This file contains the data points (expected and observed cross section limits) corresponding to Figure 3 in the Phys. Lett. B 682, 278 (2009) paper. Theorists who want to use these data points to derive limits on SUSY parameters should read carefully the following to understand the assumptions made in the derivation of the cross section limits. The theoretical assumptions are described in detail in our Phys. Lett. B 682, 278 (2009) paper and summarised below. The ttbar samples with one or both top quarks decaying into charged Higgs bosons are simulated using Pythia. We consider two different modes of charged Higgs decay: charged Higgs into tau and corresponding neutrino or charged Higgs into charm and (anti)strange quark (or short: csbar). The limits we give are parametrized as function of the charged Higgs to csbar decay, where we assume Br(H+ -> csbar)+Br(H+ ->tau nu) = 1. When generating the Monte Carlo samples, we make sure to keep the width small, in order to make the limits as model independent as possible. When deriving limits on certain models (like the examples given in the paper), it has to be ensured that the partial widths of the charged Higgs boson into decay channels different from H+ --> csbar and H+ --> tau nu are negligible (see the example of the strangephilic CPX model in the article). There should be no claim that a new limit obtained using different models is a D0 limit, but rather a limit based on D0 data which may not be fully accurate for the reason listed above. We would appreciate being informed if the D0 limits given below are used in this way and we would appreciate if this disclaimer is included in the presentation of the results. In case of further questions please contact the top group conveners or the D0 Physics Coordinators (see http://www-d0.fnal.gov/Run2Physics/WWW/physics.htm ----------------------------------------------------------------- for point 80 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.149149 & 0.168168 & 0.179179 & 0.193193 & 0.203203 & 0.21021 & 0.22022 & 0.224224 & 0.223223 & 0.224224 & 0.214214 expected (central; minus ; plus) 0.186186 0.082082 0.095095 & 0.206206 0.091091 0.1001 & 0.221221 0.096096 0.106106 & 0.238238 0.102102 0.11011 & 0.252252 0.108108 0.112112 & 0.262262 0.112112 0.112112 & 0.267267 0.11011 0.111111 & 0.269269 0.111111 0.109109 & 0.263263 0.111111 0.106106 & 0.256256 0.109109 0.101101 & 0.245245 0.109109 0.104104 for point 100 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.141141 & 0.157157 & 0.175175 & 0.191191 & 0.209209 & 0.217217 & 0.225225 & 0.231231 & 0.232232 & 0.23023 & 0.224224 expected (central; minus ; plus) 0.17017 0.0770769 0.096096 & 0.19019 0.086086 0.1001 & 0.212212 0.096096 0.108108 & 0.229229 0.1001 0.11011 & 0.248248 0.102102 0.111111 & 0.258258 0.108108 0.114114 & 0.266266 0.111111 0.113113 & 0.268268 0.108108 0.109109 & 0.265265 0.107107 0.106106 & 0.258258 0.107107 0.099099 & 0.252252 0.108108 0.104104 for point 120 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.159159 & 0.172172 & 0.187187 & 0.2002 & 0.209209 & 0.218218 & 0.219219 & 0.222222 & 0.205205 & 0.223223 & 0.221221 expected (central; minus ; plus) 0.189189 0.082082 0.098098 & 0.207207 0.09009 0.101101 & 0.224224 0.096096 0.106106 & 0.239239 0.1001 0.108108 & 0.252252 0.104104 0.11011 & 0.261261 0.108108 0.112112 & 0.262262 0.109109 0.111111 & 0.262262 0.11011 0.109109 & 0.26026 0.108108 0.103103 & 0.252252 0.105105 0.101101 & 0.249249 0.106106 0.105105 for point 140 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.173173 & 0.182182 & 0.187187 & 0.194194 & 0.201201 & 0.201201 & 0.206206 & 0.209209 & 0.21021 & 0.21021 & 0.213213 expected (central; minus ; plus) 0.196196 0.082082 0.094094 & 0.209209 0.087087 0.096096 & 0.216216 0.092092 0.098098 & 0.224224 0.092092 0.098098 & 0.233233 0.096096 0.099099 & 0.234234 0.098098 0.101101 & 0.238238 0.097097 0.098098 & 0.241241 0.099099 0.097097 & 0.239239 0.098098 0.095095 & 0.236236 0.097097 0.095095 & 0.243243 0.102102 0.101101 for point 150 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.181181 & 0.184184 & 0.19019 & 0.195195 & 0.196196 & 0.198198 & 0.197197 & 0.197197 & 0.195195 & 0.197197 & 0.194194 expected (central; minus ; plus) 0.194194 0.082082 0.087087 & 0.2002 0.085085 0.089089 & 0.206206 0.085085 0.09009 & 0.213213 0.089089 0.09009 & 0.215215 0.09009 0.091091 & 0.219219 0.092092 0.09009 & 0.218218 0.093093 0.09009 & 0.218218 0.092092 0.091091 & 0.217217 0.092092 0.089089 & 0.217217 0.092092 0.086086 & 0.221221 0.093093 0.094094 for point 155 branching H->cs 0 & 0.1 & 0.2 & 0.3 & 0.4 & 0.5 & 0.6 & 0.7 & 0.8 & 0.9 & 1 branching H->tau nu 1 & 0.9 & 0.8 & 0.7 & 0.6 & 0.5 & 0.4 & 0.3 & 0.2 & 0.1 & 0 observed 0.167167 & 0.172172 & 0.177177 & 0.18018 & 0.182182 & 0.185185 & 0.189189 & 0.191191 & 0.19019 & 0.19019 & 0.193193 expected (central; minus ; plus) 0.192192 0.083083 0.085085 & 0.197197 0.083083 0.085085 & 0.202202 0.086086 0.087087 & 0.205205 0.086086 0.087087 & 0.208208 0.088088 0.09009 & 0.21021 0.087087 0.087087 & 0.214214 0.089089 0.085085 & 0.215215 0.089089 0.084084 & 0.211211 0.087087 0.085085 & 0.211211 0.089089 0.083083 & 0.219219 0.093093 0.091091 observed 0.167167 & 0.172172 & 0.177177 & 0.18018 & 0.182182 & 0.185185 & 0.189189 & 0.191191 & 0.19019 & 0.19019 & 0.193193