Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, Massachusetts 02138, USA.
J Chem Phys. 2012 Jan 21;136(3):034303. doi: 10.1063/1.3673875.
The molecular structure of trans, planar hydridotrioxygen (HOOO) has been examined by means of isotopic spectroscopy using Fourier transform microwave as well as microwave-millimeter-wave double resonance techniques, and high-level coupled cluster quantum-chemical calculations. Although this weakly bound molecule is readily observed in an electrical discharge of H(2)O and O(2) heavily diluted in an inert buffer gas, we find that HOOO can be produced with somewhat higher abundance using H(2) and O(2) as precursor gases. Using equal mixtures of normal and (18)O(2), it has been possible to detect three new isotopic species, H(18)OOO, HO(18)O(18)O, and H(18)O(18)O(18)O. Detection of these species and not others provides compelling evidence that the dominant route to HOOO formation in our discharge is via the reaction OH + O(2) → HOOO. By combining derived rotational constants with those for normal HOOO and DOOO, it has been possible to determine a fully experimental (r(0)) structure for this radical, in which all of the structural parameters (the three bond lengths and two angles) have been varied. This best-fit structure possesses a longer central O-O bond (1.684 Å), in agreement with earlier work, a markedly shorter O-H bond distance (0.913 Å), and a more acute [angle]HOO angle (92.4°) when compared to equilibrium (r(e)) structures obtained from quantum-chemical calculations. To better understand the origin of these discrepancies, vibrational corrections have been obtained from coupled-cluster calculations. An empirical equilibrium (r(e) (emp)) structure, derived from the experimental rotational constants and theoretical vibrational corrections, gives only somewhat better agreement with the calculated equilibrium structure and large residual inertial defects, suggesting that still higher order vibrational corrections (i.e., γ terms) are needed to properly describe large-amplitude motion in HOOO. Owing to the high abundance of this oxygen-chain radical in our discharge expansion, a very wide spectral survey for other oxygen-bearing species has been undertaken between 6 and 25 GHz. Only about 50% of the observed lines have been assigned to known hydrogen-oxygen molecules or complexes, suggesting that a rich, unexplored oxygen chemistry awaits detection and characterization. Somewhat surprisingly, we find no evidence in our expansion for rotational transitions of cis HOOO or from low-lying vibrationally excited states of trans HOOO under conditions which optimize its ground state lines.
通过傅里叶变换微波以及微波-毫米波双共振技术和高精度耦合簇量子化学计算,研究了反式、平面的羟三氧(HOOO)的分子结构。尽管这种弱束缚分子很容易在含有大量惰性缓冲气体的 H(2)O 和 O(2) 的放电中被观察到,但我们发现使用 H(2)和 O(2)作为前体气体可以更大量地产生 HOOO。使用正常和(18)O(2)的等比例混合物,已经有可能检测到三种新的同位素物种,H(18)OOO、HO(18)O(18)O 和 H(18)O(18)O(18)O。这些物种的检测而不是其他物种的检测提供了令人信服的证据,表明我们放电中 HOOO 形成的主要途径是通过 OH + O(2) → HOOO 反应。通过将衍生的转动常数与正常 HOOO 和 DOOO 的转动常数相结合,我们已经有可能确定了这种自由基的完全实验(r(0))结构,其中所有结构参数(三个键长和两个角度)都已发生变化。该最佳拟合结构具有较长的中心 O-O 键(1.684 Å),与早期工作一致,较短的 O-H 键距离(0.913 Å),以及当与量子化学计算得到的平衡(r(e))结构相比时,更尖锐的[角]HOO 角(92.4°)。为了更好地理解这些差异的来源,已经从耦合簇计算中获得了振动修正。从实验转动常数和理论振动修正中得出的经验平衡(r(e) (emp))结构,与计算平衡结构和大惯性缺陷仅略有更好的一致性,表明仍然需要更高阶的振动修正(即γ项)来正确描述 HOOO 中的大振幅运动。由于我们放电膨胀中这种氧链自由基的高丰度,在 6 到 25 GHz 之间进行了非常广泛的含氧物种光谱调查。仅将观察到的线的约 50%分配给已知的氢-氧分子或复合物,这表明一种丰富的、未经探索的氧化学有待发现和表征。有些令人惊讶的是,在我们的扩展条件下,我们没有发现顺式 HOOO 的旋转跃迁或反式 HOOO 的低振动激发态的证据,而这些条件优化了其基态线。