Identification of water content in nanocavities
© Douas et al.; licensee Springer. 2013
Received: 14 December 2012
Accepted: 1 April 2013
Published: 15 April 2013
A tapered dielectric waveguide that scans, at constant height, a sample containing a viral capsid is studied by combining a lattice gas model to simulate water meniscus formation and a finite difference time domain algorithm for light propagation through the media involved. Our results show different contrasts related to different water contents and different meniscus orientations. We propose this method as a way to study water content and evaporation process in nanocavities being either biological, like viral capsides, or nonbiological, like photonic crystals.
KeywordsSNOM Viral capsid Water FDTD Lattice gas
Hydrophilic tips used in scanning near field optical microscope (SNOM) condense some water layers, leading to the formation of a water bridge (or water meniscus) between the tip and a hydrophilic sample for small tip-sample distances. The shape of such meniscus will depend on the geometry of both surfaces, their separation, and environmental conditions (temperature and relative humidity). When working in air conditions using local probes, humidity causes characteristic jump-to-contact events due to the spontaneous formation of a water meniscus between tip and sample . Presence of water at experimental relatively high humidity conditions also modifies the dielectric properties of the medium between the SNOM tip and substrate. As a consequence, the optical images of samples on surfaces are altered by humidity and water condensation. Previous studies on the optical signal under variable environmental humidity [2, 3] have shown the conditional increase in the optical signal depending on the hydrophobic character of the sample. In fact, the inclusion of water condensation should be considered for any modeling or simulation of the field enhancement effect .
On the other hand, water condensation at the nanoscale is known to play an important role in the collapse of viral capsids during desiccation, as revealed by atomic force microscopy (AFM) experiments . The meniscus formation along with the geometry of the nanocavity allows capillary force to modify the mechanical stability towards collapse . An important issue that arises from these AFM studies on biological samples is whether the condensation of water in these viral nanocavities may be detected by a direct measurement.
The previously mentioned changes on the near field optics, during the desiccation stages, may be a good tool for showing how this process takes place. Indeed, SNOM characterizes sample composition by the changes in the optical near field and, since the viral capsides are almost transparent at optical wavelengths , different water contents in these nanocavities will produce different output signals which are distinct enough to characterize and monitor the desiccation sequence by SNOM experiments.
The aim of this paper is to understand, using an adequate combination of numerical techniques, how water evaporation or condensation in a nanocontainer (viral capsid) might be detected by near-field optic measurements. To do so, we consider a tapered dielectric waveguide that scans, at constant height, a sample formed by a viral capsid with different water contents. The manuscript is organized as follows: next section describes the system under study and the set of numerical methods we have used; finally, the two sections devoted to results and conclusions will describe the changes of the optical signal due to the presence of a water meniscus and the possible use of these changes to monitor real-time evolution of water meniscus in nanocontainers.
In order to describe the tip-sample system we have considered a tapered optical fiber probe, with a final aperture of 100 nm, coated with a perfect metal. This tip is placed at a constant distance, h=50 nm, from a flat dielectric substrate with a refractive index n=2.0 and 10 nm thicknesses. This geometry is very similar to that previously described by Wang et al. Upon the substrate we have placed a simple geometry nanocontainer that simulates a viral capsid with a single porous, similar to the previously studied ϕ 29 viral particles . The considered shape of our nanocontainer is a 30-nm lateral size square with a porous of 5 nm centered at one side. The nanocontainer is almost transparent (n=1.06) and hydrophilic. The capsid might be filled up with double-stranded DNA (dsDNA) (refractive index n=1.55 at the considered wavelength)  or with different contents of water (n=1.33) that will depend on the relative humidity.
