ライフサイエンスコーパス: selection rule

1 stimulus-response rule and one higher-level selection rule.

2 nal sequence, rotational quantum number, and selection rule.

3 he transducer, in agreement with the surface selection rules.

4 se be forbidden by established spectroscopic selection rules.

5 o types of emission are governed by distinct selection rules.

6 in atomic systems due to the electric-dipole selection rules.

7 n optically addressable through polarization selection rules.

8 s transition under a perturbation obeying no selection rules.

9 isorption configuration on Ag using the SERS selection rules.

10 adiabatic due to spin-forbidden (DeltaS = 2) selection rules.

11 gly, prestimulus activity in A1 also encoded selection rule, a cognitive variable typically considere

12 ore, the reduction in symmetry relaxes these selection rules, allowing for an admixture of dipolar co

13 ond harmonic radiation governed by a special selection rule and the induced electric dipolar and magn

14 oscopic information resulting from different selection rules and a stronger enhancement due to the no

15 structures reflect modifications of optical selection rules and appearance of low-energy electronic

16 We establish the geometrical selection rules and show that, surprisingly, Min-protein

17 chieved through the valley-dependent optical selection rules and the spin-valley locking in monolayer

18 on, which leads to established spectroscopic selection rules, and an interaction that is quadratic in

19 Selection rules, applied to the elements of irregular pe

20 However, although less explored, these selection rules are also an opportunity to establish sen

21 ed, the quantum spin dynamics and associated selection rules are profoundly modulated.

22 ondition, entropic factors, rather than spin-selection rules, are the source of the reduced Arrhenius

23 l sensing, which is mediated by polarization selection rules, as well as the morphology and strength

24 alley, because the two effects obey opposite selection rules at different valleys.

25 c levels are governed by the electric dipole selection rule because electric quadrupole, magnetic dip

26 njugated organic molecules may be allowed by selection rules but not observed in solution reactions b

27 These excitons obey optical selection rules distinct from those in conventional semi

28 s series, most likely as a result of natural selection rules driven by ring strain and steric hindran

29 t establish the circularly polarized optical selection rules for addressing individual valley exciton

30 It is confirmed that the mode symmetry selection rules for FCS are the same as for Raman scatte

31 The optical polarization and the selection rules for MCD select a subset of molecular ori

32 substantially from the established consensus selection rules for the hairpin ribozyme and were not pr

33 A small number of selection rules generates a very constrained subset, sug

34 n organic molecules and violation of dipolar selection rules in atoms.

35 elix with half the period and defined by the selection rule l = -3n + 7m (where l is any integer).

36 as composed of a double helix defined by the selection rule l = n + 7m (where l is even, and n and m

37 Symmetry and selection rules locate dipoles in their half-sarcomere,

38 We also identify the high-level path selection rules nature seems to use when picking its pat

39 g nanostructured electromagnetic fields, the selection rules of absorption spectroscopy could be fund

40 on spins occurs in TIs due to spin-dependent selection rules of optical transitions.

41 llows us to establish a relation between the selection rules of the electronic light scattering spect

42 The selection rules of the observed rotational transitions a

43 ure lead to dramatic changes in symmetry and selection rules of vibrational modes.

44 ination of CO in heme proteins, whereas spin selection rules play a minor or non-existent role.

45 electromagnon was investigated, mapping its selection rule precisely.

46 ut their bisignate nature and more stringent selection rules provide greatly enhanced resolution.

47 roluminescence polarization based on quantum selection rules provides a direct measure of the sign an

48 del considering the valley-dependent optical selection rules reveals the quantum pathways that give r

49 and RR frequencies, but because of different selection rules, the intensities vary dramatically betwe

50 polarization of the incident beams exploits selection rules to achieve further separation.

51 statistical learning model called "multiple selection rule voting" (MSRV).

52 ss model reveal the breakdown of the dipolar selection rules where quadrupole and octupole transition

53 a structural and chemical basis of substrate selection rules, which define the crucial function of th

54 tion of the two-photon and one-photon valley selection rules, which have opposite helicity in the mon

55 ibrational levels are not governed by strict selection rules, which makes laser cooling difficult.

56 hat prestimulus activity in mPFC encoded the selection rule-which sound from the mixture the rat shou