ライフサイエンスコーパス: polar molecule

1 in a change in polarity from a polar to non-polar molecule.

2 lattice of hydrogen cyanide (HCN), a highly polar molecule.

3 to realize new quantum many-body systems of polar molecules.

4 xperiments with nuclear spins and ultra-cold polar molecules.

5 ver, neither method can easily separate very polar molecules.

6 studies exist of their interaction with non-polar molecules.

7 that can conduct a variety of medium-sized, polar molecules.

8 0% of attractive interactions), even for the polar molecules.

9 reshold laws for the scattering of fermionic polar molecules.

10 emical reaction rates in an ultracold gas of polar molecules.

11 ld dense gas of potassium-rubidium (40K87Rb) polar molecules.

12 , diffusion-based passage of small (<600 Da) polar molecules.

13 harmacokinetic profiles of small, ionic, and polar molecules.

14 ophobic environment which cannot accommodate polar molecules.

15 way of manipulating the dipole direction of polar molecules.

16 pplications, helping cover from polar to low polar molecules.

17 long-range interacting lattice systems using polar molecules(2-5), Rydberg atoms(2,6-8), optical cavi

18 The strong dipole-dipole interactions in polar molecule(5) and Rydberg atom(6,7) systems allow mu

19 tions, making a long-lived degenerate gas of polar molecules a reality.

20 c poling on the adsorption/desorption of two polar molecules, acetic acid and 2-propanol, and one non

21 ns in the transport of water and other small polar molecules across cell membranes in animals and pla

22 ay for the flux of ions and other charged or polar molecules across cellular membranes.

23 bsorption enhancers to promote absorption of polar molecules across membrane surfaces.

24 oid nucleus affects the ability to transport polar molecules across membranes.

25 Screening of a library of small polar molecules against Mycobacterium tuberculosis (Mtb)

26 h-throughput screening of a library of small polar molecules against Mycobacterium tuberculosis led t

27 Polar molecules align in electric fields when the dipole

28 Because water is a polar molecule and water and metal surfaces are both pol

29 Mcfp3s are highly polar molecules and contain up to 28 mol % Dopa, which r

30 2) Ability to force all charged/polar molecules and especially free ions within and arou

31 on of long-lived, dense samples of ultracold polar molecules and evaporative cooling.

32 lts in an energy barrier for the approach of polar molecules and facilitates the formation of Ng addu

33 molecules indicate that interactions between polar molecules and ferroelectric surfaces are dominated

34 vely encapsulates the MOF, shielding it from polar molecules and ions.

35 lationship between the chemical structure of polar molecules and their membrane location, the behavio

36 val of unwanted medium components (proteins, polar molecules, and apolar/neutral molecules) while sel

37 ilitate the passive movement of water, small polar molecules, and some ions.

38 Polar molecules are desirable systems for quantum simula

39 Ultracold polar molecules are promising candidate qubits for quant

40 ing is caused by magnetostriction within the polar molecule as it distorts to lower its magnetic exch

41 xpression in the brain in vivo, should these polar molecules be made transportable through the blood-

42 ilar to those resulting from the mutations.A polar molecule binding site was also created by truncati

43 We demonstrate that ions or polar molecules can be driven by fluctuating Coulombic f

44 hermore, the large electric dipole moment of polar molecules can be tuned using an external electric

45 ange dipole-dipole forces acting between two polar molecules can result in the self-assembly of nonco

46 ning the high selectivity for water over non-polar molecules characteristic of GO interlayer nanochan

47 made of electrically neutral (polar and non-polar) molecules, conductivity increases on irradiation.

48 Polar molecules confined in an optical lattice are a ver

49 presence or an explanation as to how such a polar molecule could exit the plant cell and what physio

50 nsation of greasy compounds versus the small polar molecules detected by canonical neurotransmitter r

51 system Mn(CO)(5)(arylmethyl) reveal that the polar molecules do not promote the actual alkyl migratio

52 this intriguing phenomenon on small ions and polar molecules driven on the surfaces of carbon nanotub

53 ntitatively assessing sorption capacities of polar molecules during natural petroleum migration.

54 their crucial effect on enhancing binding in polar molecules, enabling binding in nonpolar molecules,

55 ias-field technique may enable using trapped polar molecules for precision measurement and quantum in

56 -orbit coupling in two-dimensional ultracold polar molecule gases.

57 The polar molecules have a permanent electric dipole moment,

58 hift properties in other small polar and non-polar molecules have also been described over a range of

59 surfaces with induced polarity and nonpolar/polar molecules have been investigated.

60 Trapped polar molecules have been proposed as a promising quantu

61 trapping techniques, ensembles of ultracold polar molecules have emerged as a promising platform tha

62 he confining surfaces, with those containing polar molecules having their electric dipoles aligned pa

63 n we propose is general and suitable for any polar molecule in the presence of an electric field.

