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  • Matter, Materials, Crystal Structure

    and Bonding

    Chris J. Pickard

  • Why should a theorist care?

    Where the atoms are determines what they do

    Where the atoms can be determines what we can do

  • Overview of Structure and Bonding

    Atoms and Elements

    Non-crystalline materials

    Crystalline materials

    Bonding and cohesion

  • Atoms and Elements

  • Molecules

    Naphalene

    Molecules are finite collections of covalently bonded atoms

    They vary from diatomic molecules, to massive proteins

  • Polymers

    Polyethylene (or polythene)

    Polymers are long chain molecules,often with a carbon backbone(sometimes silicon)

    The repeat unit, or monomer, isrepeated and joined together manytimes

    The chemical formula for polyethyleneis (CH2)N

    Many properties depend simply on N

  • Nanoparticles

    Silver Nanoparticle

    Nanoparticles range in size from 1 100 nm and can contain from 10 to100,000 atoms

    Their properties are not necessarilythe same as the bulk material

    The physical, mechanical, electronic,magnetic, optical and chemicalproperties can all differ

  • Nanostructures

    (9,9) armchair nanotube

    More complex structure thannanoparticles

    Might be designed, and often selfassembled

    Nanotechnology is a very hot topic,with strong technological promises fornanoelectronics etc.

  • Amorphous Solids

    Amorphous Carbon

    Amorphous solids have no long rangeorder

    The are disordered, and the kind ofdisorder is structural as opposed tocompositional

    In this example both sp3 and sp2

    bonding is found

    Can have a variety of electronic andmechanical properties

  • Order in randomness

    A silica glass

    The atomic positions are rarelyentirely random

    The structural constraints imposesome order on the randomness

    The result is short range order,without long range order

    This order can be probedexperimentally

  • The radial distribution function

    0 2 4 6r (Angstrom)

    0

    5

    10

    15

    Rad

    ial d

    istr

    ibut

    ion

    func

    tion

    The RDF is the probability density offinding particle i at a given distancefrom particle j:

    Gi,j =N

    i6=j (r |ri rj|)

    Can be measured in scatteringexperiments (X-ray, neutron)

    For a crystalline solid this would justbe a set of delta spikes . . .

  • Crystalline solids

    A crystal is a homogeneous solid with a regularly repeating atomic arrangement

    The majority of the solid state physicists theoretical tools have been developedfor dealing with crystals

    Most current scientific questions concern non ideal crystals (or structures thatare simply not crystalline)

    Our tools are still useful . . .

  • Ionic crystals

    Halite (NaCl)

    The Alkali Halides are typical ioniccrystals

    Can only exist for compounds(different elements)

    Are electronic wide band gapinsulators

    Are of technological importance fortheir optical properties

  • Pure Metal

    Aluminium

    The pure form of the majority ofthe elements in the periodic table aremetallic

    Metals conduct electricity freely, andreflect light

    Many pure metals are soft, buttransition metals are harder

  • Alloys

    Ordered metallic alloy

    Alloys are mixtures of elements, notexclusively metallic and can be eitherordered or disordered

    The properties depend dramaticallyon the composition, and history ofthe alloy

    Understanding alloying is ofimmense economic and technologicalimportance

  • Covalent Crystals

    Diamond

    The strong directional covalent bondslead to mechanically strong crystals

    Covalent crystals are less wellinsulating than ionic crystal

    Carbon can form a range of differentcovalent bonds, in this case sp3

  • Graphite

    Bernal Graphite

    The graphene sheets are purely sp2

    covalently bonded

    Graphite can exist in different phases,according to the stacking

    Bernal graphite (structure found byJ. D. Bernal in 1924) has an. . . ABABABA. . . stacking

    Graphite is a semi-metal (a non-zeroDOS at the Fermi level)

  • Semiconductors

    Gallium Arsenide (GaAs)

    Semiconductors are still less insulatingthan ionic crystals

    Band-gaps range from a fraction of anelectron volt, to several

    They can be doped to control theelectronic properties

    They are the basis of thesemiconductor industry

  • Zeolites

    Ferrierite

    Built up from SiO4 tetrahedral units

    Like the flexible hybridisation ofcarbon, these units allow manystructural possibilities

