The following table presents q=1000/Q values for spheroidal mode fundamentals. Most low harmonic degree values are from applications of iterative spectral fitting, with a few values coming from averages of singlet q's determined by singlet stripping. Higher l values are from surface wave analyses Mode analyses Wid/Mast -- compilations of Widmer and Masters Maste(ss) -- singlet stripping results (unpublished) Um -- unpublished results from iterative spectral fitting Tromp -- He and Tromp, JGR,101, 20067, 1996 -- iterative spectral fitting Res/Ritz -- Resovsky and Ritzwoller (see their web page) Li -- PhD Thesis, Harvard Univ, 1990 Surface wave analyses Durek -- Durek and Ekstrom, BSSA, 86, 144, 1996 Roman -- Barbara Romanowicz (unpublished) Laske -- Gabi Laske (unpublished) NB: The discrepancies between mode and surface wave analyses are discussed in several recent preprints -- references will be provided as they become available. Mode Wid/Mast Maste(ss) Tromp Res/Ritz Um Li 0 S 3 2.63 0.31 2.67 0.59 2.92 0.51 2.61 0.17 2.40 0.27 2.28 0.14 0 S 4 2.74 0.22 2.75 0.25 2.45 0.23 2.68 0.12 2.76 0.14 2.46 0.09 0 S 5 2.86 0.10 2.86 0.15 2.66 0.23 2.79 0.09 2.66 0.09 2.67 0.08 0 S 6 2.91 0.13 3.04 0.10 2.81 0.06 2.92 0.05 2.87 0.06 2.72 0.04 0 S 7 3.21 0.15 2.70 0.13 2.96 0.07 2.85 0.08 2.89 0.07 2.70 0.04 0 S 8 2.92 0.20 2.96 0.08 3.00 0.10 2.88 0.04 3.03 0.10 0 S 9 2.80 0.12 3.12 0.08 2.97 0.10 2.92 0.07 2.99 0.04 0 S 10 2.79 0.10 3.30 0.09 2.92 0.04 0 S 11 2.94 0.07 0 S 12 2.84 0.10 2.95 0.04 0 S 13 2.84 0.10 3.11 0.05 0 S 14 3.02 0.10 3.15 0.05 0 S 15 2.93 0.08 3.18 0.05 0 S 16 3.08 0.08 3.25 0.06 0 S 17 3.28 0.08 0 S 18 3.38 0.06 0 S 19 3.53 0.06 0 S 20 3.55 0.08 3.57 0.06 0 S 21 3.61 0.06 3.70 0.07 0 S 22 3.87 0.06 0 S 23 3.86 0.06 Durek(sw) 0 S 24 3.97 0.06 4.84 0.14 0 S 25 4.13 0.08 4.98 0.14 0 S 26 4.29 0.08 Roman(sw) 5.07 0.14 0 S 27 4.36 0.08 5.26 1.00 5.14 0.12 0 S 28 4.61 0.08 5.23 0.11 0 S 29 4.50 0.08 5.36 0.80 5.32 0.10 0 S 30 4.75 0.08 5.42 0.09 0 S 31 4.95 0.08 Laske(sw) 5.49 0.80 5.50 0.10 0 S 32 5.03 0.10 5.12 0.15 5.59 0.09 0 S 33 5.24 0.10 5.69 0.09 0 S 34 5.06 0.10 5.78 0.09 0 S 35 5.33 0.10 5.92 0.85 5.87 0.09 0 S 36 5.43 0.10 5.96 0.09 0 S 37 5.37 0.10 6.05 0.09 0 S 38 5.56 0.10 6.14 0.09 0 S 39 5.58 0.10 6.42 0.85 6.25 0.09 0 S 40 5.66 0.10 6.33 0.10 0 S 41 5.88 0.10 6.41 0.10 0 S 42 5.75 0.10 6.50 0.10 0 S 43 6.00 0.12 6.29 0.15 6.82 0.95 6.59 0.10 0 S 44 6.03 0.10 6.68 0.10 0 S 45 6.01 0.10 6.77 0.10 0 S 46 6.12 0.10 6.85 0.11 0 S 47 6.10 0.12 6.94 0.11 0 S 48 6.50 0.16 7.26 1.00 7.03 0.11 0 S 49 6.61 0.15 7.13 0.11 0 S 50 6.77 0.16 7.22 0.11 0 S 51 6.99 0.16 7.32 0.11 0 S 52 6.85 0.16 7.42 0.11 0 S 53 6.83 0.15 7.70 1.15 7.52 0.12 0 S 54 7.15 0.14 7.38 0.20 7.63 0.12 0 S 55 7.03 0.14 7.75 0.12 0 S 56 7.13 0.15 7.88 0.13 0 S 57 6.80 0.13 8.02 1.25 8.02 0.14 0 S 58 7.21 0.16 8.18 0.15 0 S 59 8.40 0.17 0 S 60 7.11 0.19 0 S 61 8.22 1.20 0 S 65 8.15 0.25 0 S 67 8.54 1.25 0 S 74 8.82 1.25 0 S 76 8.85 0.30 0 S 79 8.95 1.25 0 S 86 9.00 0.30 0 S 88 9.18 1.25 0 S 97 9.25 0.30 9.32 1.25