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1 confirming the presence of a strong aromatic ring current.
2 stness of the classical benzene diatropic pi ring current.
3 e cyclobutadieno clamps disrupts the benzene ring current.
4 shifts with the magnitude of the engineered ring current.
5 igate the long-term variations of the global ring current.
6 ion with a significantly increased diatropic ring current.
7 rating a near-circular current, known as the ring current.
8 accounting for orbital contributions to the ring current.
9 a strong, albeit slightly reduced, diatropic ring current.
10 the presence of a more substantial diatropic ring current.
11 eld, and this also showed a strong diatropic ring current.
12 eared to possess a slightly larger diatropic ring current.
13 rotropiporphyrin that also showed a stronger ring current.
14 hey nevertheless retain powerful macrocyclic ring currents.
15 gnetism, which is aromaticity, via superatom ring currents.
16 nanorings provide strong evidence for global ring currents.
17 ssess significant 14pai electron diamagnetic ring currents.
18 late, confirming that they arise from global ring currents.
19 ese exhibited significantly reduced aromatic ring currents.
20 d oxidized form display residual macrocyclic ring currents.
21 eroxide oxidation ensued yielded bell-shaped ring currents.
22 r magnetic behaviour associated with induced ring currents.
23 showed the presence of enhanced diamagnetic ring currents.
24 ects can be characterized by the reversal of ring currents.
26 turn, the magnetic field generated by these ring currents affects the chemical shift of carbons on t
30 t al. and Huckel-London-Pople-McWeeny (HLPM) ring currents and bond currents that are presented here.
31 uce the experimental trends of the diatropic ring currents and filled in the data for the regioisomer
32 ipsocentric calculation to support diatropic ring currents and hence to be aromatic on the basis of m
33 hese derivatives retained strong diamagnetic ring currents and the presence of the internal alkyl sub
34 readily rationalized by analysis of aromatic ring-currents and provide sensitive probes for sites of
35 ted that the system has a strong diamagnetic ring current, and the external meso-protons showed up do
36 onfirms the presence of a strong diamagnetic ring current, and the meso-protons show up at 10 ppm, wh
37 ntracted porphyrinoids also exhibit aromatic ring currents, and the internal CH resonances shifted up
38 tionic species with slightly larger aromatic ring currents, and under strongly acidic conditions, C-p
42 currents of its components.The discovery of ring currents around a molecule with a circumference of
45 amework S(2)N(4)(CH)(2) supports a diatropic ring current, as does its analogue in which N and CH gro
46 most of the porphyrinic macrocycle aromatic ring current, as seen in their (1)H NMR spectra and mode
50 Our analysis also offers a preview of the ring current at other giant planets, such as Jupiter, wh
53 sent the observational evidence of Mercury's ring current by analysing particle measurements from MEr
54 ent drift that leads to the formation of the ring current by ions in the several tens of kiloelectron
55 logues showed no indication of a diamagnetic ring current by proton NMR spectroscopy, but addition of
56 the sensitivity of (19)F chemical shifts to ring currents by designing labels with direct contact to
57 These systems also showed large diatropic ring currents by proton NMR spectroscopy that were compa
58 gues of the porphyrins show strong diatropic ring currents by proton NMR spectroscopy where the inter
64 ndicates the presence of a strong paratropic ring current, characteristic of an antiaromatic compound
65 ne-fused annulenes shows further evidence of ring current competition as these allow for observation
68 resonances which can be accounted for by the ring current contributions of the deoxyguanosinyl and py
69 analytical expressions are used to calculate ring current contributions to the CSA (Deltasigma) of 1H
72 an interpretation supported by the diatropic ring current determined by NICS(ZZ)(r) computations, whi
74 Carbasapphyrins retain a strong diatropic ring current due to the presence of 22pi electron deloca
75 ace for many decades, the enhancement of the ring current during geomagnetic storms is still not well
76 r-containing ligands due to the porphyrin pi-ring current effect, which is also present in the di- an
78 agreement with a commonly used model of the ring-current effect as well as the overall interaction g
79 rturbation of POPC protons from the aromatic ring-current effect, as well as 1H NMR cross-relaxation
80 ndependent chemical shifts that quantify the ring current effects caused by neighboring molecules.
83 iffers by 1.26 ppm, indicative of pronounced ring current effects on the surface of this endohedral f
86 to lead to structures that support diatropic ring currents: explicit ab initio calculation of magneti
87 A/MCAD complex is proposed to arise from the ring current field from the isoalloxazine portion of the
90 , neutral aromatic molecule with a diatropic ring current following the sigma-bond path formed by Si
93 on theory reveals a significant paramagnetic ring current in 1, a feature that helps explain the (1)H
96 the ring (a 'diatropic' current), while the ring current in an antiaromatic molecule flows in the re
98 exhibited the presence of a strong diatropic ring current in benzo-benzisapphyrins, and the macrocycl
99 rum showed that it has a reduced diamagnetic ring current in comparison to other carbaporphyrins.
