Page 93 - Organic Electronics in Sensors and Biotechnology
P. 93

70    Cha pte r  T w o

               π-systems, independently from the structural packing of the D3ANT
               molecules in the solid active layer. However, as a bulk technique,
               GIXRD is unable to provide structural information on molecular
               arrangement of the first monolayer at ultrathin organic semiconductor/
               SiO  interface where field effect takes place. XRD studies only allow
                  2
               the interpretation of oligomer chain packing up to the resolution of
               several monolayers.
                   To shed more light on the two-dimensional self-organization of
               D3ANT, we investigated monolayers on highly organized pyrolitic
               graphite (HOPG) and  Au(111) by scanning tunneling microscopy
               (STM) in a liquid environment of n-tetradecane. 135–137  The STM study
               reveals 2D organization of the molecular architectures induced by the
               substrate-molecule and molecule-molecule interactions on conduct-
               ing and atomically flat substrates.
                   Two-dimensional layer consisting of highly ordered monodo-
               mains that extend over distances of 100 to 400 nm on highly oriented
               pyrolytic graphite (HOPG) was formed, as seen in Fig. 2.6b. Each
               domain consists of a closed-packed arrangement of linear and parallel
               rows of molecules. The distance between adjacent rows is 1.3 nm (in
               dark contrast) corresponding to the decyl chains in a slightly tilted posi-
               tion. The bright contrast areas correspond to the main  π-conjugated
               backbone of D3ANT with a length of ~2.0 nm, in good agreement
               with the calculated core length (1.9 nm) and the profile of frontier wave
               functions, which is mainly defined by three anthracene subunits. The
               2D unit cell parameters were measured to be a = 3.1 nm, b = 1.2 nm,
               α= 94°. Moreover, from the high-resolution STM figure, the three
               anthracene subunits of each individual molecule are clearly visible
               on HOPG surface. Such evidence proves a nearly planar adsorption
               of the entire molecule on HOPG with no twist angle and full conjuga-
               tion between the anthracene subunits.
                   D3ANT molecules adsorbed on reconstructed Au(111) (Fig. 2.6c)
               also form self-organized domains with linear and parallel row 2D
               structure very similar to that on HOPG. However, noticeable differ-
               ences in the organizing behavior of the D3ANT can be observed by
               comparing both images. The self-organized domains on  Au(111)
               surface do not extend over distances as large as on HOPG, and the
               distance between adjacent D3ANT rows on  Au(111) (~0.3 nm) is
               markedly smaller than that on HOPG. On Au surface, D3ANT cannot
               accommodate decyl chains which are probably folded below or above
               the anthracene subunits, and this results in a more densely packed 2D
               structure on Au(111) as compared to HOPG. Again, the individual
               anthracene subunits of each molecule are clearly visible.
                   As seen, for spin-coated and annealed thin films of D3ANT, the
               GIXRD analysis indicated the lack of bulk ordered, but at the same
               time the STM revealed the strong tendency to form high-order 2D
               self-assembled monolayer on both HOPG and  Au(111) surface.
   88   89   90   91   92   93   94   95   96   97   98