National Library of Energy BETA

Sample records for aj podkaminer kk

  1. A=6H (1974AJ01)

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    4AJ

  2. A=6H (1979AJ01)

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    9AJ

  3. A=13F (1976AJ04)

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    76AJ04

  4. A=13F (1981AJ01)

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    81AJ01

  5. A=13Ne (1976AJ04)

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    76AJ04

  6. A=13Ne (1981AJ01)

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    81AJ01

  7. A=20Al (1972AJ02)

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    2AJ02

  8. A=20Al (1978AJ03)

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    8AJ03

  9. A=20Al (1983AJ01)

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    83AJ01

  10. Toyo Aluminium KK | Open Energy Information

    Open Energy Info (EERE)

    Aluminium KK Jump to: navigation, search Name: Toyo Aluminium KK Place: Japan Sector: Solar Product: Japan-based aluminium powder maker for solar cell electrodes. References: Toyo...

  11. A=6C (1984AJ01)

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    4AJ01) (Not illustrated) Not observed: see (1979AJ

  12. A=5n (1988AJ01)

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    1988AJ01) (Not illustrated)

  13. A=6C (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01, 1984AJ

  14. Canadian Solar Japan KK | Open Energy Information

    Open Energy Info (EERE)

    Japan KK Jump to: navigation, search Name: Canadian Solar Japan KK Place: Shinjuku-ku, Tokyo, Japan Zip: 160-0022 Sector: Solar Product: Tokyo-based subsidiary of Canadian Solar,...

  15. A=12F (1990AJ01)

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    90AJ01) (Not illustruated) This nuclei has not been observed: see (1980AJ01, 1985AJ01

  16. A=12Ne (1990AJ01)

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    90AJ01) (Not illustruated) This nuclei has not been observed: see (1980AJ01, 1985AJ01

  17. A=20Al, etc. (1987AJ02)

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    87AJ02) (Not observed) See (1972AJ02, 1986AN07) and (1983ANZQ; theor.

  18. A=6B (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1984AJ01

  19. A=7He (59AJ76)

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    59AJ76) (Not illustrated) Not observed: see (55AJ61)

  20. A=9N (1984AJ01)

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    4AJ01) (Not illustrated) Not observed: see (1979AJ01). See also (1982NG01

  1. A=9n (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01) and (1983BE55; theor.

  2. A=11F (1990AJ01)

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    90AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01, 1985AJ01) and (1986AN07, 1987SA15

  3. A=11Ne (1990AJ01)

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    90AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01, 1985AJ01) and (1986AN07, 1987SA15

  4. A=12He (1985AJ01)

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    85AJ01) (Not illustrated) See (1983ANZQ; theor.

  5. A=16Al (1986AJ04)

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    86AJ04) (Not observed) See (1983ANZQ; theor.

  6. A=16Mg (1986AJ04)

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    86AJ04) (Not observed) See (1983ANZQ; theor.

  7. A=16Na (1986AJ04)

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    86AJ04) (Not observed) See (1983ANZQ; theor.

  8. A=16Si (1986AJ04)

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    86AJ04) (Not observed) See (1983ANZQ; theor.

  9. A=17P (1986AJ04)

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    86AJ04) (Not observed) See (1983ANZQ; theor.

  10. A=19Be (1987AJ02)

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    87AJ02) (Not observed) See (1983ANZQ; theor.

  11. A=19He (1987AJ02)

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    87AJ02) (Not observed) See (1983ANZQ; theor.

  12. A=19Li (1987AJ02)

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    87AJ02) (Not observed) See (1983ANZQ; theor.

  13. A=19Mg (1972AJ02)

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    2AJ02) (Not illustrated) See (1965GO1D

  14. A=11He (1985AJ01)

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    5AJ01) (Not illustrated) 11He has not been observed: see (1980AJ01) and (1983ANZQ

  15. A=12F (1985AJ01)

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    5AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01) and (1983ANZQ

  16. A=12Ne (1985AJ01)

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    5AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01) and (1983ANZQ

  17. A=9N (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1984AJ01) and (1983ANZQ, 1986AN40

  18. A=10n (1988AJ01)

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    8AJ01) (Not illustrated) 10n has not been observed: see (1979AJ01). See also (1986AB10; theor.)

  19. A=11F (1985AJ01)

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    5AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01) and (1982NG01, 1983ANZQ

  20. A=11He (1990AJ01)

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    1990AJ01) (Not illustrated) 11He has not been reported: see (1980AJ01). The ground state of 11He is predicted to have

  1. A=11Ne (1985AJ01)

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    5AJ01) (Not illustrated) These nuclei have not been observed: see (1980AJ01) and (1982NG01, 1983ANZQ

  2. A=12O (1975AJ02)

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    75AJ02) (Not illustrated) This nucleus has not been observed: see (1968AJ02, 1972WA07, 1973SP1A, 1974IR04

  3. A=12n (1990AJ01)

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    90AJ01) (Not illustrated) 12n has not been observed. See (1980AJ01), (1987PE1C), (1987FL1A) and (1985PO10; theor

  4. A=6n (1988AJ01)

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    88AJ01) (Not illustrated) 6n has not been observed: see (1979AJ01). See also (1984DE52) and (1987BE45

  5. A=10F (1979AJ01)

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    79AJ01) (Not illustrated) Not observed: see (1975BE3

  6. A=10N (1979AJ01)

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    79AJ01) (Not illustrated) Not observed: see (1974IR04, 1975BE3

  7. A=10Ne (1979AJ01)

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    79AJ01) (Not illustrated) Not observed: see (1975BE3

  8. A=10O (1979AJ01)

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    79AJ01) (Not illustrated) Not observeed: see (1974IR04, 1975BE3

  9. A=11F (1975AJ02)

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    75AJ02) (Not illustrated) This nucleus has not been observed: see (1974IR04

  10. A=11He (1975AJ02)

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    75AJ02) (Not illustrated) This nucleus has not been observed: see (1974IR04

  11. A=11N (68AJ02)

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    68AJ02) (Not illustrated) See (GO60P, KE66C

  12. A=12F (1975AJ02)

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    75AJ02) (Not illustrated) This nucleus has not been observed: see (1974IR04

  13. A=12Ne (1980AJ01)

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    0AJ01) (Not illustrated) This nucleus has not been observed: see (1975BE31

  14. A=13F (1986AJ01)

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    6AJ01) (Not illustrated) These nuclei have not been observed: see (1983ANZQ

  15. A=13F (1991AJ01)

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    91AJ01) (Not illustrated) These nuclei have not been observed. See (1986AN07

  16. A=13Na (1986AJ01)

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    86AJ01) (Not illustrated) These nuclei have not been observed: see (1983ANZQ

  17. A=13Na (1991AJ01)

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    91AJ01) (Not illustrated) These nuclei have not been observed. See (1986AN07

  18. A=13Ne (1986AJ01)

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    6AJ01) (Not illustrated) These nuclei have not been observed: see (1983ANZQ

  19. A=13Ne (1991AJ01)

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    91AJ01) (Not illustrated) These nuclei have not been observed. See (1986AN07

  20. A=14He (1986AJ01)

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    86AJ01) (Not illustrated) 14He has not been observed. See also (1983ANZQ; theor.

  1. A=14He (1991AJ01)

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    91AJ01) (Not illustrated) 14He has not been observed: see (1989OG1B

  2. A=14Ne (1981AJ01)

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    1AJ01) (Not illustrated) 14Ne has not been observed. See (1976BE1V

  3. A=16He (1982AJ01)

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    2AJ01) (Not illustrated) This nucleus has not been observed. See also (1978NA07

  4. A=17He (1986AJ04)

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    86AJ04) (Not illustrated) Not observed: see (1983ANZQ; theor.

  5. A=17Li (1986AJ04)

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    86AJ04) (Not illustrated) Not observed: see (1983ANZQ; theor.

  6. A=18He (1987AJ02)

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    87AJ02) (Not illustrated) Not observed: see (1982AV1A, 1983ANZQ; theor.

  7. A=18Mg, etc. (1987AJ02)

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    87AJ02) (Not observed) See (1986AN07) and (1983ANZQ; theor.

  8. A=19Mg (1983AJ01)

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    83AJ01) (Not illustrated) 19Mg has not been observed: see (1977CE05

  9. A=20Be (1987AJ02)

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    87AJ02) (Not observed) See (1983ANZQ, 1983BE55; theor.

