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config_Au_Elab1_23_no_spect_vtk_out.yaml
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config_Au_Elab1_23_no_spect_vtk_out.yaml
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# SMASH-2.0.2-201-gfbf84ebd
# Branch : gabriele-inghirami/thermodyn_out_for_spectators
# System : Linux-5.11.0-34-generic
# Compiler : GNU 9.3.0
# Build : Release
# Date : 2021-09-15T15:32:20
Version: 1.8
Logging:
{}
General:
Modus: Collider
Time_Step_Mode: Fixed
Delta_Time: 0.1
End_Time: 11.01
Randomseed: 1815587767021602092
Nevents: 1080
Lattice:
Origin: [-14.5, -14.5, -14.5]
Sizes: [29.0, 29.0, 29.0]
Cell_Number: [29, 29, 29]
Periodic: False
Potentials_Affect_Thresholds: False
Output:
Output_Interval: 1.0
Thermodynamics:
Format: [VTK]
Type: hadron
Quantities: [tmn_landau]
Modi:
Collider:
Projectile:
Particles: {2212: 79, 2112: 118}
Target:
Particles: {2212: 79, 2112: 118}
E_Kin: 1.23
Fermi_Motion: frozen
Impact:
Sample: quadratic
Range: [0, 3.3]
particles: "# NAME MASS[GEV] WIDTH[GEV] PARITY PDG\n########## unflavored mesons ##########\nπ 0.138 7.7e-9 - 111 211\nη 0.548 1.31e-6 - 221\nσ 0.800 0.400 + 9000221\nρ 0.776 0.149 - 113 213 # mass required by EOS code\nω 0.783 8.49e-3 - 223\nη' 0.958 1.96e-4 - 331\nf₀(980) 0.990 0.060 + 9010221\na₀(980) 0.989 0.075 + 9000111 9000211 # should be heavy enough for KK\n#^ The pole mass was increased to be heavy enough for the KK decay, like in UrQMD.\nφ 1.019 4.25e-3 - 333\nh₁(1170) 1.170 0.360 + 10223\nb₁(1235) 1.2295 0.142 + 10113 10213\na₁(1260) 1.23 0.42 + 20113 20213\nf₂ 1.276 0.187 + 225\nf₁(1285) 1.2819 0.0227 + 20223\nη(1295) 1.294 0.055 - 100221\nπ(1300) 1.30 0.4 - 100111 100211\na₂(1320) 1.3183 0.107 + 115 215\nf₀(1370) 1.35 0.35 + 10221\nπ₁(1400) 1.354 0.33 - 9000113 9000213\nη(1405) 1.409 0.051 - 9020221\nf₁(1420) 1.4264 0.054 + 20333\nω(1420) 1.425 0.215 - 100223\na₀(1450) 1.474 0.265 + 10111 10211\nρ(1450) 1.465 0.400 - 100113 100213\nη(1475) 1.476 0.085 - 100331\nf₀(1500) 1.507 0.109 + 9030221 # should be heavy enough for ηη'\nf₂'(1525) 1.525 0.073 + 335\nπ₁(1600) 1.662 0.24 - 9010113 9010213\nη₂(1645) 1.617 0.181 - 10225\nω(1650) 1.670 0.315 - 30223\nω₃(1670) 1.667 0.168 - 227\nπ₂(1670) 1.672 0.260 - 10115 10215\nφ(1680) 1.680 0.15 - 100333\nρ₃(1690) 1.689 0.161 - 117 217\nρ(1700) 1.720 0.25 - 30113 30213\nf₀(1710) 1.723 0.139 + 10331\nπ(1800) 1.812 0.208 - 9010111 9010211\nφ₃(1850) 1.854 0.087 - 337\n#π₂(1880) # no PDG code\nf₂(1950) 1.944 0.472 + 9050225\nf₂(2010) 2.010 0.20 + 9060225\na₄(2040) 1.995 0.257 + 119 219\nf₄(2050) 2.018 0.237 + 229\n#φ(2170) # no PDG code\nf₂(2300) 2.297 0.15 + 9080225\nf₂(2340) 2.350 0.32 + 9090225\n########## strange mesons ##############\nK 0.494 0 - 311 321\n#K*₀(700) 0.824 0.480 + 9000311 9000321 # no known decays\nK*(892) 0.892 0.050 - 313 323\nK₁(1270) 1.272 0.090 + 10313 10323\nK₁(1400) 1.403 0.174 + 20313 20323\nK*(1410) 1.421 0.236 - 100313 100323\nK*₀(1430) 1.453 0.27 + 10311 10321 # should be heavy enough for Kη'\nK*₂(1430) 1.429 0.104 + 315 325 # PDG masses and widths averaged\nK*(1680) 1.718 0.320 - 30313 30323\nK₂(1770) 1.773 0.186 - 10315 10325\nK*₃(1780) 1.776 0.159 - 317 327\nK₂(1820) 1.819 0.264 - 20315 20325\nK*₄(2045) 2.045 0.198 + 319 329\n########## N baryons ###################\nN 0.938 0 + 2112 2212\nN(1440) 1.440 0.350 + 12112 12212\nN(1520) 1.515 0.110 - 1214 2124\nN(1535) 1.530 0.150 - 22112 22212\nN(1650) 1.650 0.125 - 32112 32212\nN(1675) 1.675 0.145 - 2116 2216\nN(1680) 1.685 0.120 + 12116 12216\nN(1700) 1.720 0.200 - 21214 22124\nN(1710) 1.710 0.140 + 42112 42212\nN(1720) 