Page 38 - Carbon Nanotubes
P. 38

Physics of  carbon nanotubes                       29
                                     Table  1.  Parameters of  carbon nanotubes

          Symbol             Name                          Formula                   Value
              ___
                  carbon-carbon distance                                        1.421 *4 (graphite)
                  length of  unit  vector                                       2.46  A

                  unit vectors                                                  in  (x,y) coordinates

                  reciprocal lattice vectors                                    in (x,y) coordinates

                  chiral vector                Ch = na, + ma2 = (n,m)           n, m: integers
                  circumference  of nanotube    L= /C,I =uJn~+m2+nm             Oslmlsn
                                                   L   Jn’+m’+nm
                  diameter  of  nanotube       d,=  - z            li
                                                   7r       7r
                  chiral angle

                                                        2n + m
                                               cos 0 =
                                                     2Jn2 + m2 + nm
                                                      am
                                               tan 0  = -
                                                     2n + m
                  the highest common divisor of (n, m)
                  the highest common divisor of     d   if  n  - m not a multiple of  3d
                    (2n + m,2m + n)            dR=(
                                                    3d   if n  - m a multiple of  3d.
                  translational vector  of  1D unit cell   T  = t,a, + f2a2 = (11,12)   t, , t,:  integers
                                                   2m + n
                                               t, =  ~
                                                    dR
                                                    2n + m
                                               1,  = -~
                                                      dR
                                                   aL
                  length of  T                 T= -
                                                   dR
                                                   2(n2 + in2 + nm)
                  number of  hexagons per  1D unit  cell   N=                   2N = n,/unit  cell
                                                        dR
                  symmetry vector$              R =pa, + qa2 = (nq)             p, q: integers?
                                                 d = mp - nq, 0 5 p  s n/d, 0 5 q 5 m/d
                  number of  2n revolutions     M= [(2n + m)p + (2m + n)q]/d,   M: integer
                                               NR = MCh + dT
                  basic symmetry operation$     R  = ($17)

                  rotation operation                                            6: radians
                                                    dT
                  translation operation          71-                            T,X: length
                                                    N
             t (p, q) are uniquely determined by d = mp - nq, subject to conditions stated in table, except for zigzag tubes for which
          C, = (n,O), and we definep = 1, q = -1,  which gives M= 1.
             $R and R refer to the same symmetry operation.



          (n,O) tubules], where the translational and rotational   this  volume  for  further details  regarding  the  non-
          symmetry operations can each be executed indepen-   symmorphic space groups for chiral nanotubes.
          dently, or the symmetry group can be non-symmorphic   The  symmetry  operations  of  the  infinitely  long
          (for a general nanotube), where the basic symmetry   armchair tubule (n = m), or zigzag tubule (rn = 0), are
          operations require both a rotation  $ and translation   described  by  the  symmetry  groups Dnh or Dnd for
          r  and is  written  as R  = ($1  r)[7].  We  consider  the   even or odd n, respectively,  since inversion is an ele-
          symmorphic case in some detail  in this article,  and   ment of Dnd only for odd n, and is an element of Dnh
          refer  the reader to the paper  by  Eklund et al.[8] in   only for even n [9]. Character tables for the D, groups
   33   34   35   36   37   38   39   40   41   42   43