Saturday, February 28, 2009

Moving Boundaries and Interfaces

Moving Boundaries and Interfaces

Many physical problems involve moving boundaries. Dynamic
boundaries change position and shape in response to the
particular physics at work: examples are breaking waves in
the ocean, dancing flames in the fireplace, and milk
swirling in a cup of tea. Static boundaries, such as tumors
in medical scans and cartoon characters against a background
animation, can be just as perplexing: try finding edges in a
picture of a dalmatian lying on a rug with spots!
Surprisingly, many other interesting problems, such as
negotiating a robot around obstacles and finding the
shortest path over a mountain range, can also be cast as
evolving boundary problems.

The physics and chemistry that drive a boundary or
interface may be difficult to describe, but even when the
speed and direction of a moving interface are well
understood, following its shape can be difficult. The first
concern is what to do when sharp corners appear, as they do
in, for example, the intricate patterns of a snowflake.
Second, distant edges can blend together: the "edge" of a
forest fire changes as separate fires burn together and
sparks carried by the wind ignite distant regions. Finally,
in three dimensions (and higher), even finding a nice way to
represent---let alone move---an undulating boundary is a
challenge.

One technologically important example of interface
motion involves the manufacture of computer chips. In the
etching and deposition process, a layer of metal is
deposited on a silicon wafer, etched away, and then the
process is repeated numerous times until a final profile is
obtained. As device sizes get smaller and smaller, using
trial and error to obtain the correct design becomes
impractical. Instead, one would like to simulate these
processes as accurately as possible in order to test various
layering strategies and resulting device characteristics.
In recent years, the application of new mathematical and
numerical algorithms for interface motion has afforded real
breakthroughs in this area. Before these techniques, complex
problems involving the evolution of profiles in two
dimensions were difficult; now, fully three-dimensional
simulations involving a wide range of physical effects are
easily within grasp. The new algorithms have been
incorporated into the simulation packages at many major
semiconductor manufacturers in the United States, and are
part of the production environment in various chip lines
today.

These computational techniques, known as level set
methods and fast marching methods, rest on a fundamental
shift in how evolving fronts are viewed. Rather than focus
on the evolving front itself, these techniques discretize
the region in which the front moves. Each point in that
space keeps track of either its distance to the front or of
the time when the front passes over it; the accumulation of
all this information gives an accurate portrait of the
moving interface. The key is to define equations for the
time at which the front passes over each point and then to
solve these equations.

The equations which keep track of the front at each
grid point in the domain are variants of the Hamilton-Jacobi
equations; these equations have a long history in such areas
as optics, wave propagation, and control theory. While they
can be very complex, their derivatives bear a resemblance to
hyperbolic conservation laws and to the equations of fluid
mechanics, allowing use of the knowledge acquired in those
well-developed fields. The main breakthrough in modeling
interface motion was the realization that schemes from fluid
mechanics could be unleashed onto the equations of moving
fronts. The result is a wide range of computational tools
for tracking evolving interfaces with sharp corners and
cusps, with topological changes, and in the presence of
three-dimensional complications. These schemes have found
their way into a vast number of applications, including
fluid mechanics, dendrite solidification and the freezing of
materials, image processing, medical imaging, combustion,
and robotic navigation.

Some of the most complex interface applications appear
in simulating the manufacture of computer chips. To begin,
a single crystal ingot of silicon is extracted from molten
pure silicon. This silicon ingot is then sliced into
several hundred thin wafers, each of which is polished to a
smooth finish. A thin layer of crystalline silicon is
oxidized, a light-sensitive "photoresist" is applied, and
the wafer is covered with a pattern mask that shields part
of the photoresist. This pattern mask contains the layout of
the circuit itself. Under exposure to a light or an electron
beam, the unshielded photoresist polymerizes and hardens,
leaving an unexposed material that is etched away in a dry
etch process, revealing a bare silicon dioxide layer.
Ionized impurity atoms such as boron, phosphorus, and argon
are implanted into the pattern of the exposed silicon wafer,
and silicon dioxide is deposited at reduced pressure in a
plasma discharge from gas mixtures at a low temperature.
Finally, thin films like aluminum are deposited by processes
such as plasma sputtering, and contacts to the electrical
components and component interconnections are established.
The result is a device that carries the desired electrical
properties.