1.720 0.250 + 31214 32124\nN(1875) 1.875 0.250 - 9902114 9902214\nN(1880) 1.880 0.400 + 9952112 9952212\nN(1895) 1.895 0.120 - 9962112 9962212\nN(1900) 1.900 0.200 + 9912114 9912214\nN(1990) 1.990 0.500 + 9902118 9902218\nN(2060) 2.100 0.400 - 9922116 9922216\nN(2080) 2.000 0.350 + 9922114 9922214\nN(2100) 2.100 0.260 + 9972112 9972212\nN(2120) 2.120 0.300 - 9932114 9932214\nN(2190) 2.180 0.400 - 1218 2128\nN(2220) 2.220 0.400 + 19922119 19922219\nN(2250) 2.250 0.470 - 19932119 19932219\n########## Δ baryons ###################\nΔ 1.232 0.117 + 1114 2114 2214 2224\n#Δ(1600) 1.570 0.250 + 31114 32114 32214 32224\n#^ this results in overshooting the pi+p cross section\nΔ(1620) 1.610 0.130 - 1112 1212 2122 2222\nΔ(1700) 1.710 0.300 - 11114 12114 12214 12224\nΔ(1900) 1.860 0.250 - 11112 11212 12122 12222\nΔ(1905) 1.880 0.330 + 1116 1216 2126 2226\nΔ(1910) 1.900 0.300 + 21112 21212 22122 22222\nΔ(1920) 1.920 0.300 + 21114 22114 22214 22224\nΔ(1930) 1.950 0.300 - 11116 11216 12126 12226\nΔ(1950) 1.930 0.280 + 1118 2118 2218 2228\n# TODO(steinberg): Δ(2420)\n########## Λ baryons ###################\nΛ 1.116 0 + 3122\nΛ(1405) 1.405 0.0505 - 13122\nΛ(1520) 1.520 0.0156 - 3124\nΛ(1600) 1.600 0.1500 + 23122\nΛ(1670) 1.670 0.0350 - 33122\nΛ(1690) 1.690 0.0600 - 13124\nΛ(1800) 1.800 0.3000 - 43122\nΛ(1810) 1.810 0.1500 + 53122\nΛ(1820) 1.820 0.0800 + 3126\nΛ(1830) 1.830 0.0950 - 13126\nΛ(1890) 1.890 0.1000 + 23124\nΛ(2100) 2.100 0.2000 - 3128\nΛ(2110) 2.110 0.2000 + 23126\nΛ(2350) 2.350 0.1500 + 19903129\n########## Σ baryons ###################\nΣ 1.189 0 + 3112 3212 3222\nΣ(1385) 1.385 0.036 + 3114 3214 3224\nΣ(1660) 1.660 0.100 + 13112 13212 13222\nΣ(1670) 1.670 0.060 - 13114 13214 13224\nΣ(1750) 1.750 0.090 - 23112 23212 23222\nΣ(1775) 1.775 0.120 - 3116 3216 3226\nΣ(1915) 1.915 0.120 + 13116 13216 13226\nΣ(1940) 1.940 0.220 - 23114 23214 23224\nΣ(2030) 2.030 0.180 + 3118 3218 3228\nΣ(2250) 2.250 0.100 + 9903118 9903218 9903228\n#^ spin and parity unknown, guessed to be 7/2+\n########## Ξ baryons ###################\nΞ 1.318 0 + 3312 3322\nΞ(1530) 1.533 0.009 + 3314 3324\nΞ(1690) 1.690 0.030 + 203312 203322 # width < 30 MeV\nΞ(1820) 1.823 0.024 - 13314 13324\nΞ(1950) 1.950 0.060 + 103316 103326\nΞ(2030) 2.025 0.020 + 203316 203326\n########## Ω baryons ###################\nΩ⁻ 1.672 0 + 3334\nΩ(2250)⁻ 2.252 0.055 + 203338\n########## non-hadrons (leptons & gauge bosons) ##########\ne⁻ 0.000511 0 + 11\nμ⁻ 0.105 0 + 13\nτ⁻ 1776.86 0 + 15\nγ 0 0 + 22\n########## light nuclei #########\n# These are normally represented by neutrons and protons\n# and should be uncommented only for specific studies\n# d 1.8756 0 + 1000010020\n# Fake dibaryon resonance\n# introduced to describe Xd <-> Xnp reactions via Xd <-> Xd' <->Xnp\n# d' 1.8856 0.100 - 1000010021\n########## hadrons needed for Pythia #########################\n########## (no cross sections and decay widths yet) ##########\nD 1.86 0 - 421 411\nD*(2007) 2.0 0 - 423 413\nD₀*(2400) 2.318 0 + 10421 10411 #PDG width 0.27\nD₁(2420) 2.4214 0 + 10413 10423 #PDG width 0.0274\nD₂*(2460) 2.4626 0 + 425 415 #PDG width 0.049\nD₁(2430) 2.427 0 + 20413 20423 #pythia width 0.384\nDs 1.9683 0 - 431\nDs* 2.1121 0 + 433\nDs0*(2317) 2.3177 0 + 10431\nDs1(2460) 2.4595 0 + 20433\nDs1(2536) 2.53511 0 + 10433\nDs2*(2573) 2.5719 0 + 435 #PDG width 0.017\nB 5.28 0 - 521 511\nB* 5.3193 0 - 513 523\nB₀* 5.68 0 + 10521 10511 #pythia width 0.05\nB₂*(5747) 5.822 0 + 515 525 #PDG width 0.022\nB₁ 5.73 0 + 10523 10513 #pythia width 0.05\nB₁* 5.78 0 + 20523 20513 #pythia width 0.05\nBs 5.36681 0 - 531\nBs0* 5.92 0 + 10531 #pythia width 0.05\nBs* 5.4154 0 - 533\nBs1 5.8286 0 + 10533 #PDG width 0.27\nBs1* 6.02 0 + 20533 #pythia width 0.05\nBs2*(5840) 5.83987 0 + 535 #PDG width 0.00147\nBc 6.2751 0 - 541\nBc0* 7.25 0 + 10541 #pythia width 0.05\nBc* 6.34 0 + 543 #from Pythia\nBc1 7.3 0 + 10543 #Pythia width 0.05\nBc1* 7.3 0 + 20543 #Pythia width 0.05\nBc2* 7.35 0 + 545 #Pythia width 0.02\nηc(1S) 2.9836 0 - 441 #PDG width 0.0318\nJ/Ψ 3.097 0 - 443\nχc0 3.41475 0 + 10441 #PDG width 0.0105\nχc1 3.51066 0 + 20443\nhc 3.52538 0 + 10443\nχc2 3.5562 0 - 445 #PDG width 0.00193\nηc(2S) 3.6392 0 - 100441 #PDG width 0.0113\nΨ(2S) 3.6861 0 - 100443\nΨ(3770) 3.77315 0 - 30443 #PDG width 0.0272\nΥ(1S) 9.46030 0 - 553\nηb(1S) 9.4 0 - 551 #PDG width 0.0023\nχb0 9.8594 0 + 10551\nχb1 9.8928 0 + 20553\nhb 9.8993 0 + 10553\nχb2 9.9122 0 + 555\nΥ(2S) 10.023 0 - 100553\nΥ(3S) 10.3552 0 - 200553\nΛc 2.28646 0 + 4122\nΛc(2595) 2.59225 0 - 14122 #PDG width 0.0026\nΣc(2455) 2.45 0 + 4112 4212 4222 #PDG width 0.00183\nΣc(2520) 2.52 0 + 4114 4214 4224 #PDG width 0.0153\nΞc 2.47 0 + 4232 4132\nΞc' 2.58 0 + 4322 4312\nΞc(2645) 2.6459 0 + 4314 4324\nΞcc 3.59798 0 + 4412 4422\nΞcc* 3.65648 0 + 4414 4424\nΩc 2.6952 0 + 4332\nΩc(2770) 2.7659 0 + 4334\nΩcc 3.78663 0 + 4432\nΩcc* 3.82466 0 + 4434\nΩccc 4.91594 0 + 4444\nΛb 5.61951 0 + 5122\nΣb 5.81 0 + 5112 5222 5212 #PDG width 0.0049\nΣb* 5.83 0 + 5114 5224 5214 #PDG width 0.0075\nΞb 5.79 0 + 5232 5132\nΞb' 5.96 0 + 5322 5312\nΞb* 5.97 0 + 5324 5314\nΞbc 7.00575 0 + 5242 5142\nΞbc' 7.03724 0 + 5422 5412\nΞbc* 7.04850 0 + 5424 5414\nΞbb 10.4227 0 + 5522 5512\nΞbb* 10.4414 0 + 5524 5514\nΩb 6.0480 0 + 5332\nΩb* 6.13 0 + 5334\nΩbc 7.19099 0 + 5342\nΩbc' 7.21101 0 + 5432\nΩbc* 7.219 0 + 5434\nΩbcc 8.30945 0 + 5442\nΩbcc* 8.31325 0 + 5444\nΩbb 10.6021 0 + 5532\nΩbb* 10.6143 0 + 5534\nΩbbc 11.7077 0 + 5542\nΩbbc* 11.7115 0 + 5544\nΩbbb 15.1106 0 + 5554\n"
decaymodes: "# Format of this file:\n# anything after a # is a comment and will be ignored\n# The decays for a given particle are given as:\n# <name of decaying particle>\n# <branching ratio> <angular momentum L> <names of decay products>\n# <branching ratio> <angular momentum L> <names of decay products>\n# ...\n#################### non-strange mesons ####################\nπ\n0.98823 1 γ γ\n# 0.01174 0 e⁻ e⁺ γ\nη\n0.394 1 γ γ # 39.41 +- 0.20 %\n0.327 0 π⁰ π⁰ π⁰ # 32.68 +- 0.23 %\n0.229 0 π⁺ π⁻ π⁰ # 22.92 +- 0.28 %\n0.042 1 π⁺ π⁻ γ # 4.22 +- 0.08 %\n# 6.9e-3 0 e⁻ e⁺ γ\nσ\n1. 0 π π\nρ\n1. 1 π π\n# 4.72e-5 0 e⁻ e⁺\n# 4.55e-5 0 μ⁻ μ⁺\nω\n0.892 1 π ρ\n0.0840 0 π⁰ γ\n0.0153 1 π π\n# 7.36e-5 0 e⁻ e⁺\n# 7.4e-5 0 μ⁻ μ⁺\n# 7.7e-4 1 e⁻ e⁺ π⁰\nη'\n0.654 0 σ η # 42.6 +- 0.7 + 22.8 +- 0.8 %\n0.289 0 ρ⁰ γ # 28.9 +- 0.5 %\n0.0262 0 ω γ # 2.62 +- 0.13 %\n0.0222 1 γ γ # 2.22 +- 0.08 %\n# 4.73e-4 0 e⁻ e⁺ γ # (4.73 +- 0.30)e-4\nf₀(980)\n0.70 0 π π # dominant\n0.30 0 K K̅ # >0\n#^ taken from UrQMD\n#0.01 0 γ γ # >0\na₀(980)\n0.86 0 π η # dominant\n0.14 0 K K̅ # >0\n#^ similar to UrQMD, optimized for f₁(1285) decay branching ratios\n#0.01 1 γ γ # >0\nφ\n0.492 1 K⁺ K̅⁻ # 49.2 +- 0.5 %\n0.340 1 K⁰ K̅⁰ # 34.0 +- 0.4 %\n0.152 1 π ρ # 15.24 +- 0.33 %\n0.013 0 η γ # 1.303 +- 0.025 %\n0.00127 0 π⁰ γ # (1.30 +- 0.05)e-3\n# 2.97e-4 0 e⁻ e⁺\n# 2.86e-4 0 μ⁻ μ⁺\n# 1.08e-4 1 e⁻ e⁺ η\n# 1.33e-5 1 e⁻ e⁺ π⁰\nh₁(1170)\n1. 0 π ρ # >0\nb₁(1235)\n0.90 0 ω π # dominant\n0.10 0 η ρ # >0\n#^ taken from UrQMD\n#0.01 0 φ π # >0\n# PDG has a few other exotic looking channels\na₁(1260)\n1. 0 π ρ # >0\n#^ taken from UrQMD\n#1. 2 π ρ # >0\n#1. 0 π ρ(1450) # >0\n#1. 2 π ρ(1450) # >0\n#1. 1 π σ # >0\n#1. 1 π f0(980) # >0\n#1. 