    Zeolites are open silicates

    They are industrially important ascatalysts

  • Minerals

    Amphibole

    Minerals are materials found naturallyin the earth

    Many are silicate based (again, on theSiO4 tetrahedra)

    The structures can be very complex,contain many atomic species, anddepend on the geological history ofthe sample

    A wide range of properties

  • High Temperature Superconductors

    YBa2Cu3O7

    YBCO is a complex layered metaloxide

    It is in the Perovskite structure

    YBCO superconducts at 92K

    Oxidation state of CuO planesand chains control superconductingproperties

  • Molecular crystals

    Solid cubane

    Molecules play the role of atoms toform molecular crystals

    At non-zero temperature, themolecules will be in often complexmotion

    Molecular crystals can be organicnon-linear optical materials, andother electronic properties are oftechnological interest

  • Cubic Ice

    Cubic water ice (H2O)

    Water ice is another form of molecularcrystal

    Held together by directional, butweak, hydrogen bonds

    The H2O molecule can vibrate, buthave less freedom to rotate

  • Molecular crystal with hydrogen bonds

    Indigo

    Many organic molecules (pigmentslike Indigo, or drug molecules) are heldtogether by both hydrogen bonds, andeven weaker van der Waals bonds

    There can be very many possiblepolymorphs

    The physical properties of the crystalwill depend on the exact polymorphpresent

  • Bonding

    The energy of a collection of atoms is often lower if they are close

    The atoms stick together

    In specific ways, depending on the nature of the atoms and their neighbours

    This bonding can be classified as Covalent, Ionic, Mixed, Metallic, Molecularand Hydrogen Bonding

    Of course, in reality there is a continuum

  • Covalent Bonding

    Diamond

    The atoms involved in a covalent bondcan be said to be sharing valenceelectrons so as to attain a magicaloctet

    Visually, this expresses itself as asignificant charge density between theatoms

    Covalent bonds are strong, gettingstronger (and shorter) the moreelectrons that are shared

  • Ionic Bonding

    Halite (NaCl)

    The electrons are not shared and thereis a concentration of charge density onthe more electronegative ion

    The ion that donates electronsbecomes positively charged (cations),and the receiving electron negativelycharged (anions)

    The bond is due to the electrostaticinteraction between the oppositelycharged ions, and non-directional

  • Mixed Ionic Covalent Bonding

    III-V Semiconductor (GaAs)

    The ionicity is weaker, due to thecloser electro-negativity of the atoms,but still present

    There is an increase in charge densitybetween bonded atoms

    The bond has both covalent andionic character, and the bonding isdirectional

  • Metallic Bonding

    Aluminium

    The electrons are shared across theentire solid, and are delocalised : anextreme version of covalent bonding

    The more electrons shared, thestronger the metallic bonding: Mghas a higher melting point than Na

    The bonding is non directional, canhave a covalent character, and resultsin close packed solids

  • Hydrogen Bonding

    Cubic water ice (H2O)

    Weak directional bonds due tothe electrostatic attraction of polarmolecules (or permanent dipoleswithin molecules)

    These permanent dipoles are due todifferences in electronegativity

    Hydrogen is unusual: it cannot fullyionise (first ionisation potential toohigh), but also can form only onecovalent bond

  • Van der Waals Bonding

    Solid cubane

    Weak non-directional bonds due tothe electrostatic attraction betweenfluctuating dipoles

    Always present, but only dominatesif all other bonds are saturated orimpossible

    The charge density between van derWaals bonded elements is verysmall

  • Cohesive Energy

    2 4 6 8 10 12 14 16 18 20Lattice Parameter (Angstrom)

    -1250

    -1200

    -1150

    -1100

    -1050

    Tot

    al E

    nerg

    y (e

    V)

    The total energy of diamond withlattice parameter

    See Chapter 20 of Ashcroft andMermin for a more (slightly more ...)quantitative approach

    To do a proper job, you really needto use a first principles QM basedapproach

    See the lecture courses of Drs.Molteni and Towler next term