  10. A=20C (1972AJ02)

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    2AJ02) (Not illustrated) 20C has not been observed: see (1960ZE03

  11. A=20n (1983AJ01)

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    3AJ01) (Not illustrated) 20n has not been observed. See (1978SA1E

  12. A=20n (1987AJ02)

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    7AJ02) (Not observed) See (1983ANZQ, 1983BE55

  13. A=6B (1984AJ01)

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    4AJ01) (Not illustrated) Not observed: see (1982NG01; theor.

  14. A=6C (1979AJ01)

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    79AJ01) (Not illustrated) See (1976GO1C; theor.

  15. A=7C (1984AJ01)

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    C (1984AJ01) (Not illustrated) Not observed: see (1982NG01; theor.).

  16. A=7n (1979AJ01)

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    7n (1979AJ01) (Not illustrated) See (1977DE08).

  17. A=8N (1984AJ01)

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    N (1984AJ01) (Not illustrated) Not observed: see (1982NG01; theor.).

  18. A=9n (1984AJ01)

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    4AJ01) (Not illustrated) Not observed: see (1977DE08

  19. A=10F (1984AJ01)

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    84AJ01) (Not illustrated) Not observed: see (1979AJ01). A.H. Wapstra (private communication) suggests 39.5 MeV for the atomic mass excess of 10N. See also (1982NG0

  20. A=10O (1984AJ01)

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    84AJ01) (Not illustrated) Not observed: see (1979AJ01). A.H. Wapstra (private communication) suggests 39.5 MeV for the atomic mass excess of 10N. See also (1982NG0

  1. A=10Ne (1984AJ01)

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    84AJ01) (Not illustrated) Not observed: see (1979AJ01). A.H. Wapstra (private communication) suggests 39.5 MeV for the atomic mass excess of 10N. See also (1982NG0

  2. A=10N (1984AJ01)

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    84AJ01) (Not illustrated) Not observed: see (1979AJ01). A.H. Wapstra (private communication) suggests 39.5 MeV for the atomic mass excess of 10N. See also (1982NG0

  3. A=13B (1981AJ01)

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    1AJ01) (See Energy Level Diagrams for 13B) GENERAL: See also (1976AJ04) and Table 13.1 Table of Energy Levels (in PDF or PS). Experimental work on complex reactions in which 13B...

  4. A=16C (1982AJ01)

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    82AJ01) (See Energy Level Diagrams for 16C) GENERAL: See also (1977AJ02) and Table 16.1 Table of Energy Levels (in PDF or PS). Experimental work: (1977AR06, 1981CH1U)....

  5. A=16N (1982AJ01)

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    82AJ01) (See Energy Level Diagrams for 16N) GENERAL: See also (1977AJ02) and Table 16.4 Table of Energy Levels (in PDF or PS). Model calculations: (1979RO1J, 1980HA35). Reactions...

  6. A=12n (1985AJ01)

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    5AJ01) (Not illustrated) 12n has not been observed in the interaction of 0.7 and 400 GeV protons with uranium: see (1980AJ01)...

  7. A=14C (1991AJ01)

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    1 for E(7Li) 2 to 20 MeV: it is suggested that they are due to a forward-direction cluster transfer process: see (1976AJ04) for references. For other work see (1970AJ04,...

  8. A=5n (1984AJ01)

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    4AJ01) (Not illustrated) 5n has not been observed. It is suggested that it is unbound by 10 MeV (1981BE25; theor.). See also (1979AJ01

  9. A = 15He (1986AJ01)

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    He (1986AJ01) (Not illustrated) 15He has not been observed. See also (1983ANZQ; theor.).

  10. A=11F (1980AJ01)

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    0AJ01) (Not illustrated) These nuclei have not been observed: see (1975BE31, 1976IR1B

  11. A=11He (1980AJ01)

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    0AJ01) (Not illustrated) 11He has not been observed: see (1976IR1B; theor.

  12. A=11Ne (1980AJ01)

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    0AJ01) (Not illustrated) These nuclei have not been observed: see (1975BE31, 1976IR1B

  13. A=11O (1975AJ02)

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    75AJ02) (Not illustrated) This nucleus has not been observed: see (1972WA07, 1974IR04

  14. A=11O (1980AJ01)

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    80AJ01) (Not illustrated) These nuclei have not been observed: see (1975BE31, 1976IR1B; theor.

  15. A=12F (1980AJ01)

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    0AJ01) (Not illustrated) This nucleus has not been observed: see (1975BE31, 1976IR1B

  16. A=12O (68AJ02)

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    68AJ02) (Not illustrated) See (GO60P, GO65I, GO66J, KE66C

  17. A=13He (1986AJ01)

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    He (1986AJ01) (Not illustrated) 13He has not been observed. See also (1983ANZQ; theor.).

  18. A=14Mg (1986AJ01)

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    86AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1983ANZQ

  19. A=14Mg (1991AJ01)

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    91AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1986AN07

  20. A=14Na (1986AJ01)

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    86AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1983ANZQ

  1. A=14Na (1991AJ01)

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    91AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1986AN07

  2. A=14Ne (1986AJ01)

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    6AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1983ANZQ

  3. A=14Ne (1991AJ01)

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    91AJ01) (Not illustrated) 14Ne, 14Na and 14Mg have not been observed. See (1986AN07

  4. A=16He (1986AJ04)

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    6AJ04) (Not illustrated) This nucleus has not been observed. See also (1982AV1A, 1983ANZQ

  5. A=19Mg, etc. (1987AJ02)

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    Mg, etc. (1987AJ02) (Not observed) See (1977CE05), (1986AN07) and (1983ANZQ; theor.

  6. A=5n (1979AJ01)

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    9AJ01) (Not illustrated) 5n has not been observed: see (1972AG01) and (1977DE08

  7. A=9N (1979AJ01)

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    79AJ01) (Not illustrated) Not observed: see (1974IR04, 1975BE31, 1976IR1B

  8. A=20N (1983AJ01)

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    3AJ01) (Not illustrated) 20N is particle stable: see (1972AJ02). Assuming that the atomic mass excess is 22.0 MeV, 20N is then stable with respect to 19N + n by 1.94 MeV (see 19N). See also (1978AJ03

  9. Nippon Yusen KK NYK Link | Open Energy Information

    Open Energy Info (EERE)

    Link Jump to: navigation, search Name: Nippon Yusen KK (NYK Link) Place: Tokyo, Tokyo, Japan Zip: 100-0005 Sector: Solar Product: Logistics and shipping company moving to use...

  10. A=12He (1990AJ01)

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    90AJ01) (Not illustrated) 12He has not been observed. See (1987PE1C), (1987FL1A) and (1985PO10; theor

  11. A=5n (1974AJ01)

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    4AJ01) (Not illustrated) 5n has not been observed in the interaction of - and 14N and 16O: see (1972AG01...

  12. A=19Mg (1978AJ03)

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    8AJ03) (Not illustrated) 19Mg has not been observed: for estimates of its mass excess see (1976WA18

  13. PPaAJ~f~-"'

    Office of Legacy Management (LM)

    - PgOPO6bt OF MURD . COls'iRACT AT(lI&1)-140~ FIlli ml3 (31EXIUL CON6'E'JCTICB :i:, cbp, ., ,,. ._. SBMOL: "' PPaAJ~f~-"' :: "' ~ .' ., .~ : c !. .: ..:.. ..~ : ,. r. :;: A?TiL.C?@!, " ' If. D&do& . . . . . .' .' :: ,,,, A&g.?% Tigs mwonodum raquosts mat a cmtnot with (ho chwloal Cmetructlm Cerp.. bo jinqmrod la aw~danao with inforwtla hemlaaf4.r se4 fstb. Ski? mebere&dw proadsa a empfste reaord oizthe aego4Aa4lws leadia~ $e'the'prop~d OcDtrrrot and alro

  14. A=10F (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01). (1985WA02) suggest 39.7 ± 0.4 MeV for the atomic mass excess of 10N. See also (1982KA1D, 1983ANZQ, 1987BL18, 1987SA15

  15. A=10N (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01). (1985WA02) suggest 39.7 ± 0.4 MeV for the atomic mass excess of 10N. See also (1982KA1D, 1983ANZQ, 1987BL18, 1987SA15

  16. A=10Ne (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01). (1985WA02) suggest 39.7 ± 0.4 MeV for the atomic mass excess of 10N. See also (1982KA1D, 1983ANZQ, 1987BL18, 1987SA15

  17. A=10O (1988AJ01)

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    8AJ01) (Not illustrated) Not observed: see (1979AJ01). (1985WA02) suggest 39.7 ± 0.4 MeV for the atomic mass excess of 10N. See also (1982KA1D, 1983ANZQ, 1987BL18, 1987SA15

