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Journal articles on the topic 'Immersion solide'

Author: Grafiati

Published: 4 June 2021

Last updated: 4 May 2024

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1

ZOLA NGOYO, Matthieu, and Esaron MBUNGU MBENI. "Détermination de la densité d’un liquide inconnu par la poussée d’Archimède." Revue du Centre de Recherche Interdisciplinaire de l'Université Pédagogique Nationale 96, no. 1 (June 3, 2023): 37–51. http://dx.doi.org/10.62362/rszl9685.

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L’historique légendaire de la poussée d’Archimède montre que c’est par ce principe que le savant Archimède aurait déterminé la densité d’un corps solide (la couronne du Roi HIERON II) par immersion dans l’eau.Nos investigations se sont étendues sur ce principe jusqu’à la détermination de la densité d’un corps liquide par la poussée d’Archimède. De toutes nos théories et expériences, nous avons trouvé la densité de : - L’essence par la valeur d= 0,733± 0,026 ; - Mazout (gaz oil), par la valeur d= 0,830 ± 0,046. Comparativement aux valeurs théoriques de densités de ces 2 liquides : essence (d=0,73) et le mazout (d= 0,83). Nos valeurs trouvées ont des précisions respectives de :3,5 % et 5,5%

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2

Deng Sanyong, 邓三泳, 岳嵩 Yue Song, 张东亮 Zhang Dongliang, 刘昭君 Liu Zhaojun, 李慧宇 Li Huiyu, 柳渊 Liu Yuan, 张紫辰 Zhang Zichen, and 祝连庆 Zhu Lianqing. "固体浸没式红外超表面透镜设计." Infrared and Laser Engineering 51, no. 3 (2022): 20210360. http://dx.doi.org/10.3788/irla20210360.

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3

Lee, Won-Sup, Hyungbae Moon, Geon Lim, Guk-Jong Choi, and No-Cheol Park. "Solid-immersion lens based confocal microscopy using super-continuum generation effect." Transactions of the Society of Information Storage Systems 11, no. 2 (September 25, 2015): 22–25. http://dx.doi.org/10.9797/tsiss.2015.11.2.022.

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4

Su, Shu-Chun. "Determination of refractive index of solids by dispersion staining method: An analytical approach." Proceedings, annual meeting, Electron Microscopy Society of America 51 (August 1, 1993): 456–57. http://dx.doi.org/10.1017/s0424820100148113.

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When immersion liquids are used to determine the refractive index (RI) of non-opaque solids, the dispersion staining method is a simple, effective and precise way to determine the matching wavelength, λ0, at which the RI of an immersion liquid equals that of the solid. A series of equations has been derived to calculate the RI at any given visible wavelength such as nF, nD and vie, i.e. the RI’s at Fraunhöfer spectral lines F (486 nm), D (589 nm), and C (656 nm), from λ0 data obtained by the dispersion staining method. Two methods have been established: the Single Liquid Method and the Double Liquid Method.The Single Liquid Method is applicable for solids with known dispersion coefficients, which is defined as (nF-nC). This method uses only one immersion liquid whose RI is close to the RI of the solid to be measured so that a match between the liquid and the solid occurs in the visible range.

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5

Giraldo, Liliana, and Juan Carlos Moreno-Piraján. "Enthalpic Contribution of Ni(II) in the Interaction between Carbonaceous Material and Aqueous Solution." Journal of Chemistry 2017 (2017): 1–7. http://dx.doi.org/10.1155/2017/7308024.

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Solid adsorbents were prepared from corn cob that was modified with a solution of HNO3 6 M at different contact times. The solids are characterized by physical N2 adsorption at 77 K to know their surface area by applying the BET model and surface chemistry is determined using the Bohem method. Once we have prepared the adsorbents we determine the immersion enthalpy, ΔHim, of the solids in Ni(II) aqueous solutions of different concentrations between 20 and 800 mg·L−1, with values for ΔHim between 10.0 and 35.3 J·g−1. From the results obtained for the immersion enthalpy in function of the ion Ni(II) concentration we calculate the contribution to the immersion enthalpy that corresponds to the ion when it is treated with the system adsorbent-solution as a mixture in which the solid, the solvent, and the adsorbate are involved. The solution thermodynamics allows for establishing the enthalpic changes that bring the ion in function of the concentration and the intensity of the interaction of solid-metal ion that is favored by the presence of acid groups in the solid.