1 π f0(1370) # >0\n#1. 1 π f2 # >0\n#1. 0 K K̅*(892) # >0\n#1. 0 K̅ K*(892) # >0\n#1. 0 π γ # >0\nf₂\n0.50 2 π π # PDG value: 0.842 (modified to better fit the π⁺π⁻ cross section)\n0.45 2 ρ ρ # to emulate 4π (whose PDG value is 0.108)\n0.05 2 K K̅\nf₁(1285)\n0.335 2 ρ ρ # 0.335 +- 0.02 % for ππππ\n0.520 1 η σ # 0.35 +- 0.15 % for ηπ+ π-, 52.0 +- 0.02 % for ηππ\n0.091 1 π a₀(980) # emulating ηππ and KK̅π\nη(1295)\n1. 0 π a₀(980) # >0, emulating ηππ\n# not in UrQMD\nπ(1300)\n1. 1 π ρ # >0\n# not in UrQMD\na₂(1320)\n0.701 2 π ρ # 0.701 +- 0.027\n0.145 2 π η # 0.145 +- 0.012\n0.106 0 ω ρ # 0.106 +- 0.032\n0.049 2 K K̅ # 0.049 +- 0.008\n#5.5e-3 0 π η' # (5.5 +- 0.9)e-3\n# rest is < 1e-5\nf₀(1370)\n0.70 0 ρ ρ # >0, dominant\n0.20 0 K K̅ # >0\n0.10 0 π π # >0\nπ₁(1400)\n1. 1 π η # >0\nη(1405)\n0.50 0 π a₀(980) # >0\n0.30 1 ρ ρ # >0, <0.58\n0.10 0 η f₀(980) # >0\n0.10 1 K*(892) K̅ # >0\nf₁(1420)\n1. 1 π a₀(980) # >0, emulating ηππ and KK̅π\n#^ according to PDG, KK̅π is mostly from KK̅*(892)\nω(1420)\n1. 1 π ρ # dominant\n#^ taken from UrQMD\n#0.??? ? ω ρ # >0\n#0.??? ? π b₁(1235) # >0\na₀(1450)\n0.093 0 π η # 0.093 +- 0.020\n0.033 0 π η' # 0.033 +- 0.017\n0.082 0 K K̅ # 0.082 +- 0.028\n1.000 0 ω ρ # defined as 1\n# not in UrQMD\nρ(1450)\n0.10 1 π π # >0\n0.70 1 ρ ρ # >0\n0.10 1 ρ η # >0\n#^ modified to match π⁺π⁻ cross section\n0.10 1 K K̅ # >0\nη(1475)\n1. 0 π a₀(980) # >0, emulating ηππ and KK̅π\n# not in UrQMD\nf₀(1500)\n0.349 0 π π # 0.349 +- 0.023\n0.495 0 ρ ρ # 0.495 +- 0.033\n0.051 0 η η # 0.051 +- 0.009\n0.019 0 η η' # 0.019 +- 0.008\n0.086 0 K K̅ # 0.086 +- 0.010\nf₂'(1525)\n0.887 2 K K̅ # 0.887 +- 0.022\n0.104 2 η η # 0.104 +- 0.022\n8.2e-3 2 π π # (8.2 +- 1.5)e-3\nπ₁(1600)\n0.333 0 π b₁(1235) # >0\n0.333 1 π η' # >0\n0.333 0 π f₁(1285) # >0\nη₂(1645)\n0.25 0 π a₂(1320) # >0\n0.25 1 K̅ K*(892) # >0\n0.25 2 π a₀(980) # >0\n0.25 2 σ η # >0\nω(1650)\n0.50 1 ρ π # >0\n0.50 0 σ ω # >0\n#^ taken from UrQMD ω(1600)\n#0.333 1 η ω # >0\nω₃(1670)\n0.50 3 ρ π # >0\n0.50 2 σ ω # >0\nπ₂(1670)\n0.563 0 π f₂ # 0.563 +- 0.032\n0.3535 1 π ρ # 0.31 +- 0.04\n0.1525 2 π σ # 0.109 +- 0.034\n#0.087 0 π π π # 0.087 +- 0.034\n0.21 1 K K̅*(892) # | 0.043 +- 0.014\n0.21 1 K̅ K*(892) # |\n0.027 1 ρ ω # 0.027 +- 0.011\nφ(1680)\n0.40 1 K K̅*(892) # | dominant\n0.40 1 K̅ K*(892) # |\n0.10 1 K K̅ # >0\n0.05 0 σ ω # >0\n0.05 1 φ η # >0\nρ₃(1690)\n0.5502 1 ρ ρ # 0.67 +- 0.22\n0.16 1 ρ ω # 0.16 +- 0.06\n0.236 3 π π # 0.236 +- 0.013\n0.038 3 K̅ K*(892) # 0.038 +- 0.012\n0.0158 3 K̅ K # 0.0158 +- 0.0026\n# more have been seen\nρ(1700)\n0.80 1 ρ ρ # dominant\n0.20 1 π π # large\n#^ taken from UrQMD\n# more have been seen\nf₀(1710)\n0.25 0 K̅ K # >0\n0.25 0 η η # >0\n0.25 0 π π # >0\n0.25 0 ω ω # >0\nπ(1800)\n0.166 0 π σ # >0\n0.2 0 π f₀(980) # >0\n0.2 0 π f₀(1370) # >0\n0.2 0 η a₀(980) # >0\n0.2 0 π f₀(1500) # >0\n0.1 0 K K̅*₀(1430) # | >0\n0.1 0 K̅ K*₀(1430) # |\nφ₃(1850)\n0.50 3 K̅ K # >0\n0.25 3 K K̅*(892) # | >0\n0.25 3 K̅ K*(892) # |\nf₂(1950)\n0.2 0 K*(892) K̅*(892) # >0\n0.2 0 ρ ρ # >0\n0.2 2 η η # >0\n0.2 2 K̅ K # >0\n#0.2 0 N̅ N # >0\nf₂(2010)\n0.5 0 φ φ # >0\n0.5 2 K̅ K # >0\na₄(2040)\n0.125 4 K̅ K # >0\n0.125 4 π ρ # >0\n0.125 3 π f₂ # >0\n0.125 2 ω ρ # >0\n0.125 4 π η # >0\n0.125 4 π η' # >0\nf₄(2050)\n0.40 2 ω ω # >0\n0.17 4 π π # 0.170 +- 0.015\n0.01 4 K̅ K # (6.8 + 3.4 - 1.8)e-3\n0.002 4 η η # (2.1 +- 0.8)e-3\n0.01 2 ρ ρ # <0.012\n0.40 3 π a₂(1320) # >0\nf₂(2300)\n0.5 0 φ φ # >0\n0.5 2 K̅ K # >0\nf₂(2340)\n0.5 0 φ φ # >0\n0.5 2 η η # >0\n#################### strange mesons ####################\nK*(892)\n1.0 1 K π\n# other decays < 