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  • 1
    Online Resource
    Online Resource
    Cham :Springer International Publishing AG,
    Keywords: Nanotechnology. ; Electronic books.
    Type of Medium: Online Resource
    Pages: 1 online resource (376 pages)
    Edition: 1st ed.
    ISBN: 9783319249902
    Series Statement: Springer Series in Materials Science Series ; v.229
    Language: English
    Note: Intro -- Preface -- Contents -- Contributors -- 1 Ordered Responsive Materials for Sensing Applications -- Abstract -- 1.1 Introduction -- 1.2 One-Dimensional Ordered Materials -- 1.3 Two-Dimensional Ordered Materials -- 1.4 Three-Dimensional Ordered Materials -- 1.5 Other Noteworthy Photonic Materials for Sensing -- 1.6 Summary -- Acknowledgements -- References -- 2 Stimulus-Responsive Colored Materials for Sensing and Display Devices -- Abstract -- 2.1 Introduction -- 2.2 Stimulus-Responsive Structurally Colored Materials Using Colloidal Crystals -- 2.3 Stimulus-Responsive Structurally Colored Materials Using Colloidal Amorphous Arrays with Short-Range Order -- 2.4 Angle-Independent Colored Materials Using the Christiansen Effect -- 2.5 Conclusions -- References -- 3 Colloidal Photonic Crystals for Sensor Applications -- Abstract -- 3.1 Self-assembled Colloidal Crystals -- 3.1.1 Close-Packed Colloidal Crystals -- 3.1.2 Non-close-Packed Colloidal Crystals -- 3.2 Properties of Colloidal Crystals and Their Derivatives -- 3.2.1 Optical Property -- 3.2.2 Mechanical Property -- 3.3 Stimuli-Responsive Materials -- 3.3.1 Responsive Colloids -- 3.3.2 Responsive Matrix -- 3.4 Formats of Photonic Structures -- 3.4.1 Planar Films -- 3.4.2 Cylindrical Fibers -- 3.4.3 Spherical Granules -- 3.5 Sensor Applications -- 3.5.1 Refractive Index Sensors -- 3.5.2 Strain Sensors -- 3.5.3 Temperature Sensors -- 3.5.4 Ionic Strength and pH Sensors -- 3.5.5 Detection of Specific Ions and Small Molecules -- 3.5.6 Detection of Large Biomolecules -- 3.6 Summary and Outlook -- References -- 4 Responsive Photonic Gels Based on Block Copolymers -- Abstract -- 4.1 Introduction -- 4.2 Fundamentals of Photonic Crystals -- 4.3 Preparation of Photonic Gels -- 4.3.1 Self-assembly of Block Copolymers -- 4.3.2 Block Copolymer Photonic Gels by Swelling with Diluents. , 4.4 Stimuli Responsive Photonic Gels -- 4.4.1 Chemochromic Photonic Gels -- 4.4.2 Mechano-, Thermochromic Photonic Gels -- 4.4.3 Electrochromic Photonic Gels -- 4.4.4 Photochromic Photonic Gels -- 4.5 Summary and Outlook -- References -- 5 Photonic Crystals Fabricated via Facile Methods and Their Applications -- Abstract -- 5.1 Introduction -- 5.2 Photonic Crystals Simply Fabricated -- 5.2.1 One-Dimensional Photonic Crystals (1DPC) Prepared by Spin-Coating -- 5.2.1.1 Alternate Organic Layer Packs -- 5.2.1.2 Periodical Inorganic Layer Packs -- 5.2.1.3 Organic-Inorganic Hybrid Packs -- 5.2.2 Two-Dimensional Photonic Crystals (2DPC) Evolved by Colloidal Chemistry -- 5.2.2.1 Colloidal Lithography -- 5.2.2.2 Colloidal Self Assembly -- 5.2.3 Three-Dimensional Photonic Crystals (3DPC) Fabricated via the Assembly of Colloidal Crystal and Other Facile Methods -- 5.2.3.1 3DPCs Possess Opal or Woodpile-like Structures -- Woodpile Type 3DPCs -- Opal Type 3DPC -- 5.2.3.2 3D Photonic Crystals Perform Inverse Opal or Inverse Woodpile Structures -- Inverse Opal 3DPC -- Inverse Woodpile 3DPC -- 5.3 Applications of Photonic Crystals -- 5.3.1 Photonic Crystals Used in the Field of Display -- 5.3.1.1 Photonic Crystals Integrated in LED to Enhance Light Extraction -- 5.3.1.2 Two-Dimensional Structures for Antireflective Surfaces (ARS) -- 5.3.1.3 Photonic Crystals Used for Fluorescence Enhancement -- 5.3.1.4 Full Color Display and Photonic Paper Based