The water meniscus formation inside the container is studied using a 2D lattice gas model that has been extensively used to study water properties, including gas-liquid transition and density anomalies. This model has been also used to describe the geometry features of the water meniscus formed between an AFM tip and a substrate . The fluid is represented by a 2D square lattice with a spacing of 0.3 nm. In the model, we may assume thermal and phase equilibrium with a bulk reservoir, specified by a temperature T and a chemical potential μ. These quantities are directly related to the relative humidity R h through the expression R h =exp(μ−μ c )/kBT, being kB the Boltzmann constant and μc the critical chemical potential. We have performed a (V,T,μ) Monte Carlo (MC) numerical simulation at laboratory conditions, T=293 K, assuming that each lattice site (i,j) was either occupied with a water molecule ρ(i,j)=1 (liquid phase) or empty ρ(i,j)=0 (gas phase). The quantity ρ(i,j) is the occupation number of a given site (i,j). Each water-occupied site interacts with its (occupied) neighbor sites with an attractive energy ∈ = 9 kJ/mol. This value has been chosen in order to use a model able to fit the value of the water critical temperature. The interaction of tip and nanocontainer with a water molecule involves an interaction energy given by b T =−56 kJ/mol (hydrophilic character). The substrate has a repulsive interaction with water given by |b s| = 46 kJ/mol (hydrophobic character). The conditions considered correspond to equilibrium bulk evaporation. The concrete expression of the Hamiltonian we have considered is reported in  and includes water-water, water-tip, and water-substrate terms. For a given set of geometrical parameters and physical conditions (temperature and humidity), an approximate shape of the water meniscus is obtained from an averaging procedure involving hundreds of different configurations. Water density average at each lattice site (0<<ρ(i,j)><1) was calculated after the statistical methodology described in . Once <ρ(i,j)> was known for every site of the 2D square lattice, the effective refractive index n(i,j) at a given site is calculated, assuming that there is a linear dependence (n(i,j)=1+0.33<ρ(i,j)>) between the refractive index and the average water density . This methodology allows to determine the meniscus shape as well as the associated refractive index map for a given set of parameters (tip-sample distance, temperature, and humidity).
The local refractive index n(i,j) determines the propagation of the optical signal through the tip-sample-substrate system. The propagation of the electromagnetic radiation was studied by means of a 2D finite difference time domain (FDTD) simulation, based on Yee algorithm ], with a perfect matching layer as boundary condition [. Transverse Magnetic to the z direction fundamental mode is propagated through the dielectric coated fiber guide with frequency ν=3.77×1015 Hz (λ=500 nm). Radiated intensity, at transmission, is integrated at a plane surface, acting as light collector, located at a distance D=100 nm from the substrate. In our study, all intensities are normalized to that one obtained without any substrate. Since the lattice parameter used in the MC simulations is too small for being considered in feasible FDTD simulations, a larger integration lattice constant is required. In order to match FDTD lattice constant with the one used in the lattice gas simulation, a lattice step of 0.9 nm was considered for the FDTD simulations. In this way, the refractive index for each FDTD node was obtained by averaging those local refractive index values corresponding to the water nodes included within the FDTD cell. General assumptions were taken into account for the simulation. Indeed, all water necks calculated at equilibrium were considered to be stable during the typical times associated to the wave propagation; furthermore, we have neglected SNOM probe oscillations near the sample. In addition, water heating processes are not considered since radiation wavelength is far from those corresponding to water absorption bands.
Results and discussion
There is another interesting point that must be addressed. In this specific case, we can take advantage of the signal’s broadening to study the evaporation dynamics related to meniscus geometry induced by the asymmetry porous position. This is clearly reflected by the following important feature: the power transmitted as a function of the tip position is not symmetric. This property is due to the intrinsic virus geometry, with a single porous on one side of the viral capsid implying a nonsymmetric water disposition inside the container. Interestingly, information about virus geometry as well as water evaporation dynamics may be obtained by the position of the maximum of the transmitted signal. For example, note how a porous located at the left implies a maximum on the signal displaced to the right. This asymmetry in the power is quantified in the inset in Figure 3, where the ratio between left and right transmitted signals, at equidistant points from the geometric center in the scan direction, are plotted versus distance to center. We consider an empty capsid and a container with 50% water content. Note that for the last case, a slight asymmetry shows up with a maximum value of almost 1%.
