lower
LOD compared to simpler polynomial fitting methods.
Deep learning
phase extraction from single-shot SPRM images. (A)
Schematic representation of the CAN network, which used BFP images
as inputs to extract phase and intensity profile images. A single-shot
BFP SPRM image (B) can then be processed in the network, producing
an extracted phase profile image (C). The model was trained on simulations
derived from Fresnel equations of a 46 nm gold surface, which produced
both simulated BFP intensity (D) and phase training images (E). To
show agreement between the simulated and extracted intensities, an
extracted BFP intensity line scan is overlaid with the Fresnel-calculated
intensity profile (F). Similarly, the extracted phase profiles can
be overlaid with the Fresnel simulation phase profile (G). Reproduced
with permissions from ref . Copyright 2021 Springer Nature.
Deep learning processing has also been employed
to fill the role
of dedicated SPRM autofocusing equipment. Focusing tools are beneficial
for SPRM reproducibility because image-to-images variations in focusing
and long-term drift can produce shifts between single-tailed and double-tailed
scattering artifacts. While these can be supplemented with dedicated
focusing hardware or processing of individual images,
,
adaptable virtual refocusing tools provide an alternative that lowers
cost while adding versatility for focus across longer experiments.
Xu at al. utilized convolutional neutral networks and U-net processing
to computationally reconstruct unfocused SPRM images into more consistent,
focused images. Built upon the principles
of common path holography, their model
was trained on nanoparticle images at a variety of focal lengths and
was split into two submodels. The model’s generator component
extracted feature maps from input images and produced focused output
images, while the discriminator component’s convolutional networks
scored processed images to determine if further focusing was necessary.
The approach points to a potential future where deep learning models
can serve as powerful replacements for SPRM accessory hardware.
Beyond enhancing data analysis of
biological interactions, computational modeling plays a critical role
in the rational design and optimization of SPR imaging experimental
platforms. As noted previously, such computational-first design strategies
have been shown to accurately predict angular shifts associated with
common sensing media and reagents, including water, ethanol, polydimethylsiloxane
(PDMS), and phosphate-buffered saline (PBS). Fresnel equation simulations have also facilitated the exploration
of alternative plasmonic materials, most notably aluminum, which offers
distinct optical properties compared to traditional gold or silver
substrates. In addition, these simulations
enable systematic evaluation of surface-layer thicknesses, oxide compositions,
and multilayer architectures, supporting both the development of novel
sensor chips and the fine-tuning of established surface designs. By extending computational modeling to the design
of SPRi arrays incorporating nontraditional metals or engineered surface
architectures, it becomes possible to introduce new surface functionalities
and expand the accessible parameter space of plasmonic imaging. This
capability opens avenues for investigating biological and chemical
systems that are difficult or impossible to probe using standard gold-
or silver-based SPRi substrates.
Computational acceleration
of post-data-acquisition analysis can further enhance the development
of novel SPR imaging platforms by guiding selection of optimal experimental
parameters, such as illumination wavelength or incident angle, for
future measurements. This capability has been demonstrated using machine-learning
approaches that track reflectance minima across multiple wavelengths, enabling efficient identification of incident
wavelengths that are most informative for subsequent fixed-wavelength
experiments. Similarly, local similarity algorithms have been employed
to determine optimal operating angles for specific SPRi platforms,
allowing future experiments to be conducted under constant-angle conditions. Additional computational strategies have been
developed to rapidly process angle-scanning SPRi images and identify
optimal resonance angles for specialized surfaces. For example, Lee
et al. reported an angle-scanning SPRi approach enhanced through contrast-limited
adaptive histogram equalization (CLAHE) to improve sensitivity toward
low-molecular-weight analytes. In that
study, the method was validated by detecting gaseous acetone in nitrogen
at concentrations ranging from 1.0 to 10.2 ppm using SiO 2 /Au thin films functionalized with chloride, methyl, amine, or hydroxyl
groups. While presented as a proof of concept, this approach demonstrates
promise for multiplexed SPRi analysis of small-molecule analytes with
accelerated angle sampling. Across the full SPRi workflow, from computationally
guided experimental design and surface engineering to high-throughput
data acquisition and postprocessing of complex imaging data sets,
computational tools play an increasingly central role. The integration
of machine-learning and advanced data-processing algorithms has proven
particularly effective in managing large data sets, improving experimental
efficiency, and elucidating binding events obscured by noise, especially
in complex biological or chemical matrices.
