Page 422 - High Power Laser Handbook
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390     So l i d - S t at e   La s e r s                                                                          The National Ignition Facility Laser    391


                             1.0
                                                                Calculated
                                                                Measured
                             0.8    1.0 MJ
                            Encircled energy fraction  0.6  1.8 MJ




                             0.4


                             0.2


                             0.0
                                0     200    400    600    800   1000   1200
                                             Major axis radius (µm)

                            1.000
                                                                  Calculated
                                                                  Measured
                           Fractional power above intensity  0.100  1.8 MJ  1.0 MJ






                            0.010





                            0.001
                                 0       0.5     1.0     1.5     2.0      2.5
                                                       15
                                                             2
                                              Intensity (10  W/cm )
                      Figure 14.31  Comparison of the encircled energy fraction and the fractional
                      power above intensity (FOPAI) for the 1-MJ and the 1.8-MJ shots described in
                      Fig. 14.30. The encircled energy was calculated in elliptical coordinates, with
                      eccentricity of 0.55 for the 1-MJ case and 0.88 for the 1.8-MJ case. The total
                      power is normalized to 1 TW for each case.


                      is separable in time and space: I(x, y, t) = F(x, y)*P(t)/E, where F is the
                      measured  near-field  fluence,  P  the  time-dependent  whole-beam
                      power, and E the total energy. Equation (14.2) is, again, evaluated at
                      the time of peak power. Our models indicate that for these pulses,
                      intensity-dependent effects, such as nonlinear refractive index and
                      frequency conversion, do not cause significant changes in the focal
                      spot characteristics as a function of time, thus justifying the separability
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