We have presented a theoretical study in which we combine the lattice gas model to simulate water meniscus formation and a FDTD algorithm for light propagation through the media involved. We simulate a tapered dielectric waveguide that scans, at constant height, a sample containing a viral capsid. Our results show different contrasts related to different water contents and different meniscus orientations. We propose this method as a way to study water content and evaporation process in nanocavities being either biological, like viral capsides, or nonbiological, like photonic crystals.
This work has been funded through projects FIS2009-13403-C02-01 (MINECO), S2009-MAT-1467 (CAM), and CSD2010-00024 (MINECO).
- Sahagún E, García-Mochales P, Sacha GM, Sáenz JJ: Energy dissipation due to capillary interactions: hydrophobicity maps in force microscopy. Phys Rev Lett 2007, 98: 176106.View ArticleGoogle Scholar
- Taylor RS, Vobornik D, Lu Z, Chisholm RA, Johnston LJ: Damping behavior of bent fiber NSOM probes in water. J Appl Phys 2010, 107: 1–9.View ArticleGoogle Scholar
- Kaupp G: The enhancement effect at local reflectance and emission back to apertureless SNOM tips in the shear-force gap. Open Surf Sci J 2011, 3: 20–30. 10.2174/1876531901103010020View ArticleGoogle Scholar
- Carrasco C, Douas M, Miranda R, Castellanos M, Serena PA, Carrascosa JL, Mateu MG, Marqués MI, Pablo PJd: The capillarity of nanometric water menisci confined inside closed-geometry viral cages. Proc Nat Acad Sci 2009, 106: 5475–5480. 10.1073/pnas.0810095106View ArticleGoogle Scholar
- Serena PA, Douas M, Marqués MI, Carrasco C, Miranda R, Carrascosa JL, Castellanos M, Mateu MG, Pablo P J d: MC simulations of water meniscus in nanocontainers: explaining the collapse of viral particles due to capillary forces. Phys Status Solidi C 2009, 6: 2128–2132. 10.1002/pssc.200881738View ArticleGoogle Scholar
- Balch WM, Vaughn J, Novatny J, Drapeau D, Vaillancourt R, Lapierre J, Ashe A: Light scattering by viral suspensions. Limnol Oceanogr 2000, 45: 492–498. 10.4319/lo.2000.45.2.0492View ArticleGoogle Scholar
- Wang X, Fan Z, Tang T: Study on the power transmission and light spot size of optical probes in scanning near-field optical microscopes. Opt Com 2004, 253: 31–40.View ArticleGoogle Scholar
- Elhadj S, Singh G, Saraf RF: Optical properties of an immobilized DNA monolayer from 255 to 700 nm. Langmuir 2004, 20: 5539–5543. 10.1021/la049653+View ArticleGoogle Scholar
- Jang J, Schatz GC, Ratner MA: Liquid meniscus condensation in dip-pen nanolithography. J Chem Phys 2002, 116: 3875–3886. 10.1063/1.1446429View ArticleGoogle Scholar
- Harvey AH, Gallagher JS, Levelt Sengers JMH: Revised formulation for the refractive index of water and steam as a function of wavelength, temperature and density. J Phys Chem Ref Data 1998, 27: 761–774. 10.1063/1.556029View ArticleGoogle Scholar
- Yee KS: Numerical solution of initial boundary value problems involving Maxwell equations in isotropic media. IEEE T Antenn Propag 1966, 14: 302–307.View ArticleGoogle Scholar
- Berenger JP: A perfectly matched layer for the absorption of electromagnetic waves. J Comp Phys 1994, 114: 185–200. 10.1006/jcph.1994.1159View ArticleGoogle Scholar
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