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6

Mansfield, S. M., and G. S. Kino. "Solid immersion microscope." Applied Physics Letters 57, no. 24 (December 10, 1990): 2615–16. http://dx.doi.org/10.1063/1.103828.

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7

Givari, Teuku Augibran, La Choviya Hawa, and Angky Wahyu Putranto. "Teknik Dehidrasi Osmosis Pada Pembuatan Manisan Kulit Jeruk." JOFE : Journal of Food Engineering 1, no. 1 (January 22, 2022): 19–32. http://dx.doi.org/10.25047/jofe.v1i1.3065.

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High consumption of oranges (Citrus sinensis) leads to the increase of orange peel waste, that’s why those orange peel waste needs to be utilized as a value-added product, such as fruit candy. Fruit candy can be produced by a process called osmotic dehydration, which is the process of immersing food material in a hypertonic solution. This research was done with Randomized Block Design to understand the effect of immersion time (2, 4, and 6 hours) and blanching time as the pretreatment (2,5, 5, and 7,5 minutes). This research was done in triplicate. The parameters that were observed are solid gain (SG), water loss (WL), weight reduction (WR), water content, and colors (L*, a*, and b*). The results indicated that the increase in immersion and blanching time causes the value of solid gain (SG) and water loss (WL) to increase, weight reduction to decrease then increase, and water content to decrease. Analysis of Variance test suggests that immersion time has a significant effect on SG, WL, WR, water content, L*, and a*. On the other hand, blanching time only significantly affects SG, WL, WR, and water content. According to Multiple Attribute Utility Theory, the best treatment in this research, regarding the results of SG, WL, WR, and water content, is the treatment with 6 hours immersion time and 7,5 minutes blanching time.

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8

Bretado-Aragón, Luis A., Dora A. Cortés-Hernández, José C. Escobedo-Bocardo, J. M. Almanza-Robles, and J. Ivan Escalante G. "In Vitro Bioactivity Assessment of Ceramics in the SiO₂–CaO–MgO System." Materials Science Forum 560 (November 2007): 35–40. http://dx.doi.org/10.4028/www.scientific.net/msf.560.35.

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Both solid-state reaction and glass-ceramic methods are used to obtain bioactive materials (CaSiO3) with different concentrations of MgO (6, 8, and 10 wt %) on the basis of the stoichiometric composition of CaO·SiO2. The in vitro bioactivity assessment is performed by immersing samples in SBF (simulated body fluids) for different periods of time. The analysis of the materials before immersion indicates the presence of different phases (akermanite, wollastonite and diopside) in the materials obtained by the solid state reaction method. It is possible to obtain wollastonite with incorporation of magnesium in its structure ((Ca, Mg)·SiO6) by the glass-ceramic method. The results obtained after immersing the samples in SBF indicate that a Ca, P-rich layer is formed on all the materials tested, even in those containing a high quantity of MgO. However, the layer formed in the MgO-free CaSiO3 ceramic is thicker than that formed in the MgO-containing materials.

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9

Hernández-Monje, Diana, Liliana Giraldo, and Juan Carlos Moreno-Piraján. "Enthalpic and Liquid-Phase Adsorption Study of Toluene–Cyclohexane and Toluene–Hexane Binary Systems on Modified Activated Carbons." Molecules 26, no. 10 (May 11, 2021): 2839. http://dx.doi.org/10.3390/molecules26102839.

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The liquid-phase adsorption of toluene in cyclohexane and hexane solutions on modified activated carbons was evaluated; the energy involved in the interaction between these solutions and the solids was determined by immersion enthalpies of pure solvents and their mixtures, and the contribution of the system constituents was calculated by differential enthalpies. The thermal treatment generated modifications that favored adsorption and interaction with the evaluated solutions, since it increased the textural parameters and the basic character of the samples. Cyclohexane could create greater competition with the adsorption sites compared to hexane, but it favored the increase in adsorption capacities (0.416 to 1.026 mmol g−1) and the interactions with the solid evaluated through the immersion enthalpies. The immersion enthalpies of pure solvents (−16.36 to −112.7 J g−1) and mixtures (−25.65 to −104.34 J g−1) had exothermic behaviors that were decreasing due to the possible displacement of solvent molecules when increasing the solute concentration in the mixtures. The differential enthalpies for toluene were negative (−18.63 to −2.14 J), mainly due to the π–π interaction with the solid, while those of the solvent–solid component tended to be positive values (−4.25 to 55.97 J) due to the displacement of the solvent molecules by those of toluene.

