Baryon and meson species.

Within the UrQMD approach [3] we can tabulate properties of the $55$ different baryon species and $32$ different meson species, which are supplemented by their anti-particle and all isospin-projected states. The full baryon-antibaryon symmetry can be included. The $J^P = \frac{1}{2}^+, \frac{3}{2}^+$ baryon and baryon resonance states as well as the $J^{PC}$ meson and meson resonance states are listed below, where $J$, $P$ and $C$ denote a spin, a parity and a charge conjugation, respectively.

Table 2.1: Baryons and baryon resonances.

nucleon	delta	lambda	sigma	xi	omega
$N_{938}$	$\Delta_{1232}$	$\Lambda_{1116}$	$\Sigma_{1192}$	$\Xi_{1315}$	$\Omega_{1672}$
$N_{1440}$	$\Delta_{1600}$	$\Lambda_{1405}$	$\Sigma_{1385}$	$\Xi_{1530}$
$N_{1520}$	$\Delta_{1620}$	$\Lambda_{1520}$	$\Sigma_{1660}$	$\Xi_{1690}$
$N_{1535}$	$\Delta_{1700}$	$\Lambda_{1600}$	$\Sigma_{1670}$	$\Xi_{1820}$
$N_{1650}$	$\Delta_{1900}$	$\Lambda_{1670}$	$\Sigma_{1750}$	$\Xi_{1950}$
$N_{1675}$	$\Delta_{1905}$	$\Lambda_{1690}$	$\Sigma_{1775}$	$\Xi_{2030}$
$N_{1680}$	$\Delta_{1910}$	$\Lambda_{1800}$	$\Sigma_{1915}$
$N_{1700}$	$\Delta_{1920}$	$\Lambda_{1810}$	$\Sigma_{1940}$
$N_{1710}$	$\Delta_{1930}$	$\Lambda_{1820}$	$\Sigma_{2030}$
$N_{1720}$	$\Delta_{1950}$	$\Lambda_{1830}$
$N_{1900}$		$\Lambda_{1890}$
$N_{1990}$		$\Lambda_{2100}$
$N_{2080}$		$\Lambda_{2110}$
$N_{2190}$
$N_{2200}$
$N_{2250}$

Table 2.2: Meson and meson resonance states.

$0^{-+}$	$1^{--}$	$0^{++}$	$1^{++}$	$1^{+-}$	$2^{++}$	$(1^{--})^*$	$(1^{--})^{**}$
$\pi$	$\rho$	$a_0$	$a_1$	$b_1$	$a_2$	$\rho_{1450}$	$\rho_{1700}$
$K$	$K^*$	$K_0^*$	$K_1^*$	$K_1$	$K_2^*$	$K^*_{1410}$	$K^*_{1680}$
$\eta$	$\omega$	$f_0$	$f_1$	$h_1$	$f_2$	$\omega_{1420}$	$\omega_{1662}$
$\eta'$	$\phi$	$f_0^*$	$f_1'$	$h_1'$	$f_2'$	$\phi_{1680}$	$\phi_{1900}$