on Photonic Crystals -- 5.3.2 Photonic Crystals Used for Sensing -- 5.3.2.1 Physical Sensors -- Temperature Measuring -- Mechanical Sensor -- 5.3.2.2 Chemical Sensor -- pH Responsive -- Vapor Sensing -- Ion Detector -- Humidity Sensor -- Organic Solvents Analyzing -- Specific Chemical Substance Analysis -- 5.3.2.3 Biological Sensors -- DNA Sensing -- Protein Detecting -- Toxin, Bacteria, and Viral Analyzing. , 5.4 Summary and Perspectives -- References -- 6 Photonic Crystal Based Anti-Counterfeiting Materials -- Abstract -- 6.1 Introduction -- 6.2 Photonic Printing Based on the Tuning of Photonic Structures -- 6.3 Photonic Prints with Angular Dependent Structural Colors -- 6.3.1 Angular Dependent Effect in Photonic Crystal Patterns -- 6.3.2 Orientational Printing -- 6.4 Invisible Photonic Prints -- 6.4.1 Invisible Photonic Prints Shown by Water -- 6.4.2 Invisible Photonic Prints Shown by Deformation -- 6.4.3 Invisible Photonic Prints Shown by Magnetic Interaction -- 6.5 Photonic Crystal Based Codec -- References -- 7 Photonic Crystals as Robust Label-Free Biosensors -- Abstract -- 7.1 Introduction -- 7.2 1D-PhCs in Biosensing -- 7.3 Design, Development, and Optimization of 2D-PhCs -- 7.4 Biosensing with 2D-PhCs -- 7.5 Enhancing Sensitivity Through Directed Functionalization -- 7.6 Current Challenges and Future Outlook for 2D-PhCs -- References -- 8 Sensing on Single Plasmonics -- Abstract -- 8.1 Introduction -- 8.2 Morphology and Composition Modulated Sensors -- 8.3 Inter-particle Coupling -- 8.4 Plasmon Resonance Energy Transfer -- 8.5 Spectroelectrochemistry -- 8.6 Conclusions and Future Prospects -- References -- 9 Whispering Gallery Mode Devices for Sensing and Biosensing -- Abstract -- 9.1 Introduction -- 9.2 Theory of WGMs in Cylindrical and Spherical Geometries -- 9.2.1 Two-Layer Structures -- 9.2.2 Three-Layer Structures -- 9.3 Sensitivity and Detection Limits -- 9.3.1 Disk or Fiber -- 9.4 Surface Chemistry for Biosensing -- 9.4.1 Grafting or Covalent Binding -- 9.4.2 Physisorption -- 9.5 Fluorescent Microspheres, Fibers, and Capillaries -- 9.6 Microdisks and Toroids -- 9.6.1 Refractive Index Sensing -- 9.6.2 Displacement Sensors -- 9.6.3 Gas Sensors -- 9.6.4 Gamma-Ray Sensors -- 9.6.5 Surface Curvature Sensors -- 9.6.6 Biosensors. , 9.7 WGM Sensors: Comparison with Competing Technologies -- 9.7.1 Mass Spectroscopy -- 9.7.2 Electrochemical Methods -- 9.7.3 Optical Methods -- 9.7.4 Biosensing Technologies for Medical Diagnostics -- 9.8 Outlook -- Acknowledgments -- References -- 10 High Sensitivity Polymer Fibre Bragg Grating Sensors and Devices -- Abstract -- 10.1 Introduction -- 10.2 Polymer Optical Fibres -- 10.3 Polymer Fibre Bragg Gratings -- 10.3.1 POF Grating Fabrication -- 10.3.2 Polymer Micro-fibre Bragg Gratings -- 10.3.3 Polymer FBG Arrays -- 10.4 Characteristic Properties of Polymers Fibre Bragg Grating -- 10.4.1 Etching the POF Gratings -- 10.4.2 Temperature Sensitivity -- 10.4.3 Pressure Sensitivity -- 10.4.4 Strain Sensitivity -- 10.5 Applications of Polymer Fibre Bragg Grating -- 10.5.1 Force and Pressure Sensors -- 10.5.2 Humidity Sensors -- 10.5.3 Biochemical Concentration Sensor -- 10.5.4 Composite Materials with Embedded Polymer FBGs -- 10.6 Conclusions -- References -- 11 Photonic Materials for Holographic Sensing -- Abstract -- 11.1 Introduction -- 11.1.1 The Need for Rapid Tests for Environmental Sensing and Medical Diagnostics -- 11.1.2 Advantages of Holographic Sensors -- 11.2 Fundamentals of Holographic Sensors -- 11.2.1 Principle of Recording of the Holographic Structures -- 11.2.2 Types of Holographic Sensors -- 11.2.2.1 Sensors Based on Reflection Holograms -- 11.2.2.2 Sensors Based on Transmission Holograms -- 11.2.3 Holographic Recording