Monday, February 17, 2014

Intro to composite and nanocomposite thermoelectrics

One of the approaches to enhance the performance of thermoelectric (TE) materials (i. e.ZT), is reducing the thermal conductivity by scattering the phonons or in other words, decreasing the lattice thermal conductivity.
Addition of nano-inclusions to increase interfaces has shown a significant impact on lattice thermal conductivity reduction despite its simultaneous effect on electrical conductivity . Alternatively, composite thermoelectric materials containing several phases may enhance the performance of thermoelectric materials by conserving a relatively high electrical conductivity while introducing more interfaces leading to a decrease in the thermal conductivity.
The words, composite and nanocomposite, in the thermoelectric related literature are used with different meanings. In some reports, nanocomposite refers to adding nano-inclusions to the bulk thermoelectric materials, in some others, it pertains to mixing two or more different particle sizes ranging from nano to micro-scale of the same material, or mixing two different TE phases. In general, one can call a material, TE nanocomposites when it consists of nano-inclusions, nano-particles randomly dispersed, nano-grains, and secondary phases or precipitates. More recently several approaches have been developed to produce TE nanocomposites mainly based on the idea of the phonons scattering by introducing more interfaces in the material, such as utilizing phase decomposition to create embedded nanostructures. Several types of nanao-inclusions such as semimetals, semiconductors, metals, ceramics, and even carbon nanotubes were also used in thermoelectric materials to produce TE nanocomposites.
In TE materials with anisotropic properties, fabrication method is also an important issue. Specially, in case of powder metallurgy approach that nanostructures in the powders need to be conserved during the consolidation process. We have used hot-extrusion and microwave sintering for bismuth telluride based materials to obtain the bulk nanostructured TE materials. However, hot extrusion has shown more benefits in case of texturing.


Saturday, June 4, 2011

Introduction to Graphene and Graphene Nanoribbons-Part2

Graphene Production

Graphene was first produced by mechanical exfoliation of graphite. This method provided a small number of high-quality samples for fundamental studies. Later on, several methods have been utilized to synthesize graphene sheets which might be categorized into bottom-up and top-down approaches with carbon-containing molecules and graphite as initial materials, respectively. Cost, throughput, size of sheets, quality of sheets, chemical modification, and compatibility with the commercial chip fabrication process are among the most notable considerations in selecting a method for synthesizing graphene. Some of the groundbreaking efforts in synthesizing graphene are Mechanical exfoliation, Supported growth (thermal decomposition of carbides or epitaxial growth by CVD and wet chemical routes)

· Mechanical exfoliation: (top-down approach)

· Supported growth:

It has been known since the early 1970s that graphene could be grown directly on solid substrates and two different mechanisms can be exploited: the thermal decomposition of carbides or the epitaxial growth of graphene on metallic or metal carbide substrates by chemical vapor deposition of hydrocarbons.

Graphene Nanoribbons (GNRs)

Graphene is a zero-gap semiconductor, so a field effect transistor (FET) will not have an ‘‘off’’ state unless a forbidden gap is created. Such a gap can be produced by confining the electronic wave functions by etching narrow graphene nanoribbons (GNRs) typically of a few nanometers in width and with well-defined crystallographic orientation.

So GNRs are 1D while the Graphene layer is a 2D allotrope of carbon.