3e-3\nK₁(1270)\n0.42 0 K ρ # 0.42 +- 0.06\n0.28 1 K*₀(1430) π # 0.28 +- 0.04\n0.16 0 K*(892) π # 0.16 +- 0.05\n0.11 0 K ω # 0.11 +- 0.02\n0.03 1 K f₀(1370) # 0.03 +- 0.02\n#>0 ? γ K⁰\nK₁(1400)\n0.94 0 K*(892) π # 0.94 +- 6\n0.03 0 K ρ # 0.03 +- 0.03\n0.02 1 K f₀(1370) # 0.02 +- 0.02\n0.01 0 K ω # 0.01 +- 0.01\n#>0 ? γ K⁰\nK*(1410)\n0.8634 1 K*(892) π # >0.4\n0.066 1 K π # 6.6 +- 1.3 %\n0.07 1 K ρ # <0.07\n#>0 1 γ K⁰\nK*₀(1430)\n0.92 0 K π # 0.93 +- 0.10\n0.07 0 K η # 0.086 + 0.027 - 0.034\n0.01 0 K η' # >0\nK*₂(1430)\n0.499 2 K π # 0.499 +- 0.012\n0.247 2 K*(892) π # 0.247 +- 0.015\n0.143 2 K*(892) ρ # 0.134 +- 0.022 # m_a + m_b = 1.668\n0.087 2 K ρ # 0.087 +- 0.008\n0.029 2 K ω # 0.029 +- 0.008\n# More with branching ratio < 3e-3\nK*(1680)\n0.387 1 K π # 0.387 +- 0.025\n0.314 1 K ρ # 0.314 + 0.050 - 0.021\n0.299 1 K*(892) π # 0.299 + 0.022 - 0.050\nK₂(1770)\n1. 0 K*₂(1430) π # dominant\n# others have been seen\nK*₃(1780)\n0.31 3 K ρ # 0.31 +- 0.09\n0.20 3 K*(892) π # 0.20 +- 0.05\n0.188 3 K π # 0.188 +- 0.010\n0.30 3 K η # 0.30 +- 0.13\n0.16 2 K*₂(1430) π # <0.16\nK₂(1820)\n0.25 0 K*₂(1430) π # >0\n0.25 1 K*(892) π # >0\n0.25 0 K f₂ # >0\n0.25 1 K ω # >0\nK*₄(2045)\n0.099 4 K π # 0.099 +- 0.012\n0.147 2 K*(892) ρ # (0.09 +- 0.05) + (0.057 +- 0.032), should be K*ππ + ρKπ\n0.120 2 K*(892) ω # (0.07 +- 0.05) + (0.05 +- 0.03), should be K*πππ + ωKπ\n0.042 2 K*(892) φ # (0.028 +- 0.014) + (0.014 +- 0.007), should φKπ + φK*\n#################### N baryons ####################\nN(1440)\n0.60 1 N π # 55 - 75 %\n#0.00 0 N η # < 1 %\n0.24 1 Δ π # 6 - 27 %\n0.16 0 N σ # 11 - 23 %\nN(1520)\n0.65 2 N π # 55 - 65 %\n0.15 0 Δ π # 15 - 23 %\n0.07 2 Δ π # 7 - 11 %\n0.11 0 N ρ # serves as proxy for N(1520) dilepton Dalitz decay\n0.02 1 N σ # < 2 %\nN(1535)\n0.38 0 N π # 35 - 52 %\n0.52 0 N η # 32 - 55 %\n0.06 0 N(1440) π # 5 - 12 %\n0.02 2 Δ π # 1 - 4 %\n0.02 1 N σ # 2 - 10 %\nN(1650)\n0.51 0 N π # 50 - 70 %\n0.20 0 N η # 15 - 35 %\n0.04 0 Λ K # 5 - 15 %, HADES PWA 7 ± 4 %, tuned for Nπ->ΛK\n0.10 2 Δ π # 6 - 18 %\n0.04 1 N σ # 2 - 18 %\n0.11 0 N(1440) π # 6 - 26 %\nN(1675)\n0.42 2 N π # 38 - 42 %, tuned for πN cross section\n0.01 2 N η # < 1 %\n0.48 2 Δ π # 23 - 37 %\n0.08 3 N σ # 3 - 7 %\nN(1680)\n0.60 3 N π # 60 - 70 %, tuned for πN cross section\n0.01 3 N η # < 1 %\n0.19 2 N σ # 9 - 19 %\n0.09 1 Δ π # 4 - 10 %\n0.11 3 Δ π # 7 - 13 %\nN(1700)\n0.10 2 N π # 7 - 17 %\n0.71 0 Δ π # 50 - 80 %\n0.11 2 Δ π # 4 - 14 %\n0.07 2 N(1440) π # 3 - 11 %\n0.04 1 N(1520) π # < 4 %\nN(1710)\n0.25 1 N π # 5 - 20 %, tuned for Nπ->ΣK\n0.32 1 N η # 10 - 50 %\n0.01 1 N ω # 1 - 5 %, tuned for pp dileptons\n0.13 1 Λ K # 5 - 25 %, HADES PWA 15 ± 10 %, tuned for Nπ->ΛK\n0.01 1 Σ K # > 0, tuned for Nπ->ΣK and NN->ΣK\n0.16 1 Δ π # > 0\n0.12 0 N(1535) π # 9 - 21 %\nN(1720)\n0.15 1 N π # 8 - 14 %\n0.03 1 N η # 1 - 5 %\n0.12 1 N ω # 12 - 40 %, tuned for pp dileptons\n0.05 1 Λ K # 4 - 5 %, HADES PWA 8 ± 7 %, tuned for Nπ->ΛK\n0.44 1 Δ π # 47 - 77 %\n0.09 3 Δ π # < 12 %\n0.08 2 N σ # 2 - 14 %\n0.01 1 N ρ # 1 - 2 %, KSU value used\n0.01 1 N(1440) π # < 2 %\n0.02 0 N(1520) π # 1 - 5 %\nN(1875)\n0.03 2 N π # 3 - 11 %\n0.01 2 N η # < 1 %\n0.15 0 N ω # 15 - 25 %, tuned for pp dileptons\n0.04 2 Σ K # > 0, tuned for Nπ->ΣK and NN->ΣK\n0.05 2 Σ K*(892) # for slower kaons and Sigmas\n0.04 2 Λ K # > 0, HADES PWA 4 ± 2 %, tuned for Nπ->ΛK\n0.02 2 Λ K*(892) # for slower kaons and Lambdas\n0.13 0 Δ π # 7 - 21 %\n0.10 2 Δ π # 2 - 12 %\n0.03 0 N ρ # > 0\n0.32 1 N σ # 30 - 60 %\n0.04 2 N(1440) π # 2 - 8 %\n0.01 1 N(1520) π # < 2 %\nN(1880)\n0.03 1 N π # 3 - 9 %\n0.21 1 N η # 5 - 55 %\n0.12 1 N