Plasmonic
Surface plasmon resonance methodologies enable
quantification of
analytes at nanomolar to picomolar concentrations, owing to their
exceptional sensitivity to changes in surface refractive index. When
implemented in imaging formats, multiwell or array-based plasmonic
chips further enable multiplexed and high-throughput analysis of multiple
targets and samples in parallel. These capabilities naturally position
plasmonic imaging techniques as powerful platforms for biosensor development.
Hence, a growing body of literature has reported the application of
SPR imaging to disease biomarker detection, with representative examples
summarized in Table
. Recent studies have focused particularly on biomarkers associated
with oncological conditions, autoimmune disorders, inflammatory responses,
and infectious diseases, highlighting the broad clinical relevance
and analytical versatility of plasmonic imaging-based biosensing approaches.
Cancer diagnostics
and therapeutics have remained a major focus of biomedical research
through 2025. Analytes investigated using SPR imaging techniques span
a broad range of oncological biomarkers, including growth factors, apoptosis-related protein, and cancer-derived extracellular vesicles. One notable study examined the detection of cells overexpressing
human epidermal growth factor receptor 2 (HER2) using an SPRi-based
biosensor. In this work, nanobodies
were employed as capture ligands on an SPRi array chip, and a suspension
of cancer cells was flowed directly over the sensor surface. Cells
exhibiting HER2 overexpression were detected with a limit of detection
of ∼1 × 10 5 cells/mL. This approach is particularly
promising, as it enables rapid identification of HER2-positive cells
directly from dilute cell suspensions, requiring smaller sample volumes
and offering faster analysis compared to conventional techniques such
as flow cytometry. Neuropilin-1 detection using SPRi has also been
demonstrated through immobilization of mouse monoclonal antibodies
on a sputtered gold sensor chip. This
platform achieved high analytical sensitivity, with a limit of quantification
of 0.038 ng/mL and a linear response over the concentration range
of 0.01–25 ng/mL.
Other related work has focused on quantifying
soluble programmed death-ligand 1 (sPD-L1) in human serum using SPRi. In this approach, a DNA aptamer was hybridized
to the gold sensor surface to serve as the capture ligand, rather
than a nanobody or antibody. Signal amplification was achieved by
introducing anti-sPD-L1 antibodies conjugated to gold nanoparticles,
resulting in a significantly enhanced plasmonic response. Using this
strategy, picomolar sensitivity was obtained, with a linear detection
range of 50 pM-10 nM without signal enhancement and 100 fM-50 pM with
nanoparticle enhancement, corresponding to a minimum detection limit
of 19 fM. Recent improvements utilizing nanoparticle enhanced nucleic
acid detection have produced limits of detection as low as 0.5 attomolar.
Additional oncological and metastasis-associated
biomarkers have
likewise been quantified in complex biological matrices using SPRi.
Fibroblast growth factor 23 (FGF23), a biomarker associated with bone
carcinogenesis and metastasis, was measured directly in blood plasma,
yielding a linear working range of 1–75 pg/mL, a lower limit
of detection of 0.033 pg/mL, and a limit of quantification of 0.107
pg/mL. In related work, SPRi was employed
to evaluate candidate imaging peptides for multiple myeloma by characterizing
their binding interactions with CD38, identifying two promising probes
with K
D values of 7.4 × 10 –7 M and 8.9 × 10 –7 M. Beyond cancer-specific biomarkers, a recent study investigated poly(ADP-ribose)
polymerase-1 (PARP-1), a potential marker for pathologically altered
endometriosis, using SPRi in comparison with an enzyme-linked immunosorbent
assay (ELISA) for analysis of blood serum samples. The SPRi sensor exhibited a linear detection range of 10–1000
pg/mL and recoveries between 95% and 105%. Taken together, these studies
underscore the continued maturation of SPRi methodologies, particularly
their expanding capability to operate reliably in complex media such
as blood plasma and serum, an area that has historically posed significant
challenges for SPR imaging.