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10

Brunner, Robert, Margit Ferstl, Sungchul Hohng, Jeffrey O. White, Matthias Burkhardt, Alexander Pesch, and Oliver Sandfuchs. "Diffraction-based solid immersion lens." Journal of the Optical Society of America A 21, no. 7 (July 1, 2004): 1186. http://dx.doi.org/10.1364/josaa.21.001186.

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11

Fletcher, D. A., K. B. Crozier, K. W. Guarini, S. C. Minne, G. S. Kino, C. F. Quate, and K. E. Goodson. "Microfabricated silicon solid immersion lens." Journal of Microelectromechanical Systems 10, no. 3 (2001): 450–59. http://dx.doi.org/10.1109/84.946806.

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12

Kim, Myun-Sik, Toralf Scharf, Mohammad Tahdiul Haq, Wataru Nakagawa, and Hans Peter Herzig. "Subwavelength-size solid immersion lens." Optics Letters 36, no. 19 (September 30, 2011): 3930. http://dx.doi.org/10.1364/ol.36.003930.

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13

Wang, Lin, Mark C. Pitter, and Michael G. Somekh. "Wide-field high-resolution solid immersion fluorescence microscopy applying an aplanatic solid immersion lens." Applied Optics 49, no. 31 (October 29, 2010): 6160. http://dx.doi.org/10.1364/ao.49.006160.

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14

Zultiniar, Muhammad Kurnia Sandy, Ervan Wibowo, Desi Heltina, and Komalasari. "Coconut Fiber Extraction using Soda Pulping Method as Green Corrosion Inhibitor for ASTM A36 Steel." Journal of Physics: Conference Series 2049, no. 1 (October 1, 2021): 012094. http://dx.doi.org/10.1088/1742-6596/2049/1/012094.

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Abstract Currently, the corrosion inhibitor is a method that is widely used to control the corrosion rate of inner pipe in the chemical industry. This study aims to utilize coconut fiber as a green inhibitor, determine the effect of adding inhibitor concentration, immersing time, and determine the inhibition efficiency of coconut husk extract. The extraction method used is the soda pulping method with a solid to liquid ratio of 1:8 (w/v). The method used for testing the corrosion rate is the weight-loss method, UV-Vis Spectrophotometry and FT-IR are also used to analyze the lignin produced. The lowest corrosion rate was obtained in 1 M HCl corrosive medium with the addition of 3 g/L inhibitors at 48 hours immersion, which was 49.691 mpy. The highest inhibition efficiency was in 1 M HCl corrosive media solution with the addition of 3 g/L inhibitors at 48 hours immersion, which was 78.11%.

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15

Dwivedi, Bharti, and Suchitra Banerjee. "PHYSICO-CHEMICAL MONITORING OF LAKE WATER DURING IDOL IMMERSION." International Journal of Research -GRANTHAALAYAH 6, no. 7 (July 31, 2018): 159–63. http://dx.doi.org/10.29121/granthaalayah.v6.i7.2018.1294.

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The present study concerns on physicochemical monitoring of the water quality nature and the extent of pollution in lake due to idol immersion. Pre-immersion and post immersion samples were collected from lake and analyzed for various water quality parameters such as pH, turbidity, total dissolve solid (TDS), total solid (TS) total suspended solid (TSS), conductivity phosphate, dissolved oxygen (DO), BOD, COD and oil & grease. The results were compared with standards prescribed by WHO and ISI. From the study, it has been found that the values of these parameters significantly increased during the immersion period and the declined in post immersion period. However the general trend observed was: immersion> Post immersion> pre immersion.The article focused on the main pollution which is caused by plaster of Paris idols and chemical paints by idol immersion during Ganesh festival.

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16

Kalies, Grit, Peter Bräuer, and Rico Rockmann. "Analysis of Binary Adsorption Excess Isotherms at the Liquid/Solid Interface." Adsorption Science & Technology 25, no. 7 (September 2007): 493–501. http://dx.doi.org/10.1260/0263-6174.25.7.493.

