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1 or, whereas anomalous circular extinction is antisymmetric.
2  can be made to transition from symmetric to antisymmetric.
3 ns for the two geometries are expected to be antisymmetric about the experimental mirror plane and ex
4 cy of the 1,2-dipalmitoylphosphatidylcholine antisymmetric acyl chain CH2 stretching vibration decrea
5 s evaluated using the intensity ratio of the antisymmetric and symmetric nu(CH2) modes as well as the
6 s evaluated using the intensity ratio of the antisymmetric and symmetric nu(CH2) modes as well as the
7                                        CH(2) antisymmetric and symmetric stretching bands ( approxima
8 is assessed using the intensity ratio of the antisymmetric and symmetric v(CH2) modes as well as the
9                                        It is antisymmetric, as it predicts opposite DeltaDeltaG value
10 eterministic scheme to prepare symmetric and antisymmetric atomic states with the use of external dri
11 hows intramolecular vibrations, and also two antisymmetric broad bands, centered at +/-0.65 V, due to
12 aled that vibrational excitation of nu3 (the antisymmetric C-H stretch) activates methane dissociatio
13 e assigned to NCHgCN and NCHgHgCN from their antisymmetric C-N stretching mode absorptions at 2213.8
14  initial equilibration between symmetric and antisymmetric carbonyl vibrations.
15 ing by carboxylate side chains, reflected in antisymmetric carboxylate band shifts.
16 bitals and the need for wave functions to be antisymmetric causes computational-effort scaling propor
17 l encompassed a combination of symmetric and antisymmetric CD(2) and CD(3) stretching vibrations, dep
18 morph stability, indicating the dominance of antisymmetric CH methylene vibrations as the anhydrous m
19  the binding pocket normal modes have a more antisymmetric character, with the walls vibrating out of
20 d polariton modes, featuring a symmetric and antisymmetric charge distribution, the latter exhibits l
21 ate-like architecture that exhibits a unique antisymmetric chirality.
22 assigned, respectively, to the symmetric and antisymmetric CN stretches in the emitting triplet state
23 assigned, respectively, to the symmetric and antisymmetric CN stretching modes of the two coordinated
24 f the SB structure are the appearance of the antisymmetric CO stretch of the carboxylate group at 160
25                                          The antisymmetric CO stretch of tungsten hexacarbonyl was us
26       The 2D IR experiments conducted on the antisymmetric CO stretching mode measure spectral diffus
27                           Elucidation of the antisymmetric component is direct evidence that the Higg
28 h the Higgs mode contains both symmetric and antisymmetric components, which are excited via two dist
29 agnetic SrIr(0.8)Sn(0.2)O(3) that defies the antisymmetric constraint on the anomalous Hall effect im
30 the coexistence of significant symmetric and antisymmetric contributions plays a key role, pointing t
31 study generalized Lotka-Volterra models with antisymmetric correlations in the interactions inspired
32 e amount of coherence in the system, and the antisymmetric coupling changes the nature of the coheren
33 rder symmetric-to-symmetric and symmetric-to-antisymmetric couplings.
34 e with the symmetric strain operator and the antisymmetric curvature operator.
35 this work, is achieved by two equally strong antisymmetric dipoles.
36 ments, the formation of microstructures with antisymmetric domains and their geometrically tailored e
37  spin chain with both symmetric exchange and antisymmetric Dzyaloshinsky-Moriya couplings.
38 c columnar structures in the fluid, or their antisymmetric equivalents.
39 n to be governed by the competing effects of antisymmetric exchange (G = 36.0 +/- 0.8 cm(-1)) and sym
40 c antiferromagnetic exchange interaction and antisymmetric exchange acting within the two low-lying s
41  the {Fe2Mn} analogue, but can be modeled by antisymmetric exchange effects.
42                    The Dzyaloshinskii-Moriya antisymmetric exchange interaction (DMI) stabilises topo
43 yaloshinskii-Moriya Interaction (iDMI) is an antisymmetric exchange interaction that is induced by th
44 zyaloshinskii-Moriya interaction (DMI) is an antisymmetric exchange interaction that stabilizes spin
45 nteraction favors parallel alignment and the antisymmetric exchange interaction, namely the Dzyaloshi
46 led by first principle calculations, and the antisymmetric exchange interactions driven by the struct
47 etocrystalline anisotropy, Zeeman effect and antisymmetric exchange interactions.
48 tris(3-cumenyl-5-methylpyrazolyl)borate), an antisymmetric exchange term was required for the best fi
49                                              Antisymmetric exchange was less important for the other
50 te spin-orbit coupling of the (2)E state via antisymmetric exchange.
51 receptor proteins in the ASE neurons and the antisymmetric expression of olfactory receptor proteins
52 ng out the peculiar angular variation of the antisymmetric galvanomagnetic response with respect to t
53 822.8 cm-1 are assigned to symmetric H-Th-H, antisymmetric H-Th-H, and Th=O stretching vibrations of
54 yang coupling mechanism generates concerted, antisymmetric helix-helix packing changes within the ada
55                            Subsequently, two antisymmetric in vitro activity measurements were carrie
56 oshinskii-Moriya-Interaction (DMI), a chiral antisymmetric interaction that occurs in magnetic system
57                    However, p-wave and other antisymmetric interactions are weak in naturally occurri
58     This study underscores the importance of antisymmetric interactions, like DMI, in influencing the
59                                    After the antisymmetric linear magnetoresistance from conductive,
60 port chirality synchronous with a rare field-antisymmetric longitudinal resistance-a low-field tunabl
61 2)O(9), we discovered strongly nonlinear and antisymmetric magnetoelectric behavior above the spin-fl
62                             The phenomena of antisymmetric magnetoresistance and the planar Hall effe
63 rromagnetic domain walls, which both exhibit antisymmetric magnetoresistive behavior.
