EOP-TI – an approach for truly efficient calculations of both Förster and Dexter excitonic couplings.

an injective map f : e(g) → {±1, ±2, · · · , ±q} is said to be an edge pair sum labeling of a graph g(p, q) if the induced vertex function f*: v (g) → z − {0} defined by f*(v) = (sigma e∈ev) f (e) is one-one, where ev denotes the set of edges in g that are incident with a vetex v and f*(v (g)) is either of the form {±k1, ±k2, · · · , ±kp/2} or {±k1, ±k2, · · · , ±k(p−1)/2} u {k(p+1)/2} accordin...

This investigation was carried out to examine the effect of think-pair-share on high school learners’ academic attainment in fractions and most effective stage think-pair-share. Two research questions five hypotheses guided this study. An explanatory sequential mixed method design used. Purposive convenience sampling techniques were used select first-years 78 participants, respectively. Teacher...

We calculate the potential for Dp − Dp pair and show that the coincident Dp −Dp system has (11 − p) tachyonic modes, with (9 − p) of them due to radiative corrections. We propose that the decay width of an unstable nonBPS-Dp-brane to closed strings is given by the imaginary part of the one-loop contribution to the effective potential of the open string tachyon mode.

With a goal toward explaining the observed baryon asymmetry of Universe, we extend standard model (SM) by adding vector-vector dimension-six effective operator coupling new Dirac fermion $\ensuremath{\chi}$, uncharged under SM gauge symmetries but charged number, to quarklike up-type and two identical down-type fermions. We introduce number violation Majorana masses which splits into fermions w...