戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (１語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1 uclear quadrupole interactions from a single deuteron.
2 r hydroxylation at a carbon atom bearing the deuteron.
3 lowed by replacing exchangeable protons with deuterons.
4 ster is accessible for exchange with solvent deuterons.
5  diagnostics for determining the features of deuteron acceleration as well as monitoring neutron prod
6 deuterium mud is the exotic atom formed by a deuteron and a negative muon mu(-).
7  a distance of 2.5-2.6 A between the closest deuteron and manganese.
8 1-A distance between an acetate methyl group deuteron and the phenoxy oxygen of YZ*.
9  we compared the effects of densely-ionizing deuterons and sparsely-ionizing X-rays on two microscopi
10  is observed between the QCC values of alpha-deuterons and the inverse cube of C(alpha)-H(alpha)...O=
11 ling tensors of the hydrogen-bonded protons (deuterons) and their principal directions with respect t
12                                        These deuterons are rigid on the (2)H MAS NMR time scale (i.e.
13 r this process decreases to 7.6 s(-)(1) when deuterons are substituted for protons in the aromatic ri
14 s from many of the alanine backbone C(alpha) deuterons as well as the alanine side-chain C(beta) meth
15 s a 6th (distal) ligand; (2) to exchangeable deuterons assigned to Arg127 which may H-bond with the p
16 12)-ene (15-d(1)), which could incorporate a deuteron at the C-12 position on the pathway to doubly l
17 d(3)-thy, with three magnetically equivalent deuterons at its methyl group (-CD(3)), showing a single
18 erence in the number of protons exchanged to deuterons at specified solution conditions.
19 erence in the number of protons exchanged to deuterons (based on protein folding under pressure) coul
20 crystal is used to generate and accelerate a deuteron beam (> 100 keV and >4 nA), which, upon strikin
21 age peak of [Formula: see text] kV, produces deuteron beam first, then the re-strikes, which do not a
22 " ring of naphthalene, with the closest ring deuteron being located at a distance of approximately 4.
23 ained using CD-Bonn potential reproduces the deuteron binding energy and neutron-proton elastic scatt
24 om decay of (9)Li, formed by the high-energy deuteron bombardment of the beryllium converter.
25 evolving complex of photosystem II displaces deuterons bound very closely to the Mn cluster.
26     The mass spectrum of the m/z 166 ion for deuteron-charged methyl dihydrocinnamate showed two peak
27 ntal quadrupolar coupling constants of alpha deuterons (D(alpha) QCC) are reported for the residues o
28 ver 3 MeV X-rays and [Formula: see text] keV deuterons, demonstrating unique combined neutron-gamma e
29 measurements are consistent with substantial deuteron density in the octahedral, interstitial voids o
30 ronment was explicitly shown by exchangeable deuteron ENDOR that implied hydrogen bonding to the quin
31 alpies and entropies are reported for proton-deuteron exchange at 42 amide sites in T4 lysozyme and c
32 atography/mass spectrometry to follow proton-deuteron exchange between D(6)-acetone and water.
33              As shown by the rates of proton-deuteron exchange in ethylenes with halogen substituents
34 lmost entirely by D(2)O rather than hydrogen-deuteron exchange on the protein.
35         Acetone carboxylase-catalyzed proton-deuteron exchange was dependent upon the presence of ATP
36 M experiments investigating the proximity of deuterons exchanged into the vicinity of YZ. after incub
37 trains, but not in non-melanized ones, after deuteron exposure.
38 orded protection against high-dose (1.5 kGy) deuterons for both CN and CA (p-values < 10(-4) ).
39 on at the C(alpha)-position, incorporating a deuteron from a D(2)O solvent.
40 methyl groups, whereas signals from C(alpha) deuterons generally have not been observed for similar p
41 etry (MS) was used to determine amide proton/deuteron (H/D) exchange rates.
42                          Exchangeable proton/deuteron hyperfine couplings, consistent with terminal w
43 (I = 1/2; Fermions), symmetric for identical deuterons (I = 1; Bosons).
44 ergence of the highest energy portion of the deuterons (i.e., above 10 MeV/nucleon) from the laser ax
45                                        These deuterons impinge on a beryllium converter to generate n
46 ation of the magnetic moment and spin of the Deuteron in its ground state thanks to the isotopic comp
47 etic moment, spin and hidden variable of the Deuteron in its ground state.
48 een as a function of intercalation level for deuterons in both 1 x 1 and 1 x 2 tunnels are consistent
49  Amide protons were allowed to exchange with deuterons in buffered D2O at room temperature, pD 7.25.
50 are photochemically labile and exchange with deuterons in neutral D(2)O solution.
51 ve, degenerate exchange with solvent-derived deuterons in perdeuterated protic solvents such as D(2)O
52 ering the different bonding arrangements for deuterons in the 1 x 1 and 1 x 2 tunnels.
53 dicated by those peptides that retained more deuterons in the complex compared with control experimen
54 igate the local environments and mobility of deuterons in the manganese dioxide tunnel structures.
55  have used a short-pulse laser to accelerate deuterons in the relativistic transparency regime.
