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1   This distortion of electron density off an interatomic axis is often described as a 'banana-bond.'
2 island growth mode because of the high Rh-Rh interatomic binding energy.
3 the unit cell volume, as well as in specific interatomic bond lengths and bond angles.
4 (6) polyhedra are highly distorted, with the interatomic bond lengths ranging from 1.690 to 1.847 A a
5 rain boundary, the large Bi atoms weaken the interatomic bonding by pushing apart the Cu atoms at the
6                                              Interatomic bonding is stronger in Cr2AlC than Zr2AlC bu
7  for characterizing the atomic structure and interatomic bonding of molecules associated with extraor
8 s are retained on large deformation but weak interatomic bonds lead to compromised strength.
9                     Surface atoms have fewer interatomic bonds than those in the bulk that they often
10 ield sensitivity of the anharmonicity of the interatomic bonds that govern the probability of phonon-
11 nitrogen exhibits one of the strongest known interatomic bonds, while xenon possesses a closed-shell
12  energy based on accessible surface area and interatomic contact areas.
13 positions 10 and 97, which corresponds to 13 interatomic contacts.
14                      A well-known example is interatomic Coulombic decay, where an excited atom relax
15 ), large static disorder and dynamical bond (interatomic) disorder that is poorly modeled within the
16 on, coupled with a >30 A decrease in maximum interatomic distance (D(max)) by small angle x-ray scatt
17 rience a progressive increase in the average interatomic distance and gradually settle to form dome-s
18                This is because the increased interatomic distance at dislocation cores raises the mig
19 orobenzo[g]chrysene, where the short 2.055 A interatomic distance between bay-region F-9 and H-8, dow
20 R methods, specifically in sorting ambiguous interatomic distance constraints into classes that defin
21                                          The interatomic distance constraints were all consistent wit
22 the crystal structure of ADP-kinesin, and by interatomic distance constraints.
23 e fundamental to further analysis, including interatomic distance distribution calculation and low-re
24  lysine-lysine (K-K) cross-linkers to obtain interatomic distance information.
25 y different from uncondensed atoms, with the interatomic distance larger than the average by about 10
26 spectroscopy could be broadly applicable for interatomic distance measurements in other spin-7/2-spin
27                   Experimental data, such as interatomic distance measurements, are then used to sele
28 red amorphous Se(0) with a first shell Se-Se interatomic distance of 2.339 +/- 0.003 A.
29 sters embedded in helium droplets reveals an interatomic distance of 3.65 A, much closer to the value
30 ies was improved by the use of time-averaged interatomic distance restraints derived from (1)H NMR.
31 served on the globally derived Dmax (maximal interatomic distance), although under comparable conditi
32 es and functions were supported by sequence, interatomic distance, and B-factor information on intera
33     The extent of interaction is measured by interatomic distance, NBO second-order perturbative anal
34  binding of the two metals at an ultra-short interatomic distance.
35 etected on the radius of gyration or maximum interatomic distance.
36  irregular oscillations as a function of the interatomic distance.
37 tself as a stationary state at a preordained interatomic distance.
38 hat on average scales exponentially with the interatomic distance.
39 ngs (13.8 +/- 1.4 Hz for surface silica) and interatomic distances (3.04 +/- 0.08 A for surface silic
40                                      Deduced interatomic distances agreed closely with previous radia
41   The evolution of bond angle distributions, interatomic distances and coordination numbers are exami
42 rimental noise, FoXS explicitly computes all interatomic distances and implicitly models the first hy
43  of 2.3041(12) and 2.1949(28) A for the As-P interatomic distances and the P-P interatomic distances,
44 but technically challenging due to the small interatomic distances and the similar atomic numbers.
45                                 Although the interatomic distances are suggestive of agostic-type int
46 )/H(N), H(N)/H(alpha), and H(alpha)/H(alpha) interatomic distances as well as (1)H NMR chemical shift
47  following: (i) very close agreement between interatomic distances at the metal coordination site for
48 esonance spectroscopy, from which long-range interatomic distances can be estimated.
49                                          The interatomic distances constrain the Trp41 side-chain con
50                                    The Ge-Se interatomic distances extracted from XAS data show a two
51 cture reconstruction from precise unassigned interatomic distances for a range of clusters.
52  methodology for the measurement of specific interatomic distances from a combination of theoretical
53 nstrating the use of (17)O NMR to quantitate interatomic distances in a fully labeled dipeptide.
54  (FRET) provides a unique means of measuring interatomic distances in biological molecules in real ti
55 ls and already display significantly shorter interatomic distances in comparison to van der Waals (vd
56 ray absorption edge, can be used to identify interatomic distances in materials.
57 to the structure, light-triggered changes in interatomic distances in the azobenzene moiety are able
58 ies at intermediate angles, corresponding to interatomic distances in the range of 5-20 A, are partic
59                              Analysis of the interatomic distances in the superconducting substance K
60 riments reveal a strong sensitivity of Tc to interatomic distances in the underdoped regime (x </= 0.
