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1 ane-bound photosensitizer(9,14), abstract an electron pair.
2 e sufficient electrons to give every bond an electron pair.
3  to an in-plane hydrogen bond to an unshared electron pair.
4 porting artificial genetic systems lack this electron pair.
5 f 2'-deoxyadenosine lacking the minor groove electron pair.
6 h variations in the energy required to break electron pairs.
7  quantum-mechanical coherent fluid formed by electron pairs.
8 tive and absolute distribution of individual electron pairs.
9 nd acceptor materials in strongly bound hole-electron pairs.
10 terized by a spatially modulating density of electron pairs.
11 (c) ~ 5K) derived from spatial anisotropy of electron pairs.
12 of the copper oxides--is correlated with the electron pairing.
13 which is unrelated and perhaps competes with electron pairing.
14 er oxides, and a candidate for mediating the electron pairing.
15 eractions (X = an element having an unshared electron pair), allowing the determination of the intera
16 at substituent effects, rather than skeletal electron pairs alone, determine ground-state architectur
17 ate bonding geometry is inconsistent with an electron pair along the Fe-O bond as the Fe-O-C angle is
18 ed out by local pair natural orbital coupled-electron pair and coupled-cluster methods.
19  H2 exhibits a strongly bonded, almost inert electron pair and requires transition metals for activat
20 r's sextets in the open-shell form overcomes electron pairing and leads to the emergence of a high de
21 and thus suggest that it plays a role in the electron pairing and superconductivity.
22 der parameter that represents the binding of electron pairs and magnons.
23 en atoms, ease of alignment of the nonbonded electron pairs, and the overall size of the ligand as ga
24 ours mechanisms in which the superconducting electron pairs are pre-formed in the normal state of und
25 enerally be predicted based on the number of electron pairs around it using valence shell electron pa
26 ubbard interaction that describes real-space electron pairing as a precursor to superconductivity.
27 ined by assuming the association of the lone electron pair at sulfur to the Co-alkyne complexes.
28 results rekindle the long-standing idea that electron pairing at interfaces between two different mat
29 y reticula and that the energy released from electron pairs being passed along the electron transport
30 nvolves a twofold bonding interaction of two electron pairs between cerium and carbon.
31  simple formation of a sigma-complex through electron-paired bonding within the triplet manifold.
32 ally formed through the cleavage of covalent electron-pair bonds, play an important role in diverse f
33  that the periodicity (0)/2 is not driven by electron pairing but is the result of capacitive couplin
34 tion is limited by the low internal positron-electron pair conversion rate, the increased effective s
35 ve (CDW), this DW state could actually be an electron-pair density wave (PDW).
36 5) superconductive order parameter Delta(r), electron-pair density(16-19) and pairing energy gap(17,2
37                                  This Single Electron Pair Distribution Analysis (SEPDA) reveals quan
38      Unconventional superconductivity, where electron pairing does not involve electron-phonon intera
39 es of related heteroaryl groups with similar electron pair donor properties have also been found to f
40 least a single hydrogen bond acceptor group (electron pair donor).
41 )NH(3) serves as a good example to study the electron pair donor-acceptor complexes.
42 ence of the hydrogen-bonding acceptor or the electron-pair donor capacity of the solvent on the posit
43                            In the absence of electron-pair donor ligands, 4 aggregates (>dimer) in hy
44 of alpha-arylvinyllithiums by 0, 1, 2, and 3 electron-pair donor ligands.
45 t of substrates that neither ionize nor have electron pair donors and that are much simpler in struct
46 ts show that all BLs prefer scaffolds having electron pair donors: KPC-2 is preferentially inhibited
47 lassical picture of chemical bonds as shared-electron pairs evolved to the quantum-mechanical valence
48  group, M-M bonding consists of three shared electron pairs, except for M = Pb.
49                One explanation could be that electron pair formation and related electron-boson inter
50  bifurcating transhydrogenase that takes two electron pairs from NADPH to reduce two ferredoxins and
51 perconductivity, however, no boson mediating electron pairing has been identified.
52 -vertex heteroboranes containing 14-skeletal electron pairs, have been synthesized by the direct elec
53 f B atoms deviates from Wade's rule by three electron pairs (if treated as a distorted arachno system
54                             The mechanism of electron pairing in high-temperature superconductors is
55 he elusive pairing "glue" that gives rise to electron pairing in SrTiO(3)-based systems.
56 rect experimental insight into the nature of electron pairing in SrTiO3 has remained elusive.
57 of magnitude as that of the spin exchange of electron pairing in the high-temperature superconducting
58                                              Electron pairing in the vast majority of superconductors
59 also induce spin-triplet pairing(24) or that electron pairing in UTe(2) has a spin-singlet component.
60 tational studies support the sharing of five electron pairs in five bonding molecular orbitals betwee
61 e transfer and the charge separation of hole-electron pairs in isolated polymers versus the device fi
62  unusual gap symmetry which implies that the electron pairing interaction is repulsive at short range
63 hrieffer (BCS) explains the stabilization of electron pairs into a spin-singlet, even frequency, stat
64 ked by low-lying transition states where the electron pair is delocalized over two adjacent centers.
65 ds no information regarding how any specific electron pair is distributed.