This sequence of events produces considerable changes
in the surface profile as it undergoes various processes of
etching and deposition. Describing these changes is known
as the "surface topography problem" in microfabrication and
requires an analysis of the effects of many factors, such as
the visibility of the etching/deposition source from each
point of the evolving profile, surface diffusion along the
front, complex flux laws that produce faceting, shocks and
rarefactions, material-dependent discontinuous etch rates,
and masking profiles. The physics and chemistry that
contribute to the motion of the interface are areas of
active research. Once empirical models are formulated, one
is left with the problem of tracking the evolving front.

Here is where level set methods and fast marching
methods come into play: they provide the means to follow the
evolving profile as it is shaped by the etching and
deposition process, and they capture some of the most subtle
effects. For example, visibility has a key role; if part of
the evolving surface causes a shadow zone that blocks the
effects of the etching or deposition beam, the motion is
reduced. Computing this shadow zone was formerly a very
expensive proposition; however, the fast marching method
yields an elegant and fast way to do it.

Another example is the complex manufacturing process
called ion-milling, in which a beam of reactive ions acts
like a sandblaster and etches away at a surface. The etching
rate depends on, among other things, the angle at which the
beam hits the surface. The most effective etching angle is
not always directly straight down; the "yield function"
relates how much material is removed to the incoming angle.
Interestingly enough, this process produces beveled, rounded
edges in some areas and sharp cusps in others. While these
are difficult problems to model, they are easily handled by
level set and fast marching methods.

4 Education

The importance of strong ties between mathematics and
science is self-evident from the examples presented---which,
we stress again, are only a tiny sample from a very large
pool. Unfortunately, there is a clear shortage of people
able to bridge the gap between mathematics and the sciences,
and one of the challenges that must be faced is how to
educate more.

It is obvious to us that students of mathematics should
be able to understand problems in science, and that students
of science should understand the power and roles of
mathematics. Each area of science has its own unique
features, but the different areas share common features that
are often of a mathematical nature.

The themes of modeling, computation, and problem
solving are especially relevant to education.

- Modeling. Students in science and mathematics need to
be educated in modeling far beyond the simple paradigm
exemplified by ``do this experiment, plot the data, and
observe that they lie almost on a straight line''. Given a
physical problem and/or data, students should learn to
construct a mathematical model, explain why the model is
appropriate, perform mathematical analysis or a
computational simulation, devise experiments to check the
accuracy of their model, and then improve the model and
repeat the process.
- Computation. The view that ``anyone can compute'' is
just as wrong as the statement that ``anyone can build a
telescope''. One has to learn how. Much of the current
teaching of computation is flawed; a ``cookbook'' strategy
of using canned programs without attention to fundamentals
is completely inadequate. At the other extreme, scientists
should not waste their time implementing outmoded methods or
reinventing known algorithms and data structures. Students
in science and mathematics need to be aware of the
intellectual content and principles of modern computer
science.
- Problem-solving. In traditional academic presentations
of scientific and mathematical problems, the context is
stripped away and simplified so that students can focus on
the essentials. But, especially when developing
mathematical insights, students must learn how to approach
ill-defined, poorly formulated problems---an area in which
education is lacking. There are no shortcuts; the only way
to learn is by direct experience.

We offer a number of recommendations for education in
mathematics and science. Our primary focus is education for
students who specialize in mathematics or science; we cannot
begin to address the national problem of mathematics and
science education for all.

1. Support curriculum development in areas that are
essential for connections between mathematics and science.
Every curriculum-related activity should include production
of Web-based materials.

(a) Create modeling courses for high school, undergraduate,
and graduate students. Unlike many other skills, modeling
can be taught (at an elementary level) to students in high
school. At the undergraduate level, there would be enormous
benefits if a one-year modeling course were part of the core
curriculum in science, engineering, mathematics, and
computer science. Graduate modeling courses would deepen
the scientific knowledge of mathematics students while
enriching the mathematical skills of science students.
(b) Support development of courses that tie core computer
science to science, engineering, and mathematics.
Programming, numerical analysis, data structures, and
algorithms---each of which is a topic with serious
mathematical content---should be part of the education of
every scientist and mathematician.
(c) Encourage experiments in activities (courses, summer or
short-term workshops) that teach scientific and mathematical
problem solving. Such programs could involve not only
techniques and direct experience of problem solving, but
also group projects that teach students how to work
collaboratively with others and how to present their work.

2. Encourage students to undertake programs of study, at
both undergraduate and graduate levels, which combine
mathematics and science. That this can be done at the
graduate level has been shown by the successful
Computational Science Graduate Fellowship program of the
Department of Energy, which requires students to undertake a
demanding interdisciplinary program in exchange for a
generous fellowship.

