1. FIELD OF THE INVENTION
The present invention relates to Inhomogeneous Surface Wave Microscopy, which involves a method for improving the lateral resolution in performing fluorescence observation by the use of inhomogeneous optical surface waves known as inhomogeneous surface plasmon polaritons. Inhomogeneous surface plasmon polaritons are evanescent in axial and lateral dimensions, and generated by refraction of optical surface waves known as surface plasmon polariton across metal-metal interfaces. This invention utilizes a total internal reflection prism supporting laterally-interfaced metal nanofilms that can support the desired evanescent optical waves.
2. BRIEF SUMMARY OF INVENTION
Inhomogeneous Surface Wave Microscopy offers new capabilities for significantly enhancing the lateral resolution available in current state-of-the-art fluorescence microscopy techniques that rely on evanescent excitation of fluorophore labels, namely Total Internal Reflection Microscopy [1, 2]. This invention leverages a newly-discovered class of evanescent surface waves known as inhomogeneous surface plasmon polaritons [3]. A key part of the invention is a total internal reflection prism supporting two different metal nanofilms laterally interfaced with one another, which is used to support the desired evanescent waves. This novel substrate requires deposition of nanoscopically-thin (˜50 nm) layers of plasmonic materials (e.g. silver and gold) on a total internal reflection prism, made, for example, glass, which can have comparable form factor as a standard microscope slide or prisms used in conventional Total Internal Reflectance Fluorescence Microscopy [1,2]. Hence, this novel substrate can be integrated into existing Total Internal Reflection Microscopy setups with only minor modifications. The Inhomogeneous Surface Wave Microscopy setup is illustrated in FIG. 1, and the novel substrate is illustrated in FIG. 2. This invention addresses the pressing need to increase the lateral resolution of microscopy-based imaging without relying non-linear absorption processes or other phenomena which require high-intensity illumination that can induce molecular and cellular damage, thereby altering the underlying structures and behaviors these techniques seek to study [4].
3. BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1: Schematic illustration of the Inhomogeneous Surface Wave microscope.
FIG. 2: Schematic illustration of a total internal reflection prism on which laterally-interfaced metal nanofilms are deposited, which is a substrate that can support inhomogeneous surface plasmon polaritons for enabling Inhomogeneous Surface Wave microscopy.
FIG. 3: Top-down view of lateral interface between metal 1 nanofilm and metal 2 nanofilm, and illustration of relevant propagation directions of the optical waves.
FIG. 4: Illustration of an inhomogeneous surface plasmon polariton which is evanescent along both an axial and a lateral dimension.
4. DETAILED DESCRIPTION OF THE INVENTION
The invention and method presented here are illustrated schematically on an inverted microscope setup where the objective lens is below the sample being imaged. However, the method is applicable to upright setups where the objective lens is above the sample being imaged.
FIG. 1 shows the embodiment of the invention in an inverted microscope configuration. The substantive modification to a total internal reflection fluorescence microscope is the deposition of laterally-interfaced metal nanofilms on the total internal reflection prism. The monochromatic light of wavelength λ is focused by the objective to large angles of incident relative to the surface normal of the prism substrate on which the metal 1 nanofilm is deposited. The dielectric constant of the prism substrate will be denoted ∈prism and the dielectric constant of the metal 1 nanofilm at wavelength λ will be denoted ∈m(λ), where ∈m(λ) is understood to be a complex number which depends on the value of the wavelength, λ. A surface plasmon polariton is excited on the metal 1 nanofilm when the following condition is met:
where ∈S indicates the dielectric constant of the sample/substrate placed on top of the metal nanofilms. A general requirement is that ∈prism>∈S, such that total internal reflection would result for some critical angle of incidence of light incident from the prism side if the prism were interfaced directly with the superstrate material. This requirement can be met by many materials (see Claim 2). Similar to the optical field resulting from total internal reflection, this surface plasmon polariton field is evanescent in the axial dimension (along the z-axis) [3] (see illustration of Axially-confined evanescent field from Surface Plasmon Polariton in FIG. 1). An inhomogeneous surface plasmon polariton is created on the metal 2 nanofilm, and this wave has evanescent character in both the axial dimension (along the z-axis) and in lateral dimension 1 (along the y-axis) (see FIG. 1 and FIG. 2 for illustration of the coordinate system); it is this 2-dimensional evanescent character that allows for selective excitation of fluorophores in a limited area of the sample and thereby imparts enhanced lateral imaging resolution.