61 king of intermetallics: correlations between interatomic distances lead to the inability of a phase t
62 aphy; (ii) similarly close agreement between interatomic distances measured by EXAFS for the Pb(2+)-G
63 eptides showed significant deviations in the interatomic distances of critical electrophile-binding a
64 t, relatively large cutoffs for matching the interatomic distances of the stem residues have to be us
65 ructures with intralayer halogen bonds, with interatomic distances shorter than the sum of the van de
66 cluded were partial atomic charges and three interatomic distances that define the relative spatial d
67 ifts ((13)C and (15)N NMR) and corresponding interatomic distances which are combined into a 3D abstr
68 rt direct determination of how variations in interatomic distances within individual crystalline unit
69 differences were noted in the kringle/ligand interatomic distances within the monomeric components of
70 ion on the distribution of electron density, interatomic distances, and the orientation dependence of
71  the recolliding electron is on the order of interatomic distances, i.e., approximately 1.5 A, small
72 otoluene in DNA/RNA have indicated, based on interatomic distances, possible hydrogen bonding interac
73  an updated value of 2.1994(3) A for the P-P interatomic distances, reconciling conflicting literatur
74 r the As-P interatomic distances and the P-P interatomic distances, respectively.
75 an analysis of the lattice periodicities and interatomic distances, we rationalize why the Ba phases
76 d angles, dihedral angles, bond lengths, and interatomic distances.
77 lecular electron transfer process over large interatomic distances.
78 be weaker than deduced from the non-hydrogen interatomic distances.
79 ion at other contacts, resulting in nonideal interatomic distances.
80 l shifts in terms of polynomial functions of interatomic distances.
81 uding chemical shifts, torsional angles, and interatomic distances.
82 Upon folding, proteins develop a peak in the interatomic force distributions that falls on a universa
83 etical predictions, enabling us to probe the interatomic force parameters that are crucial to the pro
84 rdering of the lattice can occur because the interatomic forces are modified due to the excitation of
85            At high excitation densities, the interatomic forces that bind solids and determine many o
86 protein based on classical approximations of interatomic forces, giving researchers insight into prot
87 e by the number of atoms within the range of interatomic forces, is difficult to visualize directly b
88  with parametrized equations to describe the interatomic forces.
89 onding, which translates into changes in the interatomic forces.
90 g and statistical mechanics to determine the interatomic interaction energies of a molecular system e
91 ent metastable state of Ge2Sb2Te5 with muted interatomic interaction induced by a weakening of resona
92    These materials are characterized by weak interatomic interactions (van der Waals forces) between
93                        The considerations of interatomic interactions alone cannot explain the fractu
94  of non-crystalline materials using accurate interatomic interactions and experimental information.
95 ion is shown to be superfluous when suitable interatomic interactions are present.
96 nd physical systems as a result of competing interatomic interactions can be used as templates for fa
97 more itinerant electrons to soften repulsive interatomic interactions in a tight space.
98 and (2) that potential sets used to describe interatomic interactions may be sufficiently accurate to
99 ling a significant influence of strong S...S interatomic interactions on the intramolecular distance
100  other proteins, and DNA, depend on specific interatomic interactions that can be classified on the b
101 e critical tests of our understanding of the interatomic interactions that underlie molecular biology
102 ode and structural compensations for altered interatomic interactions, in which lost TCR-peptide inte
103 m size and shape is strongly affected by the interatomic interactions.
104 us overcoming usual requirement for a strong interatomic interactions.
105  temperatures, arising from the hierarchy of interatomic interactions.
106 ng, as is information on the nature of their interatomic interactions.
107 e ratio of the interplanar spacing c and the interatomic, intraplanar spacing a of the h.c.p. lattice
108          Here, we argue that actually simple interatomic magnetic exchange interaction already contai
109 theoretical calculations are reported for an interatomic multi-atom resonant photoemission (MARPE) ef
110 sis, the target genes were mapped in complex interatomic networks representing molecular pathways, ce
111 landscape, can be related to the form of the interatomic or intermolecular potential.
112  of the metal-metal (M-M) bond distances and interatomic order-of Pt nanoclusters supported on a gamm
113 llowing quantitative characterization of the interatomic potential energy surface of the highly excit
114                       The motion of atoms on interatomic potential energy surfaces is fundamental to
115 led mapping of the carrier density-dependent interatomic potential of bismuth approaching a solid-sol
116 ts the strength of the repulsive part of the interatomic potential, which can be determined from the
117 ideration of the finite-strain energy or the interatomic potential.
118   We believe that, by improving (i) existing interatomic potentials and (ii) currently available enha
119 lculations serve to test the validity of two interatomic potentials and to extend the scope of the DF
120 ines a new genetic algorithm using empirical interatomic potentials to explore the configurational ph
121       Using atomistic simulations with model interatomic potentials, we reveal a transition in the as
122 o far been based on the use of semiempirical interatomic potentials.
123 r within a free (noncoordinated) ligand: the interatomic separation between the N-donor metal-binding
124  and iodine fragments as a function of their interatomic separation set by the NIR-x-ray delay.
125  spatial wavelengths of the order of several interatomic spacings, rather than the macroscopic scales
126 fingers in two separate in vitro assays, and interatomic surface molecular modeling docked the compou
127 -) and the pyrimidine dimer by the method of interatomic tunneling currents.
128 DNA photolyase molecule, using the method of interatomic tunneling currents.

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