Table 1. Density, Aggregate Acoustic Velocities, Single-Crystal Elastic Moduli, and Adiabatic Bulk and Shear Moduli for Fp06 As a Function of Pressure P,a GPa rho, g/cm3 VP, km/s VS, km/s C11, GPa C44, GPa C12, GPa KS,b GPa micronVRH,b GPa Outside DAC (theta*= 90degrees) 0.0001 3.723(8)c 9.33(7) 5.70(5) 284(3) 147(1) 103(1) 163(3) 121(2) theta*= 80degrees (MEW1) 4.4 3.820(8) 9.61(8) 5.79(5) 320(3) 148(1) 112(1) 181(4) 128(3) 9.5(1) 3.924(9) 9.90(8) 5.96(5) 364(4) 151(2) 117(1) 199(4) 139(3) 10.8(1) 3.950(9) 9.99(8) 6.04(5) 373(4) 156(2) 116(1) 202(4) 144(3) 13.3(4) 3.997(9) 10.13(8) 6.11(5) 396(4) 157(2) 119(1) 211(4) 149(3) theta*= 50degrees (MEW2) 3.6 3.803(8) 9.54(8) 5.78(5) 313(3) 147(1) 109(1) 177(4) 127(3) 11.2(2) 3.957(9) 10.01(8) 6.02(5) 379(4) 153(2) 119(1) 206(4) 143(3) 15.2(6) 4.033(9) 10.25(8) 6.15(5) 413(4) 158(2) 124(1) 220(5) 152(3) 17.4(7) 4.073(9) 10.32(8) 6.19(5) 427(4) 160(2) 125(1) 225(5) 156(3) 20.2(10) 4.122(9) 10.49(8) 6.24(5) 450(5) 162(2) 134(1) 239(5) 160(3) 20.1(10)d 4.120(9) 10.52(9) 6.27(6) 452(5) 164(2) 134(1) 240(5) 162(3) 16.1(6)d 4.049(9) 10.29(8) 6.16(5) 418(4) 159(2) 126(1) 224(5) 154(3) 11.9(1)d 3.971(9) 10.03(8) 6.03(5) 381(4) 155(2) 121(1) 207(4) 144(3) aAverage pressure and associated uncertainties are reported from measurements made before and after each experiment. Uncertainties in pressure are determined from the standard deviation of the pressures calculated from the ruby fluorescence R1 shift [Mao et al., 1986] of up to seven rubies placed around the sample within the sample chamber. bKS = 1/3(C11 + 2C12) and micronVRH is the Voigt-Reuss-Hill average, where micronVRH is the arithmetic mean of the Voigt and Reuss bounds: micronV = 1/5(C11 - C12 + 3C44) and micronR = 15[12/(C11 - C12) + 9/C44]-1 [Watt et al., 1976]. c Room-pressure density is from Jacobsen et al. [2002]. d Measurements are taken on pressure decrease. The uncertainties in aggregate velocities, high-pressure densities, and Cij are taken from the statistical (root-mean-square) errors from the fitting procedure of the data (see text). Error propagation was used to calculate the uncertainties for KS and micronVRH. All uncertainties are given in parentheses for the last significant digit(s).