82 research outputs found

    Asymptotic Methods applied to an American Option under a CEV Process

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    We consider an American put option under the Constant Elasticity of Variance (CEV) process. This corresponds to a free boundary problem for a partial differential equation (PDE). We show that this free boundary satisfies a nonlinear integral equation, and analyze it in the limit of small ρ\rho = 2r/σ22r/ \sigma^2, where rr is the interest rate and σ\sigma is the volatility. We find that the free boundary behaves differently for five ranges of time to expiry. We then analyze option price P(S,t)P(S,t), as a function of the asset price SS and time to expiry tt. We obtain the asymptotic expansion of PP as ρ0\rho \rightarrow 0, first via an integral equation formulation, and then using the PDE satisfied by PP, and analyzing it by perturbation theory and matched asymptotic expansions

    Facile Fabrication of Highly Efficient g‑C<sub>3</sub>N<sub>4</sub>/Ag<sub>2</sub>O Heterostructured Photocatalysts with Enhanced Visible-Light Photocatalytic Activity

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    Highly efficient visible-light-driven g-C<sub>3</sub>N<sub>4</sub>/Ag<sub>2</sub>O heterostructured photocatalysts were prepared by a simple liquid phase synthesis method at room temperature. The composition, structure, morphology, and optical absorption properties of the as-prepared g-C<sub>3</sub>N<sub>4</sub>/Ag<sub>2</sub>O composites were characterized by XRD, FTIR, XPS, TEM, and UV–vis DRS, respectively. We found interestingly that the photogenerated charge carriers separations of the as-prepared g-C<sub>3</sub>N<sub>4</sub>/Ag<sub>2</sub>O composites were closely related to the mass ratio of g-C<sub>3</sub>N<sub>4</sub> and Ag<sub>2</sub>O. When the mass ratio of g-C<sub>3</sub>N<sub>4</sub> and Ag<sub>2</sub>O reached 1:4, the as-prepared composite exhibited the highest photocatalytic activity, which was almost 11 and 1.2 times as high as that of individual g-C<sub>3</sub>N<sub>4</sub> and Ag<sub>2</sub>O, respectively. The enhancement of photocatalytic activity could be attributed to the synergetic effects between g-C<sub>3</sub>N<sub>4</sub> and Ag<sub>2</sub>O as well as the improved dispersibility and the decreased particle size of Ag<sub>2</sub>O. Moreover, the as-prepared composites showed excellent stability toward the photodegradation of methyl orange (MO). Finally, a possible photocatalytic and charge separation mechanism was proposed

    Media 3: Electrically actuated liquid iris

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    Originally published in Optics Letters on 01 March 2015 (ol-40-5-831

    Media 1: Electrically actuated liquid iris

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    Originally published in Optics Letters on 01 March 2015 (ol-40-5-831

    Media 2: Electrically actuated liquid iris

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    Originally published in Optics Letters on 01 March 2015 (ol-40-5-831

    Media 1: An adaptive liquid lens with a reciprocating movement in a cylindrical hole

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    Originally published in Optics Express on 15 December 2014 (oe-22-25-31041

    Dielectric Liquid Microlens Array with Tunable Focal Length Based on Microdroplet Array Created via Dip-Coating Method

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    A dielectric liquid microlens array (LMA) with a tunable focal length was fabricated by using a microdroplet array generated through the dip-coating method. The process began with treating the octadecyltrichlorosilane (OTS) layer with selective UV/O3 irradiation for 20 min to establish a hydrophilic–hydrophobic patterning surface. The substrate was subsequently immersed in glycerol and then withdrawn at a constant rate to create a microdroplet array. Upon filling the cell with matching oil (SL5267) and placing it within a square array of a 200 μm diameter glycerol microdroplet array, the LMA was produced. The focal length ranged from approximately −0.96 to −0.3 mm within a voltage range of 0 to 60 Vrms. The glycerol microdroplets, characterized by their shapes, sizes, curvatures, and filling factors, can be precisely controlled by designing an OTS patterning or adjusting the dip-coating speed. This approach offers a rapid and high-throughput method for preparation. Our approach to fabricating tunable LMA offers several advantages, including simplicity of fabrication, uniform structural properties, cost-effectiveness, polarization independence, and excellent optical performance. These focus-tunable LMAs hold significant potential for applications in image processing, 3D displays, medical endoscopy, and military technologies
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