by Ultra-Short Laser Pulses -- 11.3 Holographic Sensing Materials -- 11.3.1 Photonic Materials in Sensing Applications -- 11.3.1.1 Silver Halide Chemistry -- 11.3.1.2 Photopolymer Chemistry -- 11.3.1.3 Sensors Containing Zeolite Nanoparticles -- 11.3.2 Strategies for Materials Functionalization -- 11.3.2.1 Structures with Redistributed Analyte-Sensitive Species. , 11.3.2.2 Structures with No Redistribution of the Analyte Sensitive Species -- 11.3.2.3 Functionalization Strategies Based on the Hydrophobicity and Hydrophilicity of the Recording Material -- 11.3.3 Design of Sensors by Dynamic Simulations of the Properties of a Multilayer Structure -- 11.4 Applications -- 11.4.1 Sensors for Gas Phase Analyte -- 11.4.1.1 O2, N2, Alkanes, Alkenes, Alkynes, and NH3 -- 11.4.1.2 Zeolite Nanoparticle Doped Sensors for the Detection of Alcohols -- 11.4.1.3 Humidity Sensors -- 11.4.2 Temperature Sensors -- 11.4.3 Pressure Sensors -- 11.4.4 Ions Sensors -- 11.4.4.1 H+ -- 11.4.4.2 Monovalent Metal Ions -- 11.4.4.3 Divalent Metal Ions -- 11.4.5 Glucose Sensors -- 11.5 Future Directions -- 11.6 Conclusions -- References -- Index.
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  • 2
    In: Quaternary international, Oxford [u.a.] : Pergamon Press, 1989, 135(2005), Seite 131-137, 1040-6182
    In: volume:135
    In: year:2005
    In: pages:131-137
    Type of Medium: Article
    ISSN: 1040-6182
    Language: Undetermined
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  • 3
    Publication Date: 2023-02-23
    Description: Radiolarians are planktonic protozoon that play an important role in marine ecosystem and paleoenvironmental construction. The South China Sea (SCS) and Malacca Strait (MLS), strongly influenced by the East Asian monsoon, are the key gateway between the Pacific and Indian Oceans. However, a few plankton studies of radiolarians are performed during winter and spring in the SCS and MLS due to the adverse sea conditions. In this study the use of a ship-board plankton net rendered it possible to obtain shallow water samples (~5 m depth) along transects from the northern SCS to MLS during the spring of 2017 and winter of 2017-2018. The results show that partitioning among Spumellaria, Nassellaria and Collodaria radiolarians differed spatially and seasonally. The high partition of Collodaria and low partition of Nassellaria are potential indicators of the strongly stratified waters with low nutrients for paleoceanographic studies in the slope and basin SCS. The radiolarian assemblages in the MLS are quite different from those in the SCS, that is, the two communities are largely independent, suggesting that advective transport between the MLS and SCS is rare. There are obvious seasonal variations in species diversity and abundance in both the MLS and SCS, generally with higher biodiversity and maximum abundances in winter. The results of Q-mode cluster analysis showed that radiolarian assemblages during winter were grouped together in the slope and basin SCS, and their distributions had moved to the southwest relative to those in spring. The results demonstrate the East Asian monsoon has a significant controlling effect on radiolarian diversity and geographic distribution in the studied areas. We also established five candidates for weakly stratified waters with high nutrients: Archiperidium hexacantha, Acanthodesmia vinculatus, Peromelissa phalacra, Dictyocoryne muelleri, and Tetrapyle octacantha. Thus, this study increases the knowledge of radiolarian geographic distribution in the tropics as a whole, as well as revealing the sensitive response of radiolarians to the regional environments, a fact which may prove useful for reconstructing the paleoceanographic changes.
