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1 eting complex vibrational spectra for larger polyatomic adsorbates.
2 dabco)(3)] where glycolate is a deprotonated polyatomic alcohol (ethylene glycol, EgO(2), 1; 1,2-prop
3 or a wide range of molecular ions, including polyatomics and species relevant for tests of fundamenta
4 cohol- and amine-functionalized amino acids, polyatomic anionic sulfur species, NO, and HNO.
5 dynamics of the two framework-forming units, polyatomic anions and pyrazines, govern both diffusion a
6 nteractions with the different anions, where polyatomic anions capable of infiltrating the film degra
7                       We describe the use of polyatomic anions for the quantitative assembly of ion-p
8 on acceptor aromatic compound, with mono- or polyatomic anions switches from the almost exclusive for
9                The complexation of bidentate polyatomic anions that are complementary in size and sha
10 or determining low concentrations of aqueous polyatomic anions using attenuated total reflectance (AT
11 ve combined new studies of the reactivity of polyatomic anions, acetate, trifuoroacetate, cyanide, an
12 sporters exchange H+ for halides and certain polyatomic anions, but exclude cations, F-, and larger p
13 iteria apply for electron transfer involving polyatomic anions.
14  to apply to more complex crystals formed of polyatomic building blocks, such as layered or framework
15                            In contrast, this polyatomic cation finds long-lived conformational states
16                                         As a polyatomic cation, guanidinium represents one of the few
17 ges and permeabilizes the plasma membrane to polyatomic cationic dyes.
18 h soft and reactive landing of mass-selected polyatomic cations and anions.
19 y (SERS) was used to detect and characterize polyatomic cations and molecules that were electrospraye
20 rences in the selectivity profiles for small polyatomic cations.
21 dividual isotopic mass distributions of each polyatomic chemical species.
22  introduced in semi-classical definitions of polyatomic configurations by their high-symmetry nuclear
23 low for the presence of functional groups in polyatomic crystal structures, and test the formula agai
24                         Our results point to polyatomic crystals as promising hosts for coherent qubi
25 ronegative elements in such compounds form a polyatomic electron-accepting molecule inside the solid,
26 esentative examples of mono-, di-, tri-, and polyatomic gases and to include some homologous series a
27       In this study, a completely new way of polyatomic interference removal in ICPMS for detection o
28 allows a significant decrease of the uranium polyatomic interferences ((235)UH(+) ions) and an accura
29                  High mass resolution allows polyatomic interferences at Fe masses to be resolved (es
30 rements at medium spectral resolution remove polyatomic interferences for some difficult elements lik
31 gSe nanocrystals has been investigated where polyatomic interferences from selenium clusters were ide
32 sed for all measurements in order to resolve polyatomic interferences on Si and P isotopes.
33 sed for all measurements in order to resolve polyatomic interferences on Si isotopes.
34 ffective chemical separation of isobaric and polyatomic interferences prior to sample introduction.
35    This inline method reduces matrix-derived polyatomic interferences that complicate traditional ICP
36 tion, while for the chromatographic analyses polyatomic interferences were minimized by the use of a
37                     For the former two cases polyatomic interferences were resolved by operating the
38 nalyte ions ((31)P, (32)S, and their on-mass polyatomic interferences).
39 ctral interferences, isobaric interferences, polyatomic interferences, and abundance sensitivity prob
40 trogen (N(2)) effectively overcomes Ar-based polyatomic interferences, enabling (ultra)trace element
41 he results of which were seriously biased by polyatomic interferences, especially from Sr and Cu, des
42 entration, low detection limits, and lack of polyatomic interferences.
43 s of analysis for masses with O- and N-based polyatomic interferences.
44 ing isotope ratios examined for isobaric and polyatomic interferences.
45 ifferences were observed between samples for polyatomic ion and amino acid concentrations.
46                          The introduction of polyatomic ion beams, particularly C60, for TOF-SIMS ana
47                          The introduction of polyatomic ion beams, such as C(60), has provided the as
48                                         This polyatomic ion has been tentatively identified as HSO3+
49 on process, forming an isotopically enriched polyatomic ion in a distance-dependent manner.