  18. A=14F (1981AJ01)

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    81AJ01) (Not illustrated) 14F has not been observed: its atomic mass excess is predicted to be 32.98 MeV (1978GU10) which would make it unstable with respect to decay into 13O + p by 2.58 MeV. See also (1976AJ0

  19. A=14F (1986AJ01)

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    86AJ01) (Not illustrated) 14F has not been observed: its atomic mass excess is predicted to be 32.98 MeV which would make it unstable with respect to decay into 13O + p by 2.58 MeV: see (1981AJ01). See also (1985WA02) and (1983ANZQ

  20. A=14F (1991AJ01)

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    91AJ01) (Not illustrated) 14F has not been observed: its atomic mass excess is predicted to be 32.98 MeV which would make it unstable with respect to decay into 13O + p by 2.58 MeV: see (1981AJ01). See also (1986AN07

  1. A=14Li (1986AJ01)

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    86AJ01) (Not illustrated) 14Li has not been observed. The calculated mass excess is 72.29 MeV: see (1981AJ01). 14Li is then particle unstable with respect to decay into 13Li + n and 12Li + 2n by 3.88 and 3.22 MeV, respectively

  2. A=15Li (1986AJ01)

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    6AJ01) (Not illustrated) 15Li has not been observed. Its atomic mass excess is calculated to be 81.60 MeV: see (1981AJ01). It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, repsectively

  3. A=15N (1986AJ01)

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    6AJ01) (See Energy Level Diagrams for 15N) GENERAL: See also (1981AJ01) and Table 15.4 Table of Energy Levels (in PDF or PS) here. Nuclear models:(1983PI03, 1983SH38, 1983VA31,...

  4. A=13C (1986AJ01)

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    6AJ01) (See Energy Level Diagrams for 13C) GENERAL: See also (1981AJ01) and Table 13.4 Table of Energy Levels (in PDF or PS). Nuclear models: (1982KU1B, 1983JA09, 1983SH38,...

  5. A=8n (1988AJ01)

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    8AJ01) (Not illustrated) 8n has not been observed in the interaction of 700 MeV or of 400 GeV protons with uranium: see (1979AJ01). See also (1987FL1A) and (1987SIZX; theor....

  6. A=18Na (1987AJ02)

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    7AJ02) (Not observed) 18Na has not been observed; its atomic mass excess has been estimated to be 25.32 MeV; it is then unbound with respect to proton emission by 1.6 MeV: see (1978AJ03). See also (1986AN07) and (1983ANZQ

  7. A=19B (1983AJ01)

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    3AJ01) (Not illustrated) Assuming the atomic mass excess to be 60.1 MeV [see (1978AJ03)], 19B is stable with respect to breakup into 18B + n by 1.8 MeV and into 17B + 2n by 0.4 MeV

  8. A=20B (1983AJ01)

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    3AJ01) (Not illustrated) 20B has not been observed. The mass excess is predicted to be 69.08 MeV (1974TH01). 20B is then unstable with respect to breakup into 19B + n by 0.9 MeV [see 19B]. See also (1978AJ03

  9. A=20B (1987AJ02)

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    7AJ02) (Not observed) The mass excess of 20B is predicted to be 69.08 MeV. 20B is then unstable with respect to breakup into 19B + n by 0.9 MeV: see 19B and (1978AJ03). See also (1983ANZQ; theor.

  10. A=6H (1984AJ01)

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    4AJ01) (Not illustrated) 6H has not been observed: see (1974AJ01). The population of excited states of 6HΣ [a Σ- hyperon in resonance with a 5He core] is reported by (1982PI02). See also (1982DO1C, 1982DO04, 1982DO1M

  11. A=7H (1984AJ01)

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    4AJ01) (Not illustrated) 7H has not been observed. Attempts have been made to detect it in the spontaneous fission of 252Cf (1982AL1H) and in the 7Li(π-, π+) reaction (1981EV01, 1981SE1J, 1981SE1B). See also (1979AJ01

  12. A=12Li (1985AJ01)

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    5AJ01) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle-unstable. The calculated value of its mass excess is 52.93 MeV [see (1980AJ01)]: 12Li would then be unstable with respect to 11Li + n, 10Li + 2n and 9Li + 3n by 3.92, 2.96 and 3.76 MeV, respectively. See also (1980AJ01) and (1982KA1D, 1983ANZQ, 1984VA06

  13. A=12Li (1990AJ01)

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    90AJ01) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle unstable. The calculated value of its mass excess is 52.93 MeV [see (1980AJ01)]: 12Li would then be unstable with respect to 11Li + n ,10Li + 2n and 9Li + 3n by 4.01, 2.96 and 3.76 MeV, respectively. The ground state of 12Li is predicted to have Jπ = 2- (1988POZS, 1985PO10; theor.). See also (1980AJ01

  14. A=14Be (1981AJ01)

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    81AJ01) (See the Isobar Diagram for 14Be) 14Be has been observed in the 4.8 GeV proton bombardment of uranium; it is particle stable: see (1976AJ04). Its atomic mass excess is calculated to be 40.69 MeV. 14Be is then bound by 2.73 and 0.55 MeV, respectively, with respect to decay into 13Be + n and 12Be + 2n (1974TH01). [See (1980AJ01) for a discussion of the mass of 12Be]. See also (1976BE1G, 1976BE1V, 1977SE1D, 1979BO22

  15. A=19C (1983AJ01)

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    3AJ01) (Not illustrated) 19C has been observed in the 4.8 GeV proton bombardment of uranium: it is particle stable (1974BO05). The calculated mass excess of 19C is 32.45 MeV using the modified form of the IMME (1975JE02): 19C would then be stable with respect to decay into 18C + n by 0.53 MeV and into 17C + 2n by 4.72 MeV [see (1982AJ01) for the mass of 17C. See also (1978AJ03

  16. A=20C (1983AJ01)

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    3AJ01) (Not illustrated) 20C has been observed in the fragmentation of 213 MeV/nucleon 48Ca by Be: it is particle stable (1981ST23). Assuming the mass excess of 20C to be 37.3 MeV [see (1978AJ03)], 20C is then stable with respect to 19 + n and 18C + 2n by 3.2 and 3.75 MeV, respectively [see 18C and 19C]. See also (1978AJ03) and (1978NA07, 1981KI04

  17. A=15B (70AJ04)

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    70AJ04) 15B has been identified in the 5.3 GeV proton bombardment of uranium. It is particle stable (PO66H). See also (ZE60A, BA61F, GA66C

  18. A=16B (1971AJ02)

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    1AJ02) 16B is predicted to be unstable with respect to decay into 15B + n by 1.0 ± 0.4 MeV (1966GA25

  19. A=17B (1971AJ02)

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    1AJ02) (Not illustrated) 17B has not been observed. (1966GA25) predict that it is unbound with respect to decay into 15B + 2n by 4.0 MeV. See also (1960ZE03

  20. A=13Be (70AJ04)

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    70AJ04) (Not illustrated) The light nuclei observed, by particle-identification techniques, to be emitted in the 5.5 GeV proton bombardment of uranium do not include 13Be. It is...

  1. A=15N (1991AJ01)

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    Diagrams for 15N) GENERAL: See also (1986AJ01) and Table Prev. Table 15.4 preview 15.4 Table of Energy Levels (in PDF or PS) here. Nuclear models:(1985KW02, 1985PH01,...

  2. A=12N (1975AJ02)

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    for 12N) GENERAL: See also (1968AJ02) and Table 12.25 Table of Energy Levels (in PDF or PS). Model calculations: (1973HA49, 1973KU1L, 1973SA30). Muon and neutrino interactions:...

  3. A=12B (1980AJ01)

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    p)12B Qm -6.886 See (1968AJ02). 7. 9Be(7Li, )12B Qm 10.462 Observed -particle groups are displayed in Table 12.3 (in PDF or PS). Angular distributions have been...

  4. A=14C (1986AJ01)

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    1 for E(7Li) 2 to 20 MeV: it is suggested that they are due to a forward-direction cluster transfer process: see (1976AJ04) for references. The elastic scattering has been...

  5. A=7H (1974AJ01)

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    4AJ01) (Not illustrated) A search for 7H in 7Li(π-, π+)7H was unsuccessful (1965GI10). See also (1968CE1A

  6. A=7H (1979AJ01)

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    9AJ01) (Not illustrated) A search for 7H in 7Li(π-, π+)7H was unsuccessful (1965GI10). See also (1975BE31, 1977SP1B; theor.

