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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.
8 we compared the effects of densely-ionizing deuterons and sparsely-ionizing X-rays on two microscopi
9 is observed between the QCC values of alpha-deuterons and the inverse cube of C(alpha)-H(alpha)...O=
10 ling tensors of the hydrogen-bonded protons (deuterons) and their principal directions with respect t
12 r this process decreases to 7.6 s(-)(1) when deuterons are substituted for protons in the aromatic ri
13 s from many of the alanine backbone C(alpha) deuterons as well as the alanine side-chain C(beta) meth
14 s a 6th (distal) ligand; (2) to exchangeable deuterons assigned to Arg127 which may H-bond with the p
15 12)-ene (15-d(1)), which could incorporate a deuteron at the C-12 position on the pathway to doubly l
17 erence in the number of protons exchanged to deuterons (based on protein folding under pressure) coul
18 crystal is used to generate and accelerate a deuteron beam (> 100 keV and >4 nA), which, upon strikin
19 " ring of naphthalene, with the closest ring deuteron being located at a distance of approximately 4.
21 The mass spectrum of the m/z 166 ion for deuteron-charged methyl dihydrocinnamate showed two peak
22 ntal quadrupolar coupling constants of alpha deuterons (D(alpha) QCC) are reported for the residues o
23 measurements are consistent with substantial deuteron density in the octahedral, interstitial voids o
24 ronment was explicitly shown by exchangeable deuteron ENDOR that implied hydrogen bonding to the quin
25 alpies and entropies are reported for proton-deuteron exchange at 42 amide sites in T4 lysozyme and c
30 M experiments investigating the proximity of deuterons exchanged into the vicinity of YZ. after incub
33 methyl groups, whereas signals from C(alpha) deuterons generally have not been observed for similar p
37 een as a function of intercalation level for deuterons in both 1 x 1 and 1 x 2 tunnels are consistent
38 Amide protons were allowed to exchange with deuterons in buffered D2O at room temperature, pD 7.25.
40 ve, degenerate exchange with solvent-derived deuterons in perdeuterated protic solvents such as D(2)O
42 dicated by those peptides that retained more deuterons in the complex compared with control experimen
43 igate the local environments and mobility of deuterons in the manganese dioxide tunnel structures.
44 approximately 415 ppm were observed for the deuterons in the tunnel structures of manganite and grou
46 peptides show some decrease in the level of deuteron incorporation upon NAD(+) binding, and another
53 no change in the number and the distance of deuterons magnetically coupled to manganese, indicating
58 talyzed addition of a solvent derived proton/deuteron occurs on the si face at Calpha of the dienoyl-
59 A sharp quartet ENDOR pattern from a nearby deuteron of substrate was detected for each substrate.
60 A sharp quartet ENDOR pattern from a nearby deuteron of the substrate in a major binding geometry (d
64 gen bond) with a slowly exchangeable proton (deuteron) of a side chain/backbone of an amino acid resi
67 onduction electrons is sufficient to allow a deuteron pair to fuse at a rate of 10(-18) sec-1, five p
68 realistic calculation of the fusion rate of deuteron pairs in palladium, this rate being 10(-23) sec
69 rements and mass spectrometry, we found that deuterons permeate through these crystals much slower th
70 in proteins have been confined to side-chain deuterons-primarily (13)CH(2)D or (13)CHD(2) methyl grou
72 cal vapour deposition, which allows a proton-deuteron separation factor of around 8, despite cracks a
73 tion, substitution of 36 methyl protons with deuterons significantly decreased the individual line wi
75 (s), during which all the rapidly exchanging deuterons such as those in amide and hydroxyl groups are
79 erence in quantum effects between proton and deuteron transfer for the enzymatic reaction than that i
80 on of GFP drives two parallel, excited-state deuteron transfer reactions with 10 ps and 75 ps time co
84 endence of the rate constants for proton and deuteron transfers: KIE(real) ranging from 17 to 26, E(a
88 and by selective detection of the exchanged deuterons using Q-band 2H Mims electron nuclear double r
89 little change in the shift of the manganite deuterons was observed, consistent with the strong antif
93 zero-point energies of incident protons and deuterons, which translates into the equivalent differen
94 times were associated with relatively mobile deuterons, which were contributed almost entirely by D(2
95 r this sample defined the location of the D1 deuteron, with respect to the g-frame of the iron center
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