3. Support summer institutes in (i) mathematical topics
that address scientific applications and (ii) scientific
topics with mathematical content.

The NSF Research Experiences for Undergraduates (REU)
program has been extremely successful in exposing students
to research at an early stage. REU and other institutes
have become important for top undergraduates interested in
science and mathematics, and it is now common to prepare for
graduate school by attending a summer school or institute.
However, these programs are overwhelmingly devoted to highly
specialized subjects. In part this is understandable; the
organizers want to give the students a taste of research,
which is more easily done in a narrow area. But because
those summer institutes often determine the direction
students will take, NSF should ensure that there are high-
quality institute programs with a multidisciplinary emphasis
centered on connections between mathematics and science.

Certain emerging areas (such as mathematical biology) are
not yet widely covered in graduate programs. Carefully
designed summer institutes would help to broaden the
education of graduate students whose home institutions lack
offerings in such fields.

4. Fund research groups that include both (i) a genuine
collaboration between scientists and mathematicians, and
(ii) a strong educational program for graduate students,
postdoctoral fellows, and possibly undergraduates. To be
effective, such funding should be as long-term as possible;
if funding is only short-term, researchers are unlikely to
make the huge investment of time needed to develop group
structures that will sustain multidisciplinary
collaborations.

5. Fund postdoctoral fellowships in environments that
combine excellence in science with excellence in
mathematics. Efforts to create industrial postdoc programs
could be expanded to create joint university/national lab
postdoctoral fellowships, as well as short-term fellowships
for scientists in mathematics programs with a strong applied
component.

Beyond the postdoctoral level, there should be programs to
encourage and support faculty who would like to become
active in collaborations outside their own discipline. The
existing NSF program in this vein, Interdisciplinary Grants
in the Mathematical Sciences (IGMS), is small and imposes
relatively strict requirements on qualification and support
by the home department.

6. Develop a program of group grants for mathematics and
science departments that encourage the creation of new
courses, experimentation with instructional formats, and
coordinated programs of hands-on experiments, modeling, and
computation. Departments that receive such grants should
have substantial science requirements for undergraduate
degrees in mathematics, and substantial mathematics
requirements for undergraduate degrees in science. Many, if
not most, U.S. undergraduates in mathematics take no, or
almost no, science courses. In certain areas of science and
engineering, undergraduates take only minimal, and sometimes
outdated, mathematics courses; even worse, those courses may
give students no understanding of the ties between their
fields and mathematics. These unfortunate situations are
likely to be corrected only if there is an incentive for
departments to change their basic programs.

5 Conclusions

Strong ties between mathematics and the sciences exist and
are thriving, but there need to be many more. To enhance
scientific progress, such connections should become
pervasive, and it is sound scientific policy to foster them
actively.

It is especially important to make connections between
mathematics and the sciences more timely. Scientists and
engineers should have access to the most recent mathematical
tools, while mathematicians should be privy to the latest
thinking in the sciences. In an earlier era of small
science, Einstein could use the geometry of Levi-Civita
within a few years of its invention. With today's vastly
expanded scientific enterprise and increased specialization,
new discoveries in mathematics may remain unknown to
scientists and engineers for extended periods of time;
already the analytical and numerical methods used in several
scientific fields lag well behind current knowledge.
Similarly, collaborations with scientists are essential to
make mathematicians aware of important problems and
opportunities.

6 References and URLs

Combustion

[1] Information about Chemkin, a registered trademark of
Sandia National Laboratories:

http://stokes.lance.colostate.edu/CHEMKIN_Collection.html
http://www.sandia.gov/1100/CVDwww/chemkin.htm
http://www.sandia.gov/1100/CVDwww/theory.htm

Cosmology

[2] M. S. Turner and J. A. Tyson (1999), Cosmology at the
Millennium, working paper.

[3] Web sites about mathematical models and numerical
simulation:

http://star-www.dur.ac.uk/~frazerp/virgo/aims.html
http://phobos.astro.uwo.ca/~thacker/cosmology/


Finance

[4] I. Karatzas and S. E. Shreve (1998), Methods of
Mathematical Finance, Springer-Verlag, New York.

[5] T. F. Coleman (1999), An inverse problem in finance,
Newsletter of the SIAM Activity Group on Optimization.

Functional Magnetic Resonance Imaging

[6] W. F. Eddy (1997), Functional magnetic resonance imaging
is a team sport, Statistical Computing and Statistical
Graphics Newsletter, Volume 8, American Statistical
Association.