ω # 12 - 28 %, tuned for pp dileptons\n0.02 1 Λ K # 12 - 28 %, HADES PWA 2 ± 1 %\n0.10 1 Σ K # 10 - 24 %\n0.23 1 Δ π # 18 - 42 %\n0.19 0 N σ # 10 - 40 %\n0.07 0 N(1535) π # 4 - 12 %\n0.02 0 N a₀(980) # 1 - 5 %\n0.01 1 Λ K*(892) # 0.5 - 1 %\nN(1895)\n0.03 0 N π # 2 - 18 %\n0.20 0 N η # 15 - 40 %\n0.16 0 N η' # 10 - 40 %\n0.01 0 N ρ # > 0\n0.03 2 N ρ # 3 - 12 %\n0.01 1 N σ # > 0\n0.16 0 N ω # 16 - 40 %, tuned for pp dileptons\n0.18 0 Λ K # 13 - 23 %, HADES PWA 18 ± 5 %\n0.11 0 Σ K # 10 - 24 %\n0.03 2 Δ π # 3 - 11 %\n0.04 0 N(1440) π # 4 - 12 %\n0.04 0 Λ K*(892) # 4 - 9 %\nN(1900)\n0.04 1 N π # 1 - 20 %\n0.12 1 N η # 2 - 14 %\n0.04 1 N η' # 4 - 8 %\n0.10 1 N ω # 7 - 13 %\n0.02 1 Λ K # 2 - 20 %, HADES PWA 5 ± 5\n0.01 1 Λ K*(892) # for slower kaons and Lambdas\n0.03 1 Σ K # 3 - 7 %, tuned for NN->ΣK\n0.01 1 Σ K*(892) # for slower kaons and Sigmas\n0.10 1 Δ π # 9 - 25 %\n0.24 3 Δ π # 21 - 45 %\n0.05 2 N σ # 1 - 7 %\n0.16 0 N(1520) π # 7 - 23 %\n0.08 2 N(1535) π # 4 - 10 %\nN(1990)\n0.12 3 N π # tuned for p π-\n0.20 3 N ρ # BR lowered to improve pp --> pp ρ cross section, shifted to N σ\n0.15 3 Δ π\n0.05 3 N(1440) π\n0.03 3 Λ K # tuned for Nπ->ΛK\n0.03 3 Λ K*(892) # for slower kaons and Lambdas\n0.03 3 Σ K # tuned for Nπ->ΛK\n0.03 3 Σ K*(892) # for slower kaons and Sigmas\n0.36 4 N σ # σ and ππ combined\n# From UrQMD, not yet confirmed by PDG\n# FIXME The UrQMD papers are ambigious whether this state produces φ\nN(2060)\n0.07 2 N π # 7 - 12 %\n0.05 2 N η # 2 - 6 %\n0.06 2 N ω # 1 - 7 %\n0.01 2 Λ K # > 0\n0.04 2 Σ K # 1 - 5 %\n0.10 2 Δ π # 4 - 10 %\n0.01 2 N ρ # > 0\n0.01 2 Λ K*(892) # 0.3-1.3 %\n0.09 3 N σ # 3 - 9 %\n0.14 2 N(1440) π # 4 - 14 %\n0.20 1 N(1520) π # 9 - 21 %\n0.22 0 N(1680) π # 8 - 22 %\nN(2080)\n0.32 1 N π # tuned for Nπ cross section\n0.04 1 N η\n0.07 1 N ω # modified relative to UrQMD to better fit\n0.20 1 N ρ # the dilepton spectra\n0.05 2 N σ\n0.10 2 N(1535) ρ\n0.10 1 Δ π\n0.005 1 Λ K # tuned for Nπ->ΛK\n0.010 1 N φ # tuned for p Nb dileptons and pp -> ppKK\n0.001 2 N f₀(980) # tuned for pp -> ppKK\n# From UrQMD, not yet confirmed by PDG\n# Crucial for pi- p cross section\nN(2100)\n0.08 1 N π # 8 - 18 %\n0.05 1 N η # > 0\n0.05 1 N η' # 5 - 11 %\n0.13 1 N ω # 10 - 25 %\n0.01 1 Λ K # > 0\n0.09 1 Δ π # 6 - 14 % | 20 - 40 % for N π π\n0.10 1 N ρ # > 0 |\n0.11 1 Λ K*(892) # 3 - 11 %, for slower kaons and Lambdas\n0.15 0 N σ # 14 - 26 %\n0.23 2 N(1520) π # 16 - 34 %\n0.010 1 N φ # tuned for p Nb dileptons and pp -> ppKK\nN(2120)\n0.05 2 N π # 5 - 15 %\n0.04 2 N η' # 2 - 6 %\n0.12 2 N ω # 4 - 20 %\n0.40 0 Δ π # 30 - 70 % | 50 - 95 % for N π π\n0.15 2 Δ π # 8 - 32 % |\n0.002 0 Λ K*(892) # < 0.2 %\n0.09 1 N σ # 7 - 15 %\n0.15 1 N(1535) π # 7 - 23 %\n0.010 2 N φ # tuned for p Nb dileptons and pp -> ppKK\nN(2190)\n0.116 4 N π # 10 - 20 %\n0.05 2 N ω # 8 - 20 %\n0.24 2 N ρ # > 0\n0.008 4 Λ K*(892) # 0.2 - 0.8 %\n0.09 3 N σ # 3 - 9 %\n0.335 2 Δ π # 19 - 31 %\n0.05 4 N(1440) π # 0\n0.10 3 N(1535) ρ # 0\n0.010 2 N φ # tuned for p Nb dileptons and pp -> ppKK\n0.001 3 N f₀(980) # tuned for pp -> ppKK\n# Similar to UrQMD\nN(2220)\n0.15 5 N π # 15 - 30 %\n0.22 3 N ρ\n0.17 4 N σ\n0.20 3 Δ π\n0.14 4 N(1535) ρ\n#0.000 5 Λ K # tuned for Nπ->ΛK\n# TODO: consider adding hyperon channels\n0.010 3 N φ # tuned for p Nb dileptons and pp -> ppKK\n0.001 4 N f₀(980) # tuned for pp -> ppKK\n# From UrQMD, confirmed by PDG\nN(2250)\n0.05 4 N π # 0.05 - 0.15\n0.25 4 N ρ\n0.20 5 N σ\n0.22 4 Δ π\n0.05 4 N(1440) π\n0.10 5 N(1535) ρ\n0.002 4 Λ K # tuned for Nπ->ΛK\n0.003 4 Λ K*(892) # for slower kaons and Lambdas\n0.010 4 N φ # tuned for p Nb dileptons and pp -> ppKK\n0.001 5 N f₀(980) # tuned for pp -> ppKK\n# From UrQMD, confirmed by PDG\n#N(2600)\n#0.10 ? N π # 3 - 8 %\n#################### Δ baryons ####################\nΔ\n1. 