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1 r shifts predicted already for these systems in vacuo.
2 ic acid by direct hydrogenation over Cu{110} in vacuo.
3 ained by desolvation of the blue solid phase in vacuo.
4 found to be the global minima configurations in vacuo.
5 explored at the MP2/6-31+G** level of theory in vacuo.
6 is worked up simply by removing the catalyst in vacuo.
7 enes) that have not been heretofore examined in vacuo.
8 lated to be 211.6 degrees and -175.1 degrees in vacuo.
10 inear triple bond is 50.4 kJ/mol less stable in vacuo according to the calculation, and the N-heteroc
12 on trapping is observed on the (101) surface in vacuo, an excess electron at the aqueous (101) interf
13 (d,p) and MP2/6-311++G(d,p) levels of theory in vacuo and aqueous phases) formulated tautomerization
16 e reactions have not heretofore been studied in vacuo and provide valuable data that can be compared
18 , but a profound difference is found between in vacuo and solvated reaction profiles, as expected.
19 e it exists as a zwitterion that is unstable in vacuo and therefore cannot be characterized using hig
21 cogen vacancies are selectively generated by in-vacuo annealing, but also focused ion beam exposure.
23 formational entropies are usually determined in vacuo by computer modeling, molecular recognition pro
26 he warming of vapor-deposited amorphous ices in vacuo, clathrate hydrates can form by rearrangements
29 he agreement between phi from experiment and in vacuo DFT indicates that the conformation is intrinsi
33 own that improvement could be achieved using in vacuo energy minimization with molecular mechanics an
34 % helium atmosphere and analysed by crushing in vacuo followed by melting, and yield a minimum olivin
36 ccurring carbonates of calcium and magnesium in vacuo has revealed that, surprisingly, anomalous isot
37 h silica gel, with the solvent being removed in vacuo, heated to 700 degrees C to remove the addends,
38 oth significantly larger than those obtained in vacuo, indicating that the difference arises from the
39 The S(1) band of the electronic spectrum in vacuo is broad, despite ion trap temperatures of 20 K
40 al activation (CA) of ions in the gas phase (in vacuo) is an important method for the study of protei
41 position at 700 degrees C of the Nd compound in vacuo led to the formation of a phase mixture of NdSe
42 ro techniques, it is instructive to consider in vacuo methodologies: for example native mass spectrom
44 We compared these experimental results with in vacuo molecular dynamics (MD) simulations of SAP, dur
45 behavior in-solution and is in line with the in vacuo observations; however, the theoretical collisio
46 cribe the controlled synthesis and isolation in vacuo of an array of charge-substituted phenylperoxyl
50 polarizable force field accurately reproduce in vacuo quantum mechanical results, experimental ion-cl
51 istillation and sublimation at 220 degrees C in vacuo, respectively, providing a promising sustainabl
52 nalog of a protonated Schiff base of retinal in vacuo reveal two excited states S1 and S2, the potent
54 rein, we provide a comprehensive overview of in vacuo tetrapyrrole metallation, addressing two-dimens
55 lvent, and evaporation of the dimethyl ether in vacuo, the alpha-methylstyrene is added and the solut
56 d from ab initio calculations on tri-glycine in vacuo to obtain an extended 3(1) helix-like structure
57 PMe3 may be thermally removed from 1-PMe3 in vacuo to produce (4)A2' (silox) 3Mo (1), which was de
59 dynamics (MD) to create in silico models of in vacuo unfolding of a well-studied protein, the N-term
60 an nuclear receptor PPARgamma were generated in vacuo using Tripos's SYBYL and used as the training s
61 ies of singly deprotonated biliverdin anions in vacuo, using a combination of cryogenic ion spectrosc
63 ll-trans amide conformer was the most stable in vacuo, while the cis-trans-cis-trans (ctct) or trans-
65 efinement calculations were carried out both in vacuo, without internally coordinated K+ cations, and
66 ht-handed helix based on molecular mechanics in vacuo yielded 46 conformations within 20 kcal/mol of
67 the 2:1 stoichiometry at 800 degrees C/72 h/in vacuo yields alpha-Zr(2)N(2)S with the expected layer