Optical properties of organic semiconductor thin films: 2,6,9,10-tetrakis(phenylethynyl)anthracene

Two kinds of anthracene derivative thin films, 2, 6-bis((4-hexylphenyl)ethynyl)-9, 10-bis(phenyl ethynyl)anthracene (B-ant-THB) and 9, 10-bis((4-hexyl phenyl)ethynyl)-2, 6-bis (phenyl ethynyl) anthracene (HB-ant-TB), were synthesized to investigate their optical properties. The difference between the two anthracene derivatives consisted of the position of the 1-ethynyl-4-hexylbenzene group substitution into an anthracene ring. We measured the optical properties of the anthracene derivatives by using photoluminescence (PL), transmittance spectroscopy, and spectroscopic ellipsometry. The dielectric functions of the two films were similar with respect to transition energies, but were different in terms of amplitudes. The optical band gap energies of the B-ant-THB and the HB-ant-TB film states were estimated to be 2.45 eV and 2.34 eV, respectively, whereas density functional theory (DFT) calculations of isolated molecular states showed the same value of 2.42 eV. The large bathochromic shift of the HB-ant-TB film state compared to the DFT calculation is attributed to strong intermolecular coupling between the HB-ant-TB molecules in the crystalline film because the HB-ant-TB film has higher crystallinity than the B-ant-THB film. The symmetric structures of the transmittance and PL spectra of the anthracene derivative films were observed as distinct peaks having similar vibrational energy levels for the singlet ground state and the first excited state.

[1]  Hadis Morkoç,et al.  Energy transfer in ZnO-anthracene hybrid structure , 2012 .

[2]  M. Cho,et al.  Semiconducting 2,6,9,10-tetrakis(phenylethynyl)anthracene derivatives: effect of substitution positions on molecular energies. , 2011, Organic letters.

[3]  Dong Hoon Lee,et al.  Organic thin-film transistor properties and the structural relationships between various aromatic end-capped triisopropylsilylethynyl anthracene derivatives , 2010 .

[4]  Yan Li Zhang,et al.  Donor−Acceptor-Substituted Anthracene-Centered Cruciforms: Synthesis, Enhanced Two-Photon Absorptions, and Spatially Separated Frontier Molecular Orbitals , 2009 .

[5]  Y. Mori,et al.  Conversion of bromoalkenes into alkynes by wet tetra-n-butylammonium fluoride. , 2009, The Journal of organic chemistry.

[6]  H. Tam,et al.  Novel host materials for single-component white organic light-emitting diodes based on 9-naphthylanthracene derivatives , 2008 .

[7]  F. Spano,et al.  Experimental and theoretical study of temperature dependent exciton delocalization and relaxation in anthracene thin films. , 2008, The Journal of chemical physics.

[8]  D. Bradley,et al.  Dimensionality of electronic excitations in organic semiconductors : A dielectric function approach , 2007 .

[9]  M. Schubert,et al.  Refractive indices and band-gap properties of rocksalt MgxZn1−xO (0.68⩽x⩽1) , 2006 .

[10]  C. Ambrosch-Draxl,et al.  Ab initio study of anthracene under high pressure , 2003 .

[11]  Charles E. Swenberg,et al.  Electronic Processes in Organic Crystals and Polymers , 1999 .

[12]  J. D. Benson,et al.  Development of a parametric optical constant model for Hg1−xCdxTe for control of composition by spectroscopic ellipsometry during MBE growth , 1998 .

[13]  P. Hodge,et al.  Synthesis of poly(anthracene-2,6-diyl) and a copolymer containing alternately anthracene-2,6-diyl and p-phenylene units , 1997 .

[14]  Cardona,et al.  Temperature dependence of the dielectric function and interband critical points in silicon. , 1987, Physical review. B, Condensed matter.

[15]  D. Aspnes Optical properties of thin films , 1982 .

[16]  R. D. Birkhoff,et al.  Optical properties of polycrystalline anthracene in the 3.2–9.3‐eV spectral region , 1980 .

[17]  T. S. Moss,et al.  Handbook on semiconductors , 1980 .

[18]  W. H. Wright Ultraviolet Optical Constants of Anthracene , 1967 .

[19]  Francis Arthur Jenkins,et al.  Fundamentals of Optics , 1976 .