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Adsorption excesses of binary liquid mixtures are the primary experimental quantity in liquid-phase adsorption onto porous or disperse solids. Binary liquid adsorption isotherms can be easily measured and allow statements to be made about the characteristics of solid and liquid mixtures, immersion behaviour at the liquid/solid interface, multi-component adsorption, etc. In this paper, a brief summary is given of different ways of interpreting and analysing binary isotherms over the whole concentration range. Experimental data and calculation examples show that thermodynamics provides a powerful tool for obtaining relevant information from such isotherms.

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17

Amanto, B. S., Samanhudi, S. Ariviani, and S. Prabawa. "Osmotic dehydration optimization of butternut squash (Cucurbita moschata Duch) using response surface methodology." Food Research 8, Supplementary 2 (April 26, 2024): 201–9. http://dx.doi.org/10.26656/fr.2017.8(s2).152.

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Butternut squash (Cucurbita moschata Duch) has a reasonably high carotene content. The flour-making process of it is related to the carotene content and antioxidant activity. It is essential to determine the optimum conditions of osmotic dehydration process by treating the concentration of the salt solution (5-15%), immersion time (60-180 mins), and stirring speed (10-40 rpm) on colour, beta-carotene content, and antioxidant activity using Response Surface Methodology (RSM) with Box-Behnken Design (BBD). All responses had a quadratic model fit (p<0.05). The R2 values are 86.7 for water loss, 84.9 for a solid gain, 96.3 for colour (ΔE), 94.3 for colour (chroma), 65.5 for beta-carotene, and 70 for antioxidant activity, respectively. The decrease in water content was strongly influenced by the salt solution concentration, stirring speed, and soaking time. However, among three factors, the salt solution concentration was the most influential. The stirring speed significantly influences the addition of solids to the material (solid gain) during the osmotic dehydration process. In contrast, ΔE and chroma were influenced by the stirring speed and immersion time for colour changes. Stirring speed influences beta-carotene levels. The amount of antioxidant activity was influenced by the stirring speed and immersion time. The optimization results obtained a salt solution concentration of 15%, a stirring speed of 25 rpm, and an immersion value of 155.8 mins. The magnitude of the three factors above provides a predictive value for water content to decrease to a maximum of 8.57%, solid gain to increase by 8.34%, beta-carotene content to decrease by 11.07% on a wet basis, antioxidant activity to decrease by 2.74, ΔE 20.22, and chroma of 71.07. The composite desirability value was 77.30%. Treating the salt concentration, soaking time, and stirring frequency affect the colour change, water loss, addition of solids, beta-carotene levels and antioxidant activity. The research finds that reducing the water content in the DO process has a significant effect, so the drying process can be carried out more quickly. In addition, the significance of the optimal conditions for the honey gourd DO process can be applied to further processing, for example, for the manufacture of industrial-scale flour

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18

Ghislain, L. P., and V. B. Elings. "Near-field scanning solid immersion microscope." Applied Physics Letters 72, no. 22 (June 1998): 2779–81. http://dx.doi.org/10.1063/1.121457.

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19

Crozier, K. B., D. A. Fletcher, G. S. Kino, and C. F. Quate. "Micromachined silicon nitride solid immersion lens." Journal of Microelectromechanical Systems 11, no. 5 (October 2002): 470–78. http://dx.doi.org/10.1109/jmems.2002.803282.

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20

Poweleit, C. D., and J. Menéndez. "Microspectroscopy Using a Solid Immersion Lens." Microscopy and Microanalysis 7, S2 (August 2001): 148–49. http://dx.doi.org/10.1017/s1431927600026817.

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Oil immersion lenses have been used in optical microscopy for a long time. The light’s wavelength is decreased by the oil’s index of refraction n and this reduces the minimum spot size. Additionally, the oil medium allows a larger collection angle, thereby increasing the numerical aperture. The SIL is based on the same principle, but offers more flexibility because the higher index material is solid. in particular, SILs can be deployed in cryogenic environments. Using a hemispherical glass the spatial resolution is improved by a factor n with respect to the resolution obtained with the microscope’s objective lens alone. The improvement factor is equal to n2 for truncated spheres.As shown in Fig. 1, the hemisphere SIL is in contact with the sample and does not affect the position of the focal plane. The focused rays from the objective strike the lens at normal incidence, so that no refraction takes place.

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21

De-Hao Chien, Chang-Heng Tsai, Shih-Shou Lo, Chii-Chang Chen, and Jenq-Yang Chang. "Solid immersion lenses in planar waveguides." Journal of Lightwave Technology 23, no. 9 (September 2005): 2746–48. http://dx.doi.org/10.1109/jlt.2005.854036.