  7. A=7He (1984AJ01)

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    4AJ01) (See the Isobar Diagram for 7He) GENERAL: See also (1979AJ01) and Table 7.1 [Table of Energy Levels] (in PDF or PS). Reactions involving pions: (1978FU09, 1979BA1M, 1979PE1C). Hypernuclei: (1978DA1A, 1978SO1A, 1979BU1C, 1981WA1J, 1982KO11). Other topics: (1979BE1H, 1981AV02, 1982AW02, 1982NG01). 1. 7Li(π-, γ)7He Qm = 128.36 See (1979AJ01). 2. 7Li(n, p)7He Qm = -10.42 At En = 14.8 MeV a proton group is reported corresponding to 7Heg.s.: Γ < 0.2 MeV: see (1979AJ01). See also

  8. A = 15Be (1986AJ01)

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    6AJ01) (Not illustrated) 15Be has not been observed. The calculated mass excess is 51.18 MeV: see (1981AJ01). It is calculated to be particle unstable with respect to decay into 14Be + n by 2.42 MeV. The binding energy of 13Be + 2n is +0.31 MeV. See also (1981SE06, 1983ANZQ; theor.

  9. A=10C (1979AJ01)

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    9AJ01) (See Energy Level Diagrams for 10C) GENERAL: See also (1974AJ01) and Table 10.22 [Table of Energy Levels] (in PDF or PS). Model calculations: (1974IR04, 1976IR1B). Special reactions (See also reaction 2 in (1974AJ01).): (1973BA81, 1974RI1A, 1975BA1Q, 1976BE1K, 1976BU16, 1977AR06). Pion reactions (See also reactions 3 and 9 here.): (1975GI1B, 1975RE01, 1977HO1B, 1977WA02, 1978AM01). Astrophysical questions: (1972PA1C, 1976VI1A, 1977SI1D). Other topics: (1974IR04, 1976IR1B, 1976VO1C).

  10. A=12Be (1980AJ01)

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    80AJ01) (See Energy Level Diagrams for 12Be) GENERAL: See also (1975AJ02) and Table 12.1 [Table of Energy Levels] (in PDF or PS). Special reactions: (1975VO09, 1977AR06, 1979NA1E). General reviews: (1973TO16, 1974CE1A). Theoretical papers: (1975BE31, 1976BA24, 1976BE1G, 1976IR1B, 1977SE1D). Mass of 12Be: The Q-value of the 10Be(t, p) reaction (-4809 ± 15 keV) (1978AL29) leads to an atomic mass excess of 25078 ± 15 keV for 12Be which we adopt. See also (1975AJ02, 1975JE02). 1. 12Be(β-)12B Qm =

  11. A=13Li (1991AJ01)

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    91AJ01) (Not illustrated) 13Li has not been observed: see (1986AJ01). The calculated value of its mass excess is 60.34 MeV [see (1981AJ01)]: 13Li would then be unstable with respect to 11Li + 2n by 3.34 MeV. (1985PO10) calculate [in a (0 + 1)ℏω model space] that the first four states of 13Li at 0, 1.42, 2.09 and 2.77 MeV have, respectively, Jπ = 3/2-, 7/2-, 1/2-, 5/2-. See also (1987PE1C, 1989OG1B) and (1988POZS, 1988ZV1A

  12. A=13O (1991AJ01)

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    91AJ01) (See the Isobar Diagram for 13O) GENERAL: (1985AN28, 1986AN07, 1987SA15, 1989AYZU). See also (1986AJ01) and Table Prev. Table 13.21 preview 13.21 [Table of Energy Levels] (in PDF or PS) here. Mass of 13O: We adopt the atomic mass excess of 23113 ± 10 keV of (1988WO1C). See also (1981AJ01). 13O is then bound with respect to 12N + p and 11C + 2p by 1.514 and 2.115 MeV, respectively. 1. 13O(β+)13N Qm = 17.767 The half-life of 13O has been reported to be 8.7 ± 0.4 ms (1965MC09), 8.95 ±

  13. A=16F (1977AJ02)

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    7AJ02) (See Energy Level Diagrams for 16F) GENERAL: See also (1971AJ02) and Table 16.27 [Table of Energy Levels] (in PDF or PS). See (1972JA14, 1973LA1G, 1973LA1H, 1973RO1R, 1974VA24, 1975BE31). 1. (a) 14N(3He, n)16F Qm = -0.969 (b) 14N(3He, np)15O Qm = -0.421 Observed neutron groups and L-values derived from angular distribution measurements are displayed in Table 16.28 (in PDF or PS) [(1973BO50); E(3He) = 13 MeV]. See (1971AJ02) for the eariler work. See also (1971ADZZ, 1975OT01). For reaction

  14. A=16F (1982AJ01)

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    82AJ01) (See Energy Level Diagrams for 16F) GENERAL: See also (1977AJ02) and Table 16.25 [Table of Energy Levels] (in PDF or PS). See (1977LA04, 1977SI1D, 1978WO1E, 1980HA35, 1981OS04). 1. (a) 14N(3He, n)16F Qm = -0.969 (b) 14N(3He, np)15O Qm = -0.421 Observed neutron groups and L-values derived from angular distribution measurements are displayed in Table 16.26 (in PDF or PS) (1973BO50). For the results from reaction (b) see Table 16.26 (in PDF or PS) (1976OT02). See also (1977AJ02). 2.

  15. A=17Ne (1977AJ02)

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    7AJ02) (See the Isobar Diagram for 17Ne) GENERAL: See also (1971AJ02) and Table 17.20 [Table of Energy Levels] (in PDF or PS). Theory and reviews: (1971HA1Y, 1973HA77, 1973RE17, 1975BE31). Mass of 17Ne: The mass excess of 17Ne, determined from a measurement of the Q-value of 20Ne(3He, 6He)17Ne is 16.48 ± 0.05 MeV (1970ME11, 1972CE1A). Then 17Ne - 17F = 14.53 MeV and Eb for p, 3He and α are, respectively, 1.50, 6.46 and 9.05 MeV. See also (1971AJ02). 1. (a) 17Ne(β+)17F* → 16O + p Qm = 13.93

  16. A=17Ne (1982AJ01)

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    82AJ01) (See the Isobar Diagram for 17Ne) GENERAL: See (1977AJ02) and Table 17.22 [Table of Energy Levels] (in PDF or PS). Theory and reviews:(1975BE56, 1977CE05, 1978GU10, 1978WO1E, 1979BE1H). Other topics:(1981GR08). Mass of 17Ne: The mass excess adopted by (1977WA08) is 16.478 ± 0.026 MeV, based on unpublished data. We retain the mass excess 16.48 ± 0.05 MeV based on the evidence reviewed in (1977AJ02). 1. (a) 17Ne(β+)17F* → 16O + p Qm = 13.93 (b) 17Ne(β+)17F Qm = 14.53 The half-life of

  17. A=17Ne (1986AJ04)

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    6AJ04) (See the Isobar Diagram for 17Ne) GENERAL: See (1982AJ01) and Table 17.20 [Table of Energy Levels] (in PDF or PS). Theory and reviews: (1983ANZQ, 1983AU1B, 1985AN28). 1. (a) 17Ne(β+)17F* → 16O + p Qm = 13.93 (b) 17Ne(β+)17F Qm = 14.53 The half-life of 17Ne is 109.0 ± 1.0 msec (1971HA05). Earlier values (see (1971AJ02)) gave a mean value of 108.0 ± 2.7 msec. The decay is primarily to the proton unstable states of 17F at 4.70, 5.52 and 6.04 MeV with Jπ = 3/2-, 3/2- and 1/2-: see

  18. A=18C (1983AJ01)

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    83AJ01) (Not illustrated) The mass of 18C has been determined in studies of the 18O(π-, π+)18C reaction at Eπ = 164 MeV (1978SE07) and of the 48Ca(18O, 48Ti)18C reaction at E(18O) = 100 MeV (1982NA04): the weighted mean of the atomic mass excess is 24.89 ± 0.14 MeV. 18C is bound with respect to particle decay by 4.20 MeV for 17C + n and 4.94 MeV for 16C + 2n. [For masses of 16C, 17C see (1982AJ01)]. For the earlier work on 18C see (1978AJ03). See also (1980NA1D, 1981SE1B) and (1981KI04

  19. A=18N (1987AJ02)

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    7AJ02) (See the Isobar Diagram for 18N) GENERAL: See (1983AJ01) and Table 18.2 [Table of Energy Levels] (in PDF or PS). See (1981NA1H, 1983ANZQ, 1983FR1A, 1983SH44, 1983WI1A, 1984AS1D, 1984HI1A, 1986AN07, 1986BI1A, 1986HA1B, 1986MA48, 1986ME1F, 1987RI03). Mass of 18N:The atomic mass excess derived from the Q-value of the 18O(7Li, 7Be)18N reaction is 13.117 ± 0.020 MeV (1983PU01). 18N is then stable with respect to breakup into 17N + n by 2.825 MeV. See (1983AJ01) for the earlier work. 1.

