Results on charged pion and kaon production in central $\mathrm{Pb}+\mathrm{Pb}$ collisions at $20A$ and $30A$ GeV are presented and compared to data at lower and higher energies. Around $30A$ GeV a rapid change of the energy dependence for the yields of pions and kaons as well as for the shape of the transverse mass spectra is observed. The change is compatible with the prediction that the threshold for production of a state of deconfined matter at the early stage of the collisions is located at low CERN Super Proton Synchroton energies.

Interaction cross sections and charged pion spectra in $p+\mathrm{C}$ interactions at 31 GeV/$c$ were measured with the large-acceptance NA61/SHINE spectrometer at the CERN SPS. These data are required to improve predictions of the neutrino flux for the T2K long-baseline neutrino oscillation experiment in Japan. A set of data collected during the first NA61/SHINE run in 2007 with an isotropic graphite target with a thickness of 4% of a nuclear interaction length was used for the analysis. The measured $p+\mathrm{C}$ inelastic and production cross sections are 257.2 $\pm$ 1.9 $\pm$ 8.9 and 229.3 $\pm$ 1.9 $\pm$ 9.0 mb, respectively. Inclusive production cross sections for negatively and positively charged pions are presented as functions of laboratory momentum in ten intervals of the laboratory polar angle covering the range from 0 up to 420 mrad. The spectra are compared with predictions of several hadron production models.

Measurements of inclusive spectra and mean multiplicities of [equation], K[equation], p and [equation]produced in inelastic p + p interactions at incident projectile momenta of 20, 31, 40, 80 and...

Results on $\Lambda ,\overline{\Lambda },{\Xi }^{-}$, and ${\overline{\Xi }}^{+}$ production in central $\mathrm{Pb}+\mathrm{Pb}$ reactions at $20A,30A,40A,80A$, and 158$A$ GeV are presented. The energy dependence of transverse mass spectra, rapidity spectra, and multiplicities is discussed. Comparisons to string hadronic models (UrQMD and HSD) and statistical hadron gas models are shown. Although the latter provide a reasonable description of all particle yields, the first class of models fails to match the ${\Xi }^{-}$ and ${\overline{\Xi }}^{+}$ multiplicities.