ライフサイエンスコーパス: quantum number

1 e of SOC implies that the spin is not a good quantum number.

2 number required by their total electron spin quantum number.

3 r DeltaJ, distributed in order by rotational quantum number.

4 lenge quantum mechanical prediction for high quantum numbers.

5 ges ('valleys') to have additional spin-like quantum numbers.

6 exotic spin excitations carrying fractional quantum numbers.

7 tion of magnetic field that changes the spin quantum number and also the existence of non-equilibrium

8 The connection between the K-quantum number and product correlations in the barrierle

9 By directly measuring the topological quantum numbers and invariants, we report the observatio

10 ccording to vibrational sequence, rotational quantum number, and selection rule.

11 aps are described by two integer topological quantum numbers, and report evidence of their recursive

12 of freedom and demonstrated that topological quantum numbers are completely determined from spin text

13 States with different quantum numbers are produced using nanometre-sized elect

14 e that Landau modes with different azimuthal quantum numbers belong to three classes, which are chara

15 The "goodness" of the K-quantum number can be related to the amount of energy in

16 hibiting different relaxation times and spin quantum numbers, facilitates the convenient modulation o

17 eases in covalency with increasing principal quantum number, in the order Ti > Zr approximately = Hf,

18 correlated vibrational distributions, the K-quantum number is found to be approximately conserved at

19 st continuum emission and (13)CO (rotational quantum number J = 2 --> 1) line emission from the disk

20 le way with increase in the angular momentum quantum number J and with change in the proton number Z

21 e on (or 'propensity rule' for) the magnetic quantum number m of the molecules, and a previously unre

22 tia with increase in J, the angular-momentum quantum number, many of the lanthanon ground-state bands

23 the anisotropy axis with an angular momentum quantum number mJ=+/-(15)/2.

24 incapable of handling Rydberg states having quantum number n > 3, so having a new tool capable of ha

25 vents when the Rydberg orbital has principal quantum number n = 3, they have proven to be incapable o

26 that a Rydberg orbital of a given principal quantum number n has a limited range of distances over w

27 As the principal quantum number n was increased beyond ~70, no more than

28 and thickness T both of which depend on the quantum number n, and (iii) assumes that strong coupling

29 ch the screening (S) and effective principal quantum number (n*) were previously obtained by fitting

30 (X(2)pi((1/2)), V = 18; V is the vibrational quantum number of NO), reaching 0.1 at the lowest veloci

31 he Kramer's doublet with a half-integer spin quantum number of S = 15/2, this relatively sharp line i

32 79)N is characterized by a half-integer spin quantum number of S = 15/2.

33 vely refer to the vibrational and rotational quantum numbers of the D(2) molecule).

34 Spin and orbital quantum numbers play a key role in the physics of Mott i

35 e v and j are the vibrational and rotational quantum numbers, respectively.

36 the dynamics of single spins with principal quantum number s = 1/2, 1, and 3/2, allowing a measureme

37 ctivity of radical modules with unequal spin quantum numbers (S), macrocyclic S = 2 and, cross-linkin

38 ependent particles in orbitals with discrete quantum numbers, subject to a mean field generated by al

39 d by exotic spin excitations with fractional quantum numbers (termed 'spinons').

40 corresponds to entanglement with the largest quantum number that has been demonstrated in an experime

41 pproximately 82-104 for the angular-momentum quantum number, that the moment of inertia is approximat

42 ayer polarization maps to the valley or spin quantum numbers.The phase diagram of bilayer graphene at

43 that plasmon modes with different azimuthal quantum numbers (topological charge) are phase-matched,

44 al excited positronium states with principal quantum numbers up to n i = 5.

45 ocalization-delocalization on the lattice of quantum numbers, we are dealing with a situation where e

46 iginates from an inversion of the rotational quantum numbers, which we propose as a criterion in the