64 branes (PEMs) selectively transport ions and polar molecules in a robust yet formable solid support.

65 Polar molecules in an optical lattice provide a versatil

66 ue, thereby realizing a long-lived sample of polar molecules in large electric fields.

67 ablished according to sorption capacities of polar molecules in migrating petroleum.

68 With the production of polar molecules in the quantum regime, long-range dipola

69 s of spin-polarized potassium-rubidium (KRb) polar molecules, in which elastic, tunable dipolar inter

70 hin 20 min and excellent resolving power for polar molecules including many isobaric metabolites.

71 way of introducing macromolecules and small polar molecules into the cytoplasm, and may have applica

72 using the common method of 2D adsorption of polar molecules layers on the metal surface, WF modifyin

73 ane (OM) that is highly impermeable to small polar molecules, making the bacteria intrinsically resis

74 ystal structure suggests that binding of non-polar molecules may be essential to the physiological fu

75 creating a long-lived ensemble of ultracold polar molecules may require confinement in a two-dimensi

76 nally, there is weak molecular adsorption of polar molecules (methylene blue) on the ta-C surface.

77 elded desorption pre-exponentials of the two polar molecules more than 11 orders of magnitude lower t

78 y difluorotoluene deoxynucleoside (F), a non-polar molecule of the same size and shape which lacks hy

79 ene switching diode, FSD), encapsulated with polar molecules of general type MX (M: metal, X: nonmeta

80 ction of a degenerate Fermi gas of ultracold polar molecules of potassium-rubidium.

81 In this context, ultracold polar molecules offer new and unique opportunities becau

82 Ultracold polar molecules offer the possibility of exploring quant

83 Charge impurities and polar molecules on the surface of dielectric substrates

84 es the activation energies for reactions, of polar molecules on the surfaces of ferroelectric materia

85 Here we use dipolar interactions of polar molecules pinned in a three-dimensional optical la

86 Rotational states of ultracold polar molecules possess long lifetimes, microwave-domain

87 The least polar molecule PY diffuses deeply into and interacts ext

88 erimentally demonstrate laser cooling of the polar molecule strontium monofluoride (SrF).

89 That is, they are able to separate polar molecules such as a polar stationary phase and non

90 10 000-fold increase in signal intensity for polar molecules such as amino acids, which has important

91 They can solubilize complex polar molecules such as cyclodextrins and glycopeptides.

92 ovide insight into the export of other large polar molecules such as DNA and proteins.

93 ar faces inward in nonpolar solvents to bind polar molecules such as sugar derivatives.

94 Small polar molecules, such as hydrogen sulphide (H(2)S), pene

95 ectric devices or as active surfaces to bind polar molecules, such as toxic gas, methanol, or DNA.

96 This device allows uncharged polar molecules, such as water, to rapidly pass through

97 s tending toward metabolism and hydrophilic, polar molecules tending toward passive or active excreti

98 ding the vaginal delivery of larger and more polar molecules that currently require parenteral admini

99 Fluorocarbons are lipophobic and non-polar molecules that exhibit remarkable biocompatibility

100 ong-field ionization studies in polar vs non-polar molecules that have the same chemical composition.

101 Polar molecules that permeate across the outer membrane

102 ue to penetrability problems of these highly polar molecules that possess sulfonamide moieties.

103 Seven representative polar molecules that preferentially docked to the polar

104 tonation [M+H](+) of unpolar as well as some polar molecules the homogeneous DBDI can be used to ioni

105 a wide range of sizes: from 500-Da targeted polar molecules to 150,000-Da tagged immunoglobulins int

106 these calculations agree with experiments on polar molecules to at best 25 per cent accuracy and fail

107 Here we use cold polar molecules to measure the electron EDM at the highe

108 As such, the use of polar molecules to passivate defects and tailor the IEA

109 y bound CT complexes allowed its constituent polar molecules to relax and hence the observed rotation

110 ment factors were obtained for smaller, more polar molecules using the 1-hexyl-3-methylimidazolium FA

111 To evaluate potential binding sites for non-polar molecules, we screened a number of hydrophobic lar

112 pported through simulation analysis in which polar molecules were bound most strongly to MOF-199, ref

113 The two polar molecules were found to adsorb significantly more

114 by progressively assembling amphiphilic and polar molecules, which form an elastic structure that ca

115 in a change in polarity from a polar to non-polar molecule, while for the VP4, amino acid difference

116 hanism of intermolecular attractions between polar molecules with a dipole moment due to uneven charg

117 Microscopic control over polar molecules with tunable interactions enables the re

118 A quantum gas of ultracold polar molecules, with long-range and anisotropic interac

119 Ultracold polar molecules, with their long-range electric dipolar