Simpson M J, Tuckett R P, Dunn K F, Hunniford C A, Latimer C J
School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom.
J Chem Phys. 2009 May 21;130(19):194302. doi: 10.1063/1.3137103.
Using synchrotron radiation, negative ions are detected by mass spectrometry following vacuum-UV photoexcitation of trifluorochloromethane (CF(3)Cl), trifluorobromomethane (CF(3)Br), and trifluoroiodomethane (CF(3)I). The anions F(-), X(-), F(2)(-), FX(-), CF(-), CF(2)(-), and CF(3)(-) are observed from all three molecules, where X = Cl, Br, or I, and their ion yields recorded in the range of 8-35 eV. With the exception of Br(-) and I(-), the anions observed show a linear dependence of signal with pressure, showing that they arise from unimolecular ion-pair dissociation. Dissociative electron attachment, following photoionization of CF(3)Br and CF(3)I as the source of low-energy electrons, is shown to dominate the observed Br(-) and I(-) signals, respectively. Cross sections for ion-pair formation are put onto an absolute scale by calibrating the signal strengths with those of F(-) from both SF(6) and CF(4). These anion cross sections are normalized to vacuum-UV absorption cross sections, where available, and the resulting quantum yields are reported. Anion appearance energies are used to calculate upper limits to 298 K bond dissociation energies for D(o)(CF(3)-X), which are consistent with literature values. We report new data for D(o)(CF(2)I(+)-F) < or = 2.7+/-0.2 eV and Delta(f)H(o)(298)(CF(2)I(+)) < or = (598+/-22) kJ mol(-1). No ion-pair formation is observed below the ionization energy of the parent molecule for CF(3)Cl and CF(3)Br, and only weak signals (in both I(-) and F(-)) are detected for CF(3)I. These observations suggest that neutral photodissociation is the dominant exit channel to Rydberg state photoexcitation at these lower energies.
利用同步辐射,在对三氟氯甲烷(CF(3)Cl)、三氟溴甲烷(CF(3)Br)和三氟碘甲烷(CF(3)I)进行真空紫外光激发后,通过质谱法检测负离子。从这三种分子中均观察到了阴离子F(-)、X(-)、F(2)(-)、FX(-)、CF(-)、CF(2)(-)和CF(3)(-),其中X = Cl、Br或I,并记录了它们在8 - 35电子伏特范围内的离子产率。除了Br(-)和I(-)外,观察到的阴离子信号与压力呈线性关系,这表明它们源自单分子离子对解离。CF(3)Br和CF(3)I光致电离后产生的低能电子引发的解离电子附着分别主导了观察到的Br(-)和I(-)信号。通过用来自SF(6)和CF(4)的F(-)信号强度校准信号强度,将离子对形成的截面换算到绝对尺度。这些阴离子截面在可用时被归一化为真空紫外吸收截面,并报告了所得的量子产率。利用阴离子出现能计算了D(o)(CF(3)-X)在298 K时键解离能的上限,其与文献值一致。我们报告了新的数据:D(o)(CF(2)I(+)-F) ≤ 2.7±0.2电子伏特,以及Δ(f)H(o)(298)(CF(2)I(+)) ≤ (598±22)千焦每摩尔。对于CF(3)Cl和CF(3)Br,在母体分子的电离能以下未观察到离子对形成,而对于CF(3)I仅检测到微弱信号(I(-)和F(-)中均有)。这些观察结果表明,在这些较低能量下,中性光解离是里德堡态光激发的主要出射通道。