Additional efforts have focused
on oncological biomarkers for which
effective capture reagents are not yet commercially available. One
such example is ETV1, a transcription factor commonly associated with
prostate cancer when overexpressed, for which no suitable monoclonal
antibody currently exists. To address
this limitation, researchers generated and cultured polyclonal rabbit
antibodies and evaluated their binding performance using both ELISA
and SPRi. Antibody development was largely successful, yielding high-affinity
interactions with a measured K
D of 479
pM, demonstrating the feasibility of SPRi as a platform for validating
newly developed capture agents for previously inaccessible oncological
targets.
Similar oncological developments have been seen in
prostate cancer
diagnostics where multiplexed SPRi has been investigated to improve
throughput and selectivity of screening. In a recent example, traditional
testing for prostate cancer using prostate specific antigen (PSA)
was augmented with multiplex SPRi detection by simultaneously detecting
PSA with three other antigens to create an assay resistant to false
positives from benign prostatic hyperplasia and prostatitis ( Figure
). The biosensor utilized a home-built SPRi system with a
3D-printed microfluidic flowcell to simultaneously detect the four
nanoparticle-conjugated analytes, PSA, insulin-like growth factor
1 (IFG-1), vascular endothelial growth factor D (VEGF-D), and cluster
of differentiation 14 (CD14), in a single sample injection with pg/mL
sensitivity for each analyte ( Figure
, also Table
). Magnetic nanoparticles utilization allowed for sensitivity
100-fold greater than traditional ELISA and enabled removal of analytes
from native media to prevent interference from complex matrix conditions.
While patient samples were not tested, previous work by the authors
utilizing a similar immunoassay showed 84.7% accuracy in discriminating
cancer samples from benign controls with the SPRi samples showing
improved sensitivity and throughput.
SPRi
assay for sensitive and high-throughput cancer diagnostics.
(left) Graphical depiction of the SPRi setup and assay. Antigens (Ag)
are preincubated with biotinylated antibodies (AB 2 ) bound
to streptavidin coated 1 μm diameter superparamagnetic particles
(MBs). The MG-AB 2 -Ag samples are then captured using antibodies
for the antigen (AB 1 ) covalently immobilized on the sensor
chip. (right) SPRi signals for three analytes, CD14, IGF-1, and VEGFD,
contrasted to a BSA control. Each spot represents a different concentration
of the injected protein. Reproduced with permission from ref . Copyright 2025 Elsevier.
Another oncologically relevant analyte is vascular
endothelial
growth factor receptor 2 (VEGF-R2), which plays a central role in
angiogenesis and metastasis. One research group developed two SPRi
biosensor platforms for VEGF-R2 detection in plasma by immobilizing
monoclonal rabbit antibodies via cysteamine linkers onto either a
pure gold sensor surface or a silver/gold bimetallic chip. The gold sensor exhibited superior analytical
performance, achieving a precision of 1.4% and a broader linear detection
range (0.03–2 ng/mL), compared to the silver/gold bimetallic
chip, which showed a precision of 2.2% and a linear range of 0.03–1
ng/mL. The binding parameters were further characterized using both
SPRi and quartz crystal microbalance (QCM), yielding K
D values of 2.05 × 10 –12 M and
2.10 × 10 –12 M, respectively, highlighting
strong agreement between the two techniques. Building on this work,
the same group applied similar SPRi strategies in plasma and peritoneal
fluid to evaluate proteasome and immunoproteasome levels as potential
diagnostic markers for endometriosis and to assess anti-CDH12 monoclonal antibodies for Cadherin-12 biosensing. While proteasome-based markers did not show
a statistically significant correlation with endometriosis, the Cadherin-12
sensor exhibited exceptional sensitivity and diagnostic promise, with
a reported K
D of 7.52 × 10 –9 M, a limit of detection of 1.49 pg/mL, and a linear working range
of 1–80 pg/mL.
