School of Chemistry and Chemical Engineering, Key Laboratory of Mesoscopic Chemistry of MOE, Nanjing University, Nanjing, Jiangsu, People's Republic of China.
J Phys Chem B. 2011 Mar 31;115(12):2801-13. doi: 10.1021/jp110152q. Epub 2011 Mar 10.
Simulations of vibrational circular dichroism (VCD) spectroscopy of optical active aggregates of chiral molecules in the amorphous solid encounter great difficulties in the description of complicated intermolecular interactions by using the conventional quantum mechanical (QM) methods. The fragmentation approach is applied to calculate the VCD spectra of the covalently bonded oligomers and nonbonded molecular aggregates of (S)-alternarlactam, a new fungal cytotoxin with cyclopentenone and isoquinolinone scaffolds. Starting from the statistically averaged configurations that are sampled from the molecular dynamic simulations, the target oligomers or packing systems are divided into several fragments with a proper treatment of boundary effects on the separated segments. Each fragment is embedded in the background point charges centered on the distant atoms to simulate the long-range electrostatic interactions. The total VCD signals are assembled from the rotational strength of all the fragments. Test calculations on the σ-bonded oligomers and molecular aggregates using fragmentation method show good agreement with the conventional QM results. The packing effects on the infrared (IR) absorption and VCD spectroscopies of amorphous (S)-alternarlactam solid are investigated with density of 0.5 and 0.8 g/cm(3), respectively. The fragment-based VCD calculations on (S)-alternarlactam aggregates give a better agreement with experimental spectra than the Boltmann-weighted spectra of various possible monomeric, dimeric, and trimeric configurations. Hydrogen-bonded networks are the dominant packing configurations at the density of 0.5 g/cm(3). The (C═)O···H-N hydrogen-bonding interactions result in the signal splitting of IR and VCD spectra at the C═O stretching vibrational regions. When the density is increased to 0.8 g/cm(3), π-π stacking turns to be the dominating intermolecular interaction pattern. The computational cost of fragmentation calculation scales linearly with the number of the molecular fragments, facilitating the future applications to a wide range of the large-sized chiral systems.
模拟非晶态中手性分子的光学活性聚集体的振动圆二色性(VCD)光谱在描述复杂的分子间相互作用时遇到了很大的困难,这需要使用传统的量子力学(QM)方法。碎片方法被应用于计算共价键合低聚物和非键合分子聚集体的 VCD 光谱,这些低聚物和分子聚集体是一种新型真菌细胞毒素(S)-alternarlactam 的结构,该毒素具有环戊烯酮和异喹啉酮骨架。从分子动力学模拟中采样的统计平均构象出发,将目标低聚物或堆积系统划分为几个片段,并对分离片段的边界效应进行适当处理。将每个片段嵌入以远离原子为中心的背景点电荷中,以模拟远程静电相互作用。将所有片段的旋转强度组装成总 VCD 信号。使用碎片方法对σ键合低聚物和分子聚集体进行的测试计算与传统 QM 结果吻合良好。分别研究了堆积密度为 0.5 和 0.8 g/cm(3)时非晶态(S)-alternarlactam 固体的红外(IR)吸收和 VCD 光谱的堆积效应。与各种可能的单体、二聚体和三聚体构象的 Boltmann 加权光谱相比,基于碎片的(S)-alternarlactam 聚集体的 VCD 计算给出了与实验光谱更好的一致性。在堆积密度为 0.5 g/cm(3)时,氢键网络是主要的堆积构型。(C═)O···H-N 氢键相互作用导致 C═O 伸缩振动区域的 IR 和 VCD 光谱信号分裂。当密度增加到 0.8 g/cm(3)时,π-π 堆积成为主要的分子间相互作用模式。碎片计算的计算成本与分子碎片的数量呈线性关系,这有利于将来在更广泛的大型手性体系中应用。