Schwerdtfeger Peter, Bast Radovan, Gerry Michael C L, Jacob Christoph R, Jansen Martin, Kellö Vladimir, Mudring Anja V, Sadlej Andrzej J, Saue Trond, Söhnel Tilo, Wagner Friedrich E
Theoretical and Computational Chemistry Research Center (TCCRC), Institute of Fundamental Sciences, Massey University (Albany Campus), Private Bag 102904, North Shore MSC, Auckland, New Zealand.
J Chem Phys. 2005 Mar 22;122(12):124317. doi: 10.1063/1.1869975.
An attempt is made to improve the currently accepted muonic value for the 197Au nuclear quadrupole moment [+0.547(16)x10(-28) m2] for the 3/2+ nuclear ground state obtained by Powers et al. [Nucl. Phys. A230, 413 (1974)]. From both measured Mossbauer electric quadrupole splittings and solid-state density-functional calculations for a large number of gold compounds a nuclear quadrupole moment of +0.60x10(-28) m2 is obtained. Recent Fourier transform microwave measurements for gas-phase AuF, AuCl, AuBr, and AuI give accurate bond distances and nuclear quadrupole coupling constants for the 197Au isotope. However, four-component relativistic density-functional calculations for these molecules yield unreliable results for the 197Au nuclear quadrupole moment. Relativistic singles-doubles coupled cluster calculations including perturbative triples [CCSD(T) level of theory] for these diatomic systems are also inaccurate because of large cancellation effects between different field gradient contributions subsequently leading to very small field gradients. Here one needs very large basis sets and has to go beyond the standard CCSD(T) procedure to obtain any reliable field gradients for gold. From recent microwave experiments by Gerry and co-workers [Inorg. Chem. 40, 6123 (2001)] a significantly enhanced (197)Au nuclear quadrupole coupling constant in (CO)AuF compared to free AuF is observed. Here, these cancellation effects are less important, and relativistic CCSD(T) calculations finally give a nuclear quadrupole moment of +0.64x10(-28) m2 for 197Au. It is argued that it is currently very difficult to improve on the already published muonic value for the 197Au nuclear quadrupole moment.
人们试图改进目前公认的由鲍尔斯等人[《核物理》A230, 413 (1974)]得出的197Au核四极矩[+0.547(16)×10(-28) m2],该值是针对3/2+核基态的。通过对大量金化合物的穆斯堡尔电四极分裂测量以及固态密度泛函计算,得到了核四极矩为+0.60×10(-28) m2。近期对气相AuF、AuCl、AuBr和AuI的傅里叶变换微波测量给出了197Au同位素的精确键长和核四极耦合常数。然而,对这些分子进行的四分量相对论密度泛函计算得出的197Au核四极矩结果不可靠。对于这些双原子体系,包括微扰三重激发的相对论单双耦合簇计算[CCSD(T)理论水平]也不准确,因为不同场梯度贡献之间存在很大的抵消效应,随后导致场梯度非常小。在此,需要非常大的基组,并且必须超越标准的CCSD(T)程序才能获得金的任何可靠场梯度。从杰里及其同事近期的微波实验[《无机化学》40, 6123 (2001)]中观察到,与自由AuF相比,(CO)AuF中(197)Au核四极耦合常数显著增强。在此,这些抵消效应不太重要,相对论CCSD(T)计算最终给出197Au的核四极矩为+0.64×10(-28) m2。有人认为,目前很难改进已发表的197Au核四极矩的μ子值。