Library of Stationary PDR Models B.T. Draine Princeton University Observatory Peyton Hall, Princeton NJ 08544-1001, USA draine@astro.princeton.edu and Frank Bertoldi Max-Planck-Institut fur Extraterrestrische Physik D-85748 Garching, Germany fkb@mpe-garching.mpg.de (last modified 97.09.30) The ftp directory draine/pdr contains H2 quadrupole emission spectra calculated for 24 models of stationary photodissociation fronts. The physical assumptions and method of calculation is described by Draine & Bertoldi (1996), and some of the results for these models (e.g., 1-0S(1) surface brightnesses) are presented there. Please note one ***IMPORTANT CHANGE***: due to a numerical error in the original pdr code, the model results presented by Draine & Bertoldi (1996) were actually computed using an H2 formation rate given by dn[H_2] ------- = 3 * 10^{-18} * sqrt(T/K) * n(H) * n_H cm^3 s-1 (1) dt instead of the coefficient of 6*10^{-18} stated in the text. [This error was discovered recently, and an erratum is being submitted to Ap.J.] The results presented in this directory assume the formation rate of eq. (1), and therefore are consistent with the model results presented in Draine & Bertoldi (1996). In addition, we note that the model results which were stored in this directory prior to 97.09.30 inadvertently failed to list O(2) lines (due to an oversight in the program used to prepare the line lists). O(2) lines are included in the spectra tabulated here. Intensities are given for all of the H2 quadrupole lines with intensities exceeding 0.1% of the intensity of the 1-0S(1) line. Intensities are calculated for viewing angle theta (theta=0 is "face-on"). For each model, the spectrum is contained in a file 'spdf.irs.modl' where 'modl' is a string identifying the model. 26 models are available: Model n_H chi sigma_d T_0 cos(theta) (cm-3) (1e-22cm2) (K) ----------------------------------------------- am3d 10^2 1 20 300 1 am3o 10^2 1 6 300 1 aw3d 10^2 1 20 500 1 aw3o 10^2 1 6 500 1 bw3d 10^2 10 20 500 1 bw3o 10^2 10 6 500 1 bh3d 10^2 10 20 1000 1 bh3o 10^2 10 6 1000 1 Bm3o 10^3 10 6 300 1 Bw3o 10^3 10 6 500 1 Cw3o 10^3 10^2 6 500 1 Ch3o 10^3 10^2 6 1000 1 Gm3o 10^4 10^2 6 300 1 Gw3o 10^4 10^2 6 500 1 Hw3o 10^4 10^3 6 500 1 Hh3o 10^4 10^3 6 1000 1 Iv3o 10^4 10^4 6 1500 1 Ix3o 10^4 10^4 6 2000 1 Jv3o 10^4 10^5 6 1500 1 Jx3o 10^4 10^5 6 2000 1 Lm3o 10^5 10^3 6 300 1 Lw3o 10^5 10^3 6 500 1 Mw3o 10^5 10^4 6 500 1 Mh3o 10^5 10^4 6 1000 1 Mv3o 10^5 10^4 6 1500 1 Mx3o 10^5 10^4 6 2000 1 Nv3o 10^5 10^5 6 1500 1 Nx3o 10^5 10^5 6 2000 1 Ov3o 10^5 10^6 6 1500 1 Ox3o 10^5 10^6 6 2000 1 Qm3o 10^6 10^4 6 300 1 Qw3o 10^6 10^4 6 500 1 Qv3o 10^6 10^4 6 1500 1 Qx3o 10^6 10^4 6 2000 1 Rw3o 10^6 10^5 6 500 1 Rh3o 10^6 10^5 6 1000 1 Rv3o 10^6 10^5 6 1500 1 Rx3o 10^6 10^5 6 2000 1 Sv3o 10^6 10^6 6 1500 1 Sx3o 10^6 10^6 6 2000 1 n2023a 10^5 5000 6 500 0.2 n2023b 10^5 5000 6 900 0.2 n_H = H nucleon density (assumed constant throughout the PDR) chi = uv intensity incident on PDR, in units of Habing intensity (see eq. ?? of Draine & Bertoldi 1996). sigma_d = effective dust attenuation cross section at 1000A sigma_d=20e-22 cm2 for "diffuse cloud dust" with R_V=3.1; sigma_d= 6e-22 cm2 for "dense cloud dust" with R_V=5.5 T_0 = parameter determining temperature profile of PDR (see eq.41 of Draine & Bertoldi (1996): T = T_0/(1+tau_{d,1000}) theta = viewing angle (theta=0 is "face-on"). If you are interested in H2 vibration-rotation spectra for PDRs characterized by other values of n_H, chi, sigma_d, T_0, or cos(theta), contact draine@astro.princeton.edu . References: Draine, B.T., \& Bertoldi, F. 1996, "Structure of Stationary Phodissociation Fronts", Ap. J., 468, 269