56  approximately 415 ppm were observed for the deuterons in the tunnel structures of manganite and grou
57                                     When the deuteron incorporation of the protein-derived peptides w
58                                              Deuteron incorporation reveals that the tip of the C-ter
59  peptides show some decrease in the level of deuteron incorporation upon NAD(+) binding, and another
60 rest of this domain is highly flexible (>40% deuteron incorporation), and its flexibility only decrea
61 ably folded in the autoinhibited state (~20% deuteron incorporation), whereas the rest of this domain
62                                              Deuterons increased XTT activity in melanized strains of
63 sis in vivo, but the chemical pathway of the deuterons into fat remains unclear.
64                                          The deuteron is the simplest compound nucleus, composed of o
65         A simple model of a metal containing deuterons is considered.
66                                          The deuteron line shapes give an excellent fit to a three-mo
67                                     Ruetschi deuterons, located in the cation vacancy sites in EMD, w
68 was applied with great success in proton and deuteron magnetic moment measurements(5), which culminat
69  no change in the number and the distance of deuterons magnetically coupled to manganese, indicating
70                                Comparing the deuteron modulation of the S(2)-state multiline signal o
71 headpiece subdomain protein at 140-4 K using deuteron NMR longitudinal relaxation measurements.
72             The main techniques employed are deuteron NMR quadrupolar echo line shape analysis, and T
73 s while broadband decoupling both proton and deuteron nuclei.
74 talyzed addition of a solvent derived proton/deuteron occurs on the si face at Calpha of the dienoyl-
75  A sharp quartet ENDOR pattern from a nearby deuteron of substrate was detected for each substrate.
76  A sharp quartet ENDOR pattern from a nearby deuteron of the substrate in a major binding geometry (d
77 arlier solid-state NMR measurements in alpha deuterons of glycine.
78 coupling is observed between nonexchangeable deuterons of methyl-deuterated acetate and YZ..
79                                      The two deuterons of the reactive carbons, D1 and D2, are closes
80 gen bond) with a slowly exchangeable proton (deuteron) of a side chain/backbone of an amino acid resi
81             The orientation of the proton or deuteron on the (13)Calpha-atom of glycine was assigned
82 ometry (MS), there is an unavoidable loss of deuterons, or back-exchange.
83 in the number of labile protons exchanged to deuterons, or vice versa.
84 onduction electrons is sufficient to allow a deuteron pair to fuse at a rate of 10(-18) sec-1, five p
85  realistic calculation of the fusion rate of deuteron pairs in palladium, this rate being 10(-23) sec
86 rements and mass spectrometry, we found that deuterons permeate through these crystals much slower th
87 in proteins have been confined to side-chain deuterons-primarily (13)CH(2)D or (13)CHD(2) methyl grou
88                                              Deuteron properties such as the root-mean-square charge
89  methods typically use light-ion (protons or deuteron) reactions on materials of similar mass to the
90 ce, and that the substitution of protons for deuterons results both in lower potentials for the hydro
91 cal vapour deposition, which allows a proton-deuteron separation factor of around 8, despite cracks a
92 tion, substitution of 36 methyl protons with deuterons significantly decreased the individual line wi
93 of 1 with biologically derived olefins and a deuteron source (TEMPOD) resulted in deuterium incorpora
94 -deutero alpha-halo acids using D(2)O as the deuteron source.
95 (s), during which all the rapidly exchanging deuterons such as those in amide and hydroxyl groups are
96                     CA was more resistant to deuterons than CN, and similar resistance was observed f
97 60 ps before the O radical cation can lose a deuteron to water.
98 vealed by the incorporation of a pair of cis deuterons to serve as a stereochemical lighthouse.
99           The unique capacity of protons and deuterons to travel through graphenic layers unlocks the
100 erence in quantum effects between proton and deuteron transfer for the enzymatic reaction than that i
101 on of GFP drives two parallel, excited-state deuteron transfer reactions with 10 ps and 75 ps time co
102 ee's were observed in all cases since proton/deuteron transfer was slowed down.
103 4 +/- 0.1 and E(a) = 35.1 +/- 0.7 kJ/mol for deuteron transfer.
104 of a 2-pocket active site where the observed deuteron transfers could occur.
105 endence of the rate constants for proton and deuteron transfers: KIE(real) ranging from 17 to 26, E(a
106 gy surface of the hydrogen-bonded proton (or deuteron/triton) was determined.
107 temperatures below 60 K are dominated by the deuteron tunneling mechanism.
108 ng and slow-growing fungi from high doses of deuterons under physiological conditions.
109  and by selective detection of the exchanged deuterons using Q-band 2H Mims electron nuclear double r
110  little change in the shift of the manganite deuterons was observed, consistent with the strong antif
111                 The smaller shift of the EMD deuterons was primarily ascribed to the smaller number o
112                                    Exchanged deuterons were "frozen" in the exchanged state by quench
113                                      Solvent deuterons were not incorporated into product, which impl
114  zero-point energies of incident protons and deuterons, which translates into the equivalent differen
115 times were associated with relatively mobile deuterons, which were contributed almost entirely by D(2
116 r this sample defined the location of the D1 deuteron, with respect to the g-frame of the iron center

 
Page Top