Table 6.
SW-Kr composition and fluences calculated assuming trapped 132Xe/84Kr = 0.036 (atmospheric), and 132Xe/84Kr = 0.041 (derived from the minimization of the SW-Kr and SW-Xe fluencies scattering).
| Sample, extraction method | Assumed Trapped 132Xe/84Kr | 86Kr/84Kr | 83Kr/84Kr | 82Kr/84Kr | 80Kr/84Kr | 78Kr/84Kr | SW 84Kr retrieved, 107 at/cm2 |
|---|---|---|---|---|---|---|---|
| A-π/8 (a) | atm. | .3018 (11) | .2031 (6) | .2047 (6) | .0406 (3) | .00628 (7) | 1.23 (9) |
| .041 | .3018 (11) | .2032 (6) | .2047 (6) | .0406 (3) | .00629 (7) | 1.20 (8) | |
| A-π/8 (b) | atm. | .3007 (7) | .2043 (5) | .2060 (4) | .0414 (2) | .00657 (8) | 1.20 (14) |
| .041 | .3007 (7) | .2043 (5) | .2060 (4) | .0415 (2) | .00657 (8) | 1.19 (12) | |
| A-π/4 | atm. | .3025 (28) | .2033 (22) | .2063 (20) | .0412 (8) | .00658 (37) | 1.11 (31) |
| .041 | .3019 (34) | .2037 (27) | .2072 (25) | .0416 (9) | .00669 (45) | 1.02 (11) | |
| A-π | atm. | .3011 (10) | .2021 (9) | .2066 (9) | .0411 (4) | .00644 (25) | 1.13 (19) |
| .041 | .3011 (10) | .2021 (9) | .2067 (9) | .0411 (4) | .00645 (26) | 1.11 (18) | |
| P-π/4 | atm. | .3015 (6) | .2032 (3) | .2050 (3) | .0420 (3)b | .00640 (19) | 0.95 (11) |
| .041 | .3014 (6) | .2033 (3) | .2051 (3) | .0421 (3)b | .00641 (19) | 0.90 (9) | |
| All data (free fit) | .3010 (22) | .2035 (15) | .2055 (14) | .0413 (7) | .00646 (30) | ||
| All data (fixed trapped comp.)a | .3012 (4) | .2034 (2) | .2054 (2) | .0412 (2) | .00642 (5) | 1.08 (5) | |
| Diamondc | .302 (3) | n.d. | n.d. | n.d. | n.d. | 1.22 (10) | |
| Silicond | .303 (1) | n.d. | n.d. | n.d. | n.d. | 1.22 (6) | |
| Atm. Kre | .036 | .30524 (25) | .20136 (21) | .20217 (4) | .03960 (2) | .006087 (20) |
Weighted average from all data assuming trapped 132Xe/84Kr = 0.041.
Polished Aluminum Collector (PAC) 80Kr/84Kr is excluded because of the “change of charge” effect.
ETH (Heber et al., 2009).
ETH (Vogel et al., 2011).
From Basford et al., 1973.