Soft x-ray emission spectroscopy XES and x-ray absorption spectroscopy XAS are employed to investigate the occupied and unoccupied electronic structures in rocksalt-phase single-crystal CdO. Resonant XES at the OK edge reveals a clear Cd 4d–O 2p hybridized peak and momentum-dependent coherent contributions to the resonant emission spectra. Good agreement is obtained between the above-threshold ...

A balanced bipartite graph G is said to be 2p-Hamilton-biconnected if for any balanced subset W of size 2p of V (G), the subgraph induced by V (G)\W is Hamilton-biconnected. In this paper, we prove that “ Let p ≥ 0 and G be a balanced bipartite graph of order 2n with minimum degree δ(G) ≥ k, where n ≥ 2k − p + 2 and k ≥ p. If the number of edges e(G) > n(n − k + p− 1) + (k+2)(k−p+1), then G is ...

Let G = (V,E) be a graph of order p and size q. It is known that if G is super edge-magic graph then q ≤ 2p− 3. Furthermore, if G is super edge-magic and q = 2p− 3, then the girth of G is 3. It is also known that if the girth of G is at least 4 and G is super edge-magic then q ≤ 2p − 5. In this paper we show that there are infinitely many graphs which are super edge-magic, have girth 5, and q =...

Two-photon (2P) microscopy is a high-resolution imaging technique that was initially applied by neurobiologists and developmental cell biologists but has subsequently been broadly adapted by immunologists. The value of 2P microscopy is that it affords an unparalleled view of single-cell spatiotemporal dynamics deep within intact tissues and organs. As the technology develops and new transgenic ...

In an experiment with the BigRIPS separator at the RIKEN Nishina Center, we observed two-proton (2p) emission from ^{67}Kr. At the same time, no evidence for 2p emission of ^{59}Ge and ^{63}Se, two other potential candidates for this exotic radioactivity, could be observed. This observation is in line with Q value predictions which pointed to ^{67}Kr as being the best new candidate among the th...

In this paper we give a combinatorial interpretation for the coefficient of sν in the Kronecker product s(n−p,p) ∗ sλ, where λ = (λ1, . . . , λ`(λ)) ` n, if `(λ) ≥ 2p − 1 or λ1 ≥ 2p − 1; that is, if λ is not a partition inside the 2(p − 1) × 2(p − 1) square. For λ inside the square our combinatorial interpretation provides an upper bound for the coefficients. In general, we are able to combinat...

The existence of n-particle n-hole deformed yrare bands in the N=28 isotones is explored using full pf -shell diagonalizations and the Lanczos Strength Function method. We find different 2p-2h and 4p-4h collective bands that, when allowed to mix, more often disappear. Only the 2p-2h yrare band in Cr and the 4p-4h yrare band in Ni survive, and only in this latter case, due to the reduced density...

The CLEO Collaboration has observed the first hadronic transition among bottomonium (bb̄) states other than the dipion transitions among vector states, Υ(nS)→ππΥ(mS). In our study of Υ(3S) decays, we find a significant signal for Υ(3S)→γωΥ(1S) that is consistent with radiative decays Υ(3S)→γχb1,2(2P ), followed by χb1,2(2P )→ωΥ(1S). The branching ratios we obtain are B(χb1(2P )→ωΥ(1S)) = 1.63 +0...

For every p ≥ 2, we obtained an explicit construction of a family of W(2, 2p − 1)-modules, which decompose as direct sum of simple Virasoro algebra modules. Furthermore, we classified all irreducible self-dual W(2, 2p − 1)-modules, we described their internal structure, and computed their graded dimensions. In addition, we constructed certain hidden logarithmic intertwining operators among two ...