64 SE right (ASER), while it is expressed in an antisymmetric manner in the olfactory neuron pair AWC le
65 ed-ion qubits by creating both symmetric and antisymmetric maximally entangled states with fidelities
66 s at 959 and 927 cm(-1) to the symmetric and antisymmetric Mo O stretching modes, respectively, of an
67  occurs near 1520 cm(-1), and a less intense antisymmetric mode appears in the Raman spectra near 168
68                       We observe a symmetric-antisymmetric mode splitting giving rise to epsilon-near
69 tion of suppressed vortex excitations in the antisymmetric mode.
70 rform IR difference spectroscopy, assign the antisymmetric modes, and accurately describe bonding.
71  difference spectroscopy, but until now, the antisymmetric modes, which require IR difference spectro
72 bitals to the antibonding combination of the antisymmetric N and aromatic orbitals using TD-DFT calcu
73 econd mid-infrared (MIR) spectroscopy in the antisymmetric N(3)-stretching region.
74 y of 15.1 kcal/mol with one quantum of CH(4) antisymmetric (nu(3)) stretching vibrational excitation
75 lve, secreted by 2 mantle lobes, may present antisymmetric ornamental patterns of varying regularity
76                                     Exchange-antisymmetric pair wavefunctions in fermionic systems ca
77                        This is known as the "antisymmetric path problem" and leads to inverted amino
78 e MS/MS spectra, specifically addressing the antisymmetric path problem.
79  tags are selected from all maximum weighted antisymmetric paths in the graph and their reliabilities
80 es followed by energy minimization along the antisymmetric pathways led to enantiomeric pairs.
81 ed via a noise-correlation method, while the antisymmetric phase fluctuations are directly captured b
82 tion of the interlayer tunnelling by a layer-antisymmetric 'phason' mode of the moire system.
83  P-O and C-O torsions, whereas symmetric and antisymmetric phosphodioxy (PO2-) stretching modes are l
84                           Both symmetric and antisymmetric phosphoester stretching modes are highly s
85 gnetism arises owing to the excitation of an antisymmetric plasmon resonance.
86                                              Antisymmetric pressure between SM and ST supported the c
87 two dissimilar clusters in the 7/2- band and antisymmetric resonance in the 9/2- band.
88 ansmission minima occur at the symmetric and antisymmetric resonances of the coupled crosses.
89 symmetric (rotation-symmetry-preserving) and antisymmetric (rotation-symmetry-breaking) strain channe
90 nveiled in 2D NbSe(2) through multi-reversal antisymmetric second harmonic magnetoresistance isotherm
91 nsion) but leads to sliding of planes in the antisymmetric shear eigenmode of the elastic waveguide.
92                            Relaxation due to antisymmetric shielding tensor components is significant
93 odal-line semimetals, characterized by large antisymmetric spin-orbit couplings and by hourglass-like
94 magnetization, in some of them an additional antisymmetric spin-spin interaction arises owing to a st
95                                 We find that antisymmetric strain couples to the underlying order par
96 eflects a quadratic increase of entropy with antisymmetric strain, analogous to the role magnetic fie
97 as 10 times more reactive than ones with the antisymmetric stretch excited.
98  second-order chiral-optical response at the antisymmetric stretch frequency of parallel beta-sheet a
99 x sequential rovibrational lines of the nu 4 antisymmetric stretch fundamental of C7 are probed by ga
100 hift of approximately 4 cm(-1) (for the COO- antisymmetric stretch in Asp) from 1565 to 1569 cm(-1) i
101 e frequencies of its C=O stretch and -COO(-) antisymmetric stretch shift substantially should any rel
102 vibrational modes, such as the symmetric and antisymmetric stretches in CH3D or CH4, lead to very dif
103  in the frequency and amplitude of the azide antisymmetric stretching band.
104 ed near 1809 wave numbers and assigned to an antisymmetric stretching fundamental in the 1 sigma g+ g
105 e infrared (IR) frequency of the carboxylate antisymmetric stretching mode (v(a)OCO) is related to th
106 CX(-) were assigned to the symmetric and the antisymmetric stretching modes in ECX(*) radicals.
107                       This is assigned to an antisymmetric stretching vibration of the CO2- group bou
108                                              Antisymmetric tensor elements were found to be relativel
109 nt that the overall nuclear wave function be antisymmetric to exchange of identical protons (I = 1/2;
110 re assessed using the intensity ratio of the antisymmetric to symmetric v(CH2) modes as well as the f
111 is assessed using the intensity ratio of the antisymmetric to symmetric v(CH2) modes as well as the f
112  ratios and frequencies of the symmetric and antisymmetric transient infrared vibrations in the CN re
113  difference spectrum is therefore due to the antisymmetric vibration of both C=O groups of one electr
114  mode frequency calculations predict that an antisymmetric vibration of both C=O groups of the phyllo
115 equires the assignment of both symmetric and antisymmetric vibrational modes.
116 ransfer (CT) states induced by low-frequency antisymmetric vibrations and polar/polarizable solvents.
117              Biasing three-terminal JJs with antisymmetric voltages, for example, results in a direct
118 tations likely require interactions that are antisymmetric with respect to the direction of light pro

 
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