O3_O1D_IUPAC10
! j(O3_O1D) IUPAC(2010)                                 
! O3 = O1D                                              
! From IUPAC Subcommittee on Gas Kinetic Data Evaluation
! Data Sheet POx2, updated 2nd October, 2001            
! values below 280 nm from JPL2011                                
! These are point values                                
Begining (the mechanism evaluated with this format)
!WL(nm) XSEC(cm2) QY
FAC=1.0
121.6 2.990E-17 0.900
186.1 6.220E-19 0.900
187.8 5.760E-19 0.900
189.6 5.260E-19 0.900
191.4 4.770E-19 0.900
193.2 4.290E-19 0.900
195.1 3.850E-19 0.900
197.0 3.490E-19 0.900
199.0 3.240E-19 0.900
201.0 3.150E-19 0.900
203.1 3.260E-19 0.900
205.1 3.630E-19 0.900
207.3 4.330E-19 0.900
209.4 5.390E-19 0.900
211.6 6.930E-19 0.900
213.9 9.030E-19 0.900
216.2 1.180E-18 0.900
218.6 1.540E-18 0.900
221.0 1.990E-18 0.900
223.5 2.550E-18 0.900
226.0 3.220E-18 0.900
228.6 4.010E-18 0.900
231.2 4.900E-18 0.900
233.9 5.900E-18 0.900
236.7 6.930E-18 0.900
239.5 8.020E-18 0.900
242.4 9.080E-18 0.900
245.4 1.000E-17 0.900
248.5 1.080E-17 0.900
251.6 1.130E-17 0.900
254.8 1.150E-17 0.900
258.1 1.120E-17 0.900
261.4 1.060E-17 0.900
264.9 9.680E-18 0.900
268.5 8.400E-18 0.900
272.1 6.980E-18 0.900
275.9 5.470E-18 0.900
279.7 4.060E-18 0.900
280.0 4.020E-18 0.900
281.0 4.020E-18 0.900
282.0 2.770E-18 0.900
283.0 2.770E-18 0.900
284.0 2.770E-18 0.900
285.0 2.770E-18 0.900
286.0 1.790E-18 0.900
287.0 1.790E-18 0.900
288.0 1.790E-18 0.900
289.0 1.790E-18 0.900
290.0 1.090E-18 0.900
291.0 1.090E-18 0.900
292.0 1.090E-18 0.900
293.0 1.090E-18 0.900
294.0 1.090E-18 0.900
295.0 6.240E-19 0.900
296.0 6.240E-19 0.900
297.0 6.240E-19 0.900
298.0 6.240E-19 0.900
299.0 3.430E-19 0.900
300.0 3.430E-19 0.900
301.0 3.430E-19 0.900
302.0 3.430E-19 0.900
303.0 1.850E-19 0.900
304.0 1.850E-19 0.900
305.0 1.850E-19 0.900
306.0 1.850E-19 0.884
307.0 1.850E-19 0.862
308.0 9.800E-20 0.793
309.0 9.800E-20 0.671
310.0 9.800E-20 0.523
311.0 9.800E-20 0.394
312.0 9.800E-20 0.310
313.0 5.000E-20 0.265
314.0 5.000E-20 0.246
315.0 5.000E-20 0.239
316.0 5.000E-20 0.233
317.0 5.000E-20 0.222
318.0 2.490E-20 0.206
319.0 2.490E-20 0.187
320.0 2.490E-20 0.166
321.0 2.490E-20 0.146
322.0 2.490E-20 0.128
323.0 1.200E-20 0.113
324.0 1.200E-20 0.101
325.0 1.200E-20 0.092
326.0 1.200E-20 0.086
327.0 1.200E-20 0.082
328.0 6.170E-21 0.080
329.0 6.170E-21 0.080
330.0 6.170E-21 0.080
331.0 6.170E-21 0.080
332.0 6.170E-21 0.080
333.0 2.740E-21 0.080
334.0 2.740E-21 0.080
335.0 2.740E-21 0.080
336.0 2.740E-21 0.080
337.0 2.740E-21 0.080
338.0 1.170E-21 0.080
339.0 1.170E-21 0.080
340.0 1.170E-21 0.080
341.0 1.170E-21 0.080
342.0 1.170E-21 0.080
343.0 5.900E-22 0.080
344.0 5.900E-22 0.080
345.0 5.900E-22 0.080
346.0 5.900E-22 0.080
347.0 5.900E-22 0.080
348.0 2.700E-22 0.080
349.0 2.700E-22 0.080
350.0 2.700E-22 0.080
351.0 2.700E-22 0.080
352.0 2.700E-22 0.080
353.0 1.100E-22 0.080
354.0 1.100E-22 0.080
355.0 1.100E-22 0.080
356.0 1.100E-22 0.080
357.0 1.100E-22 0.080
358.0 5.000E-23 0.080
359.0 5.000E-23 0.080
360.0 5.000E-23 0.080
361.0 5.000E-23 0.080
362.0 5.000E-23 0.080
363.0 5.000E-23 0.080
364.0 5.000E-23 0.080
365.0 5.000E-23 0.080
366.0 0.000E+00 0.000
409.0 0.000E+00 0.000
410.0 1.200E-23 0.000
420.0 2.200E-23 0.000
440.0 1.120E-22 0.000
460.0 3.280E-22 0.000
480.0 6.840E-22 0.000
500.0 1.220E-21 0.000
520.0 1.820E-21 0.000
540.0 2.910E-21 0.000
560.0 3.940E-21 0.000
580.0 4.590E-21 0.000
600.0 5.110E-21 0.000
620.0 4.000E-21 0.000
640.0 2.960E-21 0.000
660.0 2.090E-21 0.000
680.0 1.360E-21 0.000
700.0 9.100E-22 0.000
701.0 0.000E+00 0.000
