ライフサイエンスコーパス: selection rule

1 al resolution in TERS and the gradient-based selection rule.

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

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

4 ly explained by the proposed Floquet optical selection rules.

5 s whose behavior violates conventional Raman selection rules.

6 tic fields, defying the conventional optical selection rules.

7 phonon replica emission and modified valley-selection rules.

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

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

10 se be forbidden by established spectroscopic selection rules.

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

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

13 n optically addressable through polarization selection rules.

14 s transition under a perturbation obeying no selection rules.

15 isorption configuration on Ag using the SERS selection rules.

16 roximity effects, and spin-dependent optical-selection rules.

17 Furthermore, the spin-valley optical selection rules(12-14) of transition metal dichalcogenid

18 ene heterostructures can relax a restrictive selection rule(8,9) to allow quasielastic electron coupl

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

20 On the basis of a binary statistical selection rule, a difference in the proportion of treatm

21 Selection rules act to restrict the intrinsic anharmonic

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

23 anced Raman spectroscopy (TERS) exhibits new selection rule and sub-nanometer spatial resolution, whi

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

25 a retro-cue working memory task in which the selection rule and the memory content varied independent

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

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

28 Unconventional T cells follow specific selection rules and are poised to recognize self or evol

29 rsion symmetries to manipulate Raman optical selection rules and for exploring emergent magneto-optic

30 he larger size of Ce(III) ions, relaxing the selection rules and impacting the upconversion quantum y

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

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

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

34 Selection rules, applied to the elements of irregular pe

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

36 The Raman selection rules are determined by both the crystal symme

37 Selection rules are of vital importance in determining t

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

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

40 oluminescence, and unusual excitonic optical selection rules arise from the nature of the two- and mu

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

42 Landau levels (LLs) are described by simple selection rules associated with the LL index N.

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

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

45 ymmetric stacking further enriches excitonic selection rules, broadening opportunities for spin-photo

46 relationship not by defying symmetry-imposed selection rules but by invoking a photophysical process

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

48 te the magneto-electrical control over these selection rules by activating or suppressing Raman activ

49 experimental probes are governed by dipolar selection rules, collective multipolar excitations have

50 al transitions that violate the conventional selection rules Delta|N| = +/- 1.

51 e optical spectrum match exactly the optical selection rules derived by means of group theory.

52 fic value of this parameter, with additional selection rules determining the shape and size of stalag

53 nversion symmetry governs the optical parity selection rule, differentiating between accessible and i

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

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

56 chalcogenide moire superlattice, new optical selection rules, early evidence of moire excitons, and h

57 Optical selection rules endorsed by symmetry are crucial for und

58 Consequently, the specific magneto-optical selection rules exist for diverse excitation categories

59 e fundamental working mechanism and material selection rule for achieving optimal MC-OSCs.

60 ated polymers, here, we present an empirical selection rule for polymer candidates for textbook-like

61 d, secondly, the breaking down of the dipole-selection rule for radiative transitions in isolated ato

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

63 tion lifts the inter-Landau-level transition selection rules for dark trions, manifested by a distinc

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

65 This work sets up rational selection rules for ionic chemicals to passivate transit

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

67 xpected based on bulk absorbance spectra and selection rules for nonlinear hyperpolarizabilities.

68 eory, also predicting two previously unknown selection rules for PECD from fields with dynamical inve

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

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

71 lenge, primarily due to the different parity selection rules governing the electric and magnetic dipo

72 spin-phonon coupling, we derive group theory selection rules governing which vibrational symmetries c

73 tional spectroscopy (which is not subject to selection rules) has allowed the observation of all the

74 ns of the Woodward-Hoffmann orbital symmetry selection rules have now been elucidated by these calcul

75 des, coupled with valley-contrasting optical selection rules, holds great potential for future electr

76 Selection rules identified 92 NMTRC003B patients who par

77 The optical selection rules identified in the optical spectrum match

78 Here we show, by investigating the selection rules imposed by particle-hole symmetry and un

79 band structure and valley-dependent optical selection rule in group VI transition metal dichalcogeni

80 With the valley optical selection rule in the monolayer WSe(2), the electrolumin

81 The selection rule in the orientation dependence of the Jose

82 hysics associated with the nonlinear optical selection rule in WS(2) monolayer precisely determines t

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

84 tries and asymmetries of the laser drive and selection rules in PECD have not yet been derived.

85 tional Rashba system are obeyed as true spin selection rules in this correlated electron liquid and d

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

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

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

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

90 Herein, the selection rule of the donor/acceptor blend is demonstrat

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

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

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

94 The selection rules of the observed rotational transitions a

95 rsion behavior originates from the different selection rules of the parallel energy bands in the BaTi

96 Exploiting the optical selection rules of transition metal dichalcogenide monol

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

98 Thanks to the different selection rules on spin and charge currents, a pure spin

99 show that the otherwise invisible impact of selection rules on three-phonon scattering can be expose

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

101 On the basis of the selection rules, polyvinyl chloride, used widely in indu

102 electromagnon was investigated, mapping its selection rule precisely.

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

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

105 nt study shows a rare example where symmetry selection rules, rather than the Franck-Condon principle

106 We demonstrate that the spin-orbital selection rules relevant for conventional Rashba system

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

108 brational freedom can relax symmetry-related selection rules, significantly enhancing 2PA.

109 t demonstrations of logic gates using chiral selection rules suggest that optical chirality could pro

110 We find the selection rules that connect the doubly excited, spin-si

111 of opposite parity, which exhibit divergent selection rules that depend on inversion symmetry and th

112 mensional (3D) shapes and what are the shape selection rules that determine their final configuration

113 challenges, here we provide guide RNA (gRNA) selection rules that enable high phenotypic penetrance o

114 ifically, we extract from the X-TEC-revealed selection rules that the Cd and Re displacements are app

115 ere selected using explicit and quantitative selection rules that were then encoded in our hierarchic

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

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

118 nstruction remain underdeveloped and monomer selection rules to achieve this are elusive.

119 , a theory connecting the underlying optical selection rules to the microscopic electronic structure

120 e spectral properties of polaritons, such as selection rules, transition moments, and lifetimes are p

121 introduce momentum-resolved Floquet optical selection rules using group theory to elucidate the pump

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

123 e crystal symmetry-enabled well-known chiral selection rules, we demonstrate the viability of the con

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

125 h apparent deviation from the Laporte parity selection rule, which may be attributed to Hertzberg-Tel

126 te this behavior to a spin-occupancy-induced selection rule, which occurs when singlet spin coupling

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

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

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

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