ライフサイエンスコーパス: adsorbed molecule

1 ires knowing the entropy and enthalpy of the adsorbed molecule.

2 irections and the C-H bond directions in the adsorbed molecule.

3 dressable gate electrode and the presence of adsorbed molecules.

4 hanical sensitivity as well as the number of adsorbed molecules.

5 rp lasing emission that is ultrasensitive to adsorbed molecules.

6 gies often lack sufficient interactions with adsorbed molecules.

7 quilibrium constants for reactions involving adsorbed molecules.

8 ive to both the amount and the energetics of adsorbed molecules.

9 ical intermediates produced by photolysis of adsorbed molecules.

10 mal coupling between the laser pulse and the adsorbed molecules.

11 e (S/N) spectra from femtomole quantities of adsorbed molecules.

12 d to amplify the spectroscopic signatures of adsorbed molecules.

13 olecules, enabling the transfer of charge to adsorbed molecules.

14 n with possible lateral interactions between adsorbed molecules.

15 templating interaction of the interface with adsorbed molecules.

16 tes without significant interactions between adsorbed molecules.

17 tects physicochemical characteristics of the adsorbed molecules along with the adsorbed mass.

18 t more than one molecular location within an adsorbed molecule and the new method is named electron s

19 edicted to show no diffusion limitations for adsorbed molecules and extremely high CO(2)/N(2) adsorpt

20 NMR techniques to measure and assess dilute adsorbed molecules and their molecular interactions on l

21 all and we have to reckon with the motion of adsorbed molecules, and there is no "bulk" fluid region.

22 Adsorbed molecules are involved in many reactions on sol

23 Presumably, the adsorbed molecules are semiquinones, that is, are the in

24 ange of molecular structure of catalysts and adsorbed molecules as the reactions proceed with changes

25 Adsorbed molecules can significantly affect the properti

26 The adsorbed molecules change the local carrier concentratio

27 (CID), where surface plasmons are damped by adsorbed molecules, enabling the transfer of charge to a

28 The induced dissociation of the intact adsorbed molecule for both reagents occurred at an energ

29 he developed model can predict the number of adsorbed molecules for new cases within seconds, while M

30 strate that the faster the AFM tip displaces adsorbed molecules in a monolayer, the more heterogeneou

31 Hence, also strongly adsorbed molecules in soils and aquatic environments may

32 hindrance effect exerted on the neighboring adsorbed molecules increases, and the geometrical packin

33 nd then back to large pore) as the number of adsorbed molecules increases, which is explained in term

34 nergy, and the LUMO density extends onto the adsorbed molecule, increasing the donor-acceptor interac

35 -dependent in situ spectra indicate that the adsorbed molecule is the benzotriazole anion (BTA-) at a

36 t electron transfer between the TiO2 and the adsorbed molecules is governed by competition between el

37 Clustering of the adsorbed molecules is promoted by high ionic strength an

38 How this affects individual adsorbed molecules is shown for the incipient ferroelect

39 ric repulsion resulting in area exclusion by adsorbed molecules is taken into account by treating the

40 ssibility of attractive interactions between adsorbed molecules is taken into account in a limited fa

41 Long-range order within adsorbed molecules is very often a desirable property fo

42 Doping also occurs when surface adsorbed molecules modify the Fermi level of low dimensi

43 The strongly adsorbed molecules must be mobile to free up these sites

44 osed of 2D boron nitride (BN) nanosheet with adsorbed molecules of BCL-2 inhibitor, Navitoclax (NAVI)

45 rgely focused on model systems consisting of adsorbed molecules on flat metallic surfaces with minima

46 uring the molecular self-assembly of complex adsorbed molecules on surfaces.

47 measurements of the nonlocal manipulation of adsorbed molecules on the Si(111)-7 x 7 surface in the s

48 etection and also to calculate the number of adsorbed molecules on the surface.

49 ical response due to radial diffusion of the adsorbed molecules outward from the microspots onto the

50 erent ML models for predicting the number of adsorbed molecules over time, including linear regressio

51 greater than the ionization potential of the adsorbed molecules, photoelectrons were collected that o

52 led understanding of the conformation of the adsorbed molecule relative to the Cu(110) crystal lattic

53 w way to determine the standard entropies of adsorbed molecules (S(ad)(0)) on single crystal surfaces

54 Importantly, the smallest concentration of adsorbed molecules shows the largest Raman enhancements

55 ch other, despite the fact that the directly adsorbed molecules take up less than 10% of the silica s

56 ron-acceptor molecule and as an irreversibly adsorbed molecule that heals natural oxygen vacancy defe

57 Adsorbed molecules that do not show a charge transfer co

58 For exohedrally adsorbed molecules, the dielectric screening is found to

59 ver, with glutaraldehyde fixation of already adsorbed molecules, the resolution of both GroEL and Gro

60 because they are not wide enough to host non-adsorbed molecules; this is the case for samples with le

61 luable information on energy transfer to the adsorbed molecules through the resonance linewidth.

62 ements, thus allowing picogram quantities of adsorbed molecules to be characterized.

63 e injected charge spreads out, it can induce adsorbed molecules to react.

64 Monolayer dynamics enable adsorbed molecules to reorganize according to the underl

65 ration and increase in the loading of weakly adsorbed molecules upon raising the temperature above ro

66 Resonant excitation of adsorbed molecules using IR radiation causes the cantile

67 ely on the ability to tune the properties of adsorbed molecules, we anticipate that the ability to sy

68 ect this conclusion to apply to all types of adsorbed molecules where van der Waals interactions gove

69 rphology and spectroscopic signatures of the adsorbed molecule, where modern probes are only now bein

70 equired) and can be applied to low masses of adsorbed molecules, which we demonstrate here by quantif

71 Subtleties in the redox chemistries of adsorbed molecules, which were difficult to monitor with

72 e the local potential energy landscape of an adsorbed molecule with a carbon monoxide (CO)-terminated

73 l matching of the rotational symmetry of the adsorbed molecule with that of the underlying metal surf

74 milarly, selective vibrational excitation of adsorbed molecules with an STM tip to induce motion or d

75 dependence of the amount of adsorbed and non-adsorbed molecules within micropores, which experience s