ライフサイエンスコーパス: antisymmetric

1 or, whereas anomalous circular extinction is antisymmetric.

2 cy of the 1,2-dipalmitoylphosphatidylcholine antisymmetric acyl chain CH2 stretching vibration decrea

3 s evaluated using the intensity ratio of the antisymmetric and symmetric nu(CH2) modes as well as the

4 s evaluated using the intensity ratio of the antisymmetric and symmetric nu(CH2) modes as well as the

5 CH(2) antisymmetric and symmetric stretching bands ( approxima

6 is assessed using the intensity ratio of the antisymmetric and symmetric v(CH2) modes as well as the

7 eterministic scheme to prepare symmetric and antisymmetric atomic states with the use of external dri

8 hows intramolecular vibrations, and also two antisymmetric broad bands, centered at +/-0.65 V, due to

9 aled that vibrational excitation of nu3 (the antisymmetric C-H stretch) activates methane dissociatio

10 ing by carboxylate side chains, reflected in antisymmetric carboxylate band shifts.

11 morph stability, indicating the dominance of antisymmetric CH methylene vibrations as the anhydrous m

12 the binding pocket normal modes have a more antisymmetric character, with the walls vibrating out of

13 ate-like architecture that exhibits a unique antisymmetric chirality.

14 assigned, respectively, to the symmetric and antisymmetric CN stretches in the emitting triplet state

15 assigned, respectively, to the symmetric and antisymmetric CN stretching modes of the two coordinated

16 f the SB structure are the appearance of the antisymmetric CO stretch of the carboxylate group at 160

17 The antisymmetric CO stretch of tungsten hexacarbonyl was us

18 The 2D IR experiments conducted on the antisymmetric CO stretching mode measure spectral diffus

19 e amount of coherence in the system, and the antisymmetric coupling changes the nature of the coheren

20 spin chain with both symmetric exchange and antisymmetric Dzyaloshinsky-Moriya couplings.

21 c columnar structures in the fluid, or their antisymmetric equivalents.

22 n to be governed by the competing effects of antisymmetric exchange (G = 36.0 +/- 0.8 cm(-1)) and sym

23 c antiferromagnetic exchange interaction and antisymmetric exchange acting within the two low-lying s

24 the {Fe2Mn} analogue, but can be modeled by antisymmetric exchange effects.

25 etocrystalline anisotropy, Zeeman effect and antisymmetric exchange interactions.

26 tris(3-cumenyl-5-methylpyrazolyl)borate), an antisymmetric exchange term was required for the best fi

27 Antisymmetric exchange was less important for the other

28 te spin-orbit coupling of the (2)E state via antisymmetric exchange.

29 receptor proteins in the ASE neurons and the antisymmetric expression of olfactory receptor proteins

30 822.8 cm-1 are assigned to symmetric H-Th-H, antisymmetric H-Th-H, and Th=O stretching vibrations of

31 yang coupling mechanism generates concerted, antisymmetric helix-helix packing changes within the ada

32 Subsequently, two antisymmetric in vitro activity measurements were carrie

33 SE right (ASER), while it is expressed in an antisymmetric manner in the olfactory neuron pair AWC le

34 occurs near 1520 cm(-1), and a less intense antisymmetric mode appears in the Raman spectra near 168

35 rform IR difference spectroscopy, assign the antisymmetric modes, and accurately describe bonding.

36 difference spectroscopy, but until now, the antisymmetric modes, which require IR difference spectro

37 bitals to the antibonding combination of the antisymmetric N and aromatic orbitals using TD-DFT calcu

38 y of 15.1 kcal/mol with one quantum of CH(4) antisymmetric (nu(3)) stretching vibrational excitation

39 This is known as the "antisymmetric path problem" and leads to inverted amino

40 e MS/MS spectra, specifically addressing the antisymmetric path problem.

41 tags are selected from all maximum weighted antisymmetric paths in the graph and their reliabilities

42 es followed by energy minimization along the antisymmetric pathways led to enantiomeric pairs.

43 P-O and C-O torsions, whereas symmetric and antisymmetric phosphodioxy (PO2-) stretching modes are l

44 Both symmetric and antisymmetric phosphoester stretching modes are highly s

45 gnetism arises owing to the excitation of an antisymmetric plasmon resonance.

46 Antisymmetric pressure between SM and ST supported the c

47 two dissimilar clusters in the 7/2- band and antisymmetric resonance in the 9/2- band.

48 ansmission minima occur at the symmetric and antisymmetric resonances of the coupled crosses.

49 nsion) but leads to sliding of planes in the antisymmetric shear eigenmode of the elastic waveguide.

50 Relaxation due to antisymmetric shielding tensor components is significant

51 as 10 times more reactive than ones with the antisymmetric stretch excited.

52 second-order chiral-optical response at the antisymmetric stretch frequency of parallel beta-sheet a

53 x sequential rovibrational lines of the nu 4 antisymmetric stretch fundamental of C7 are probed by ga

54 hift of approximately 4 cm(-1) (for the COO- antisymmetric stretch in Asp) from 1565 to 1569 cm(-1) i

55 e frequencies of its C=O stretch and -COO(-) antisymmetric stretch shift substantially should any rel

56 vibrational modes, such as the symmetric and antisymmetric stretches in CH3D or CH4, lead to very dif

57 in the frequency and amplitude of the azide antisymmetric stretching band.

58 ed near 1809 wave numbers and assigned to an antisymmetric stretching fundamental in the 1 sigma g+ g

59 e infrared (IR) frequency of the carboxylate antisymmetric stretching mode (v(a)OCO) is related to th

60 CX(-) were assigned to the symmetric and the antisymmetric stretching modes in ECX(*) radicals.

61 This is assigned to an antisymmetric stretching vibration of the CO2- group bou

62 Antisymmetric tensor elements were found to be relativel

63 nt that the overall nuclear wave function be antisymmetric to exchange of identical protons (I = 1/2;

64 re assessed using the intensity ratio of the antisymmetric to symmetric v(CH2) modes as well as the f

65 is assessed using the intensity ratio of the antisymmetric to symmetric v(CH2) modes as well as the f

66 ratios and frequencies of the symmetric and antisymmetric transient infrared vibrations in the CN re

67 difference spectrum is therefore due to the antisymmetric vibration of both C=O groups of one electr

68 mode frequency calculations predict that an antisymmetric vibration of both C=O groups of the phyllo

69 equires the assignment of both symmetric and antisymmetric vibrational modes.