1 N π\n# 4.2e-5 1 e⁻ e⁺ N⁺\n# 4.2e-5 1 e⁻ e⁺ N⁰\n#Δ(1600)\n#0.175 1 N π # 0.08 - 0.24\n#0.825 1 Δ π # 0.72 - 0.82\n#0.000 3 Δ π # < 0.02\n#0.000 1 N(1440) π # 0.15 - 0.25\n#^ disabled, because it overshoots the pi+p cross section\nΔ(1620)\n0.30 0 N π # 25 - 35 %, tuned for Nπ\n0.53 2 Δ π # 52 - 72 %\n0.05 0 N ρ # > 0\n0.07 2 N ρ # > 0\n0.05 0 N(1440) π # 3 - 9 %\nΔ(1700)\n0.20 2 N π # 10 - 20 %, tuned for Nπ\n0.24 0 Δ π # 5 - 35 %\n0.16 2 Δ π # 4 - 16 %\n0.30 0 N ρ # > 0\n0.05 0 Δ η # 3 - 7 %\n0.04 1 N(1520) π # 1 - 5 %\n0.01 1 N(1535) π # 0.5 - 1.5 %\nΔ(1900)\n0.11 0 N π # 4 - 12 %\n0.01 0 Σ K # seen\n0.01 0 Σ K*(892) # for slower kaons and Lambdas\n0.35 2 Δ π # 30 - 70 %\n0.09 0 N ρ # 8 - 16 %\n0.20 2 N ρ # 18 - 28 %\n0.17 0 N(1440) π # 8 - 32 %\n0.05 1 N(1520) π # 2 - 10 %\n0.01 2 Δ η # 0 - 2 %\nΔ(1905)\n0.10 3 N π # 9 - 15 %, tuned for Nπ\n0.26 1 Δ π # 23 - 43 %\n0.50 3 Δ π # 56 - 72 %\n0.06 1 N ρ # seen, KSU value used\n0.02 1 Δ η # 2 - 6 %\n0.01 2 N(1535) π # < 1 %\n0.05 1 N(1680) π # 5 - 15 %\nΔ(1910)\n0.30 1 N π # 15 - 30 %, tuned for Nπ\n0.39 1 Δ π # 34 - 66 %\n0.04 1 Σ K # 4 - 14 %, tuned for Nπ->ΣK\n0.06 1 Σ K*(892) # for slower kaons and Sigmas\n0.09 1 N(1440) π # 3 - 9 %\n0.12 1 Δ η # 5 - 13 %\nΔ(1920)\n0.15 1 N π # 5 - 20 %\n0.03 1 Σ K # 2 - 6 %\n0.04 1 Σ K*(892) # for slower kaons and Sigmas\n0.12 1 Δ π # 8 - 28 %\n0.47 3 Δ π # 44 - 72 %\n0.03 1 N(1440) π # < 4 %\n0.04 0 N(1520) π # < 5 %\n0.01 2 N(1535) π # < 2 %\n0.01 2 N a₀(980) # > 0\n0.10 1 Δ η # 5 - 17 %\nΔ(1930)\n0.15 2 N π # 5 - 15 %, tuned for Nπ->ΣK\n0.42 2 Δ π\n0.37 2 N(1440) π\n0.04 2 Σ K # tuned for Nπ->ΣK, NN->ΣK\n0.02 2 Σ K*(892) # for slower kaons and Sigmas\n# From UrQMD\nΔ(1950)\n0.25 3 N π # 35 - 45 %, tuned for Nπ total cross section\n0.005 3 Σ K # 0.3 - 0.5 %, tuned for Nπ->ΣK, NN->ΣK\n0.005 3 Σ K*(892) # for slower kaons and Sigmas\n0.09 3 Δ π # 1 - 9 %\n0.55 3 N(1440) π # Introduced to fill up missing branching ratio\n0.09 1 N(1680) π # 3 - 9 %\n0.01 3 Δ η # < 0.6 %\n#################### Σ baryons ####################\nΣ(1385) # 1(1.5+)\n0.870 1 Λ π\n0.117 1 Σ π\n0.0125 0 Λ γ\n7.0e-3 0 Σ⁺ γ\n#2.4e-4 0 Σ⁻ γ # <2.4e-4\nΣ(1660) # 1(0.5+)\n0.35 1 N K̅ # 0.1-0.3\n0.15 1 Λ π # >0, tuned for K- n -> Lambda pi- cross section\n0.15 1 Σ π # >0, tuned for K- n -> Sigma- pi0 cross section\n0.15 1 Σ(1385) π # not measured\n0.20 2 Λ(1520) π # not measured\nΣ(1670) # 1(1.5-)\n0.15 2 N K̅ # 0.07-0.13\n0.18 2 Λ π # 0.05-0.15, tuned for K- n -> Lambda pi- cross section\n0.45 2 Σ π # 0.3-0.6, tuned for K- n -> Sigma- pi0, K- n -> Lambda pi-, K- p -> Sigma+ pi- cross section\n0.13 0 Σ(1385) π # not measured\n0.14 1 Λ(1520) π # not measured\nΣ(1750) # 1(2.5-)\n0.40 0 N K̅ # 0.1-0.4, tuned for K- p cross section\n0.14 0 Λ π # >0, tuned for K- n -> Lambda pi- cross section\n0.08 0 Σ π # <0.08\n0.28 0 Σ η # 0.15-0.55\n0.10 0 N K̅*(892) # 0.04-0.12\nΣ(1775) # 1(2.5-)\n0.40 2 N K̅ # 0.37-0.43, tuned for K- p cross section\n0.16 2 Λ π # 0.14-0.20, tuned for K- n -> Lambda pi-, K- p -> Lambda pi0 cross section\n0.05 2 Σ π # 0.02-0.05, tuned for K- n -> Sigma- pi0\n0.14 2 Σ(1385) π # 0.08-0.12\n0.26 1 Λ(1520) π # 0.17-0.23\nΣ(1915) # 1(2.5+)\n0.20 3 N K̅ # 0.05-0.15, tuned for K- n cross section\n0.07 3 Λ π # >0, tuned for K- n -> Lambda pi- cross section\n0.09 3 Σ π # >0, tuned for K- n -> Sigma- pi0, K- n -> Sigma0 pi-\n0.05 1 Σ(1385) π # <0.05\n#^ We use the similar values as UrQMD here.