September 9, 2026

Zero-Mode Waveguides

Extending Single-Molecule Fluorescence to Higher Concentrations

At higher concentrations, the challenge is often not detecting a fluorophore, but isolating its signal from the many molecules occupying a diffraction-limited observation volume. Zero-mode waveguides change that volume itself.
Comparison of fluorescence detection in a diffraction-limited confocal volume and a zero-mode waveguide (ZMW) nanoaperture. At elevated fluorophore concentrations, the conventional confocal observation volume contains a large number of molecules (N > 1000), whereas confinement of the excitation field within the ZMW reduces the effective observation volume and consequently the molecular occupancy (N < 10), enabling FCS measurements at higher concentrations.

When Concentration Becomes the Limiting Variable

Single-molecule fluorescence experiments rely on detecting signals or fluctuations from individual fluorescent molecules against the surrounding background. In a conventional confocal microscope, this is generally achieved by combining a tightly focused excitation beam with spatially selective detection. The resulting observation volume is typically on the femtoliter scale.

This works well as long as the average number of fluorescent molecules within that volume remains sufficiently small. Increasing the bulk concentration changes this condition. More molecules simultaneously occupy the observation volume, their fluorescence contributions begin to overlap, and fluctuations associated with individual molecules become increasingly difficult to distinguish.

The relevant limitation is therefore not a fixed concentration threshold. It is the relationship between concentration and observation volume.

For a given concentration, the average molecular occupancy scales with the volume being observed. A smaller observation volume contains fewer molecules at the same bulk concentration. Conversely, reducing the observation volume makes it possible to increase the concentration while maintaining a similar average number of detected molecules.

This relationship is particularly apparent in fluorescence correlation spectroscopy. FCS analyzes temporal fluorescence fluctuations as molecules diffuse into and out of the observation volume. As the average number of molecules within that volume increases, the relative fluctuations become smaller and the correlation amplitude decreases. High concentrations can therefore make the fluctuations of interest increasingly difficult to resolve. The same basic issue is relevant to other freely diffusing single-molecule measurements. If several molecules contribute photons simultaneously, assigning fluorescence bursts or molecular states to individual molecules becomes more difficult.

Zero-mode waveguides address this problem at its physical origin by reducing the optically probed volume itself.

What Is a Zero-Mode Waveguide?

A zero-mode waveguide (ZMW) is a subwavelength aperture formed in an opaque metallic film. Its dimensions are chosen such that, at the excitation wavelength, the aperture operates below the cutoff for propagating waveguide modes.

Instead of propagating through the structure as it would through a conventional waveguide, the excitation field is strongly confined near the entrance of the aperture and decays rapidly with distance into it. Fluorophores close to the bottom of the aperture can therefore be excited efficiently, while molecules farther away contribute much less to the detected fluorescence.

The result is an optically accessible region with dimensions far below those of the conventional diffraction-limited confocal focus.

This distinction is important. A ZMW is not simply a smaller pinhole added to a microscope. It modifies where light can interact with fluorophores. The effective observation volume is therefore defined by the combination of the aperture geometry, the metallic film, the excitation wavelength, and the optical field within the nanoaperture rather than solely by the diffraction-limited focal volume of the microscope.

ZMWs can nevertheless be integrated into a confocal fluorescence measurement relatively directly. The nanoaperture array replaces the conventional glass sample surface, while excitation and fluorescence detection can still be performed through a high numerical aperture microscope objective.

Comparison of fluorescence detection in a diffraction-limited confocal volume and a zero-mode waveguide (ZMW) nanoaperture. At elevated fluorophore concentrations, the conventional confocal observation volume contains a large number of molecules (N > 1000), whereas confinement of the excitation field within the ZMW reduces the effective observation volume and consequently the molecular occupancy (N < 10), enabling FCS measurements at higher concentrations.
Comparison of fluorescence detection in a diffraction-limited confocal volume and a zero-mode waveguide (ZMW) nanoaperture. At elevated fluorophore concentrations, the conventional confocal observation volume contains a large number of molecules (N > 1000), whereas confinement of the excitation field within the ZMW reduces the effective observation volume and consequently the molecular occupancy (N < 10), enabling FCS measurements at higher concentrations.

Why a Smaller Observation Volume Changes the Concentration Regime

The direct consequence of nanoscale confinement is a reduction in the number of molecules contributing simultaneously to the measurement.

Consider two observation volumes containing the same fluorescent solution. If one volume is reduced by a factor of 100, its average molecular occupancy is also reduced by approximately the same factor at the same concentration. Alternatively, the concentration could in principle be increased by a similar factor while maintaining comparable average occupancy.

This is the central reason why zero-mode waveguides are relevant for high-concentration single-molecule fluorescence measurements. The scale of this effect can be seen in a recent study by Khelidj et al, Small (2026)1. For their approximately 230 nm diameter ZMWs, FCS measurements yielded effective detection volumes in the range of about 10 aL, compared with the approximately 1 fL scale associated with the confocal reference. This corresponds to roughly a 100-fold reduction in observation volume for the investigated structures.

A single-molecule burst experiment in the same study illustrates what this means experimentally. Alexa Fluor 647 was measured at 5 nM in the ZMW and at 40 pM in the confocal reference. Despite the more than two orders of magnitude difference in concentration, fluorescence lifetime correlation spectroscopy determined a comparable average occupancy of approximately 0.04 molecules in both observation volumes.

The important result is not the specific concentration value. Different aperture geometries, fluorophores and experimental conditions will produce different limits. The important point is that concentration and molecular occupancy are no longer tied to a diffraction-limited observation volume. For experiments that require higher bulk concentrations, this changes the available experimental parameter space.

