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21.
Dörr FA Kovačevi B Maksi ZB Pinto E Volmer DA 《Journal of the American Society for Mass Spectrometry》2011,22(11):2011-2020
The aim of this study was to investigate the unusual gas-phase dissociation behavior of two epimer pairs of protonated gonyautoxins
(GTX) following electrospray ionization in comparison to their deprotonated counterparts. The chemical structures of the investigated
GTX1-4 variants vary in their substitution pattern at N-1 and the stereochemical orientation of the hydroxysulfate group at C-11
(11α for GTX1/2 versus 11β for GTX3/4). The direct comparison of mass spectra in positive and negative ion modes illustrated two distinct features: first, an intriguing
difference between protonated 11α and 11β species, where 11α conformations exhibited almost complete dissociation of [M +
H]+ ions via facile SO3 elimination, while 11β species remained mostly intact as [M + H]+; and second, the lack of such differences for the deprotonated counterparts. In this study, we propose an acid-catalyzed
elimination mechanism from density functional theory calculations, initiated by a proton transfer of a guanidinium proton
to the hydroxysulfate group with simultaneous SO3 release, which is only possible for the 11α conformation based on intramolecular distances. The same mechanism explains the
lack of a comparable SO3 loss in the negative ion mode. CID experiments supported this proposed mechanism for GTX1 and GTX2. Computational modeling of product ions seen in the CID spectra of GTX3 and GTX4 established that the lowest energy dissociation pathway for the 11β epimers is elimination of water with the possibility
for further SO3 release from the intermediate product. Experimental data for structurally analogous decarbamoyl gonyautoxins confirmed the
evidence for the GTX compounds as well as the proposed elimination mechanisms. 相似文献
22.
We verify the critical case of Strauss' conjecture [30] concerning the blow-up of solutions to semilinear wave equations with variable coefficients in , where . The perturbations of Laplace operator are assumed to be smooth and decay exponentially fast at infinity. We also obtain a sharp lifespan upper bound for solutions with compactly supported data when . The unified approach to blow-up problems in all dimensions combines several classical ideas in order to generalize and simplify the method of Zhou [43] and Zhou & Han [45]: exponential “eigenfunctions” of the Laplacian [37] are used to construct the test function for linear wave equation with variable coefficients and John's method of iterations [13] is augmented with the “slicing method” of Agemi, Kurokawa and Takamura [1] for lower bounds in the critical case. 相似文献
23.
It is proven that the completely integrable general Kirchhoff case of the Kirchhoff equations for B ?? 0 is not an algebraic complete integrable system. Similar analytic behavior of the general solution of the Chaplygin case is detected. Four-dimensional analogues of the Kirchhoff and the Chaplygin cases are defined on e(4) with the standard Lie-Poisson bracket. 相似文献
24.
25.
We give a bivariate analog of the Micchelli–Rivlin quadrature for computing the integral of a function over the unit disk using its Radon projections. 相似文献
26.
Roland H. Pawelke Michael Felderhoff Claudia Weidenthaler Borislav Bogdanovíc Ferdi Schüth Prof. Dr. 《无机化学与普通化学杂志》2009,635(2):265-270
Ternary halide systems KMIICl3 (MII = Ti, Cr, Mn, Fe, Co, Ni, Cu, Zn) have been prepared by mechanochemical synthesis. Furthermore, TiCl2 was converted to Ti7Cl16 by mechanochemical treatment. For most samples, the X‐ray powder diffraction patterns could either be assigned to isotypic structures or were found in accordance with reference data. The monochloride systems of Ti, Co and Zn were extended to their double chloride stoichiometry K2MIICl4. 相似文献
27.
Periodica Mathematica Hungarica - We establish direct estimates of the rate of weighted simultaneous approximation by the Szász–Mirakjan operator for smooth functions in the supremum... 相似文献
28.
B. D. Bojanov 《Analysis Mathematica》1980,6(3):185-197
(v
k)
1
n
, 1v
kr, v1+...+vn
r, p(;r) — =(x
1,v
1),...,(x
n,v
n), v
1+...+v
n-r
(r(;·)=1. , (*;t) [, ] (;t) x
1<... n v
1 ...,v
n. (*;t) . 相似文献
29.
30.