\n0.59 2 Λ(1520) π # not measured\nΣ(1940) # 1(1.5-)\n0.20 2 N K̅ # <0.2\n0.07 2 Λ π # >0, tuned for K- n -> Lambda pi-\n0.06 2 Σ π # >0, tuned for K- n -> Sigma- pi0\n0.16 0 Σ(1385) π # >0\n0.17 1 Λ(1520) π # >0\n0.16 0 Δ K̅ # >0\n0.16 0 N K̅*(892) # >0\nΣ(2030) # 1(3.5+)\n0.25 3 N K̅ # 0.17-0.23, tuned for K- n cross section\n0.17 3 Λ π # 0.17-0.23, tuned for K- n -> Lambda pi- cross section\n0.05 3 Σ π # 0.05-0.10, tuned for K- n -> Sigma- pi0 cross section\n0.02 3 Ξ K # <0.02\n0.15 3 Σ(1385) π # 0.05-0.15\n0.195 2 Λ(1520) π # 0.1-0.2\n0.16 3 Δ K̅ # 0.1-0.2\n0.05 3 N K̅*(892) # <0.05\nΣ(2250) # 1(? ?)\n0.20 3 N K̅ # <0.1, tuned for K-n cross section\n0.15 3 Λ π # >0, tuned for K- p -> Lambda pi0 cross section\n0.65 3 Σ π # >0\n#################### Λ baryons ####################\nΛ(1405) # 0(0.5-)\n1. 0 Σ π # 1.00\nΛ(1520) # 0(1.5-)\n0.462 2 N K̅ # 0.45+-0.01, tuned for K- p cross section\n0.42 2 Σ π # 0.42+-0.01, tuned for K- p -> Sigma pi cross section\n0.10 1 Λ σ # 0.10+-0.01\n0.009 0 Σ ρ # 0.009+-0.001\n# ππ replaced with σ to conserve detailed balance\n0.009 1 Λ γ # 0.0085+-0.0015\nΛ(1600) # 0(0.5+)\n0.15 1 N K̅ # 0.15-0.30, tuned for K- p cross section\n0.20 1 Σ π # 0.1-0.6, tuned for K- p -> Sigma0 pi0, Sigma+ pi- cross section\n0.35 1 N K̅*(892) # not measured\n0.30 1 Σ(1385) π # not measured\nΛ(1670) # 0(0.5-)\n0.292 0 N K̅ # 0.2-0.3\n0.442 0 Σ π # 0.25-0.55\n0.216 0 Λ η # 0.1-0.25\n0.05 2 N K̅*(892) # 0.05+-0.04\nΛ(1690) # 0(1.5-)\n0.25 2 N K̅ # 0.2-0.3\n0.3 2 Σ π # 0.2-0.4\n#0.25 1 Λ π π # ca. 0.25\n0.25 1 Λ σ # to conserve detailed balance\n#0.2 1 Σ π π # ca. 0.20\n0.2 0 Σ ρ # to conserve detailed balance\nΛ(1800) # 0(0.5-)\n0.40 0 N K̅ # 0.25-0.40\n0.06 0 Σ π # >0, tuned for K- p -> Sigma0 pi0\n0.17 2 Σ(1385) π # >0\n0.11 0 Λ η # 0.06+-0.05\n0.16 0 N K̅*(892) # >0\nΛ(1810) # 0(0.5+)\n0.34 1 N K̅ # 0.2-0.5\n0.10 1 Σ π # 0.1-0.3, tuned for K- p -> Sigma0 pi0\n0.12 1 Σ(1385) π # >0\n0.44 1 N K̅*(892) # 0.3-0.6\nΛ(1820) # 0(2.5+)\n0.65 3 N K̅ # 0.55-0.65, tuned for K- p cross section\n0.06 3 Σ π # 0.08-0.14, tuned for K- p -> Sigma0 pi0\n0.08 1 Σ(1385) π # 0.05-0.10\n0.03 1 N K̅*(892) # 0.03+-0.01\nΛ(1830) # 0(2.5-)\n0.03 2 N K̅ # 0.03-0.1\n0.30 2 Σ π # 0.35-0.75, tuned for K- p -> Sigma0 pi0\n0.52 2 Σ(1385) π # 0.52+-0.06\n0.20 4 Σ(1385) π # >0.15\nΛ(1890) # 0(1.5+)\n0.40 1 N K̅ # 0.2-0.35, tuned for K- p cross section\n0.10 1 Σ π # 0.03-0.1\n0.25 1 Σ(1385) π # >0\n0.20 1 N K̅*(892) # >0\n#^ The guesses are taken from UrQMD, which also has a 5% omega Lambda channel.\nΛ(2100) # 0(3.5-)\n0.45 4 N K̅ # 0.25-0.35, tuned for K- p cross section\n0.05 4 Σ π # 0.05\n0.03 4 Λ η # <0.03\n0.03 4 Ξ K # <0.03\n0.08 2 Λ ω # <0.08\n0.20 2 N K̅*(892) # 0.1-0.2\nΛ(2110) # 0(3.5+)\n0.30 3 N K̅ # 0.05-0.25, tuned for K- p cross section\n0.25 3 Σ π # 0.1-0.4\n0.05 1 Λ ω # >0\n0.05 1 Σ(1385) π # >0\n0.35 1 N K̅*(892) # 0.1-0.6\nΛ(2350) # 0(4.5+)\n0.50 5 N K̅ # 0.12\n0.50 5 Σ π # 0.10\n#################### Ξ baryons ####################\nΞ(1530) # 0.5(1.5+)\n1. 1 Ξ π\nΞ(1690) # 0.5(? ?)\n0.33 1 Λ K̅ # >0\n0.33 1 Σ K̅ # >0\n0.33 1 Ξ π # >0\nΞ(1820) # 0.5(1.5-)\n0.70 2 Λ K̅ # large\n0.10 2 Σ K̅ # small\n0.10 2 Ξ π # small\n0.10 0 Ξ(1530) π # small\nΞ(1950) # 0.5(? ?)\n0.40 3 Λ K̅ # >0\n0.10 3 Σ K̅ # possibly >0\n0.40 3 Ξ π # >0\nΞ(2030) # 0.5(>2.5?)\n0.20 3 Λ K̅ # 0.2\n0.80 3 Σ K̅ # 0.8\n#0.10 1 Ξ π # small\n#0.10 1 Ξ(1530) π # small\n#0.00 1 Λ K̅ π # small\n#0.00 1 Σ K̅ π # small\n########## Ω baryons ###################\nΩ(2250) # 0(? ?)\n1. 3 Ξ(1530) K̅ # >0\n######### Light nuclear resonances ########\n# d'\n# 1. 1 N N\n"