Exciton-Lattice Phonon Coupling in Organic Semiconductor Crystals beyond the Static Disorder

被引:8
|
作者
Raimondo, Luisa [1 ]
Silvestri, Leonardo [2 ]
Borghesi, Alessandro [1 ]
Tavazzi, Silvia [1 ]
机构
[1] Univ Milano Bicocca, Dipartimento Sci Mat, I-20125 Milan, Italy
[2] Univ New S Wales, Sch Elect Engn & Telecommun, Sydney, NSW 2052, Australia
来源
JOURNAL OF PHYSICAL CHEMISTRY C | 2013年 / 117卷 / 49期
关键词
NUMERICAL EXPERIMENTS; POLARIZED ABSORPTION; OPTICAL-PROPERTIES; LINE-SHAPE; QUATERTHIOPHENE; LINESHAPE; GROWTH; VIBRATIONS; SPECTRA; ENERGY;
D O I
10.1021/jp409611q
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Investigations of the physical properties of pi-conjugated organic semiconductor single crystals represent the first step for understanding their role as active materials in devices and for determining what limits device performance. In this respect, the role of both static and dynamic disorder is pivotal, affecting exciton and charge-carrier mobility. Here, the effects of disorder on the optical response of a paradigmatic class of organic semiconductors, namely oligothiophenes, are addressed. The temperature dependence of the optical response in the spectral range related to the lowest-energy state is investigated by comparing the results of three different samples. The spectral features are identified and a peak never reported in the literature is discussed in the framework of the new classification of the exciton-phonon coupling in molecular aggregates (Spano et al., J. Chem. Phys. 2007, 127, 184703). The temperature dependence of the line shape of the low-energy tail of the lowest-energy peak is discussed in the framework of the so-called Urbach tail analysis for discriminating between the contribution of the static and dynamic disorder to the optical response of the crystals. The energy of the low-energy phonon modes coupled to the lowest-energy exciton is determined, and a measure of its strength is given.
引用
收藏
页码:26248 / 26254
页数:7
相关论文
共 50 条
  • [31] Study of strong coupling between surface plasmon and exciton in an organic semiconductor
    Bonnand, Clement
    Bellessa, Joel
    Plenet, Jean-Claude
    JOURNAL OF NON-CRYSTALLINE SOLIDS, 2006, 352 (9-20) : 1683 - 1685
  • [32] Quantum dot Rabi rotations beyond the weak exciton-phonon coupling regime
    McCutcheon, Dara P. S.
    Nazir, Ahsan
    NEW JOURNAL OF PHYSICS, 2010, 12
  • [33] EXCITONIC PROCESSES IN AROMATIC MOLECULAR-CRYSTALS OF STRONG EXCITON-PHONON COUPLING
    MATSUI, AH
    PURE AND APPLIED CHEMISTRY, 1995, 67 (03) : 429 - 436
  • [34] VIBRONIC COUPLING IN EXCITON STATES OF RIGID-LATTICE MODEL OF MOLECULAR CRYSTALS
    PHILPOTT, MR
    JOURNAL OF CHEMICAL PHYSICS, 1967, 47 (11): : 4437 - &
  • [35] Exciton-phonon coupling and disorder in the excited states of CdSe colloidal quantum dots
    Salvador, Mayrose R.
    Graham, Matthew W.
    Scholes, Gregory D.
    JOURNAL OF CHEMICAL PHYSICS, 2006, 125 (18):
  • [37] The unbalanced phonon-induced superconducting state on a square lattice beyond the static boundary
    Szewczyk, K. A.
    Jarosik, M. W.
    Durajski, A. P.
    Szczesniak, R.
    PHYSICA B-CONDENSED MATTER, 2021, 600
  • [38] Anderson localization in synthetic photonic lattice with static random coupling disorder
    Pankov, Artem, V
    Vatnik, Ilya D.
    Churkin, Dmitry, V
    Derevyanko, Stanislav A.
    2019 CONFERENCE ON LASERS AND ELECTRO-OPTICS EUROPE & EUROPEAN QUANTUM ELECTRONICS CONFERENCE (CLEO/EUROPE-EQEC), 2019,
  • [39] Raman antenna effect from exciton-phonon coupling in organic semiconducting nanobelts
    Wang, Mao
    Gong, Yi
    Alzina, Francesc
    Svoboda, Ondrej
    Ballesteros, Belen
    Sotomayor Torres, Clivia M.
    Xiao, Senbo
    Zhang, Zhiliang
    He, Jianying
    NANOSCALE, 2017, 9 (48) : 19328 - 19336
  • [40] Weak exciton-plasmon and exciton-phonon coupling in chemically synthesized Ag/CdSe metal/semiconductor hybrid nanocomposite
    Okasha, Aly
    Mohamed, Mona B.
    Negm, Sohair
    Talaat, H.
    PHYSICA E-LOW-DIMENSIONAL SYSTEMS & NANOSTRUCTURES, 2012, 44 (10): : 2094 - 2098