50                                            A polyatomic ion is observed on mass 81 in a synthetic sul
51 anic systems is demonstrated against another polyatomic ion source (e.g., SF(5)(+)).
52 (+) product ion, allowing for the removal of polyatomic ions ((16)O(1)H(+) and (16)O(1)H(2)(+)) gener
53                                              Polyatomic ions and neutrals larger than a triatomic pla
54 Ambient ion soft landing, a process in which polyatomic ions are deposited from air onto a surface at
55                                              Polyatomic ions are observed on masses 79 and 81 in a sy
56 we illustrate that the gas-phase mobility of polyatomic ions conforms to Blanc's law.
57                                        These polyatomic ions do not interfere with the detection of b
58                                        These polyatomic ions have been tentatively identified as PO3+
59                                          For polyatomic ions in particular, truly state-selective mea
60 ties to measure metabolites, drugs, or small polyatomic ions without the loss of structural isotopic
61  leaves, and chemical data were obtained for polyatomic ions, amino acids, sugars and organic acids.
62 the maximum in prior FAIMS or IMS studies of polyatomic ions.
63 er UV-absorbing groups in a variety of large polyatomic ions.
64 r the controlled deposition of mass selected polyatomic ions.
65 olecules has enabled significant advances in polyatomic laser cooling and trapping.
66                                          The polyatomic model of CF4(aq) studied gives a satisfactory
67 he retrieval of multiple bond lengths from a polyatomic molecule by simultaneously measuring the C-C
68 eter to mole ratios is complicated because a polyatomic molecule containing enriched atoms will resul
69 ements, the reaction dynamics of a prototype polyatomic molecule such as CH4 (and isotopologues) in i
70 we demonstrate magneto-optical trapping of a polyatomic molecule, calcium monohydroxide (CaOH).
71 ts properties within the context of a floppy polyatomic molecule.
72 molecular hydrogen, H(3)(+), is the simplest polyatomic molecule.
73    Optically addressable electronic spins in polyatomic molecules are a promising platform for quantu
74 rational Stark-associated phenomena of small polyatomic molecules are modelled using extensive spectr
75                                    Ultracold polyatomic molecules are promising candidates for experi
76  and associated radiation damage of atoms in polyatomic molecules can be inferred from the charge tha
77 nt studies suggest that the DIB carriers are polyatomic molecules containing carbon.
78        So far, all spectroscopy of gas phase polyatomic molecules has been restricted to large molecu
79 asibility of laser-cooling larger, nonlinear polyatomic molecules has remained unknown because of the
80            Compared with diatomic molecules, polyatomic molecules have distinct rotational and vibrat
81                                              Polyatomic molecules have long served as a platform for
82                                    Ultracold polyatomic molecules have potentially wide-ranging appli
83                                              Polyatomic molecules have rich structural features that
84 should be routinely considered when studying polyatomic molecules in intense laser fields.
85 the breaking and making of chemical bonds in polyatomic molecules is poised to open new pathways for
86                     Laser-driven dynamics in polyatomic molecules poses a complex many-body problem.
87 iate and observe such electronic dynamics in polyatomic molecules represents a crucial step forward i
88  necessary in order to assign spectra of hot polyatomic molecules such as water.
89  show that the femtosecond response of small polyatomic molecules that contain one heavy atom to ultr
90 ic generation and strong-field ionization in polyatomic molecules undergoing bonding or configuration
91 ronic and nuclear dynamics in both atoms and polyatomic molecules using multidimensional high harmoni
92 le a variety of experiments using individual polyatomic molecules with arbitrary spatial arrangement.
93 ge ultrafast structural changes in gas-phase polyatomic molecules with sub-Angstrom spatial and femto
94 ollision theory, then isotopologue masses of polyatomic molecules would be affected by isotopes of mu
95                       For example, ultracold polyatomic molecules would be uniquely suited to applica
96 ing energies have been measured for about 90 polyatomic molecules(1-6), an accurate ab initio theoret
97 spatio-temporal evolution of atoms, diatoms, polyatomic molecules, and nanoparticles in situ.