    Keywords: Acanthodesmia vinculata; Acrobotrissa cf. cribrosa; Actinomma arcadophorum; Amphispyris hertwigi; Amphispyris reticulata; Arachnocorys circumtexta; Arachnosphaera myriacantha; Archiperidium hexacantha; Astrosphaera hexagonalis; Biodiversity; Botryocyrtis scutum; Buccinosphaera invaginata; Centrocubus octostylus; Counting, radiolarians; Dictyoceras virchowii; Dictyocoryne elegans; Dictyocoryne muelleri; Dictyocoryne profunda; Dictyocoryne truncatum; Dictyocryphalus? acrostoma; Dictyocryphalus? democriti; Dictyocryphalus? variabilis; Didymocyrtis tetrathalamus tetrathalamus; East Asian monsoon; Eucyrtidium acuminatum; Event label; Flustrella perispira; Geographic distribution; Heliodiscus spp.; Identification; LATITUDE; Lipmanella prismaticum; Living radiolarians; LONGITUDE; Myelastrum lobum; Neosemantis distephanus; Perichlamydium venustum; Peromelissa phalacra; Phorticium polycladum; Plectacantha oikiskos; Plegmosphaerella spongiacea; Pseudocubus obeliscus; Pterocanium praetextum praetextum; Pterocorys fastuosa; Pterocorys sabae; Pylodiscus spinulosa; Radiolarians indeterminata; Rhizosphaera medianum; SCS/MS_1; SCS/MS_11; SCS/MS_13; SCS/MS_15; SCS/MS_16; SCS/MS_17; SCS/MS_18; SCS/MS_2; SCS/MS_20; SCS/MS_22; SCS/MS_23; SCS/MS_25; SCS/MS_27; SCS/MS_28; SCS/MS_30; SCS/MS_31; SCS/MS_4; SCS/MS_5; SCS/MS_7; SCS/MS_72; SCS/MS_74; SCS/MS_76; SCS/MS_77; SCS/MS_78; SCS/MS_80; SCS/MS_82; SCS/MS_84; SCS/MS_86; SCS/MS_88; SCS/MS_9; SCS/MS_90; SCS/MS_92; SCS/MS_94; SCS/MS_96; Siphonosphaera abyssi; South China Sea; Sphaerolarnacillium cochleatum; Sphaeropylolena spp.; Sphaerozoum bifurcum; Spirocyrtis scalaris; Spongaster pentas; Spongaster tetras tetras; Spongastriscus ellipticus; Spongocyclia cycloides; Spongodiscus heliodes; Spongodiscus resurgens; Spongosphaera streptacantha; Spongospira sp.; Stylodictya arathnia; Stylodictya cf. hertwigii; Tetrapyle circularis; Tetrapyle fruticosa; Tetrapyle octacantha; Tetrapyle spp.; Time coverage; tropics; Water sample; WS; Zygocircus acacia; Zygocircus piscicaudatus; Zygocircus productus
    Type: Dataset
    Format: text/tab-separated-values, 2142 data points
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  • 4
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 2929-2937 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Computational solutions to the Rayleigh–Taylor fluid mixing problem, as modeled by the two-fluid two-dimensional Euler equations, are presented. Data from these solutions are analyzed from the point of view of Reynolds averaged equations, using scaling laws derived from a renormalization group analysis. The computations, carried out with the front tracking method on an Intel iPSC/860, are highly resolved and statistical convergence of ensemble averages is achieved. The computations are consistent with the experimentally observed growth rates for nearly incompressible flows. The dynamics of the interior portion of the mixing zone is simplified by the use of scaling variables. The size of the mixing zone suggests fixed-point behavior. The profile of statistical quantities within the mixing zone exhibit self-similarity under fixed-point scaling to a limited degree. The effect of compressibility is also examined. It is found that, for even moderate compressibility, the growth rates fail to satisfy universal scaling, and moreover, increase significantly with increasing compressibility. The growth rates predicted from a renormalization group fixed-point model are in a reasonable agreement with the results of the exact numerical simulations, even for flows outside of the incompressible limit.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Palo Alto, Calif. : Annual Reviews
    Annual Review of Environment and Resources 27 (2002), S. 397-431 
    ISSN: 1056-3466
    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
    Topics: Energy, Environment Protection, Nuclear Power Engineering
    Notes: Abstract China is rapidly developing as evidenced by enhanced urbanization and industrialization and greatly increased energy consumption. However, these have brought Chinese cities a variety of urban air pollution problems in recent decades. During the 1970s, black smoke from stacks became the characteristic of Chinese industrial cities; in the 1980s, many southern cities began to suffer serious acid rain pollution; and recently, the air quality in large cities has deteriorated due to nitrous oxides (NOx), carbon monoxide (CO), and photochemical smog, which are typical of vehicle pollution. Some cities now have a mixture of these. Urban air pollution influences both the health of citizens and the development of cities. To control air pollution and protect the atmospheric environment, the Chinese government has implemented a variety of programs. This paper first reviews the current status of air quality in Chinese cities, especially key cities, then describes the characteristics of some major urban air pollutants, including total suspended particles (TSP), respirable particles 10 microns or less in diameter (PM10), very fine particles 2.5 microns or less in diameter (PM2.5), sulfur dioxide (SO2), acid rain, NOx, and photochemical smog. Two specific topics, SO2 and acid rain control and vehicle emission control, are used to illustrate the actions that the government has taken and future plans. Finally, a case study of the Chinese capital, Beijing, is presented with a discussion of its main air pollution problems, recently implemented control measures and their effects, and future strategies for urban air quality improvement.