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1  the ordering is determined by the principal quantum number.
2 r DeltaJ, distributed in order by rotational quantum number.
3 e of SOC implies that the spin is not a good quantum number.
4 Rydberg states with a predetermined magnetic quantum number.
5  a cluster of vibrational frequencies by one quantum number.
6 e GAM is, in some situations, an appropriate quantum number.
7 number required by their total electron spin quantum number.
8 lenge quantum mechanical prediction for high quantum numbers.
9 ges ('valleys') to have additional spin-like quantum numbers.
10  exotic spin excitations carrying fractional quantum numbers.
11 asiparticle excitations can carry fractional quantum numbers.
12 otal angular momentum (TAM) serves as a good quantum number(7-9).
13 tion of magnetic field that changes the spin quantum number and also the existence of non-equilibrium
14                 The connection between the K-quantum number and product correlations in the barrierle
15        By directly measuring the topological quantum numbers and invariants, we report the observatio
16 ides a building block in manipulating valley quantum numbers and scalable valleytronics.
17 ccording to vibrational sequence, rotational quantum number, and selection rule.
18 aps are described by two integer topological quantum numbers, and report evidence of their recursive
19 of freedom and demonstrated that topological quantum numbers are completely determined from spin text
20                        States with different quantum numbers are produced using nanometre-sized elect
21 possess distinct features in level spacings, quantum numbers, as well as field dependencies.
22 e that Landau modes with different azimuthal quantum numbers belong to three classes, which are chara
23                      The "goodness" of the K-quantum number can be related to the amount of energy in
24 l as a fragment with different sets of local quantum numbers (e.g., charge and excitation number).
25 hibiting different relaxation times and spin quantum numbers, facilitates the convenient modulation o
26  decay energies and orbital angular momentum quantum numbers for both parent and daughter nuclei.
27 eases in covalency with increasing principal quantum number, in the order Ti > Zr approximately = Hf,
28                             This topological quantum number is connected to polarization transport an
29  correlated vibrational distributions, the K-quantum number is found to be approximately conserved at
30 st continuum emission and (13)CO (rotational quantum number J = 2 --> 1) line emission from the disk
31 le way with increase in the angular momentum quantum number J and with change in the proton number Z
32 including super-rotor states with rotational quantum number (j) as high as 170, using a broad-band op
33 e on (or 'propensity rule' for) the magnetic quantum number m of the molecules, and a previously unre
34 tia with increase in J, the angular-momentum quantum number, many of the lanthanon ground-state bands
35 the anisotropy axis with an angular momentum quantum number mJ=+/-(15)/2.
36 al characteristics, represented by molecular quantum numbers (MQNs), that contribute to variance in C
37  incapable of handling Rydberg states having quantum number n > 3, so having a new tool capable of ha
38 vents when the Rydberg orbital has principal quantum number n = 3, they have proven to be incapable o
39  that a Rydberg orbital of a given principal quantum number n has a limited range of distances over w
40                             As the principal quantum number n was increased beyond ~70, no more than
41  and thickness T both of which depend on the quantum number n, and (iii) assumes that strong coupling
42 ch the screening (S) and effective principal quantum number (n*) were previously obtained by fitting
43 berg states characterized by large principal quantum numbers (n).
44 is to good approximation conserved and has a quantum number of 15/2 for both triatomic molecules.
45 see text]F Rydberg states, up to a principal quantum number of [Formula: see text].
46              Second, the large electron spin quantum number of Gd (7/2) results in notably larger PRE
47 (X(2)pi((1/2)), V = 18; V is the vibrational quantum number of NO), reaching 0.1 at the lowest veloci
48 he Kramer's doublet with a half-integer spin quantum number of S = 15/2, this relatively sharp line i
49 79)N is characterized by a half-integer spin quantum number of S = 15/2.
50 and angular distributions on the vibrational quantum number of the N(2)(+) product.
51     We construct many-body local RSIs as the quantum numbers of a set of symmetry operators on open b
52 vely refer to the vibrational and rotational quantum numbers of the D(2) molecule).
53 e symmetry axis is a conserved quantity with quantum number Omega and we study the polynomial Omega d
54                             Spin and orbital quantum numbers play a key role in the physics of Mott i
55 e v and j are the vibrational and rotational quantum numbers, respectively.
56 d j represent the vibrational and rotational quantum numbers, respectively.
57  the dynamics of single spins with principal quantum number s = 1/2, 1, and 3/2, allowing a measureme
58 ctivity of radical modules with unequal spin quantum numbers (S), macrocyclic S = 2 and, cross-linkin
59 ments in the periodic table and to principal quantum number six, and constitutes a new approach to el
60 ependent particles in orbitals with discrete quantum numbers, subject to a mean field generated by al
61 d by exotic spin excitations with fractional quantum numbers (termed 'spinons').
62 corresponds to entanglement with the largest quantum number that has been demonstrated in an experime
63 n has been inhibited by the spin and orbital quantum numbers that give way to J = 0 in the trivalent
64 pproximately 82-104 for the angular-momentum quantum number, that the moment of inertia is approximat
65 ayer polarization maps to the valley or spin quantum numbers.The phase diagram of bilayer graphene at
66  has, however, been debated if k is a useful quantum number to describe the band structure in quantum
67  that plasmon modes with different azimuthal quantum numbers (topological charge) are phase-matched,
68 al excited positronium states with principal quantum numbers up to n i = 5.
69 ocalization-delocalization on the lattice of quantum numbers, we are dealing with a situation where e
70 ally, for lasing lines with lower rotational quantum numbers, we observe a stronger coupling between
71 alization centers, peculiar distributions of quantum numbers, well-behaved and abnormal energy spectr
72  possess a binary flavor known as the valley quantum number which can be used as a basis to encode in
73 iginates from an inversion of the rotational quantum numbers, which we propose as a criterion in the