e-capture and beta-decay rates for sd-shell nuclei (A=17-28) obtained with USDB Coulomb effects are included. H. Toki, T. Suzuki, K. Nomoto, S. Jones and R. Hirschi, Phys. Rev. C88, 015806 (2013) Experimental energies and GT transition strengths available are taken into account. The following quantities are tabulated. density: log_{10}(\rho Y_e): temperature: log_{10}T: chemical potential: mu Coulomb effect parameters: shift in Q-value: dQ shift in chemical potential: Vs e-capture rate or beta-decay rate: e-cap-rate: log_{10}(rate) neutrino energy-loss rate: nu-energy-loss: log_{10}(rate) gamma-ray heating rate: gamma-energy: log_{10}(rate) e.g. !Log(rhoY) Log(T) mu dQ Vs e-cap-rate nu-energy-loss gamma-energy ! (MeV) (MeV) (MeV) (1/s) (MeV/s) (MeV/s) 8.00 7.00 2.43160 0.05613 0.01435 -0.14470E+00 0.47340E+00 -0.16099E+02 8.00 7.20 2.43190 0.05591 0.01435 -0.14474E+00 0.47337E+00 -0.16099E+02 8.00 7.40 2.43230 0.05561 0.01435 -0.14496E+00 0.47314E+00 -0.16100E+02 8.00 7.60 2.43260 0.05521 0.01435 -0.14517E+00 0.47294E+00 -0.16100E+02 8.00 7.80 2.43260 0.05468 0.01435 -0.14495E+00 0.47324E+00 -0.16100E+02 8.00 8.00 2.43240 0.05397 0.01435 -0.14438E+00 0.47395E+00 -0.16099E+02 8.00 8.05 2.43230 0.05376 0.01435 -0.14424E+00 0.47412E+00 -0.16099E+02 8.00 8.10 2.43230 0.05353 0.01435 -0.14411E+00 0.47429E+00 -0.16099E+02 8.00 8.15 2.43220 0.05329 0.01435 -0.14400E+00 0.47444E+00 -0.16099E+02 8.00 8.20 2.43220 0.05303 0.01435 -0.14389E+00 0.47460E+00 -0.16099E+02 8.00 8.25 2.43210 0.05276 0.01435 -0.14377E+00 0.47476E+00 -0.16098E+02 8.00 8.30 2.43200 0.05246 0.01435 -0.14368E+00 0.47490E+00 -0.16097E+02 8.00 8.35 2.43190 0.05215 0.01435 -0.14357E+00 0.47507E+00 -0.16003E+02 8.00 8.40 2.43180 0.05182 0.01435 -0.14343E+00 0.47528E+00 -0.14922E+02 8.00 8.45 2.43160 0.05146 0.01435 -0.14332E+00 0.47547E+00 -0.13387E+02 8.00 8.50 2.43140 0.05108 0.01435 -0.14316E+00 0.47572E+00 -0.11991E+02 8.00 8.55 2.43110 0.05068 0.01435 -0.14297E+00 0.47601E+00 -0.10746E+02 8.00 8.60 2.43080 0.05025 0.01435 -0.14274E+00 0.47637E+00 -0.96363E+01 8.00 8.65 2.43040 0.04980 0.01435 -0.14253E+00 0.47674E+00 -0.86472E+01 8.00 8.70 2.42990 0.04932 0.01435 -0.14222E+00 0.47722E+00 -0.77661E+01 8.00 8.75 2.42920 0.04882 0.01435 -0.14188E+00 0.47778E+00 -0.69812E+01 8.00 8.80 2.42840 0.04828 0.01435 -0.14145E+00 0.47847E+00 -0.62802E+01 8.00 8.85 2.42730 0.04772 0.01435 -0.14096E+00 0.47927E+00 -0.56568E+01 8.00 8.90 2.42600 0.04712 0.01435 -0.14036E+00 0.48026E+00 -0.51002E+01 8.00 8.95 2.42430 0.04649 0.01435 -0.13964E+00 0.48145E+00 -0.46042E+01 8.00 9.00 2.42220 0.04583 0.01435 -0.13873E+00 0.48294E+00 -0.41616E+01 8.00 9.05 2.41950 0.04514 0.01435 -0.13762E+00 0.48477E+00 -0.37671E+01 8.00 9.10 2.41620 0.04442 0.01435 -0.13621E+00 0.48707E+00 -0.34152E+01 8.00 9.15 2.41200 0.04367 0.01435 -0.13443E+00 0.48993E+00 -0.31012E+01 8.00 9.20 2.40680 0.04288 0.01435 -0.13217E+00 0.49355E+00 -0.28208E+01 8.00 9.25 2.40010 0.04206 0.01435 -0.12930E+00 0.49810E+00 -0.25705E+01 8.00 9.30 2.39170 0.04120 0.01435 -0.12567E+00 0.50381E+00 -0.23470E+01 8.00 9.35 2.38120 0.04032 0.01435 -0.12106E+00 0.51099E+00 -0.21471E+01 8.00 9.40 2.36800 0.03940 0.01435 -0.11526E+00 0.51997E+00 -0.19680E+01 8.00 9.45 2.35130 0.03846 0.01435 -0.10809E+00 0.53105E+00 -0.18071E+01 8.00 9.50 2.33030 0.03748 0.01435 -0.99263E-01 0.54471E+00 -0.16620E+01 8.00 9.55 2.30380 0.03881 0.01435 -0.89012E-01 0.56066E+00 -0.15306E+01 8.00 9.60 2.27050 0.03806 0.01435 -0.76112E-01 0.58076E+00 -0.14095E+01 8.00 9.65 2.22870 0.03437 0.01435 -0.60108E-01 0.60576E+00 -0.12960E+01 %% Oct. 27, 2015 %%%%%%%%% %% Toshio Suzuki %%%%%% %% suzuki@phys.chs.nihon-u.ac.jp %%%%%