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22

Gan, Q., G. Song, and L. Chen. "Oil-immersion or solid-immersion power enhancement of very-small-aperture lasers." Laser Physics Letters 3, no. 6 (June 1, 2006): 278–82. http://dx.doi.org/10.1002/lapl.200610005.

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23

Azoubel, P. M., and F. E. X. Murr. "Optimisation of Osmotic Dehydration of Cashew Apple (Anacardium Occidentale L.) in Sugar Solutions." Food Science and Technology International 9, no. 6 (December 2003): 427–33. http://dx.doi.org/10.1177/1082013203040908.

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Osmotic dehydration of cashew apple in sucrose and corn syrup solids solutions as influenced by temperature (30-50 C), sugar syrup concentration (40-60% w/w) and immersion time (90-240 min) was studied through response surface methodology. Responses of water loss (%) and solid gain (%) were fitted to polynomials, with multiple correlation coefficients ranging from 0.92 to 0.99. The fitted functions were optimised for maximum water loss and minimised incorporation of solids in order to obtain a product resembling non-processed fruit. Three optimum sets were selected for each solute and the ascorbic acid content was determined. The ascorbic acid losses were similar to those reported for osmotic dehydration processes.

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24

Li, Yijing, and Jernej Barbič. "Immersion of self-intersecting solids and surfaces." ACM Transactions on Graphics 37, no. 4 (August 10, 2018): 1–14. http://dx.doi.org/10.1145/3197517.3201327.

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25

Silvestre-Albero, J. "Characterization of microporous solids by immersion calorimetry." Colloids and Surfaces A: Physicochemical and Engineering Aspects 187-188, no. 1-3 (August 31, 2001): 151–65. http://dx.doi.org/10.1016/s0927-7757(01)00620-3.

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26

Knight, Brian R., A. V. Itagi, T. Rausch, C. Mihalcea, K. Pelhos, and T. E. Schlesinger. "Comatic Aberration in a Solid Immersion Mirror." Journal of the Magnetics Society of Japan 30, no. 6−2 (2006): 637–40. http://dx.doi.org/10.3379/jmsjmag.30.637.

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27

Ramsay, Euan. "Solid immersion lens applications for nanophotonic devices." Journal of Nanophotonics 2, no. 1 (December 1, 2008): 021854. http://dx.doi.org/10.1117/1.3068652.

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28

Chernomyrdin, N. V., A. S. Kucheryavenko, A. O. Schadko, G. A. Komandin, V. E. Karasik, V. V. Tuchin, and K. I. Zaytsev. "Biomedical applications of terahertz solid immersion microscopy." EPJ Web of Conferences 195 (2018): 10017. http://dx.doi.org/10.1051/epjconf/201819510017.

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29

Jaroniec, M., and R. Madey. "Enthalpy of immersion of a microporous solid." Journal of Physical Chemistry 92, no. 13 (June 1988): 3986–88. http://dx.doi.org/10.1021/j100324a059.

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30

Kim, Youngsik, Jun Zhang, and Tom D. Milster. "GaP Solid Immersion Lens Based on Diffraction." Japanese Journal of Applied Physics 48, no. 3 (March 23, 2009): 03A047. http://dx.doi.org/10.1143/jjap.48.03a047.

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31

Zhang, Bei, Cuiling Zhang, and Tianyu Xiao. "A Practical Apertometer for Solid Immersion Objective." IEEE Transactions on Instrumentation and Measurement 70 (2021): 1–8. http://dx.doi.org/10.1109/tim.2020.3035194.

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32

Stotz, J. A. H., and M. R. Freeman. "A stroboscopic scanning solid immersion lens microscope." Review of Scientific Instruments 68, no. 12 (December 1997): 4468–77. http://dx.doi.org/10.1063/1.1148416.

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33

Breitenstein, Otwin, Frank Altmann, Thorsten Riediger, and Dieter Karg. "Lock-in Infrared Microscopy with 1.4 μm Resolution Using a Solid Immersion Lens." EDFA Technical Articles 8, no. 2 (May 1, 2006): 4–13. http://dx.doi.org/10.31399/asm.edfa.2006-2.p004.

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Abstract Backside optical analysis is often aided by solid immersion lenses (SILs), but as the authors of this article explain, SILs improve the resolution of front side thermography as well. The authors describe the physics behind solid immersion lenses and provide examples that demonstrate the advantages and limitations of their use from the font side.