  20. A=20C (1987AJ02)

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    7AJ02) (Not illustrated) 20C has been observed in the fragmentation of 60 MeV/A argon ions: its mass excess is 37.20 ± 1.13 MeV (1987GI1E). It is then stable with respect to 19C + n and 18C + 2n by 3.3 and 3.9 MeV, respectively. See also (1978AJ03, 1983AJ01). The half-life of 20C is calculated to be 9.3 × 10-3 sec (1984KL06). See also (1985AN1B, 1985LA03, 1986AN07, 1986GU1D) and (1982AV1A, 1983ANZQ, 1987SA15

  1. A=20Na (1983AJ01)

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    3AJ01) (See Energy Level Diagrams for 20Na) GENERAL: See also (1978AJ03) and Table 20.36 [Table of Energy Levels] (in PDF or PS). (1977SI1D, 1978WO1E, 1979BE1H, 1980OK01, 1981AY01). J = 2 (1975SC20); μ = 0.3694 ± 0.0002 nm (1975SC20). 1. 20Na(β+)20Ne Qm = 13.887 20Na decays by positron emission to 20Ne*(1.63) and to a number of other excited states of 20Ne: see Table 20.33 (in PDF or PS) and reaction 63 in 20Ne. The half-life of 20Na is 446 ± 3 msec; Jπ = 2+: see (1978AJ03). 2. 16O(12C,

  2. A=20Na (1987AJ02)

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    87AJ02) (See Energy Level Diagrams for 20Na) GENERAL: See (1983AJ01) and Table 20.27 [Table of Energy Levels] (in PDF or PS). (1981WA1Q, 1983ANZQ, 1983BR29, 1985AN28, 1985HA1N, 1985RO1N, 1986AN07, 1986GA1I). 1. 20Na(β+)20Ne Qm = 13.887 20Na decays by positron emission to 20Ne*(1.63) and to a number of other excited states of 20Ne: see Table 20.26 (in PDF or PS) and reaction 53 in 20Ne. The half-life of 20Na is 447.9 ± 2.3 msec [weighted mean of values quoted in (1978AJ03) and in (1983CL01)];

  3. A=5H (1984AJ01)

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    4AJ01) (Not illustrated) Attempts to study this nucleus in the 3H(t, p), 7Li(6Li, 8B) and 9Be(α, 8Be) reactions, as well as in 7Li + π- have been unsuccessful: no sharp states are observed [see (1974AJ01, 1979AJ01)]. A recent study of the spectrum of π+ from 7Li + π- suggests that 5H may be nearly stable to decay into 3H + 2n (1981SE1J). The work of (1967AD05) on the 3He(3He, n)5Be reaction suggested, on the basis of analog considerations, that 5H is unstable by more than 2.1 MeV to decay

  4. A=7B (1984AJ01)

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    4AJ01) (See the Isobar Diagram for 7B) GENERAL: (See also (1979AJ01).) See (1979BE1H, 1982NG01). Mass of 7B:This nucleus has been studied in the 7Li(π+, π-)7B and 10B(3He, 6He)7B reactions. In the (π+, π-) work (1981SE1B; preliminary) find the mass excess to be 27.80 ± 0.10 MeV and Γ for the ground state is 1.2 ± 0.2 MeV. In the earlier (3He, 6He) work [see (1974AJ01)] M-A was reported to be 27.94 ± 0.10 MeV, Γ=1.4 ± 0.2 MeV. We adopt 27.87 ± 0.10 MeV, Γ = 1.3 ± 0.2 MeV. The

  5. A=7B (1988AJ01)

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    8AJ01) (See the Isobar Diagram for 7B) The mass excess of 7B from a study of the 10B(3He, 6He)7B reaction is 27.94 ± 0.10 MeV and the width of the ground state is Γ = 1.4 ± 0.2 MeV: see (1974AJ01). 7B is unbound with respect to 6Be + p, 5Li + 2p and 4He + 3 p by 2.28, 1.68 and 3.65 MeV, respectively. The other work described in (1984AJ01) has not been published. See also (1985AN28), (1986HU1D; astrophysics) and (1982KA1D, 1983ANZQ, 1983AU1B; theor.

  6. A=7He (1988AJ01)

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    8AJ01) (See the Isobar Diagram for 7He) GENERAL: See also (1984AJ01) and Table 7.1 [Table of Energy Levels] (in PDF or PS). Hypernuclei: (1982KA1D, 1983FE07, 1984AS1D, 1985KO1G, 1986DA1B, 1986DO01, 1986ME1F). Other topics: (1983ANZQ, 1984FR13, 1984VA06, 1986GI10, 1986SH1L, 1987BO40, 1987GOZN, 1987PE1C). Mass of 7He: The atomic mass excess of 7He is 26.11 ± 0.03 MeV: 7He is then unbound with respect to decay into 6He + n by 0.44 MeV: see (1984AJ01). The ground state is calculated to have Jπ =

  7. A=8B (1984AJ01)

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    4AJ01) (See Energy Level Diagrams for 8B) GENERAL: See also (1979AJ01) and Table 8.11 [Table of Energy Levels] (in PDF or PS). Special states: (1980OK01). Complex reactions involving 8B (The reactions 6Li(6Li, 4H)8B, 12C(6Li, 10Be)8B, 9Be(7Li, 8He)8B and 12C(7Li, 11Be)8B have been studied at E(6Li) = 72 MeV and E(7Li) = 83 MeV (1982AL08): see 8He, 10Be, as well as 11Be in (1985AJ01).): (1979BO22, 1980GR10, 1981MO20). Astrophysical questions: (1981BA17, 1983LI01). Reactions involving pions: (

  8. A=8He (1979AJ01)

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    9AJ01) (See the Isobar Diagram for 8He) GENERAL: See also (1974AJ01). See (1973AL1B, 1973TO16, 1974IR04, 1974MA1E, 1975AB1D, 1975BE31, 1976BE1G, 1976IR1B, 1976VA29, 1978KO1H, 1978NA07). Mass of 8He: The atomic mass excess of 8He is 31596 ± 7 keV (1977TR07). See also (1974CE05, 1975JA10, 1975KO18, 1978RO01). 8He is then stable with respect to decay into 6He + 2n by 2.141 MeV. See also (1974AJ01, 1976TR1B) and (1975JE02; theor.). The IMME coefficients based on the latest masses of the T = 2

  9. A=8He (1984AJ01)

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    4AJ01) (See the Isobar Diagram for 8He) GENERAL: See also (1979AJ01) and Table 8.1 [Table of Energy Levels] (in PDF or PS). Complex reactions involving 8He (See (1979AJ01) for comments on the 18O(α, 8He) and 26Mg(α, 8He) reactions.): (1978VO10, 1978MA1D, 1979BE60, 1979BO22, 1980BO31, 1981BO1X, 1981SE1B, 1982BO35, 1982BO1Y, 1982GU1H, 1982OG02). Hypernuclei: (1978PO1A, 1978SO1A, 1981WA1J). Other topics: (1979BE1H, 1981AV02, 1982NG01). Mass of 8He: A study of the 64Ni(α, 8He)60Ni reaction leads

  10. A=8He (1988AJ01)

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    8AJ01) (See the Isobar Diagram for 8He) GENERAL: See also (1984AJ01) and Table 8.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1984VA06, 1985PO10, 1987BL18). Complex reactions involving 8He: (1982AL33, 1983AN13, 1985MA13, 1985TA1D, 1986SA30, 1987AR1G, 1987BO40, 1987KO1Z, 1987PE1C, 1987TAZU, 1988GA10, 1988ST06, 1988TA1A). Hypernuclei: (1982KA1D, 1983DO1B, 1984BO1H, 1985AH1A, 1985IK1A, 1986BA1W, 1986DA1B, 1987MI38, 1987PO1H). Other topics: (1983GL1B, 1985AN28, 1987AJ1A,

  11. A=9C (1988AJ01)

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    8AJ01) (See the Isobar Diagram for 9C) GENERAL: See also (1984AJ01) and Table 9.11 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1983AU1B). Complex reactions involving 9C: (1983FR1A, 1983OL1A, 1986HA1B, 1987SN01). Reactions involving pions: (1983AS1B, 1984BR22, 1985PN01). Other topics: (1982KA1D, 1985AN28, 1986AN07). Ground state of 9C: (1983ANZQ, 1983AU1B, 1985AN28, 1987SA15). 1. 9C(β+)9B Qm = 16.498 The half-life of 9C is 126.5 ± 0.9 msec: see (1974AJ01). The decay is

