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

8 quilibrium constants for reactions involving adsorbed molecules.

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

10 ical intermediates produced by photolysis of adsorbed molecules.

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

12 d to amplify the spectroscopic signatures of adsorbed molecules.

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

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

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

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

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

18 Adsorbed molecules are involved in many reactions on sol

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

20 Adsorbed molecules can significantly affect the properti

21 The adsorbed molecules change the local carrier concentratio

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

44 Adsorbed molecules that do not show a charge transfer co

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

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

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

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

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

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

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

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

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

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

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

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

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

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