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The paper is organized as follows. Section 2 we provide our slightly modified take on [BN14] on Twisted differential spectra for the purpose of constructing their AHSS. In
If the atom is moving, however, then a photon emitted in the direction of motion of the atom will have, by virtue of the Doppler shift, a higher frequency and hence a higher
With the lowest J = 0 GCM states as ground states of the initial and final nuclei, we can finally calculate the 0 νββ decay matrix element M 0ν in Eq.. CALCULATIONS
The comparison between HEGB results and the other studies suggests not only that the GB diffusion dominates the bulk diffusion, but also that the HEGB is one of the fastest
Probability distributions for radii as a function of mass for the baseline data set and baseline model (upper left panel), for the baseline data set with Model C (upper right),
The hit function distribution, H ( z ), can be defined to be gauge invariant, although since the potential enters the path integral as a phase it now becomes complex val- ued.. We
The ground state can then be determined by minimiza- tion of energy, and the parameters of the functional optimized to reproduce certain selected observables of finite nuclei (such
Taking advantage of the high acceptance and axial symmetry of the WASA-at-COSY detector, and the high degree of the polarized proton beam of COSY, the reaction ~ pp → ppη has