The inherent
multiplexing capability of SPR imaging makes it a powerful platform
for categorizing antibody–antigen interactions in autoimmune
disease research. Multiple sclerosis (MS), a neurodegenerative autoimmune
disorder, arises from aberrant immune responses against components
of the central nervous system, most notably the myelin sheath surrounding
neurons. Of particular interest are antibodies secreted by B cells
that erroneously recognize neuronal membrane constituents, especially
gangliosides. These antiganglioside antibodies have been correlated
with specific MS symptoms, positioning them as promising disease biomarkers.
However, their clinical utility has been limited by their low abundance
in blood and the analytical challenges associated with detecting such
targets in complex biological matrices. Malinick et al. introduced
a fixed-angle SPR imaging methodology designed to quantitatively probe
interactions between gangliosides immobilized on a nearly superhydrophobic
sensor surface and MS-associated antibodies spiked into human serum. This approach enabled sensitive, multiplexed
analysis of ganglioside-antibody binding and represented a significant
advance in both biosensor development and mechanistic understanding
of neurodegenerative immune processes ( Figure
). The ganglioside
self-assembled monolayer (SAM) employed in this work exhibited strong
antifouling behavior, attributable to its near-superhydrophobic character,
which facilitated reliable detection of MS-specific antibodies in
10% human serum. To further address the complexity of serum-based
measurements, the same research team subsequently integrated SPRi
with machine-learning-assisted analysis, combining k-nearest neighbor
classification and neural networks to differentiate binding interactions
between multiple ganglioside species and individual antibodies. This SPRi-ML framework enabled quantitative
discrimination across a working concentration range of 1–100
ng/L and achieved low limits of detection of 6.6 ng/mL for anti-GA1,
5.6 ng/mL for anti-GM1, and 4.5 ng/mL for anti-GT1b in whole human
serum. Notably, these detection limits fall well within the clinically
relevant concentration range for MS-associated antibodies (3–25
ng/mL), underscoring the potential of SPRi-based, data-driven platforms
to interrogate the molecular underpinnings of autoimmune neurodegeneration
with diagnostic relevance.
Additional SPRi-based studies have
focused on biomarker panels for the diagnosis of relapsing-remitting
multiple sclerosis (RRMS). In one such investigation, SPRi was employed
to quantify ubiquitin carboxyl-terminal hydrolase L1 (UCHL1), leptin,
and fibronectin directly in serum collected from 100 RRMS patients
and 46 healthy controls. Among the three
analytes, UCHL1 demonstrated the strongest diagnostic performance,
achieving a negative predictive value of 100%, compared to 43% for
leptin and 92% for fibronectin. Despite its superior diagnostic specificity,
UCHL1 exhibited a relatively narrow linear dynamic range, with linearity
observed only between 0.5 and 3.0 ng/mL. In contrast, leptin and fibronectin
displayed broader linear ranges of 0.1–10 ng/mL and 5–400
ng/mL, respectively. These results highlight a common trade-off between
diagnostic specificity and analytical dynamic range in biomarker development.
Importantly, the multiplexed and high-throughput nature of SPRi biosensor
platforms enables the simultaneous monitoring of multiple biomarkers,
suggesting that combined analysis of UCHL1, leptin, and fibronectin
may provide a more robust and clinically informative strategy for
RRMS diagnosis than any single marker alone.