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34

Kamenicky, Robin, Michael Frank, Dimitris Drikakis, and Konstantinos Ritos. "Film Boiling Conjugate Heat Transfer during Immersion Quenching." Energies 15, no. 12 (June 9, 2022): 4258. http://dx.doi.org/10.3390/en15124258.

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Boiling conjugate heat transfer is an active field of research encountered in several industries, including metallurgy, power generation and electronics. This paper presents a computational fluid dynamics approach capable of accurately modelling the heat transfer and flow phenomena during immersion quenching: a process in which a hot solid is immersed into a liquid, leading to sudden boiling at the solid–liquid interface. The adopted methodology allows us to couple solid and fluid regions with very different physics, using partitioned coupling. The energy equation describes the solid, while the Eulerian two-fluid modelling approach governs the fluid’s behaviour. We focus on a film boiling heat transfer regime, yet also consider natural convection, nucleate and transition boiling. A detailed overview of the methodology is given, including an analytical description of the conjugate heat transfer between all three phases. The latter leads to the derivation of a fluid temperature and Biot number, considering both fluid phases. These are then employed to assess the solver’s behaviour. In comparison with previous research, additional heat transfer regimes, extra interfacial forces and separate energy equations for each fluid phase, including phase change at their interface, are employed. Finally, the validation of the computational approach is conducted against published experimental and numerical results.

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35

Chernomyrdin, N. V., M. Skorobogatiy, D. S. Ponomarev, V. V. Bukin, V. V. Tuchin, and K. I. Zaytsev. "Terahertz solid immersion microscopy: Recent achievements and challenges." Applied Physics Letters 120, no. 11 (March 14, 2022): 110501. http://dx.doi.org/10.1063/5.0085906.

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Unique effects of terahertz (THz)-wave–matter interaction push rapid progress in THz optoelectronics aimed at bridging the problematic THz gap. However, majority of modern methods of THz spectroscopy and imaging are still hampered by low spatial resolution. Common lens/mirror-based THz optics fails to overcome the Abbe barrier and usually provides resolution larger than a free-space wavelength λ (i.e., hundreds of micrometers or even few millimeters). To mitigate this difficulty, supperresolution THz imaging modalities were introduced recently, among which we particularly underline different methods of THz scanning-probe near-field microscopy. They not only rely on strong light confinement on sub-wavelength probes and provide resolution down to [Formula: see text]–[Formula: see text] but also suffer from small energy efficiency or presume an interplay among imaging resolution, signal-to-noise ratio, and performance. In this paper, we consider reflection-mode THz solid immersion (SI) microscopy that offers some compromise between the high imaging resolution of [Formula: see text] and high energy efficiency, which is due to the absence of any subwavelength probe in an optical scheme. Recent achievements, challenging problems, and prospects of SI microscopy are overviewed with an emphasis on resolving the inverse problem and applications in THz biophotonics.

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36

HAMIN, H. J., B. D. TERRIS, and D. RUGAR. "OPTICAL DATA STORAGE USING A SOLID IMMERSION LENS." Journal of the Magnetics Society of Japan 19, S_1_MORIS_94 (1995): S1_409–412. http://dx.doi.org/10.3379/jmsjmag.19.s1_409.

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37

Ghislain, L. P., V. B. Elings, K. B. Crozier, S. R. Manalis, S. C. Minne, K. Wilder, G. S. Kino, and C. F. Quate. "Near-field photolithography with a solid immersion lens." Applied Physics Letters 74, no. 4 (January 25, 1999): 501–3. http://dx.doi.org/10.1063/1.123168.

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38

Zhang, Shuyan, Alexander Soibel, Sam A. Keo, Daniel Wilson, Sir B. Rafol, David Z. Ting, Alan She, Sarath D. Gunapala, and Federico Capasso. "Solid-immersion metalenses for infrared focal plane arrays." Applied Physics Letters 113, no. 11 (September 10, 2018): 111104. http://dx.doi.org/10.1063/1.5040395.

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39

Lang, Matthew, Tom D. Milster, Takahisa Minamitani, and Gregg Borek. "Investigation of Micro Solid Immersion Lens Mounting Systems." Japanese Journal of Applied Physics 46, no. 6B (June 22, 2007): 3737–40. http://dx.doi.org/10.1143/jjap.46.3737.