[7] Information about functional image analysis software:

http://www.stat.cmu.edu/~fiasco

Hybrid System Theory and Air Traffic Management

[8] C. Tomlin, G. J. Pappas, and S. Sastry (1998), Conflict
resolution for air traffic management: a case study in multi-
agent hybrid systems, IEEE Transactions on Automatic
Control, 43, 509---521.

Internet Analysis, Reliability, and Security

[9] Willinger and V.\ Paxson (1998), Where mathematics meets
the Internet, Notices of the American Mathematical Society
45, 961---970.

[10] The Web site of the Network Research Group, Lawrence
Berkeley Laboratory:

http://www-nrg.ee.lbl.gov

Materials Science

[11] Research trends in solid mechanics (G. J. Dvorak, ed),
United States National Committee on Theoretical and Applied
Mechanics, to appear in International Journal of Solids and
Structures, 1999.

[12] G. Friesecke and R. D. James (1999), A scheme for the
passage from atomic to continuum theory for thin films,
nanotubes and nanorods, preprint.

Mixing in the Oceans and Atmospheres

[13] P. S. Marcus (1993), Jupiter's great red spot and other
vortices, The Annual Review of Astronomy and Astrophysics
31, 523---573.

Physiology

[14] J. Keener and J. Sneyd (1998), Mathematical Physiology,
Springer-Verlag , Berlin.

[15] Details about modeling melanophore in the black tetra
(the home page of Eric Cyntrynbaum, the University of Utah):

http://www.math.utah.edu/~eric/research

Diagnosis Using Variational Probabilistic Inference

[16] T. S. Jaakkola, T. S. and M. I. Jordan (1999).
Variational methods and the QMR-DT database, submitted to
Journal of Artificial Intelligence Research.

[17] M. I. Jordan (1998), Learning in Graphical Models, MIT
Press, Cambridge, Massachusetts.

Iterative Control of Nuclear Spins

[18] R. Tycko, J. Guckenheimer, and A. Pines (1985), Fixed
point theory of iterative excitation schemes in NMR, J.
Chem. Phys. 83, 2775---2802.

[19] A. Lior, Z. Olejniczak, and A. Pines (1995), Coherent
isotropic averaging in zero-field NMR, J. Chem. Phys. 103,
3966---3997.


http://www.nsf.gov/pubs/2000/mps0001/mps0001.txt

Saturday, February 21, 2009

Qdots

Quantum Dots:

Designing building blocks for next-generation photonics

The nanometre-sized pyramids of Indium Arsenide (InAs) that form during the interrupted growth of InAs on a Gallium Arsenide (GaAs) substrate are attractive to electrons, trapping any that enter and quantizing their motion in the process. Electrons confined to these quantum dots exhibit an atomic-like spectrum of energies which depends greatly on the dot size and composition. Quantum dots are sometimes referred to as "designer atoms" because of the way their electronic and optical properties can be tailored. Figure 1 below shows an InAs quantum dot.

New Castle Univ
http://cmt.phys.ncl.ac.uk/
http://www.qcadesigner.ca/

Friday, February 20, 2009

VLS process explained





The Vapour Liquid Solid VLS process is used for the growth of Si nanowire by using Au clusters as the solvent at high temperature. Based on Si_Au binary phase diagram, Si (from the decomposition of SiH4 , for example) and Au will form a liquid alloy when the temperature is higher than the eutectic point. The liquid surface has a
large accommodation coefficient and is therefore a preferred deposition site for incoming Si vapor. After the liquid alloy becomes supersaturated with Si, Si nanowire growth occurs by precipitation at the solid } liquid interface.

Recently, real-time observation of Ge nanowire growth was conducted in a high-temperature in situ transmission electron microscope (TEM). The experiment result clearly shows three growth stages: formation of Au_Ge alloy, nucleation of Ge nanocrystal and elongation of Ge nanowire. This experiment unambiguously demonstrates the validity of the VLS mechanism for nanowire growth. The establishment of VLS mechanism at the nanometer scale is very important for the rational control of inorganic nanowires, since it provides the necessary underpinning
for the prediction of metal solvents and preparation conditions.

Based on our mechanism study of the nanowire growth, it is conceivable that one can achieve controlled growth of nanowires at different levels. First of all, one can, in principle, synthesize nanowires of different compositions by choosing suitable solvents and growth temperatures. A good solvent should be able to form a liquid alloy with the desired nanowire material, ideally they should be able to form a eutectic alloy. Meantime, the growth temperature should be set between the eutectic point and the melting point of the nanowire material.