Fibronectin has
also been investigated as a serum biomarker for
bladder cancer using SPRi by an independent research group. In this
study, patients with transitional cell carcinoma (TCC) of the bladder
exhibited elevated serum levels of laminin-5, fibronectin, and collagen
IV relative to healthy control populations. While all three extracellular matrix proteins demonstrated strong
diagnostic sensitivity (98–100%), their specificity varied
considerably, ranging from 92% down to 62%. These findings highlight
both the promise and the limitations of early SPRi-based biosensors
operating in complex media, where nonspecific interactions and biological
variability can significantly impact assay selectivity. Similarly,
a lectin-modified SPRi detector surface was developed to probe aberrant
glycosylation patterns on circulating glycoproteins. This platform enabled correlation of disease progression
from myelodysplastic syndromes (MDS) to acute myeloid leukemia (AML)
by monitoring changes in glycan structures, specifically increased
sialylation and truncation of O-glycans.
Fetal and neonatal
alloimmune thrombocytopenia (FNAIT) represents
another clinically significant condition amenable to SPRi-based biosensing.
In FNAIT, maternal IgG antibodies recognize and bind platelet antigens
expressed by the neonate, which can lead to severe thrombocytopenia
and life-threatening hemorrhage. To address limitations of current
diagnostic approaches, researchers proposed a cellular SPRi assay
that quantifies FcγRIII binding to antibody-coated platelets
as an alternative to established IgG glycoanalytics based on mass
spectrometry. This SPRi-based method
was validated using 143 plasma samples and demonstrated strong discriminatory
power between clinically relevant sample groups, with results showing
good agreement with mass spectrometry-based analyses.
Although less prevalent
in the literature than oncological and autoimmune applications, surface
plasmon resonance imaging techniques have increasingly been applied
to characterize inflammatory and anti-inflammatory interactions. Pfizer researchers employed SPRM to complement
their investigation of lipid ligands that bind chemokine receptor-like
2 (CCRL2). SPRM was used to quantify
binding kinetics between CCRL2-expressing cells and candidate ligands,
including chemerin, revealing that chemerin binds HEK-huCCRL2 cells
with a K
D of 5.49 nM. SPRi has been similarly
utilized to elucidate the interaction of TLR4 with cycloastragenol. SPRi has also been utilized to evaluate anti-inflammatory
compounds with potential cardiovascular relevance. One recent study
investigated ethyl ferulate, the active component of the traditional
Chinese medicine Ligusticum chuanxiong, as a therapeutic agent for
preventing myocardial infarction in at-risk patients. SPRi measurements demonstrated that ethyl ferulate
binds transforming growth factor-β receptor 1 (TGF-βR1)
with a K
D of 4.01 nM, providing a molecular
basis for the compound’s reported cardioprotective and anti-inflammatory
effects. Similarly, SPRi was applied to study anti-inflammatory constituents
of another traditional Chinese medicine, Glycyrrhizae . In this work, investigators examined
whether glycyrrhizin-derived compounds (GL) interact with toll-like
receptor 4 (TLR4), a key mediator of inflammatory signaling. Binding
studies revealed that licochalcone A (LicoA) exhibited high affinity
toward TLR4, with a measured K
D of 387
nM. Complementary Western blot analyses further showed that GL extracts
reduced TLR4 protein expression in lung tissue. Collectively, these
results supported the molecular binding models and suggested that
the anti-inflammatory activity of Glycyrrhizae arises from both inhibition and downregulation of TLR4 signaling
pathways.
Compared to oncological
and autoimmune applications, SPR imaging-based biosensors remain relatively
underexplored for direct infectious disease diagnostics. To date,
most SPRi studies in this area have focused on characterizing molecular
binding interactions and probing immunological mechanisms rather than
clinical detection. For example, SPRi has been used to quantify the
interaction between the HIV-neutralizing monoclonal antibody CH31
and the HIV envelope glycoprotein AE.A244 gp120, yielding a K
D of 1.61 × 10 –8 M. SPRi has also been applied to elucidate protein
function in bacterial pathogens, including Staphylococcus
aureus . Previous work
has shown that functional amyloid motifs in S. aureus exhibit diverse biological roles, yet the function of one important
protein class, phenol-soluble modulins (PSMs), has remained poorly
understood. One proposed mechanism suggests
that PSMs may act as bioadhesives or contribute to biofilm stabilization.
