The reaction of ZnEt2 with HO(O)P(OtBu)2 gives the insoluble polymer {Zn[O2P(OtBu)2]2}n (1). In the presence of slight amounts of water, this reaction produces good yields of the oxo-centered tetranuclear cluster Zn4(μ4-O)[O2P(OtBu)2]6 (2), which has been characterized by X-ray crystallography. Compound 2 is thermally labile and eliminates isobutene and water over the temperature range 130−220 °C. The ceramic yield at 900 °C corresponds to the theoretical yield for a Zn4P6O19 material, and the observed products at this temperature are α-Zn2P2O7 and β-Zn(PO3)2 (by XRD). When heated in ethanol at 85 °C for 30 h, 2 converts to polymer 1 and ZnO. This transformation is facilitated by acids, which allow the conversion to occur at room temperature. Polymer 1, characterized by X-ray crystallography, adopts a zigzag structure with zinc atoms linked alternately by one and then three bridging phosphate groups. This structure is therefore different from that adopted by the other two organozincophosphate {Zn[O2P(OR)2]2}n polymers that are known, which exist as linear chains with the zinc atoms bridged by two phosphate groups. Polymer 1 undergoes a quantitative pyrolytic conversion to β-Zn(PO3)2. Diffusion of a toluene solution of 2 into a dichloromethane solution of 1,6-hexanediamine produces a coordination network with the formula {Zn[O2P(OtBu)2]2[H2N(CH2)6NH2]}n (3), with elimination of ZnO. The network structure of 3 consists of {Zn[O2P(OtBu)2]2[H2N(CH2)6NH2]}n polymer strands interconnected via hydrogen bonds between the N−H and PO groups to form layers stacked along the crystallographic b axis. Each polymer chain contains four-coordinate zinc atoms bonded to two monodentate di-tert-butylphosphate ligands and linked by 1,6-hexanediamine groups. Slabs of the layered structure are held together by a dense array of hydrogen bonds involving the N−H and PO functionalities. These layers possess zinc phosphate/1,6-hexanediamine cores and are coated with tert-butyl groups such that there are only van der Waals interactions between layers. Thermogravimetric analysis and XRD studies show that 3 undergoes thermolysis to a mixture of crystalline α-Zn2P2O7 and β-Zn(PO3)2.
Objectives.
In this second paper in a series we present measurements of spectral features\nof 432 low-redshift (z < 0.1) optical spectra of 261 Type Ia supernovae (SNe\nIa) within 20 d of maximum brightness. The data were obtained from 1989 through\nthe end of 2008 as part of the Berkeley SN Ia Program (BSNIP) and are presented\nin BSNIP I (Silverman et al. 2012). We describe in detail our method of\nautomated, robust spectral feature definition and measurement which expands\nupon similar previous studies. Using this procedure, we attempt to measure\nexpansion velocities, pseudo-equivalent widths (pEW), spectral feature depths,\nand fluxes at the centre and endpoints of each of nine major spectral feature\ncomplexes. We investigate how velocity and pEW evolve with time and how they\ncorrelate with each other. Various spectral classification schemes are employed\nand quantitative spectral differences among the subclasses are investigated.\nSeveral ratios of pEW values are calculated and studied. The so-called Si II\nratio, often used as a luminosity indicator (Nugent et al. 1995), is found to\nbe well correlated with the so-called "SiFe" ratio and anticorrelated with the\nanalogous "SSi ratio," confirming the results of previous studies. Furthermore,\nSNe Ia that show strong evidence for interaction with circumstellar material or\nan aspherical explosion are found to have the largest near-maximum expansion\nvelocities and pEWs, possibly linking extreme values of spectral observables\nwith specific progenitor or explosion scenarios. [Abridged]\n