Surface plasmon polaritons propagate along the surface of the metal 1 nanofilm with a direction that will be dictated by the angle (θI) of the polarization vector of the incident light in the lateral plane (in the x-y plane). The precise angle θI of the polarization vector in the x-y plane can be controlled using a polarization filter, as illustrated in FIG. 1, and has direct correspondence to the angle θI illustrated in FIG. 3 that shows the relative angle of the surface plasmon polariton propagation direction normal to the metal 1/metal 2 interface.
When the surface plasmon polariton propagates across the metal 1/metal 2 interface, it will undergo a complex refraction process. The refraction process is referred to as complex because the propagation vector of the surface plasmon polariton is a complex quantity: it has a real component related to its momentum, and an imaginary component related to its evanescent character. The refraction of these components usually occurs at different angles, leading to a complex generalization of Snell's law, with a set of relations for the refraction angle of the real component of the propagation vector (θ2) and a set of relations for the refraction angle of the imaginary component of the propagation vector (φ2).
FIG. 2 shows illustrate that the metal nanofilms should be approximately 50 nm in thickness along the axial dimension (along the z-axis in the figure coordinate system) in order to allow efficient excitation of surface waves. The lateral dimension 1 of the nanofilms (along the y-axis in the figure coordinate system) can be much larger, and may be determined according to specifications relating to the specimen sizes and desired coverage of specimens. Lateral dimension 2 of the nanofilm (along the x-axis in the figure coordinate system) should be on the order of ˜100 micrometers; surface plasmon polaritons will lose significant electric field intensity after propagating more than 100 micrometers, which will limit the efficacy of fluorophore excitation beyond this distance from the interface between metal 1 and metal 2. As illustrated in FIG. 3, these angles can be substantially different, causing the components of the refracted propagation vector to point in substantially different directions. A wave of this type is called an inhomogeneous wave, and a surface plasmon polariton with this character is called an inhomogeneous surface plasmon polariton [3]. When the difference between θ2 and φ2 is large, then the inhomogeneous surface wave can take on substantial evanescent character in the lateral dimension. This feature is illustrated in FIG. 4. The degree of evanescent character can be quantified by a measured called the confinement length which is defined by
where λ is the incident wavelength, and K2 will depend on the material properties of both metal interfaces, the angle of incidence (θI), and on λ [3]. The confinement length has dimensions of length and determines the distance over which the electric field intensity decays by a factor of e in the lateral dimension. That is, the shorter the confinement length, the more laterally confined the inhomogeneous surface plasmon polariton wave is, and the smaller the fluorophore excitation area is. Therefore, higher the lateral resolution is achieved for smaller confinement lengths. For a given wavelength and set of materials, the confinement length can be modulated by changing θI which is controllable externally by the polarization filter (see FIG. 1, FIG. 3, and FIG. 4).
6. REFERENCES
- 1. D. Axelrod, N. L. Thompson, T. P. Burghard, “Total internal reflection Microscopy”, J. Microsc., 129, 19-28, (1983)
- 2. Y. Aono, T. Mochizuki, K. Osa, “Total internal reflection fluorescence microscope”, U.S. Pat. No. 7,385,758 B2
- 3. J. J. Foley IV, J. M. McMahon, G. C. Schatz. H. Harutyunyan, G. P. Wiederrecht, S. K. Gray, “Inhomogeneous surface plasmon polaritons”, ACS Photonics, 1, 739-745, (2014)
- 4. L. Schermella, R. Heintzmann, H. Leonhardt, “A guide to super-resolution fluorescence microscopy”, J. Cell. Biol., 190 165-175 (2010).
Patent Application
20170336612