  12. A=10C (1988AJ01)

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    8AJ01) (See Energy Level Diagrams for 10C) GENERAL: See also (1984AJ01) and Table 10.18 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1984SA37, 1987BL18). Special states: (1986AB10). Astrophysical questions: (1987RA1D). Complex reactions involving 10C: (1983FR1A, 1983OL1A, 1986HA1B, 1987AR19, 1987BEYI, 1987RI03, 1987SN01, 1987TAZU, 1988BEYJ, 1988CA06, 1988KI05, 1988SA19). Reactions involving pions and other mesons (See also reactions 2 and 4.): (1985LI1E, 1987SI18). Other

  13. A=13B (1986AJ01)

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    6AJ01) (See Energy Level Diagrams for 13B) (Reactions on which no new work is reported are not always discussed.) GENERAL: See also (1981AJ01) and Table 13.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1981SE06, 1984VA06). Complex reactions involving 13B: (1983EN04, 1983MA06, 1983OL1A, 1983WI1A, 1984HI1A). Muon and neutrino capture and reactions: (1984KO1U). Pion capture and reactions (See also reactions 4 and 5.): (1981OS04, 1982CH16, 1983LI15). Hypernuclei: (1983FE07). Other

  14. A=13Be (1981AJ01)

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    1AJ01) (Not illustrated) 13Be has not been observed. 13Be is predicted to have an atomic mass excess of 35.35 MeV (1974TH01), 34.60 MeV (1975JE02). It is then unstable with respect to decay into 12Be + n by 2.20 MeV or by 1.45 MeV, respectively, based on the atomic mass excess of 12Be, 25.078 MeV (1978AL29). See also (1976AJ04) and (1977SE1D; theor

  15. A=13Li (1986AJ01)

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    86AJ01) (Not illustrated) 13Li has not been observed. The calculated value of its mass excess is 60.34 MeV [see (1981AJ01)]: 13Li would then be unstable with respect to 11Li + 2n by 3.26 MeV. (1980BO31) have not observed 13Li in the bombardment of 124Sn by 6.7 GeV protons but state that the statistics were poor in the region of interest and that it is not excluded that 13Li may be stable. See also (1983ANZQ

  16. A=14O (1991AJ01)

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    91AJ01) (See Energy Level Diagrams for 14O) GENERAL: See also (1986AJ01) and Table Prev. Table 14.22 preview 14.22 [Table of Energy Levels] (in PDF or PS) here. Nuclear models: (1985BA75, 1987BL15). Electromagnetic transitions: (1989RA16, 1989SP01). Astrophysical questions: (1985TA1A, 1987RA1D). Applied work: (1989AR1J). Complex reactions involving 14O: (1987PE1C, 1988ST1D, 1989BA92, 1989DR03, 1989KI13). Reactions involving pions (See also reactions 5 and 7.): (1986BA1C, 1986BO1N, 1986FO06,

  17. A=15Be (1991AJ01)

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    91AJ01) (Not illustrated) 15Be has not been observed. The calculated mass excess is 51.18 MeV: see (1981AJ01). 15Be is then unstable with respect to 14Be + n and 13Be + 2n by 3.4 and 0.04 MeV, respectively. (1985PO10) calculate [in a (0 + 1))ℏω model space] that the first four states of 15Be at 0, 0.07, 2.32, 3.10 MeV have, respectively, Jπ = 5/2+, 3/2+, 9/2+, 7/2+. See also (1987SA15; theor

  18. A=18Ne (1978AJ03)

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    8AJ03) (See Energy Level Diagrams for 18Ne) GENERAL: See also (1972AJ02) and Table 18.22 [Table of Energy Levels] (in PDF or PS). Model calculations: (1972EN03, 1974LO04). Electromagnetic transitions: (1970SI1J, 1972EN03, 1974LO04, 1976SH04, 1977BR03, 1977SA13). Special states: (1972EN03, 1972RA08). Muon- and pion-induced capture and reactions (See also reaction 5.): (1972MI11, 1974LI1N, 1975LI04, 1976HE1G, 1977MA2Q, 1977RO1U). Other theoretical calculations: (1970SI1J, 1972CA37, 1972RA08,

  19. A=18Ne (1983AJ01)

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    83AJ01) (See Energy Level Diagrams for 18Ne) GENERAL: See also (1978AJ03) and Table 18.21 [Table of Energy Levels] (in PDF or PS). Model calculations: (1979DA15, 1979SA31, 1980ZH01). Electromagnetic transitions: (1977HA1Z, 1979SA31, 1982LA26). Special states: (1977HE18, 1978KR1G, 1979DA15, 1979SA31, 1980OK01, 1982ZH1D). Astrophysical questions: (1978WO1E). Complex reactions involving 18Ne: (1979HE1D). Pion-induced capture and reactions (See also reaction 6.): (1977PE12, 1977SP1B, 1978BU09,

  20. A=18Ne (1987AJ02)

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    7AJ02) (See Energy Level Diagrams for 18Ne) GENERAL: See (1983AJ01) and Table 18.22 [Table of Energy Levels] (in PDF or PS). Model calculations:(1982ZH01, 1983BR29, 1984SA37, 1985RO1G). Special states:(1982ZH01, 1983BI1C, 1983BR29, 1984SA37, 1985RO1G, 1986AN10, 1986AN07). Electromagnetic transitions:(1982BR24, 1982RI04, 1983BR29, 1985AL21, 1986AN10). Astrophysical questions:(1982WI1B, 1987WI11). Complex reactions involving 18Ne:(1986HA1B). Pion capture and reactions (See also reaction

  1. A=19Na (1983AJ01)

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    3AJ01) (See the Isobar Diagram for 19Na) A study of this nucleus via the 24Mg(3He, 8Li)19Na reaction at E(3He) = 76.3 MeV leads to an atomic mass excess of 12.928 ± 0.012 MeV for 19Na; it is then unstable with respect to breakup into 18Ne + p by 320 ± 13 keV. An excited state at Ex = 120 ± 10 keV is also reported (1975BE38). See also (1978AJ03, 1978GU10, 1979BE1H

  2. A=19Ne (1978AJ03)

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    8AJ03) (See Energy Level Diagrams for 19Ne) GENERAL: See (1972AJ02) and Table 19.24 [Table of Energy Levels] (in PDF or PS). Nuclear models: (1972EN03, 1972NE1B, 1972WE01, 1973DE13, 1977BU05). Electromagnetic transitions: (1972EN03, 1972LE06, 1973HA53, 1973PE09, 1977BU05). Special states: (1972EN03, 1972GA14, 1972HI17, 1972NE1B, 1972WE01, 1977BU05, 1977SC08). Complex reactions involving 19Ne: (1976HI05, 1977BU05). Astrophsyical questions: (1973CL1E). Muon capture: (1972MI11). Pion capture and

  3. A=8B (1988AJ01)

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    8AJ01) (See Energy Level Diagrams for 8B) GENERAL: See also (1984AJ01) and Table 8.9 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1983SH38). Special states: (1982PO12, 1988KH03). Complex reactions involving 8B: (1982AL08, 1983OL1A, 1984GR08, 1986HA1B, 1987TAZU, 1988AR05, 1988KI05). Astrophysical questions: (1984HA1B, 1985BO1E, 1985GI1C, 1985KL1A, 1985LA1C, 1988BA86). Reactions involving pions: (1983SP06). Hypernuclei: (1983SH38). Other topics: (1985AN28). Ground state of

  4. A=9C (1984AJ01)

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    4AJ01) (See the Isobar Diagram for 9C) GENERAL: (See also (1979AJ01) for other references in this category and for some reactions on which no new work has been done.) and Table 9.12 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1979LA06). Complex reactions involving 9C: (1981MO20). Reactions involing pions: (1979AS01, 1979NA1E, 1980BU15, 1983HU02). Other topics: (1979BE1H, 1979LA06, 1982NG01). Mass of 9C: The recent Q0 value for the 12C(3He, 6He)9C reaction (see reaction 3)

  5. A=9He (1979AJ01)

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    9AJ01) (Not illustrated) 9He has not been observed: see (1974AJ01). It is predicted to be particle unstable. Particle instability with respect to 8He + n, 7He + 2n and 6He + 3n implies atomic mass excesses greater than 39.667, 42.253 and 41.808 MeV, respectively. The calculated mass excess of 9He is 43.49 MeV based on the modified form of the mass equation (1975JE02). See also (1974TH01) and (1974IR04, 1975BE31, 1976IR1B; theor.

