聚苯并[c]-噻吩薄膜的椭圆偏振和原位红外联合研究

P. Christensen, J. Kerr, S. Higgins, A. Hamnett
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引用次数: 23

摘要

用两种方法从该单体在乙腈溶液中生长了聚苯并[c]噻吩[聚异噻吩]薄膜。首先,在四氟硼酸盐存在下,阴离子聚合在铂电极上产生稳定的聚合物(I型薄膜)。其次,用Br2作为电化学生成的中间体进行氧化聚合,会得到一种完全不同的材料(II型薄膜)。通过椭偏法发现I型薄膜相对致密,在中性形式下含有很少的溶剂。当从中性变为氧化态时,薄膜随着溶剂和反阴离子的吸收而膨胀。发现II型薄膜具有更开放的形式,椭偏和库仑法的估计与溶剂含量高4的因素一致。这些薄膜的潜在循环似乎对它们的厚度几乎没有影响。在I型薄膜上进行的原位红外测量与氧化形式的溶剂吸收一致,但光谱主要是由集中在4000 cm-1以上的强电子吸收的发展所主导,该吸收在高电位下向低频率转移。该电子带在1000 ~ 1400 cm-1之间伴有强吸收带的出现,与五元含s环有关,并与电子吸收最大值的位移有关。增强的振动峰是由于醌类振动与移动电荷缺陷耦合引起的“振幅模式”效应。随着电位的变化,红外光谱的演变可以与载流子的变化特性联系起来。
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A combined ellipsometric and in situ infrared (SNIFTIRS) study of poly(benzo-[c]-thiophene) films
Films of poly(benzo[c]thiophene)[poly(isothianaphthene)] have been grown from a solution of the monomer in acetonitrile by two methods. First, anionic polymerisation onto a platinum electrode in the presence of tetrafluoroborate affords a stable polymer (type I film). Secondly, oxidative polymerisation with Br2 as an electrochemically generated intermediate gives a rather different material (type II film). Films of type I are found by ellipsometry to be relatively dense, containing very little solvent in the neutral form. On switching from the neutral to the oxidised form, the film swells as solvent and counter anions are absorbed. Type II films are found to have a much more open form and estimates from ellipsometry and coulometry are consistent with a factor of four greater solvent content. Potential cycling of these films appears to have little effect on their thickness. The in situ i.r. measurements, carried out on a type I film, are consistent with absorption of solvent in the oxidised form, but the spectra are dominated by the development of a strong electronic absorption centred above 4000 cm–1 that shifts towards lower frequency at higher potentials. This electronic band is accompanied by the appearance of strong absorption bands between 1000 and 1400 cm–1 associated with the five-membered S-containing ring and correlating with the shift in electronic absorption maximum. The enhanced vibrational peaks are due to ‘amplitude-mode’ effects arising from the coupling of the quinonoid vibrations to the mobile charge defect. The evolution of the i.r. spectra with potential can then be associated with the changing character of the charge carriers.
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