Wednesday, May 25, 2011

Introduction to Graphene and Graphene Nanoribbons-Part1

Carbon is the fourth most abundant element in the universe after hydrogen, helium, and oxygen.
Soon after the discovery of the X-Ray diffraction in 1912, these two fundamental crystal structures i.e. cubic diamond and hexagonal graphite were identified
After the Second World War, in the middle of the last century, further tremendous progress in the science of carbon has lead to unexpected and fascinating discoveries.
Carbon Bonds: Because the outermost shell of a carbon atom contains only four electrons, these atoms can gain stability by losing four electrons, adding four electrons, or sharing four additional electrons from another atom. Carbon can form three different kinds of bonds that involve the sharing of electrons. These are called single, double, and triple bonds, depending on how many pairs of electrons are being shared with another atom. This can be another carbon atom, or it can be an atom of another element. In a single bond, two atoms share one pair of electrons. In this electron pair, both electrons can come from one atom or each atom can donate an electron. In a double bond, two atoms share two pairs of electrons. In a triple bond, two atoms share three pairs of electrons.
Diamon Crystal
FORMS OF CARBON (Carbon Alothrops) Some elements have several different forms. These different forms of an element are called allotropes. Carbon Allotropes: Because of the flexibility of its bonding, carbon-based systems show an unlimited number of different structures with an equally large variety of physical properties. These physical properties are, in great part, the result of the dimensionality of these structures. (diamond and graphite (3D) to graphene (2D), nanotubes (1D) or fullerenes (0D)) Fullerenes are molecules where carbon atoms are arranged spherically, and hence, from the physical point of view, are zero dimensional objects with discrete energy states. Carbon nanotubes are obtained by rolling graphene along a given direction and reconnecting the carbon bonds. Hence carbon nanotubes have only hexagons and can be thought of as one-dimensional _1D_ objects. Graphene A graphene crystal is an infinite two-dimensional layer consisting of sp2 hybridized carbon atoms , which belongs to one of the five 2D Bravais lattices called the hexagonal (triangular) lattice. It is noteworthy that by piling up graphene layers, in an ordered way, one can form 3D graphite. Graphene was initially considered as a theoretical building block used to describe the graphite crystal, and to study the formation of carbon nanotubes (rolled graphene sheets), and predict their fascinating electronic properties. This 2D atomic (one atom thick) crystal of carbon has as fingerprint a unique electronic structure with linear dispersion close to the Fermi level. Charge carriers in graphene are better described as massless Dirac fermions, which result in new phenomena. Graphite, a three dimensional _3D_ allotrope of carbon, became widely known after the invention of the pencil in 1564, and its usefulness as an instrument for writing comes from the fact that graphite is made out of stacks of graphene layers that are weakly coupled by van der Waals forces. We can define graphite as an infinite three-dimensional crystal made of stacked layers consisting of sp2 hybridized carbon atoms ; each carbon atom is connected to other three making an angle of 120◦ with a bond length of 1.42 Ã…. Depending on the layers stacking, these crystals could be hexagonal (ABABAB. . .) or rhombohedral (ABCABC. . .). In both 3D crystals, the layers interact weakly through van der Waals forces. Graphite crystals can be found naturally, and can also be artificially synthesized by thermolytic processes; such as the production of highly oriented pyrolytic graphite (HOPG).
Carbon allotrops
Graphene: Among systems with only carbon atoms, graphene, a two-dimensional (2D) allotrope of carbon, plays an important role since it is the basis for the understanding of the electronic properties in other allotropes. Graphene is made out of carbon atoms arranged on a honeycomb structure made out of hexagons , and can be thought of as composed of benzene rings stripped out from their hydrogen atoms Although graphene is the mother for all these different allotropes and has been presumably produced every time someone writes with a pencil, it was only isolated 440 years after its invention Having the title of the strongest material ever measured3, graphene is a two-dimensional (one-atom-thickness) allotrope of carbon with a planar honeycomb lattice . It is regarded as the basic building block of carbon nanotubes and large fullerenes. The properties of carbon nanotubes originate from graphene sheets. With the exception of diamond, it is possible to think of fullerenes, nanotubes and graphite as different structures built from the same hexagonal array of sp2 carbon atoms, namely graphene. Indeed, fullerenes and nanotubes can be mentally visualized as a graphene sheet rolled into a spherical and cylindrical shape, respectively, and graphite can be described as a stack of alternately shifted graphene sheets.
The infinite plane of a perfect graphene shows a zero electronic band gap with electrons having zero effective mass where valance and conduction bands meet4. This makes graphene an anomalous material, which does not behave as either a metal or a semiconductor. Graphene exhibits a number of exotic physical properties, previously not observed at the nanoscale. The observation of room-temperature quantum Hall Effect, ultrahigh electron mobility and ballistic transport, long electron mean free paths, superior thermal conductivity, great mechanical strength, and remarkable flexibility are among the striking properties of graphene. Hence, its desirability in electronics. Graphene has first attracted the curiosity of mesoscopic physicists owing to its peculiar electronic behavior under magnetic field and at low temperature. The investigation and tailoring of its transport properties from macroscopic to molecular scales captures a large share of the current research effort. Technologists and materials scientists have rapidly grabbed some of the assets of graphene and are already exploring the ways of incorporating graphene into applied devices and materials. Eventually, chemists and surface physicists remembered their ancient recipes which could provide solutions to mass produce the elusive carbon monolayer either in bulk suspensions or in substrate-supported forms. Now, graphene is a new and hot research topic with a strong vow to address the global demand for a new revolutionary material.
To be continued...
1. West, K., Carbon Chemistry. 2008: Infobase Publishing.
2. Loiseau, A., Understanding carbon nanotubes : [ressource âelectronique] from basics to
applications. Lecture notes in physics; ; 677. 2006, Berlin ; New York: Springer. xvi, 552 p.