Electronics

Download e-book for kindle: 2D materials for nanoelectronics by Michel Houssa, Athanasios Dimoulas, Alessandro Molle

By Michel Houssa, Athanasios Dimoulas, Alessandro Molle

ISBN-10: 1498704182

ISBN-13: 9781498704182

"Major advancements within the semiconductor are at the horizon by using second fabrics resembling graphene and transition steel dichalcogenides for built-in circuits. This e-book presents the 1st entire remedy of the sphere with an emphasis on functions in nanoelectronic units. Chapters are divided by way of the 3 significant households of such fabrics, protecting graphene for analog and photonic Read more...

summary: "Major advancements within the semiconductor are at the horizon by utilizing 2nd fabrics corresponding to graphene and transition steel dichalcogenides for built-in circuits. This ebook offers the 1st accomplished remedy of the sector with an emphasis on purposes in nanoelectronic units. Chapters are divided by means of the 3 significant households of such fabrics, protecting graphene for analog and photonic purposes, MoS2 (molybdenum disulfide) for good judgment functions and novel fabrics resembling silicene, germanene, stanene and phosphorene"

Show description

Read or Download 2D materials for nanoelectronics PDF

Best electronics books

Download PDF by Michael Gradias: Nikon D90

Цифровой зеркальный фотоаппарат Nikon D90. Компактный, мощный и универсальный, он является идеальным в осовоении всех возможных видов зеркальной фотосъемки, от портретов до интерьеров, архитектуры и пейзажей. Sie wollen mehr? In diesem Buchtitel beschreibt der Autor detailliert die neue D90 von Nikon.

Read e-book online The Handbook of Electrical Resistivity: New Materials and PDF

This re-creation of the acclaimed electric Resistivity instruction manual brings jointly advances within the box over the past twenty years during which a lot has been accomplished within the fields of latest fabrics and superconductivity.

This is a massive reference e-book compiling resistivity info, as a functionality of temperature, for metals, alloys and semiconductor fabrics.

Acoustics, aeroacoustics and vibrations by Fabien Anselmet, Pierre-Olivier Mattei PDF

This didactic e-book provides the most parts of acoustics, aeroacoustics and vibrations. Illustrated with a number of concrete examples associated with strong and fluid continua, Acoustics, Aeroacoustics and Vibrations proposes a variety of purposes encountered within the 3 fields, no matter if in room acoustics, delivery, power creation platforms or environmental difficulties.

Additional resources for 2D materials for nanoelectronics

Sample text

96) is the strain tensor (x1 = x and x2 = y). There are many different types of static deformations of the honeycomb lattice that can affect the propagation of Dirac fermions. The simplest one is due to changes in the area of the unit cell due to either dilation or contraction. Changes in the unit-cell area lead to local changes in the density of electrons and, therefore, local changes in the chemical potential in the system. 97) and their effect is diagonal in the sublattice index. The NN hopping depends on the length of the carbon bond.

The series of surface reconstructions are listed below:16 1000 °C 1080° C (3 × 3) → (1 × 1) → ( 3 × 3 ) → (6 3 × 6 3 ) + Graphene The process starts with a hydrogen-etched sample and the preparation of the Si-rich (3 × 3) phase. Heating this surface to about 950°C leads to a ( 3 × 3 )R 30° phase. This phase can be considered as a 1/3 monolayer of Si adatoms atop the SiC substrate. Further annealing to 1100–1150°C sublimes more silicon from the surface and leads to the formation of a well-ordered (6 3 × 6 3 )R 30° phase, in which the SiC is covered by a carbon layer.

74) For such a gauge, [H, py] = 0, and py is a good quantum number. Owing to the translational invariance along the y direction, we can assume solutions of the form Ψ(x,y) = exp(i kyy)(a(x),b(x))T, with T denoting the transpose of the row vector. 75)  ) a = Eb. 77) where c− = a and c+ = b. 77 are the well-known Hermite polynomials H(x). 78) with the lowest level: E0 = 2 vF B . 79) Repeating this procedure for c+ = b gives b(x ) = exp(− z 2 /4)H E2 /2 (x + k y ) with the spectrum: En = ± vF B 2n ∝ nB .

Download PDF sample

2D materials for nanoelectronics by Michel Houssa, Athanasios Dimoulas, Alessandro Molle


by Robert
4.3

Rated 4.54 of 5 – based on 16 votes