  6. A=9He (1984AJ01)

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    4AJ01) (Not illustrated) 9He has been observed in the 9Be(π-, π+)9He reaction at Eπ- = 194 MeV; the atomic mass excess is 40.81 ± 0.12 MeV. 9He is then unstable with respect to decay into 8He + n by 1.14 MeV (1981SE1B, 1980NA1D, 1980SE1C, 1980SE1F). See also (1979AJ01) and (1982PO1C; hypernuclei) and (1982NG01; theor

  7. A=13O (1986AJ01)

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    See also (1981AJ01) and (1981KO27; theor.). 2. 12C(p, -)13O Qm -155.389 At Ep 613 MeV the ground state of 13O and an excited state at Ex 2.82 0.24 MeV are...

  8. A=18C (1978AJ03)

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    MeV 22Ne ions (1975VO09) and in the 4.8 GeV proton irradiation of uranium (1974BO05). At Ep 4.8 GeV, the production cross section is 100 b (1974BO05). See also (1972AJ02)....

  9. A=17N (1977AJ02)

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    See also (1971AJ02) and Table 17.1 Table of Energy Levels (in PDF or PS). Theory and reviews: (1973PA1F, 1973RE17, 1973TO16, 1973WI15, 1974HA61, 1975BE31). Experimental...

  10. A=17N (1986AJ04)

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    (1982AJ01) and Table 17.1 Table of Energy Levels (in PDF or PS). Theoretical papers and reviews: (1983ANZQ, 1983AU1B, 1983EN04, 1983FR1A, 1983MA06, 1983WI1A, 1984AS1D, 1984BA24,...

  11. A=17N (1982AJ01)

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    (1977AJ02) and Table 17.1 Table of Energy Levels (in PDF or PS). Theoretical papers and reviews:(1978KR19, 1979AL22, 1979BE1H, 1979BO22, 1980MI1G, 1981OS04). Experimental...

  12. A=16O (1977AJ02)

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    for 16O) GENERAL: See also (1971AJ02) and Table 16.9 Table of Energy Levels (in PDF or PS). Shell model: (1969BO1B, 1969FE1A, 1969IK1A, 1969WI1C, 1970BO33, 1970BO1J,...

  13. A=15N (1976AJ04)

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    for 15N) GENERAL: See also (1970AJ04) and Table 15.4 Table of Energy Levels (in PDF or PS) here. Shell model: (1968GO01, 1969UL03, 1970CO1H, 1970FR11, 1970GO1H, 1970HS02,...

  14. A = 16O (1986AJ04)

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    for 16O) GENERAL: See also (1982AJ01) and Table 16.10. Table of Energy Levels (in PDF or PS) here. Shell model: (1978WI1B, 1981AN18, 1981BR16, 1981CO1X, 1981DE2G, 1981FO12,...

  15. A=16O (1982AJ01)

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    for 16O) GENERAL: See also (1977AJ02) and Table 16.11 Table of Energy Levels (in PDF or PS). Shell model: (1976AP01, 1976BE1W, 1976NA1L, 1977AP01, 1977BR26, 1977CA02,...

  16. A=16O (71AJ02)

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    Diagrams for 16O) GENERAL: See also (59AJ76) and Table 16.9 Table of Energy Levels (in PDF or PS). Shell model: (WI57H, BR59M, FE59C, PA59A, TA60H, TA60L, BA61N, TR61, BA62F,...

  17. A=14N (1986AJ01)

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    for 14N) GENERAL: See also (1981AJ01) and Table 14.12 Table of Energy Levels (in PDF or PS) here. Nuclear models: (1983KA1K, 1983SH38, 1983VA31, 1984AS07, 1984VA06,...

  18. A = 15Be (1981AJ01)

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    1AJ01) (Not illustrated) 15Be has not been observed. It is calculated to be particle unstable with respect to decay into 14Be + n by 2.42 MeV. The binding energy of 13Be + 2n is +0.31 MeV. The calculated mass excess is 51.18 MeV (1974TH01

  19. A=11Li (68AJ02)

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    68AJ02) (See the Isobar Diagram for 11Li) 11Li has been identified in the 5.3 GeV proton bombardment of uranium. It is particle stable (PO66H). See also (GA66C, CO67A

  20. A=14F (1976AJ04)

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    76AJ04) (Not illustrated) 14F has not been observed: its atomic mass excess is predicted to be 33.38 MeV which would make it unstable with respect to decay into 13O + p by ≈ 3 MeV (1973BA3

  1. A=14Li (1976AJ04)

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    76AJ04) (Not illustrated) 14Li has not been observed: it is calculated to be particle unstable with a binding energy of -2.66 MeV for decay into 13Li + n and of -3.23 MeV for decay into 12Li + 2n. The calculated mass excess is 72.29 MeV (1974TH01)

  2. A=15F (1976AJ04)

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    76AJ04) (Not illustrated) 15F has not been observed. It is predicted to be unstable with respect to proton emission by 2.32 MeV: the mass excess of 15F is then 17.62 MeV (1966KE16). See also (1972WA07

  3. A=15F (59AJ76)

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    59AJ76) (Not illustrated) Mass of 15F: Calculation of Coulomb and (n - 1H) mass differences from 15C indicates that 15F should be unstable to proton emission by 2.3 MeV (MU57A): the mass excess of 15F is 22.0 ± 1 MeV

  4. A=15F (70AJ04)

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    70AJ04) Mass of 15F: A calculation using an isobaric mass formula predicts that 15F is unstable with respect to proton emission by 2.32 MeV: the mass excess of 15F is then 17.62 MeV (KE66C). See also (MU57A, BA61F

  5. A=15Li (1976AJ04)

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    76AJ04) (Not illustrated) 15Li has not been observed: its atomic mass excess is calculated to be 81.60 MeV. It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, respectively (1974TH01)

  6. A=15Li (1981AJ01)

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    1AJ01) (Not illustrated) 15Li has not been observed: its atomic mass excess is calculated to be 81.60 MeV. It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, respectively (1974TH01). See also 13Li

  7. A=18B (1978AJ03)

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    78AJ03) (Not illustrated) 18B has not been observed: it is predicted to have a mass excess of 53.85 MeV. 18B is then unstable with respect to 17B + n by 1.39 MeV (1976JA23; and see (1976WA18)). See also (1974TH01) and (1975BE31; theor.

  8. A=18B (1983AJ01)

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    3AJ01) (Not illustrated) 18B has not been observed: it is predicted to have a mass excess of 53.85 MeV. 18B is then unstable with respect to 17B + n by 1.4 MeV (1976JA23

  9. A=10Be (1979AJ01)

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    Special levels: (1974IR04, 1976IR1B, 1977JA14). Electromagnetic transitions: (1976VO1C, ... 0.2) 106 y; log ft 13.42: see (1974AJ01). The spectrum is of the D2 type (1950WU1A). ...

  10. A=14Be (1991AJ01)

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    +)14B reaction (1984GI09), in the interaction of 30 MeVA 18O ions with 181Ta (1986CU01) and in the spallation of thorium by 800 MeV protons (1988WO09). See also (1986AJ01). ...

  11. A=11B (1990AJ01)

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    a broad maximum at E 5.1 MeV (max 40 mb) is observed (1984OL05). For the earlier work see Table 11.7 (in PDF or PS) in (1980AJ01) and Table 11.7 (in PDF or PS) in...

  12. A=11Li (1975AJ02)

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    by GeV protons. Its mass excess is 40.9 0.1 MeV (1973KL1C). 11Li is bound: Eb for breakup into 9Li + 2n and 10Li + n are 0.2 and 0.3 MeV, respectively see (1974AJ01) for a...

  13. A=10Li (1988AJ01)

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    MeV) corresponds to the ground state. 10Lig.s. would then be unbound with respect to breakup into 9Li + n by 0.80 0.25 MeV: see (1979AJ01). See also (1986GI10, 1987AB15),...

  14. A=15F (1986AJ01)

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    atomic mass excess of 15F is 16.77 0.13 MeV. 15F is unstable with respect to breakup into 14O + p by 1.47 MeV: see (1981AJ01). 1. 12C(3He, -)15F Qm -141.41 This...

  15. A=13Be (1986AJ01)

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    the atomic mass excess of 13Be is 35.0 0.5 MeV. It is then unstable with respect to breakup into 12Be + n by 1.9 MeV (1983AL20). See also (1981AJ01), (1984BE1C) and (1981SE06,...

  16. A=18Be (1987AJ02)

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    have a mass excess of 78.43 MeV: see (1978AJ03). 18Be is then unstable with respect to breakup into 16Be + 2n, 15Be + 3n, 14Be + 4n, 13Be + 5n, 12Be + 6n, 11Be + 7n and 10Be + 8n...