66 ts for Ca(H(2)O)(n2)(+) indicate that an ion-electron pair is formed when clusters with more than app
67 ial aromaticity provided their nitrogen lone electron pair is sufficiently available to participate i
68                                  Remarkably, electron pairing is found upon infinitesimal doping, giv
69                                              Electron pairing is stable at temperatures as high as 90
70                                 Formation of electron pairs is essential to superconductivity.
71  the quantum condensation of superconducting electron pairs is understood as a Fermi surface instabil
72             This phase is an electride, with electron pairs localized in interstices, forming eight-c
73 vertheless, the poisonous nature of its free electron pairs makes sulfur containing substrates inacce
74 all regime have been attributed to an exotic electron pairing mechanism.
75         The main theme of this review is the electron-pairing mechanism responsible for their superco
76 onductors, providing deeper insight into the electron pairing mechanisms of superconductivity.
77   All three classes of compounds have a free electron pair near Arg364, a residue that if mutated con
78  stereochemical expression (SE) of the ns(2) electron pair (NSEP) on group IV metal cations.
79 s crucial as this is the background in which electron pairing occurs.
80 of the conventional type, involving the lone electron pair of an oxygen donor, the latter is perpendi
81 occupied by a sterically active free valence electron pair of chlorine.
82  of the silylidyne radical to the nonbonding electron pair of nitrogen forming an HSiNH(3) collision
83                     We propose that the lone electron pair of Pb(II) precludes Pb(II) to function in
84 nd OP identification confirmed that the lone electron pair of the amine-N is the predominant site of
85 e closed outer-most [Formula: see text] lone electron pair of the lanthanide atom intact in sharp con
86 ng the short axis and bonds through the lone electron pair of the nitrogen atom instead, and both qui
87 d by an n -> pai* interaction between a lone electron pair of the oxygen atom of the spiroketal ring
88 erconductors, but their possible role in the electron pairing of superconductivity remains an open qu
89                                     The lone electron pairs of -NH and -CO units of MBAA are designed
90 mpty p orbital of the carbene and nonbonding electron pairs of heteroatoms of the solvent.
91 erent types of hyperconjugation between lone electron pairs of nitrogen atoms and sigma*C-N orbitals
92 d that the alkylation of 2 involves the lone electron pairs of the N-N-O atoms, and the calculated ac
93 ater-interface interaction is weaker and the electron pairs of water can solvate S(+) ions.
94 resence of a sterically active, free valence electron pair on Xe.
95  reactant through weak interactions with the electron pairs on alcohol O, while water and parent alco
96  aromatic ring that allows delocalisation of electron pairs on the oxygen atom.
97 ing constants confirm that the inward-facing electron pairs on the pyridyls destabilize the 1:1 compl
98 d here highlights the influence of preformed electron pairs on the transport properties of LAO/STO an
99 sition metals can form bonds with six shared electron pairs, only quadruply bonded compounds can be i
100 ts on these chiral nanowires reveal enhanced electron pairing persisting to high magnetic fields (up
101 riginating from the annihilation of positron-electron pairs produced by high-energy X-rays travelling
102 most claimed mechanisms, including preformed electron pairing, quantum criticality or density-wave fo
103 Concepts from the very general Valence Shell Electron Pair Repulsion (VSEPR) model to the most esoter
104 electron pairs around it using valence shell electron pair repulsion (VSEPR) theory.
105 d(10) species is stabilized by valence shell electron pair repulsion (VSEPR).
106 glet states is attributed to the decrease in electron pair repulsion resulting from increased delocal
107 Using computational analysis, we reveal that electron pair repulsion within the deprotonated anion is
108 l, thereby restoring the availability of the electron pair (reservoir emptying).
109 tice vibrations) drives the formation of the electron pairs responsible for conventional superconduct
110                                     The lone electron pair revealed on Na and the negative Laplacian
111 manium and tin, as well as greater nonbonded electron pair stabilization for tin, are more important
112      Specifically, orbital ordering and lone electron pair stereochemical activity compete, giving ri
113                  This enabled control of the electron pairing symmetry by tuning the degree of magnet
114 empty bridge in the catalytic cycle, and the electron pair that constitutes this bond thus plays a cr
115         In conventional superconductors, the electron pairing that allows superconductivity is caused
116 addle-wheels, rotational motion of localized electron pairs that couples to and facilitates ion diffu
117 d in terms of underlying polyhedral skeletal electron pair theory (PSEPT) concepts.
118  when oxidized to oxaloacetate, transfers an electron pair to reduce NAD to NADH.
119 ently, these organic species transfer proton-electron pairs to O(2)-derived surface species via pathw
120 er of molecules of MgATP hydrolyzed for each electron pair transferred to substrate, from ca. 5 (the
121 nic nematicity that again coincides with the electron pairing transition, unveiling a rotational symm
122 ar, a fundamentally different picture of the electron pairs, which are believed to be formed locally
123 ion between itinerant electrons that creates electron pairs, which condense into a macroscopic quantu
124 tronic ordering mechanism that can influence electron pairing with broken time reversal symmetry.
125 n-triplet superconductors are condensates of electron pairs with spin 1 and an odd-parity wavefunctio
126 ted in single-layer graphene (SLG), with the electrons pairing with a p-wave or chiral d-wave symmetr
127 including low-density superconductivity, and electron pairing without superconductivity for which the
128  Here we report a direct correlation between electron pairing without superconductivity, anomalous Ha
129 stence of a robust electronic phase in which electrons pair without forming a superconducting state.

 
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