How ZMWs Affect Fluorescence Beyond Volume Reduction

Reducing molecular occupancy is the central consequence of the confined observation volume, but the nanophotonic environment inside a ZMW can also influence the detected fluorescence itself. The local excitation field and the interaction of the fluorophore with its optical environment can alter fluorescence brightness and emission dynamics.

In the ZMW system studied by Khelidj et al., fluorescence brightness in the linear excitation regime was enhanced by approximately 4.5 to 8.4 times relative to the confocal reference, depending on the fluorophore and excitation wavelength. Fluorescence lifetimes were also reduced for all three Alexa Fluor dyes investigated, indicating modified photodynamics within the metallic nanoaperture. A shorter lifetime should not be interpreted by itself as improved fluorescence performance, since the photonic environment can affect both radiative emission and losses to the metal.

Higher molecular brightness can nevertheless have a direct experimental consequence. In measurements with Alexa Fluor 647, fluorescence bursts remained distinguishable with 100 µs time binning in the ZMW, whereas they became difficult to resolve in the confocal reference. The confined excitation field also reduces fluorescence contributions from molecules outside the aperture, which is particularly relevant at higher bulk concentrations.

The magnitude of these effects depends on factors such as aperture geometry, wavelength, fluorophore properties and excitation conditions. They should therefore be understood as characteristics of a specific ZMW and measurement configuration rather than universal enhancement factors.

Fluorescence bursts from diffusing Alexa Fluor 647 molecules measured in a zero-mode waveguide and a confocal reference. The higher fluorescence signal in the ZMW allows individual bursts to remain distinguishable at shorter time binning. Adapted from Khelidj et al., Small (2026).
Fluorescence bursts from diffusing Alexa Fluor 647 molecules measured in a zero-mode waveguide and a confocal reference. The higher fluorescence signal in the ZMW allows individual bursts to remain distinguishable at shorter time binning. Adapted from Khelidj et al., Small (2026).

What Zero-Mode Waveguides Enable Experimentally

Reducing molecular occupancy while maintaining higher bulk concentrations makes ZMWs relevant to several established single-molecule methods. For FCS, the smaller observation volume allows fluorescence fluctuations to be studied under concentration regimes that would produce substantially higher molecular occupancy in a diffraction-limited confocal volume. The smaller spatial extent of the detection volume also results in shorter molecular transit times through the optically probed region, shifting the relevant FCS correlation dynamics toward shorter timescales.

Fluorescence burst analysis benefits from the same principle. Individual molecules can pass through the confined excitation region and generate distinguishable bursts even when the surrounding solution contains a considerably higher concentration of fluorescent molecules.

The nanoscale confinement and broad spectral response of ZMWs can support multicolor approaches such as single-molecule Förster resonance energy transfer (smFRET), although the nanophotonic environment can modify donor and acceptor photophysics and therefore needs to be accounted for quantitatively. In the study discussed above, freely diffusing donor-acceptor DNA constructs were measured using pulsed interleaved excitation in ZMWs, demonstrating the applicability of established smFRET methods in the nanoaperture geometry.

These examples share the same underlying requirement: preserving information about individual molecules or molecular fluctuations while moving toward concentration regimes that are difficult to access with a conventional diffraction-limited observation volume.

From Nanoscale Confinement to Reproducible Fluorescence Measurements

Zero-mode waveguides address a fundamental limitation of diffraction-limited single-molecule fluorescence by changing the observation volume itself. Their nanoscale confinement reduces the average number of molecules contributing to a measurement at a given bulk concentration, while the nanophotonic environment can additionally influence molecular brightness, fluorescence dynamics, and background contributions.

This makes ZMWs particularly relevant when single-molecule information is required under concentration conditions that are difficult to access with a conventional confocal observation volume. For techniques such as FCS, translating nanoscale confinement into quantitative measurements also requires connecting the ZMW sample with a suitable fluorescence microscopy and single-photon detection workflow.

PicoQuant’s Luminosa provides such a platform for confocal single-photon counting measurements, combining fluorescence imaging with time-resolved detection and FCS analysis. In this way, the physical advantages of nanoscale optical confinement can be integrated into a practical experimental workflow for studying molecular dynamics at higher concentrations.

Luminosa configuration for FCS measurements in zero-mode waveguides (ZMWs). The ZMW sample consists of an aluminum film with nanometer-sized apertures on a glass coverslip and is measured from below using a water-immersion objective. The enlarged cross-section illustrates the confinement of the excitation field within an individual ZMW and fluorescence collection through the objective.
Luminosa configuration for FCS measurements in zero-mode waveguides (ZMWs). The ZMW sample consists of an aluminum film with nanometer-sized apertures on a glass coverslip and is measured from below using a water-immersion objective. The enlarged cross-section illustrates the confinement of the excitation field within an individual ZMW and fluorescence collection through the objective.

1 Reference: Hamza Khelidj, Anthony Gourdin, Igor Ozerov, Antonin Moreau, Badre Kerzabi, David Grosso, Jérôme Wenger, High-Throughput Fabrication of Zero-Mode Waveguide Nanoaperture Arrays with Sol-Gel Nanoimprint Lithography for Enhanced Single Molecule Fluorescence Detection. Small 22, no. 2 (2026): e10587. https://doi.org/10.1002/smll.202510587

We will soon take a closer look at this experimental workflow and share corresponding ZMW-FCS results in an upcoming application note. Subscribe to the PicoQuant newsletter to stay informed when these resources become available.

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Evangelos Sisamakis

Product Manager, PicoQuant

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