To test these hypotheses, a recent study employed a multifaceted membrane-mimetic
SPRi platform to examine PSM aggregation on surfaces with varying
hydrophobicity and surface charge, including positively charged, negatively
charged, and neutral hydrophilic oxidized polystyrene, as well as
hydrophobic polystyrene substrates Kinetic
analysis revealed that PSMs exhibit adaptive binding behavior, with
a pronounced preference for surfaces that are traditionally considered
low-binding. These findings support a functional role for PSMs as
versatile bioadhesives and suggest their importance in biofilm adhesion
and structural integrity within bacterial communities.
Conclusion
This review highlights the
growing capabilities of surface plasmon
resonance imaging and surface plasmon resonance microscopy for characterizing
a broad spectrum of biological and inorganic entities. Continued advances
in instrumental design have significantly improved spatial resolution,
sensitivity, and analytical specificity, thereby expanding the applicability
of these techniques across biosensing, nanoscience, and environmental
research. In parallel, innovations in surface chemistry and signal-amplification
strategies have enabled more reliable detection of low-molecular-weight
and low-abundance analytes while mitigating nonspecific adsorption
and cross-reactivitychallenges that have historically limited
SPR-based analyses in complex media.
The integration of computational
methods, particularly machine
learning, has further accelerated progress in SPR imaging. Data-driven
approaches now support both postacquisition signal interpretation
and the rational design of next-generation SPRi platforms, enabling
improved noise reduction, enhanced sensitivity, and increased adaptability
to diverse experimental conditions. When combined with advanced surface
chemistries and amplification reagents, these computational tools
substantially broaden the versatility and analytical power of SPRi
and SPRM methodologies.
Application-wise, SPR imaging has been
most extensively explored
in oncological and autoimmune disease research, where multiplexing
and label-free detection offer clear advantages. In contrast, emerging
areas such as virology, drug-target characterization, extracellular
vesicle analysis, and environmental sensing remain comparatively underdeveloped
and present significant opportunities for future investigation. In
particular, the continued adoption of machine learning-assisted analysis
is expected to play a critical role in enhancing specificity for small
analytes in complex biological matrices.
Despite substantial
advances in hardware and software, several
factors continue to limit the broader adoption of SPRi and SPRM, particularly
in clinical settings. Conventional SPR instruments have evolved into
standardized, largely “black box” platforms through
the integration of automated fluid delivery, degassing, and simplified
software. By contrast, SPRi and SPRM systems remain less mature commercially.
Many reported implementations rely on custom-built optical assemblies
constructed from general-purpose components. While this modularity
is suitable for academic studies due to simple modification, it increases
operational complexity and restricts routine use to laboratories with
specialized expertise.
The use of SPRi and SPRM places greater
technical demands on users
than traditional SPR. In addition to understanding SPR fundamentals,
imaging- and scattering-related effects must be considered during
data interpretation and assessment of reproducibility. These requirements
increase training demands and limit robustness in environments where
consistent operation by nonspecialist users is required. Data processing
and standardization represent additional challenges for clinical translation.
SPRi and SPRM experiments typically generate large, image-based data
sets that require extensive postprocessing before being interpreted.
At present, analysis workflows are often implemented using custom
scripts or general image analysis software rather than standardized
pipelines. Variability in data formats, processing methods, and reporting
practices complicates interlaboratory comparison and presents obstacles
for standardization, verification, as well as regulatory acceptance.
Recent developments nonetheless suggest pathways toward broader
adoption. Continued progress in instrument design and increased commercial
development are expected to improve robustness while reducing SPRi/SPRM
system complexity. In parallel, computational approaches, including
machine learning and AI-assisted methods, are increasingly being applied
to address challenges in calibration, image interpretation, and large-scale
data processing. These advances may reduce user-dependent variability
and improve reproducibility, lowering barriers to wider use. It remains
to be seen if recent advances in AI can be leveraged to assist in
the processing and interpretation of SPRi and SPRM data. As these
efforts advance, SPRi and SPRM are likely to complement established
SPR techniques by enabling spatially resolved measurements in applications
where the added information justifies the increased complexity.