Both physical methods (laser ablation, arc discharge, thermal evaporation) and chemical methods (chemical vapour transport and chemical vapour deposition) can be used to generate the vapor species required during the nanowire growth.

Wu, Y. et al., 2002 ‘Inorganic Semiconductor Nanowires: Rational Growth, Assembly, and Novel Properties’, Chemistry – A European Journal, vol. 8, issue 6, pp.1260-1268.

Monday, February 16, 2009

Boron Buckyballs



We are all familiar with the well known Buckminsterfullerene; discovered some years ago in 1985 by a group of scientists in the UK and US. including Robert Curl, Harold Kroto and Richard Smalley. They discovered that 60 Carbon atoms can form a stable and hollow spherical type molecule in the shape of a geodesic dome. The dome resembles a building designed by the architect Richard Bukminster Fuller.

A few years ago scientists at Rice University were eventually successful in producing bucky balls made entirely of Boron atoms, and more recently a group at the Graduate University of Chinese Academy of Sciences, led by Prof. Gang Su, made significant progress in the prediction of pure boron buckyballs [Yan et al., physical review B (2008) 78, 201401].

As Boron and Carbon are neighbours in the periodic table you an imagine they share many similar properties, this has led to considerable interest and research in Boron over the past few years. If this is indeed the case then many new opportunities may arise from this new class of compound and may even result in a cost effective route to bulk production of this buckyball.

Su et al have now proposed a generic constructing scheme that shows how to generate a family of novel boron monoelemental, hollow fullerenes which exhibit amongst their properties remarkable stability. They also go on to present an electron counting rule and an isolated hollow rule to show why the predicted boron S-fullerenes are stable and how the electrons in these particular fullerenes are bonded, thereby establishing the relationship between the geometrical and electronic structures of the boron fullerenes.

The scientists behind this discovery are already discussing the relationship between these molecules and those of B80 and boron sheet (NBS), which will lead to a better understanding of their interlinked stability. These findings and continued research will boost further investigations on boron nanostructures both theoretical and experimental and should lead to many new nanostructure discoveries.

Jonathan Agbenyega
Materials Today
http://www.materialstoday.com/archive/2009/12-01/news02.html

The Field of Separation Science

In 1992, a new family of aluminosilicates (M41S) with pores sizes between 20 and 100 Å in diameter were reported by Mobil researchers (Beck et al. 1992; Kresge et al. 1992). One of particular interest is MCM-41, which consists of hexagonal arrays of uniform 2 to 10 nanometer-sized cylindrical pores. Not only can such materials be synthesized, but novel structures such as "tubules-within-a-tubule" have been fabricated as mesoporous molecular sieves in MCM-41 (Lin and Mou 1996). Of particular interest is the possibility of expanding the so-called "liquid crystal templating" mechanism (Chen et al. 1993) to non-aluminum dopants within the silicate MCM-41 framework (Tanev et al. 1994) and to derive non-siliceous MCM-41 type of materials (Braun et al. 1996).

Another approach to synthesizing large pore and large single crystals of zeolytic materials is being pioneered by Geoffrey Ozin and his group at the University of Toronto, who have demonstrated that crystals as large as 5 mm can be synthesized (Kupperman et al. 1993). The ability to synthesize such large crystals has important implications for discovery of new sensors (selective chemical adsorbants) and membrane devices (selective transport of molecular species), since large single crystals can now be available to the laboratory researcher to carry out fundamental studies of adsorption and diffusion properties with such materials. These materials are expected to create new opportunities for applications in the fields of separations science, for use directly as molecular sieves or as new molecular sieving sorbant materials; in catalysis, as heterogeneous catalysts; and as supports for other catalytic materials as well as other novel applications (Bowes et al. 1996; Brinker 1996; Sayari 1996). The ability to synthesize zeolitic materials of precise pore size in the range between 4 and 100 Å continues to expand the possibilities for research and technological innovation in the catalytic, separations, and sorption technologies (Ruthven et al. 1994; Karger and Ruthven 1992).

http://www.wtec.org/loyola/nano/04_03.htm
http://www.begbroke.ox.ac.uk
http://www.conted.ox.ac.uk