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40

Chen, Rui, Krishna Agarwal, Colin J. R. Sheppard, Jacob C. H. Phang, and Xudong Chen. "Resolution of aplanatic solid immersion lens based microscopy." Journal of the Optical Society of America A 29, no. 6 (May 30, 2012): 1059. http://dx.doi.org/10.1364/josaa.29.001059.

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41

Peng, Chubing, Christophe Mihalcea, Kalman Pelhos, and William A. Challener. "Focusing characteristics of a planar solid-immersion mirror." Applied Optics 45, no. 8 (March 10, 2006): 1785. http://dx.doi.org/10.1364/ao.45.001785.

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Zhang, Yaoju. "Design of high-performance supersphere solid immersion lenses." Applied Optics 45, no. 19 (July 1, 2006): 4540. http://dx.doi.org/10.1364/ao.45.004540.

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Zhang, J., C. W. See, and M. G. Somekh. "Imaging performance of widefield solid immersion lens microscopy." Applied Optics 46, no. 20 (June 20, 2007): 4202. http://dx.doi.org/10.1364/ao.46.004202.

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Gambin, Yann, Olivier Legrand, and Stephen R. Quake. "Microfabricated rubber microscope using soft solid immersion lenses." Applied Physics Letters 88, no. 17 (April 24, 2006): 174102. http://dx.doi.org/10.1063/1.2194477.

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Lu, Yang, Thomas Bifano, Selim Ünlü, and Bennett Goldberg. "Aberration compensation in aplanatic solid immersion lens microscopy." Optics Express 21, no. 23 (November 8, 2013): 28189. http://dx.doi.org/10.1364/oe.21.028189.

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Chernomyrdin, Nikita V., Aleksander O. Schadko, Sergey P. Lebedev, Viktor L. Tolstoguzov, Vladimir N. Kurlov, Igor V. Reshetov, Igor E. Spektor, Maksim Skorobogatiy, Stanislav O. Yurchenko, and Kirill I. Zaytsev. "Solid immersion terahertz imaging with sub-wavelength resolution." Applied Physics Letters 110, no. 22 (May 29, 2017): 221109. http://dx.doi.org/10.1063/1.4984952.

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Lin, Chun-Hung, Yu-Chu Lin, and Chia-Ching Liang. "Solid immersion interference lithography with conformable phase mask." Microelectronic Engineering 123 (July 2014): 136–39. http://dx.doi.org/10.1016/j.mee.2014.07.005.

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Fletcher, Daniel. "THERMAL MICROSCOPY WITH A MICROFABRICATED SOLID IMMERSION LENS." Microscale Thermophysical Engineering 7, no. 4 (January 2003): 267–73. http://dx.doi.org/10.1080/10893950390245985.

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Yano, T., S. Shibata, and T. Kishi. "Fabrication of micrometer-size glass solid immersion lens." Applied Physics B 83, no. 2 (March 24, 2006): 167–70. http://dx.doi.org/10.1007/s00340-006-2178-1.

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Triyono, T., N. Muhayat, A. Supriyanto, and L. Lutiyatmi. "Effect of Degassing Treatment on the Interfacial Reaction of Molten Aluminum and Solid Steel." Archives of Foundry Engineering 17, no. 2 (June 27, 2017): 227–39. http://dx.doi.org/10.1515/afe-2017-0080.

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Abstract:

AbstractThe gas porosity is one of the most serious problems in the casting of aluminum. There are several degassing methods that have been studied. During smelting of aluminum, the intermetallic compound (IMC) may be formed at the interface between molten aluminum and solid steel of crucible furnace lining. In this study, the effect of degassing treatment on the formations of IMC has been investigated. The rectangular substrate specimens were immersed in a molten aluminum bath. The holding times of the substrate immersions were in the range from 300 s to 1500 s. Two degassing treatments, argon degassing and hexachloroethane tablet degassing, were conducted to investigate their effect on the IMC formation. The IMC was examined under scanning electron microscope with EDX attachment. The thickness of the IMC layer increased with increasing immersion time for all treatments. Due to the high content of hydrogen, substrate specimens immersed in molten aluminum without degasser had IMC layer which was thicker than others. Argon degassing treatment was more effective than tablet degassing to reduce the IMC growth. Furthermore, the hard and brittle phase of IMC, FeAl3, was formed dominantly in specimens immersed for 900 s without degasser while in argon and tablet degasser specimens, it was formed partially.

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