Polaron pair versus bipolaron on oligothiophene chains:: A theoretical study of the singlet and triplet states
Polaron pair versus bipolaron on oligothiophene chains:: A theoretical study of the singlet and triplet states
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DOI:
10.1002/cphc.200200446
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发表时间:
2003-04-14
期刊:
影响因子:
2.9
通讯作者:
Brédas, JL
中科院分区:
文献类型:
--
作者:
Geskin, VM;Brédas, JL
The geometry of p-conjugated oligomers and polymers is very sensitive to the amount of charge the chains carry. Given this strong electron±phonon coupling, it has been shown that excess charge can concentrate and lead to structural distortions extending over a limited section of the chain. Such a selflocalization of defects in p-conjugated chains has been amply documented.[1] Not only a single charge can be trapped in this way forming a polaron (radical-ion species), but also a double charge is supposed to form a bipolaron (di-ion) structure.[1, 2] Direct structural data for charged species are scarce; the form of charge storage has therefore been deduced from various spectral and electrochemical experiments; these results can sometimes lead to different interpretations. In addition to single polarons and bipolarons on isolated chains, p dimers involving two polarons on two chains [3, 4] and polaron pairs on a single chain [5] have been invoked (it can be noted here that in some instances, spectral assignments considered early on as a signature of bipolarons were later reassigned to polarons [6]). In the case of a bipolaron, it is useful to discriminate between intrinsic and relative stability. A molecular species is intrinsically stable when the potential energy surface presents a minimum corresponding to its structure. However, such a species can turn out to be unstable relative to a species of the same composition but of a different geometry and/or in a different electronic state. Herein, we ask the question of whether a bipolaron on an isolated oligothiophene chain in the absence of counterions is intrinsically stable and whether it is relatively stable versus a dissociated polaron pair; excluding counterions is especially relevant when this question is addressed to the case of charges additional preparation steps. Fatty acids of different length (Sigma Aldrich) were dissolved in 1-phenyloctane without any additional purification or drying of the molecules or the solvent. A droplet of this solution was transferred to the substrate with a glass pipette and the tip was immersed into the droplet (typical tunneling conditions: I% 500 pA, Ubias% 750 mV depending on the investigated system). After inspection of the template layer by means of STM the adsorbates such as urea or palladium (II) acetate (Sigma Aldrich), also dissolved in 1-phenyloctane, were carefully added to the droplet to maintain the tip position. The concentration of the adsorbate solution should be saturated since the concentration of the template molecules should remain approximately constant. To exclude STM artifacts due to different tunneling conditions the tunneling parameters were kept unchanged for the imaging of the decorated template layers. All STM images were recorded in constant height mode.The authors acknowledge fruitful discussions with Prof. Dr. Gerhard Erker and Dr. Jˆrg Wonnemann (Organisch Chemisches Institut, University of M∏ nster, Germany), who also provided NMR investigations and the SH-C14H28-COOH material. This work has been financially supported by the Deutsche Forschungsgemeinschaft (SFB 424).