ライフサイエンスコーパス: effective charge

1 their respective binding sites dilutes their effective charge.

2 6C than for L361C and V363C mutant channels (effective charge 2.19, 1.41 and 1.45, respectively).

3 orce(1), for example, by increasing the Born effective charges(2).

4 ight packing of nanoscale components enables effective charge and exciton transport in supraparticles

5 retical scaling form, extract values for the effective charge and the interaction parameter of the qu

6 O-solvated Zn(2+) possesses largely reduced effective charge and thus reduced electrostatic interact

7 lations are reported between oligonucleotide effective charges and current blockages, and between the

8 We report effective charges and diffusion constants of several dif

9 is found to have a substantial influence on effective charges and diffusion constants.

10 nthetic vesicles of known surface potential, effective charges and intrinsic partition coefficients w

11 discriminate the protein tags based on their effective charges and masses revealed through a generic

12 ability which generates large anomalous Born effective charges and strong coupling of low energy pola

13 Anomalous effective charges are reported, including the first repo

14 An effective charge-assisted H-bonding approach is develope

15 We found that measured effective charges at low salts are approximately 1/5th o

16 evealed that these microspheres exhibited an effective charge buildup in the presence of such species

17 We demonstrate that the measured effective charge captures subtle differences in molecula

18 rface between g-C(3)N(4) and titania permits effective charge carrier separation, leading to enhanced

19 apparent KD of 1 mM) Sr2+ and Ba2+ were less effective charge carriers and Na+ was not conducted to a

20 taneously setting anions and lithium ions as effective charge carriers.

21 ced polarization, high drift mobilities, and effective charge collection, which are excellent for thi

22 ons served as conducting band states for the effective charge delocalization between particle-bound f

23 sly reduces the nongeminate recombination by effective charge delocalization.

24 Meanwhile, its effective charge density can be further improved as the

25 Its effective charge density can reach up to ~8.80 mC m(-2)

26 electric field at a rate that depends on the effective charge density of the molecule.

27 membrane interface when bound and alters the effective charge density on the membrane interface by ap

28 ic screening that ascribes to the polymer an effective charge density that is independent of force an

29 coefficient of each ion species, the average effective charge distribution on the wall of the pore, a

30 = 3 was determined to be e(*) = 1, where the effective charge e(*) is normalized to the charge of an

31 charge-pair states is observed, followed by effective charge extraction.

32 including the first report of negative Born effective charges for nominal +2 cations.

33 ostatic interaction term based on the use of effective charges, (ii) a term describing the electrosta

34 The role of dynamical (or Born effective) charges in classification of octet AB-type bi

35 ecessitates the development of extensive and effective charging infrastructure.

36 nt years has necessitated the development of effective charging infrastructures.

37 te contact between layers, which facilitates effective charge injection and transport under strain af

38 ch its relationship to abnormally large Born effective charges is also unambiguously revealed.

39 Through experimentally measured effective charge measurements, under low ion normality w

40 Our experiments suggest that the effective charge near the presumed intracellular mouth o

41 ) greater virus-floc binding affinity due to effective charge neutralization and hydrophobic interact

42 to higher electronic dimensionality; 3) Born effective charges not being anomalously high, which, com

43 study the relationship between diffusion and effective charge of a fluorescently labeled 40-base poly

44 By sensitively probing the effective charge of a molecule, electrometry provides a

45 Monovalent cation binding reduces the effective charge of an A-tract-containing oligomer, decr

46 We find that the difference in the Born effective charge of atoms at the interface can be used a

47 Since the effective charge of labeled DNA molecules was equal to t

48 acellular pH is below 6, suggesting that the effective charge of membrane components might be a cruci

49 isfy a Nernst-Einstein relation in which the effective charge of RNA is reduced by the charge of tran

50 n coefficient, electrophoretic mobility, and effective charge of ssDNA in a solid-state nanopore.

51 he first demonstration of the measurement of effective charge of ssDNA in relation to Mg2+ concentrat

52 Taking into account that the effective charge of the carboxylic acid residues is a ke

53 However, the effective charge of the counterions is lowered by their

54 bulk-phase diffusion coefficients and of the effective charge of the nucleotides in 1.0 M NaCl sugges

55 sting that there is a slight decrease in the effective charge of the selenium.

56 The effective charge of the ssDNA could then be determined u

57 usion of the ssDNA also increased, while the effective charge of the ssDNA decreased.

58 In addition it is found that the effective charges of the TS do not follow the previously

59 eractions with the phosphate and/or that the effective charge on the 5'-phosphate may be substantiall

60 or transport through the pore as well as the effective charge on the dye, all in the absence of an in

61 es revealed that chemical shifts concur with effective charges on sp-carbon atoms in para-tolanes, wh

62 M acetic acid and the corresponding average effective charges (q(eff)).

63 c character of the heterostructure, creating effective charge redistribution within the system.

64 indicate that these differences reflect more effective charge reorganization upon deprotonation of Mo

65 icate that protein reorganization leading to effective charge screening may be a necessary structural

66 charge density, diffusion channel size, and effective charge screening on ligand-assisted solid stat

67 ctor in electrostatic equilibrium is zero by effective charge screening; free carriers within a metal

68 ifically, PNRs are demonstrated to act as an effective charge-selective interlayer by enhancing hole

69 3)N(4) heterojunction is designed to promote effective charge separation and enhance the photoelectro

70 of the heterojunctions that facilitate more effective charge separation and generation with more OP

71 Its interconnected structure facilitated effective charge separation and transport, leading to be

72 that provide an additional driving force for effective charge separation in perovskite CQD solar cell

73 trons and holes at the same time, leading to effective charge separation was directly proved by ultra

74 ctrum and the heterogeneous architecture for effective charge separation, films of this material show

75 n mechanism and to design nanostructures for effective charge separation.

76 d that the hybrid GA@UiO-66-NH(2) acts as an effective charge storing material with a capacitance of

77 ice improve sensing performance by promoting effective charge transfer and surface interactions with

78 induce nanowire growth depends strongly upon effective charge transfer between the organic molecules

79 Establishing highly effective charge transfer channels in carbon nitride (C(

80 developed by Stoddart and colleagues, forms effective charge transfer complexes with a variety of el

81 II band alignment in STM junction to achieve effective charge-transfer state decoupling.

82 as broad implications for the design of more effective charge-transfer systems.

83 An effective charge transference from donor to acceptor via

84 We further show that comparing the measured effective charge with calculations for a rigid, charged

85 We compare measurements of molecular effective charge with theoretically calculated values fo