100 contributions arising from an aromatic-like ring current in cyclopropane, involving six electrons in
101 s reveal the presence of a global paratropic ring current in its 4+ and 8+ oxidation states and of a
102 d that the peak location of the suprathermal ring current in local time oscillates between post-midni
103 is still a lack of observational evidence of ring current in Mercury's magnetosphere, which has a sig
104 for conventional pi-ring currents, the sigma-ring current in tangential p-p bonded systems is dominat
107 s were used to probe the distribution of the ring current in the 4+, 6+, and 8+ oxidation states by (
108 + oxidation states and of a global diatropic ring current in the 6+ state of the partially fused ring
109 quires much more energy and has a paratropic ring current in the TS pointing to antiaromatic, cyclope
110 ne), both of which exhibit a weak paratropic ring current in their 1H NMR spectra and are oxygen sens
111 he introduction contains the fundamentals of ring currents in aromatic and antiaromatic systems, foll
114 ings provides a motivation for investigating ring currents in molecules of an intermediate size.
117 cating weak global aromatic and antiaromatic ring currents in the 10+ and 12+ oxidation states, which
119 does not compromise their ability to exhibit ring currents in the presence of an external magnetic fi
121 trongly elucidating sustained weak diatropic ring currents in twisted macrocycles both in neutral for
122 shifts in cyclopentadienes have a diatropic ring current indicating aromatic, cyclopentadienide anio
124 culations of the effect of the cyt b(5) heme ring current-induced magnetic dipole on cyt c were used
125 ence of CH...pi interaction is provided from ring current-induced upfield displacement of Pro(1) C(al
126 emical shifts for paramagnetic and porphyrin ring current influences in the paramagnetic substrate co
128 cate that the modulation of the suprathermal ring current is closely related to the solar cycle.
134 matic, with enhanced stability and diatropic ring currents (magnetic shielding inside the ring), wher
135 n gradually decreases the magnitude of their ring currents, making them less aromatic and less antiar
140 hanges lead to modulation of the strength of ring currents near the site of addition and, in turn, th
147 ng its oxidation state to suppress the local ring currents of its components.The discovery of ring cu
148 he design of confined ultrafast switching of ring currents of nonplanar molecules and further current
149 While in NMR spectroscopy the effects of ring currents on the chemical shifts of nearby protons a
154 t a nearly 11-year cycle of the suprathermal ring current populations in Saturn's magnetosphere.
155 pect to the fundamental orbital symmetry and ring-current rules, Si bonds at greater internuclear dis
157 the monomer 1,N(2)-epsilondG, attributed to ring current shielding, consistent with their intrahelic
158 e linear correlations that exist between the ring-current shielding shifts for the axial ligand C(1)
159 , as indicated by NOEs and the large upfield ring current shift (approximately 4 ppm) of A37 HN.
161 f the NH pairs, such as hydrogen bonding and ring current shifts, and are observed for residues in th
162 lly unfavorable in solution, with a peculiar ring current stabilizing the aromatic character of the n
163 e-containing 4 showed the weakest paratropic ring-current strength for the s-indacene unit, while 1-3
167 uantities with easily computed Huckel-London ring currents suggests a simply calculated measure for d
170 the dianion of 4 reveal a distinct diatropic ring current that should aid in its characterization.
171 lectric current around a planet known as the ring current, that has been observed in the intrinsic ma
172 9(+) (1), which supports a pinched diatropic ring current, the C(2v) transition state (2) for inversi
173 ontrol the enhancement and decay rate of the ring current, the main cause of the geomagnetic field pe
176 a reasonable estimate of the contribution of ring currents to the full shielding tensor a series of d
177 ion is developed so that the contribution of ring currents to the full shielding tensor can be calcul
178 nd Bovey only quantifies the contribution of ring currents to the isotropic component of the shieldin
179 ed, allowing an estimate of the influence of ring currents upon the chemical shielding anisotropy (CS
180 changes associated with the styrene aromatic ring current were noted for S-SOA6 H2 and H1', T16 N3H,
182 lder adduct 17 showed an increased diatropic ring current where the internal proton shifted beyond -9
183 affords dications with enhanced diamagnetic ring currents where the internal CH shifts to ca. -3 ppm
185 r 110 pai-electrons, display global aromatic ring currents, whereas even-numbered belts, with 80, 100
186 fect on an aromatic molecule is the aromatic ring current, which can be thought of as an induction of
188 ctric current around the planet known as the ring current, which regulates the field configuration of
190 for these compounds showed strong diatropic ring currents with the internal CH resonance upfield abo
191 tral naphthalene ring, showed more localized ring currents, with stronger paratropic ring currents on