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The measured branching fractions of both decays are compatible with SM predictions.
In addition, we observe an enhancement in the D0K+ invariant mass around 2350 2500 MeV=c2 in both decays B 0 → D−D0K+ and B + → D0D0K+, which we are not able to interpret.
Both decays happen on the same time scale and match the faster plasmonic redshift rate.
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Likelihood contours for (B0 µ+µ−) versus are shown in Fig. 3. One-dimensional likelihood scans for both decay modes are displayed in the same figure.
The use of both decay and continuous contamination experimental techniques are discussed and related to the models presented.
The antiparticle and the particle B0 can both decay into two muons and no attempt is made in this analysis to determine whether the antiparticle or particle was produced (untagged method).
A series of test simulations are used to demonstrate the accuracy and numerical stability of the scheme for both decaying and forced compressible turbulence.
Microbes are thus something of a double-edged sword facilitating both decay and preservation.
Both decay and growth rate factors for all age-groups are listed in Table 1.
Although 68Ga and 18F both decay via positron emission, differences in their decay characteristics are expected to lead to different gamma counter efficiencies, and these data are shown in Table 1.
Both G H and G ex show two sharp peaks around ω ~ ± (ε 0 - μ) (causing the increase in G and the shift in its peaks), and both decay rather fast outside this region.
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