Sunday, February 15, 2009

Stoichiometry

Stoichiometry ( in Greek - measuring element) takes account of quantity of elements involved in a chemical reaction and is based upon the principal of mass conservation, which applies to chemical reactions that by definition do not affect the mass of reactants nor transmute into other elements. The word is also used for molar proportions of elements that are discrete numbers.
Non-stoichiometric compound refers to the ratio of atoms not being an integer, such as Vanadium Oxide varieties from VO 0.79 to VO 1.29, and others TiOx, NixO, UOx and LiWO3. extrinsic defects are introduced into crystal through impurities, that is by adding dopants. For example if ClNa is heated in an environment of sodium vapour, the Na+ ion changes to Na(1+x) Cl. Sodium ions now moved to the crystal and occupy cation sites and leave same quantity of unoccupied anion sites behind which then will be occupied by anion vacancies. This state of solid is non-stoichiometric mix.
Refs.

http://www.chem.ox.ac.uk/vrchemistry/solid/Page17.htm
www.wikipedia.com

Kirkendall effect

Kirkendall effect refers to the rate of diffusion of components of alloy and a metal. Eg. if molybdenum signifies as marker of diffusion between copper and brass (copper-zinc alloy) – molybdenum will direct diffusion toward the alloy brass, since zinc is more rapidly diffused than copper. This effect has significant effects on creation of voids that are formed at the interfaces of alloys and metals, and are called kirkendall voids. Kirkendall effect in wire bonding technology was demonstrated to show importance of impurities. And that was for the rate of impurities in forming precipitation at the wire bonds, where voids in intermetallics were formed following the difference between diffusion rates of two metals. These voids would cause weakness and would develop in numbers when heat applied. Nanoscale hollow structures can grow according to Kirkendall effect that demonstrates the influence of surface diffusion on the morphology evolution. The influence is based on counterdiffusion at the reaction interfaces. There was observation that after formation of voids the second stage of surface diffusion follows that show rapid growth of fast diffusing material along the pore surface.

Fan Influence of surface diffusion on the formation of hollow nanostructures induced by the Kirkendall effect: the basic concept, Nano letter, 2007 Apr. vol 7 (4): pp993-7
http://www.ncbi.nlm.nih.gov/pubmed/17381161
Yin, Formation of hollow nanocrystals through the nanoscale Kirkendall effect, Science, 2004 Apr 30, 304 (5671), pp 711-4

http://nepp.nasa.gov/wirebond/horsting%20analysis.htm

http://www.wikipedia.com

The Discovery and Acceptance of the Kirkendall Effect: The Result of a Short Research Career, http://www.tms.org/pubs/journals/JOM/9706/Nakajima-9706.html

Saturday, February 14, 2009

Mesoporous single-crystal nanowires

Porous materials have a wide variety of applications in bioengineering, catalysis, environmental engineering, and sensor systems because of their high surface-to-volume ratio. Normally, most of these mesoporous structures are composed of amorphous materials and porosity is achieved by solvent-based organic or inorganic reactions. There are few reports of mesoporous structures based on crystalline material. We have reported a novel wurtzite ZnO nanowire structure that is a single crystal but is composed of mesoporous walls/volumes. The synthesis is based on a modified solid-vapour process. ZnO nanowires grown on a Si substrate coated with a thin layer of Sn catalyst, the typical length of the nanowires varies from 100 μm to 1 mm and the diameter mask and self-assembled submicron spheres. We have combined this self-assembly-based mask technique with the surface epitaxial approach to grow large-area hexagonal arrays of aligned ZnO nanorods. The synthesis process involves three main steps. The hexagonally patterned ZnO nanorod arrays are grown on a single-crystal Al2O3 substrate on which patterned Au catalyst particles have been dispersed. First, a two-dimensional, large area, self-assembled and ordered monolayer of submicron polystyrene spheres is introduced onto the single-crystal Al2O3 substrate. Second, a thin layer of Au particles is deposited onto the self-assembled monolayer; the spheres are then etched away, leaving a patterned Au catalyst array. Finally, nanowires are grown on the substrate using the VLS process. The spatial distribution of the catalyst particles determines the pattern of the nanowires. This step can be achieved using a variety of mask technologies for producing complex configurations. By choosing the optimum match between the substrate lattice and the nanowires, the epitaxial orientation relationship is in the range of 50-500 nm. The porous structure of ZNO:

(0001) zno || (001) zn2sio4, [2110]zno||[100]zn2sio4

A corresponding electron diffraction pattern from the nanowire presents two sets of structures.
the formation of Zn2SiO4 on the surface of the nanowires with an epitaxial orientation relationship as follows, Zn2SiO4 is formed on the surface of the Si substrate, but covers only a fraction of the surface area because of the large lattice mismatch with ZnO. As a result, resublimation of ZnO in the nanowire forms the mesoporous structure. The high porosity, single-crystal wire-like structures have potential applications as filters, catalyst supports, and gas sensors.