Introduction
When investigating biomolecular
interactions, a wide range of analytical
tools are available to probe, elucidate, and quantify binding processes. The choice of method is often governed by factors
such as spatial and temporal resolution, sensitivity, throughput,
and ease of implementation, all of which influence experimental efficiency
and data reliability. In recent years,
label-free techniques, most notably surface plasmon resonance (SPR),
have emerged as robust alternatives for real-time analysis of biomolecular
interactions while maintaining high sensitivity. Beyond conventional spectroscopic SPR, surface plasmon
resonance imaging (SPRi) extends these capabilities by enabling parallel,
high-throughput, and multiplexed detection across spatially resolved
sensing surfaces.
−
The advances in SPRi and related imaging-based plasmonic techniques
in the past decade have substantially broadened their applicability
in bioanalysis through the development of new optical configurations,
computationally assisted data analysis for complex data sets, improved
surface and nanostructure characterization, and targeted strategies
for biomarker screening.
The excitation of surface plasmons
using a prism-based optical
coupler was first reported by Kretschmann, a configuration that remains widely employed in modern SPR instrumentation.
In conventional spectroscopic SPR measurements, a sensorgram is generated
by monitoring shifts in the resonance condition, typically angular
or wavelength changes, which reflect association, dissociation, steady-state
binding, and surface regeneration processes.
,
Integration
with microfluidic systems further enhances performance by enabling
controlled and efficient analyte delivery across plasmonic sensor
surfaces. In SPRi, the entire sensing
surface is interrogated simultaneously using a charge-coupled device
(CCD), allowing high-throughput and multiplexed analysis that is not
readily achievable with point-detection SPR spectroscopy ( Scheme
). While SPRi generally employs optical configurations similar
to those used in spectroscopic SPR, detection is typically performed
at a fixed angle. Alternative interrogation
modes include wavelength-scanning SPRi and phase-interrogation SPRi, each
offering distinct advantages in sensitivity and contrast. Comprehensive
discussions of these variations have been reported elsewhere.
,
a Developments in SPRi
platforms
have included the incorporation of plasmonic waveguides and expansion
into terahertz sensing while developments in SPRM have added far-field
scattering and interferometric imaging analysis.
Developments in SPRi
platforms
have included the incorporation of plasmonic waveguides and expansion
into terahertz sensing while developments in SPRM have added far-field
scattering and interferometric imaging analysis.
Surface plasmon resonance microscopy (SPRM) shares conceptual similarities
with SPRi but differs fundamentally in optical implementation. In
SPRM, the prism coupler is replaced by a high-numerical-aperture (NA)
objective lens, and the signal arising from the evanescent plasmonic
field is directly imaged
−
( Scheme
). In many operations, the reflected light
associated with surface plasmon excitation is also recorded. While
SPRM can offer enhanced spatial resolution and access to single-particle
or single-event measurements, the detected signal is generally weak.
Thus, signal enhancement is often utilized through plasmonically active
nanoparticles on the sensor surface.
,
SPRi and SPRM
represent two complementary extensions of classical SPR that transform
refractive-index sensing into spatially and temporally resolved, information-rich
measurements. Both approaches retain the core advantages of SPR, capable
of real-time, label-free detection and quantitative kinetic analysis.
This review focuses on recent progress in SPRi and SPRM with representative
literature published prior to 2025 to provide a comprehensive overview
of the field. We first discuss advances in instrumental design and
optical configuration, followed by emerging applications of machine
learning and computational approaches for SPR-based data analysis.
We then present key applications of SPRi and SPRM for information-rich
characterization of molecular interactions on bioinspired and nanoscale
interfaces. A substantial portion of the review is devoted to recent
developments in disease biomarker assessment by imaging-based approaches.
Finally, we present perspectives on the role of SPRi and SPRM in disease
research, with emphasis on multiplexed analysis and underexplored
areas that may offer significant opportunities for future investigation.
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