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 8 (1996), S. 816-825 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The Rayleigh–Taylor instability of an interface separating fluids of distinct density is driven by an acceleration across the interface. Low order statistical moments of fluctuating fluid quantities characterize the hydrodynamics of the mixing zone. A new model is proposed for the momentum coupling between the two phases. This model is validated against computational data for compressible flows, including flows near the incompressible limit. Our main result is a zero parameter first order closure for ensemble averaged two phase flow equations. We do not, however, fully solve the closure problem, as the equations we derive are missing an (internal) boundary condition along any surface for which either phase goes to zero volume fraction. In this sense, the closure problem is reduced from a volume to a surface condition, rather than being solved completely. We compare two formulations of the statistical moments, one based on two phase flow and the other on turbulence models. These formulations describe different aspects of the mixing process. For the problem considered, the two phase flow moments appear to be preferable, in that they subsume the turbulence moments but not conversely. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 9 (1997), S. 1106-1124 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A shock driven material interface between two fluids of different density is unstable. This instability is known as Richtmyer–Meshkov (RM) instability. In this paper, we present a quantitative nonlinear theory of compressible Richtmyer–Meshkov instability in two dimensions. Our nonlinear theory contains no free parameter and provides analytical predictions for the overall growth rate, as well as the growth rates of the bubble and spike, from early to later times for fluids of all density ratios. The theory also includes a general formulation of perturbative nonlinear solutions for incompressible fluids (evaluated explicitly through the fourth order). Our theory shows that the RM unstable system goes through a transition from a compressible and linear one at early times to a nonlinear and incompressible one at later times. Our theoretical predictions are in excellent agreement with the results of full numerical simulations from linear to nonlinear regimes. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 1167-1181 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Linearized Euler equations of a general stationary multiple layer stratified system for both compressible and incompressible inviscid fluids are analyzed. The main result is that many features of a multilayer system are universal, in the sense they do not depend on such details as the number of layers, their thicknesses, equations of state for the fluids, and equilibrium density distributions. Necessary and sufficient conditions of stability are determined. For compressible fluids, it is possible for the system to be unstable even if there is no density inversion anywhere. It is shown that a compressible system is always more unstable than the corresponding incompressible one. A universal upper bound for the growth rate for a given perturbation wave number is given. General Rayleigh–Taylor unstable modes are characterized, and the range of unstable wave numbers is determined. Properties of stable modes are discussed. Numerical algorithms for solving the eigenvalue problem of the set of linearized Euler equations are given.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 1856-1873 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This paper presents a new analysis of small amplitude Richtmyer–Meshkov instability. The linear theory for the case of reflected rarefaction waves, a problem not treated in previous work, is formulated and numerically solved. This paper also carries out a systematic comparison of Richtmyer's impulsive model to the small amplitude theory, which has identified domains of agreement as well as disagreement between the two. This comparison includes both the reflected shock and reflected rarefaction cases. Additional key results include the formulation of criteria determining the reflected wave type in terms of preshocked quantities, identification of parameter regimes corresponding to total transmission of the incident wave, discussion of an instability associated with a rarefaction wave, investigation of phase inversions and the related phenomenon of freeze-out, and study of the sensitivity of the numerical solutions to initial conditions.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 10 (1998), S. 974-992 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: As an incident shock wave hits a material interface between two fluids of different densities, the interface becomes unstable. Small disturbances at the interface start to grow. This interfacial instability is known as a Richtmyer–Meshkov (RM) instability. It plays an important role in the studies of inertial confinement fusion and supernova. The majority of studies of the RM instability were in plane geometry—namely, plane shocks in Cartesian coordinates. We present a systematic numerical study of the RM instability driven by cylindrical shocks for both the imploding and exploding cases. The imploding (exploding) case refers to a cylindrical shock colliding with the material interface from the outside in (inside out). The phenomenon of reshock caused by the waves reflected from the origin is also studied. A qualitative understanding of this system has been achieved. Detailed studies of the growth rate of the fingers at the unstable interface are presented. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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