In ZNO the nanostructures can have novel applications in optoelectronics, sensors, transducers, and biomedical science because it is bio-safe.

Wang, Nanostructures of Zinc Oxide, Materials Today, Volume 7, Issue 6, June 2004, Pages 26-33

http://www.sciencedirect.com/science?_ob=ArticleURL&_udi=B6X1J-4CCCNYB-12&_user=10&_coverDate=06%2F30%2F2004&_rdoc=1&_fmt=full&_orig=search&_cdi=7244&_sort=d&_docanchor=&view=c&_acct=C000050221&_version=1&_urlVersion=0&_userid=10&md5=242cabdfdaea486f1589b862581a05e1#toc4

Quantum Networks & Faster nanowires

Mesoscopic systems and large molecules are often modeled by graphs of one-dimensional wires connected at vertices. In this paper, we discuss the solutions of the Schrodinger equation on such graphs, which have been named "quantum networks". Such solutions are needed for finding the energy spectrum of single electrons on such finite systems or for finding the transmission of electrons between leads which connect such systems to reservoirs. Specifically, we compare two common approaches. In the "continuum" approach, one solves the one-dimensional Schrodinger equation on each continuous wire and then uses the Neumann-Kirchoff-de Gennes matching conditions at the vertices. Alternatively, one replaces each wire by a finite number of "atoms" and then uses the tight binding model for the solution. Here, we show that these approaches cannot generally give the same results, except for special energies, unless the lattice constant of the tight binding model tends to zero. Even in the limit of the vanishing lattice constant, the two approaches coincide only if the tight binding parameters obey very special relations. The different consequences of the two approaches are then demonstrated via the example of a T-shaped scatterer.

Aharony et al: J Phys Chem B. 2008 Nov 24.



Electricity moves through nanowires very differently from ordinary electrical wires. "If you add electrons to a typical metal wire, a domino effect moves them along the wire until they dump out the other end," says Chidsey. The electrons in metal wire move at a constant speed as they bump each other across the wire. Cut the length of a metal wire in half and it will take half as long for electrons to pass through it.

But organic nanowires don't conduct electricity that way. The rate of speed increases exponentially as the wires get shorter. For example, a 3-nanometer wire of OPV would conduct 950 times faster than a wire that's twice as long. That's because instead of bumping each other across the wire domino style, electrons "tunnel" through nanowires. When they tunnel, electrons bypass barriers they normally would not be able to climb without violating the law of conservation of energy. The chance they'll make it through to the other side drops exponentially with distance.

The OPV nanowire allows tunneling to occur relatively easily. In computer chips, tunneling is mostly a bad thing, Chidsey says: When electrons tunnel through a thin insulator around a circuit, they may cause it to short out. "I'm interested in seeing if we can understand and get control over tunneling through molecules," he says. And if he succeeds, tunneling may get a better reputation in electronics, as it may be harnessed for moving electrons between nanostructures.

http://www.stanford.edu/dept/news/pr/01/nanowire314.html

Self-Organized Ultrathin Oxide Nanocrystals

Uniform ultrathin nanorods were grown in a self assembled fashion by the use of surfactants such as oleylamine and oleic acid that acted as nanocrystal capping as well as directing agent. A 1-2 nm nanocrystal was syntheses using 0.5 g of titanium isopropoxide or titanium butoxide dissolved in dry octadecene 18g and oleic acid 16g under 80C for approx 4 hours. After adding 7 g of oleylamin to this mix, it was heated at 260 C under a nitrogen atmosphere and then cooled to room temp and used centrifugation at 2000 rpm for 10 min to separate the ribbon like structures from the bulk. It was shown by EDS analysis that these were ultrathin TiO2 nanorods 2nm x 20 nm growing spantenously along the c axis, and orderly stacked together side by side without the need of any post processing.
Same synthetic method was applied to ZnO quantum rods generated from ordinary acetate precursors – was further developed with cooperative growth/assembly hypothesis to synthesize transition metal oxide nanowires with sub-2-nm dimension. Mesoscopic oxide nanocrystals were spontaneously formed as ribbon like superstructures. The process involved complexion of precursor species with surfactants that would grow metal-surfactant-monomers. After high temperature it turned into metal oxygen network through an ester elimination process. NRs were then evolved from the layered mesostructures, then disrupted , to allow for nanorods to spontaneously self assemble as 1D superstructures.
• Motte,L., Billoudet,F., Lacaze,E. & Pileni,M. P. Self-organization of size-selected nanoparticles into three-dimensional superlattices. Adv. Mater. 8, 1018–1020 (1996). | ISI | ChemPort |
• Sager,W. F. C. Controlled formation of nanoparticles from microemulsions. Curr. Opin. Colloid Interf. Sci. 3, 276–283 (1998). | ISI | ChemPort |