98 on of an optical tweezer array of individual polyatomic molecules, CaOH, with quantum control of thei
99    Here, we present a new approach to CEI of polyatomic molecules, detecting up to eight ionic fragme
100                                           In polyatomic molecules, however, the electronic states are
101 nar microcavities under strong coupling with polyatomic molecules, hybrid modes formed between all di
102 le (about 4 electron volts) are reported for polyatomic molecules, including (CH3)2CO (acetone), CH3C
103 nic, rotational, and vibrational energies of polyatomic molecules.
104 system, and is applicable even to un-aligned polyatomic molecules.
105 ablish a path for eEDM searches with trapped polyatomic molecules.
106 n measurement and quantum control of complex polyatomic molecules.
107 58 electrons, showing relevance to realistic polyatomic molecules.
108  reconstructing two-dimensional structure of polyatomic molecules.
109 ion barrier) in the mechanical activation of polyatomic molecules.
110 nts in the atomic manipulation of individual polyatomic molecules.
111 l coupled electronic and nuclear dynamics in polyatomic molecules.
112 f the structure of a vibrating excited-state polyatomic organic molecule has remained unworkable.
113 nce of tunneling to the surface diffusion of polyatomic organic molecules.
114 (+) should be thought of as covalently bound polyatomic precursors or fragments that can react and be
115 attributed to the sputter characteristics of polyatomic primary ion bombardment (SF5+) as compared to
116 dary ion mass spectrometry employing an SF5+ polyatomic primary ion source was utilized to obtain a s
117 pectrometry (cluster SIMS) employing an SF5+ polyatomic primary ion sputter source in conjunction wit
118                        This study shows that polyatomic primary ions can be used for the molecular de
119  depth and high sputter rates obtained using polyatomic primary ions have facilitated their use for t
120 generated by impacts of the kiloelectronvolt polyatomic primary ions on NaNO3 were markedly different
121 he depth profiling of polymer surfaces using polyatomic primary ions.
122  coincidence counting allowed the atomic and polyatomic projectile impacts on a particular sample sur
123 eaks produced by the kiloelectronvolt energy polyatomic projectile impacts on NaNO2 were NO2- and Na(
124 omer abundance can be increased by using the polyatomic projectile ReO4- (approximately 5 keV).
125 ear dynamics that make up a multidimensional polyatomic reaction coordinate.
126  of the dynamics of elementary (bimolecular) polyatomic reactions in the gas-phase have occurred.
127 mulations have advanced to such a level that polyatomic reactions with relevance to extreme astrochem
128 uding those reported in this work, for these polyatomic reactions.
129 he proximal distributions evaluated here for polyatomic solutes accurately reconstruct the observed d
130 by the endothermic chemical reactions of the polyatomic species inside the collapsing bubble.
131 ration of well-defined interfaces containing polyatomic species ranging from small ions to nanocrysta
132 g and magneto-optical trapping of many other polyatomic species(24-27) will be both feasible and prac
133 ule, so many other molecular ions, including polyatomic species, could be treated using the same meth
134 ing this step, particularly the spillover of polyatomic species, have rarely been studied.
135 ventually, optical tweezer arrays of complex polyatomic species.
136 so far precluded the realization of MOTs for polyatomic species.
137 ssibly due to the increase in protonation in polyatomic sputtering, and coronene was found to further
138                   Phenol represents an ideal polyatomic system for demonstrating photon catalysis bec
139 formation-specific stereodynamics of complex polyatomic systems and illustrates the capability of adv
140 ns, manipulation of structural properties of polyatomic systems targeting the JTE and PJTE, and appli
141 te dynamics to increasingly multidimensional polyatomic systems.
142 henomena related to structural properties of polyatomic systems.
143 nderstanding of mode-selective reactivity in polyatomic systems.
144 collisional relaxation is prevalent in other polyatomic systems.
145 ers, ammonia clusters, and mixed dimers with polyatomic units are reviewed for completion and compari

 
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