Asaoka Sadayuki, Takeda Norihiko, Iyoda Tomokazu, Cook Andrew R, Miller John R
Chemistry Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA.
J Am Chem Soc. 2008 Sep 10;130(36):11912-20. doi: 10.1021/ja800426z. Epub 2008 Aug 13.
Polyfluorenes (pF) were synthesized having anthraquinone (AQ) or naphtylimide (NI) end caps that trap electrons or di- p-tolylaminophenyl (APT2) caps that trap holes. The average lengths of the pF chains in these molecules varied from 7 to 30 nm. End capping was found not to be complete in these molecules so that some were without caps. Electrons or holes were injected into these polymers in solution by pulse radiolysis. Following attachment, the charges migrated to the end cap traps in times near 2 ns in pF12AQ or 5 ns in pF35NI. From these observations, electron mobilities for transport along single chains to the end caps in THF solution were determined to be smaller by a factor of 100 than those observed by microwave conductivity. Despite this, the mobilities were sufficiently large to provide encouragement to the use of such single chains in solar photovoltaics. Most charges were observed to transport over substantial distances in these polymers, but 23, 18, and 37% of the charges attached to pFNI, pFAQ, and pFAPT2, respectively, were trapped in the pF chains and decayed by slower bimolecular reactions. For pFAQ and pFAPT2, all of the trapped charges were accounted for by estimates of the fraction of molecules having no end cap traps. For pF35NI, 23% of the attached electrons were found to be trapped in the chains, but only 4% of chains were expected to have no end caps. This could indicate some trapping by kinks or other defects but may just reflect uncertainties in the capping of this long polymer. When the charges reach the trap groups, their spectra have no features of pF(-) or pF(+), nor do the principal bands of the trapped ions resemble spectra of the radical ions of isolated trap molecules. The optical absorption spectra are rather dominated by new bands identified as charge-transfer transitions, which probably reinject electrons or holes into the pF chains. The energies of those bands correlate well with measured redox potentials.
合成了带有蒽醌(AQ)或萘二甲酰亚胺(NI)端基的聚芴(pF),其中蒽醌和萘二甲酰亚胺端基用于捕获电子,二对甲苯氨基苯基(APT2)端基用于捕获空穴。这些分子中pF链的平均长度在7至30纳米之间。发现这些分子中的封端并不完全,因此有些分子没有端基。通过脉冲辐解将电子或空穴注入到这些聚合物的溶液中。附着后,电荷在pF12AQ中约2纳秒或pF35NI中约5纳秒的时间内迁移到端基陷阱。从这些观察结果来看,在四氢呋喃溶液中沿着单链向端基传输的电子迁移率比通过微波电导率观察到的迁移率小100倍。尽管如此,迁移率足够大,为在太阳能光伏中使用此类单链提供了鼓励。观察到大多数电荷在这些聚合物中传输了相当长的距离,但分别附着在pFNI、pFAQ和pFAPT2上的电荷中有23%、18%和37%被困在pF链中,并通过较慢的双分子反应衰减。对于pFAQ和pFAPT2,所有被困电荷都可以通过对无端基陷阱分子比例的估计来解释。对于pF35NI,发现23%的附着电子被困在链中,但预计只有4%的链没有端基。这可能表明存在由扭结或其他缺陷导致 的一些捕获,但也可能只是反映了这种长聚合物封端的不确定性。当电荷到达陷阱基团时,它们的光谱没有pF(-)或pF(+)的特征,被困离子的主要谱带也不像孤立陷阱分子的自由基离子的光谱。光学吸收光谱相当程度上由被确定为电荷转移跃迁的新谱带主导,这些谱带可能将电子或空穴重新注入到pF链中。这些谱带的能量与测量的氧化还原电位有很好的相关性。