Friday, February 13, 2009

the truth is fractal and far from simple

To better understand growth mechanism (and defusion), examining thin film deposition interfaces growth leads us to features that have tendency towards spherical symmetry as in fractal curves, similar to many growing interfaces in nature and biology such as fluid flow in porous media, adatom and vacancy islands on surfaces, atoms at borders of crystalline facets, bacterial growth, wetting fronts, etc. Their geometry evolves exponentially – that is a matter of great concern in scaling which is dynamic in nature. Surface diffusion show transition from smooth to unstable growth. Some studies prove initial stability of ordered structures in growth may result in instability at longer times which ends to epitaxial breakdown. Such dynamism in growth has great implications in medicine, such as tumour growth and in semiconductors as it concerns crystal growth. It may have implications on self assembly methods.

http://www.ox.ac.uk/media/science_blog/080328.html

Ref.:
Carlos Escudero, Dynamic Scaling of Non-Euclidean Interfaces, Physical Review Letters, Vol 100, 116101 (21 March 2008)
http://scitation.aip.org/getpdf/servlet/GetPDFServlet?filetype=pdf&id=PRLTAO000100000011116101000001&idtype=cvips&prog=normal
Haselwandlter C A, Renormalization of stochastic lattice models: Epitaxial surfaces; ISI Web of Knowledge; Physical Review E, Vol 77 Issue 6, June 2008
Escudero C, Geometric principles of surface growth, PHYSICAL REVIEW LETTERS Volume: 101 Issue: 19

Wednesday, February 04, 2009

Calcinid flints as white as flower

Robert Hooke recorded in his diary for July 29 1673 : "with Dr [Christopher] Wren to the new Glashouse at the Savoy. Saw calcind flints as white as flower, Borax, Niter and tarter, with which he [Ravenscroft] made his glasse he denyd to use arsenick he shewd pretty representations of Agates by glasse etc.”


The Diary of Robert Hooke, M A M D, F.R.S. 1672-1680 ed. Henry W. Robinson and Walter Adams (London 1935), p 53. see also ibid p 89.




Changes in the glass industry were slow with mold-blowing still practiced in similar fashion. L M Angus-Butterworth, author of Chapter 12 (pp 358-378), does well to concentrate on the various processes used in making lenses, tubing, rod, mirrors, and window glass rather than on domestic ware which, being eagerly sought by collectors, has always received a disproportionate amount of publicity. He also gives a useful section on coloured glasses. The curiosities of industry and applied sciences by George Dodd – London, 1852. the plate-Glass-Book by a glasshouse clerk , London 1771; treatise on the origin, progressive improvement and present state of the manufacture of porcelain and glass, by G R Porter London; the crown glass cutter and glazier’s manual, by William Cooper, Edinburg, 1835; and treatise on the Art of Glass Making, by William Gillinder, Birmingham, 1851.


Anotnio Neri, at the beginning of 17th century; The Art of Glass, 1662

Colorimetric Screening

Probes were prepared by functionalizing two separate batches of 13-nm gold particles with two different thiolmodified oligonucleotide strands, DNA-1 (5’-CTCCCTAATAACAATTTATAACTATTCCTA- A10-SH-3’) and DNA-2(5’-TAGGAATAGTTATAAATTGTTATTAGGGAG-A10- SH-3’). These functionalized particles are denoted DNAAuNP-1 and DNA-AuNP-2. DNA-1 and DNA-2 are complementary to each other. Therefore, DNA-AuNP-1 and DNA-AuNP-2 can hybridize to form a cross-linked network
of nanoparticles, which is purple in color owing to the redshifted plasmon band of the gold nanoparticles (13 nm). This red-shifting is a well-understood process and is a highly diagnostic feature of aggregate formation.[11] These aggregates can then be used as colorimetric indicators of endonuclease activity (Scheme 1). As the endonuclease degrades the DNA-duplex interconnects, particles are released, regenerating a red color due to the dispersed nanoparticles. The color can be observed with the naked eye, or the absorbance (520 nm) can be measured by UV/Vis spectroscopy.
http://www3.interscience.wiley.com/cgi-bin/fulltext/114202374/PDFSTART