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t,lor,cj l4"rl ar Ann^-ol..i N E.S SoSe 2015 Room BER/105/H,4th Wed 22.04.2015 (Set TU Dresden, Chair Materials Science and Nanotechnology Assignments to Nanostructured Materials / Nanostrukturierte Materialien Prof. Dr. G. Cuniberti, Dr. D. Ryndyk (HAL 106) Dr. V. Bezugly (HAL 119), Dipl.-Phys. T. Lehmann DL 1) couEe wiki hrlps ,',r"r. r, a..!a.ri leiieacl n8w ( r' send solutions to: l.i.rrLc.rio rurlrcaden de Problem set: Crystal structures 1,1. Crystal structure The following picture represents a two-dimensional lattice with two difFerent types of atoms. 6!1irye fr -boi^ o o .l . O ----=-. bc*^ ^jorn '{b'} .' ..-.; vn.fr( e':-ih". '^'L re1 d,4 l"s)jL, (a) Explain the following keywords. lf possible, mark them in the picture. Which one is obvious? r^tlirc blavais lattice - t':[,,.'. ' ,' "r.,, . ,i t,;. .t' r it t , 't''< il"^r lattice point t',t-. . ,-"t11 ur ,.r-,11, ,..1c" .,1,,,..1 f "- .".t lattice vectors l" '.e lr.r'J . - primitive unit cell f"il;,. 1c,,"1,r al 1,.,'i,),.'^r c..1rc.l !.1 lic ,{c.^r in ( -,.1 r^l u,,l c, l.l , Lqlli(c fd-r J -
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  • t,lor,cj l4"rl ar Ann^-ol..iN E.S

    SoSe 2015

    Room BER/105/H,4thWed 22.04.2015 (Set

    TU Dresden, Chair Materials Science and Nanotechnology

    Assignments toNanostructured Materials / Nanostrukturierte Materialien

    Prof. Dr. G. Cuniberti, Dr. D. Ryndyk (HAL 106)Dr. V. Bezugly (HAL 119), Dipl.-Phys. T. Lehmann

    DL1)

    couEe wiki hrlps ,',r"r. r, a..!a.ri leiieacl n8w ( r'send solutions to: l.i.rrLc.rio rurlrcaden de

    Problem set: Crystal structures

    1,1. Crystal structure

    The following picture represents a two-dimensional lattice with two difFerent types ofatoms.

    6!1irye

    fr -boi^

    oo

    .l . O ----=-. bc*^ ^jorn'{b'} .'

    ..-.;vn.fr( e':-ih". '^'L re1 d,4 l"s)jL,

    (a) Explain the following keywords. lf possible, mark them in the picture. Whichone is obvious? r^tlirc

    blavais lattice - t':[,,.'. ' ,' "r.,, . ,i t,;. .t' r it t , 't''< il"^rlattice point t',t-. . ,-"t11 ur ,.r-,11, ,..1c" .,1,,,..1 f "- .".tlattice vectors l" '.e lr.r'J .

    - primitive unit cell

    f"il;,. 1c,,"1,r al 1,.,'i,),.'^r c..1rc.l !.1 lic ,{c.^r in (-,.1 r^l u,,l c, l.l

    ,

    Lqlli(c fd-r J -

  • - basis atoms and basis vecto.s

    - crystal structure

    Which Bravais lattice suits with the illustrated crystal structure? Explain yourdecision.

    Draw a simple cubic lattice and indicate the lattice planes corresponding to thefollowing Miller indices:

    (001)(110)

    - (020)

    - (323)

    1,2, Atomic structute of graphene

    A graphene sheet is a honeycomb lattice of carbon atoms (see Figure below). Letthe distance between carbon atoms be oe = 0.141 nm.

    (b)

    (.)

    -5"3I cdl

    A good model for graphene is to consider a single plane in which there is one valenceelectron per carbon atom. The unit cell spanned by al and a, contains tlvo carbonatoms convent;onally labelled as A and B atom. There are several possibilities tochoose a unit cell, the dotted lines indicate one in real space which has the shape ofa rhombus, as shown in the Figure.

    (a) Determine the three Cartesian components ofthe lattice vectors al and a2 interms of the C-C bond len6h oa 6.

    I t..a:'.

  • l+ r'-

    IlPT

  • Lc) Itller i,.' d.jder ql, a"d 5i-pl a

    (0"o.) T

    l\l-mt ;[",n*Lre oft Iu Jtfnene'kr, le,,', o.r, (omponerJ,a 66 lor;,0

    lL

    \& \roJi,s O, or. ,1..

    a4

    Talz1".1

    o'/l.l

    $lb tL

    )de .r?,6pleyl t",*,f )h". l* r,3 .c'., t