  17. A=16Ne (1977AJ02)

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    predicts M - A 25.15 0.6 MeV (1968CE1A); 16Ne is then unbound with respect to breakup into 14O + 2p by 2.6 MeV: see (1971AJ02) for the earlier work. See also (1972WA07)...

  18. A=15F (1991AJ01)

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    15FThe atomic mass excess of 15F is 16.77 0.13 MeV. 15F is unstable with respect to breakup into 14O + p by 1.47 MeV: see (1981AJ01). 1. 12C(3He, -)15F Qm -141.41 This...

  19. A=17Be (1986AJ04)

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    is calculated to be 70.67 MeV: see (1977AJ02). It is then unstable with respect to breakup into 16Be + n and 15Be + 2n by 3.38 and 3.35 MeV, respectively. See also (1983ANZQ;...

  20. A=16Be (1986AJ04)

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    atomic mass excess is calculated to be 59.22 MeV. It is then unstable with respect to breakup into 14Be + 2n by 2.98 MeV: see (1974TH01, 1986AJ01). The first three excited states...

  1. A=10n (1979AJ01)

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    79AJ01) (Not illustrated) 10n has not been observed in the interaction of 0.7 and 400 GeV protons with uranium: the cross section is < 0.7 10-5 b (1977TU02) at 0.7 GeV and <...

  2. A=10n (1984AJ01)

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    4AJ01) (Not illustrated) 10n has not been observed in the interaction of 0.7 and 400 GeV protons with uranium: the cross section is < 0.7 10-5 mb (1977TU02) at 0.7 GeV and < 0.5...

  3. A=12n (1980AJ01)

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    0AJ01) (Not illustrated) 12n has not been observed in the interaction of 0.7 and 400 GeV protons with uranium: the cross section is < 1.0 10-5 b (1977TU02) and 0.7 GeV and <...

  4. A=6n (1984AJ01)

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    6n (1984AJ01) (Not illustrated) 6n has not been observed in the interaction of 700 MeV protons or of 400 GeV protons with uranium: the cross section is < 1.1 10-3 b (1977TU02;...

  5. A=8n (1979AJ01)

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    79AJ01) (Not illustrated) 8n has not been observed in the interaction of 0.7 and 400 GeV protons with uranium: the cross section is < 2.3 10-5 b (1977TU02) at 0.7 GeV and <...

  6. A=8n (1984AJ01)

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    4AJ01) (Not illustrated) 8n has not been observed in the interaction of 700 MeV or of 400 GeV protons with uranium: the cross section is < 2.3 10-5 b (1977TU02; 700 MeV), <...

  7. A=6n (1979AJ01)

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    79AJ01) (Not illustrated) 6n has not been observed in the interaction of 700 MeV protons or of 400 GeV protons with uranium: the cross section is < 1.1 10-3 b (1977TU02; 700...

  8. A=18Na (1972AJ02)

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    2AJ02) (Not illustrated) A calculation using an isobaric mass formula predicts that the mass excess of 18Na is 25.4 ± 0.4 MeV (1966KE16): 18Na is then unbound with respect to proton emission by 1.6 MeV. See also (1965JA1C

  9. A=18Na (1978AJ03)

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    8AJ03) (Not illustrated) 18Na has not been observed: its atomic mass excess has been estimated to be 25.32 MeV: it is then unbound with respect to proton emission by 1.55 MeV (1977WA08). See also (1976JA23, 1976WA1E

  10. A=18Na (1983AJ01)

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    3AJ01) (Not illustrated) 18Na has not been observed: its atomic mass excess has been estimated to be 25.32 MeV: it is then unbound with respect to proton emission by 1.55 MeV (1977WA08). See also (1978GU10

  11. A=19C (1972AJ02)

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    2AJ02) (Not illustrated) 19C may have been observed in the 3 GeV proton bombardment of a 197Au target: if so it is particle stable (1970RA1A). Its mass excess must then be < 37.9 MeV (18C + n). See also (1960ZE03, 1971BU1E

  12. A=20B (1978AJ03)

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    78AJ03) (Not illustrated) 20B has not been observed. The mass excess is predicted to be 69.08 MeV (1974TH01). 20B is then unstable with respect to breakup into 19B + n by 0.9 MeV [see 19B]. See also (1976JA23, 1976WA18) and (1975BE31; theor.

  13. A=20N (1972AJ02)

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    2AJ02) (Not illustrated) 20N has been observed in the bombardment of 232Th by 122 MeV 18O ions (1969AR13, 1970AR1D) and in the 3 GeV proton bombardment of 197Au (1970RA1A): it is particle stable. See also (1960ZE03, 1961BA1C, 1971BU1E

  14. A=5Be (1988AJ01)

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    1988AJ01) (See the Isobar Diagram for 5Be) The absence of any group structure in the neutron spectrum in the reaction 3He(3He, n)5Be at E(3He) = 18.0 to 26.0 MeV indicates that 5Be(0)

  15. A=10B (1979AJ01)

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    9AJ01) (See Energy Level Diagrams for 10B) GENERAL: See also (1974AJ01) and Table 10.5 [Table of Energy Levels] (in PDF or PS). Shell and deformed models: (1973BO1C, 1974BO29, 1974BO54, 1974BO1P, 1975DI04, 1977JA14). Cluster and α-particle models: (1976GA34, 1977NA20, 1977OK1C). Special levels: (1974BO29, 1974BO1P, 1974IR04, 1974NI1A, 1975DI04, 1976GA34, 1976IR1B, 1977BI1D, 1977JA14, 1977NA20). Electromagnetic transitions: (1974BO29, 1974BO54, 1974BO1P, 1974HA1C, 1974MU13, 1977BO1V, 1977DO06,

  16. A=10B (1984AJ01)

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    4AJ01) (See Energy Level Diagrams for 10B) GENERAL: See also (1979AJ01) and Table 10.5 [Table of Energy Levels] (in PDF or PS). Shell and deformed models: (1978FU13, 1979FL06, 1979KU05, 1980NI1F, 1981BO1Y, 1981DE2G, 1982BA52). Cluster and α-particle models: (1979AD1A, 1980FU1G, 1980NI1F, 1980OK1B, 1981KR1J, 1983RO1G). Special states: (1979FL06, 1980BR21, 1980FU1G, 1980NI1F, 1980OK1B, 1980RI06, 1981BA64, 1981BO1Y, 1981DE2G, 1981KU04, 1981SE06, 1982BA52, 1983GO1R). Electromagnetic tranisitions

  17. A=10B (1988AJ01)

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    8AJ01) (See Energy Level Diagrams for 10B) GENERAL: See also (1984AJ01) and Table 10.5 [Table of Energy Levels] (in PDF or PS). Shell and deformed models: (1983VA31, 1984VA06, 1984ZW1A, 1987KI1C, 1988OR1C, 1988WO04). Cluster and α-particle models: (1983SH38, 1984NI12, 1985KW02). Special states: (1983BI1C, 1983FE07, 1983VA31, 1984NI12, 1984VA06, 1984ZW1A, 1985GO1A, 1985HA18, 1985HA1J, 1986BA1X, 1986XU02, 1987AB1H, 1987BA2J, 1987KI1C, 1988KW02). Electromagnetic transitions and giant resonances:

  18. A=11Be (1980AJ01)

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    80AJ01) (See Energy Level Diagrams for 11Be) GENERAL: See also (1975AJ02) and Table 11.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1974TA1E, 1975MI12, 1976IR1B, 1977SE1D, 1978BO31, 1979BE1H). Special reactions: (1975FE1A, 1976OS04, 1977AR06, 1977YA1B). Muon capture (See also reaction 2.): (1978DE15). Pion reactions: (1975CO06, 1976CO1M, 1977DO06, 1977GE1D). Ground state of 11Be: (1975BE31, 1978BO31). 1. 11Be(β-)11B Qm = 11.508 The decay proceeds to 11B*(0, 2.12, 5.02, 6.79,

  19. A=11Be (1985AJ01)

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    85AJ01) (See Energy Level Diagrams for 11Be) GENERAL: See also (1980AJ01) and Table 11.3 [Table of Energy Levels] (in PDF or PS). Model calculations:(1981RA06, 1981SE06, 1983MI1E, 1984VA06). Electromagnetic transitions:(1980MI1G). Complex reactions involving 11Be:(1979BO22, 1980WI1L, 1983EN04, 1983WI1A, 1984GR08, 1984HI1A). Hypernuclei:(1979BU1C, 1982IK1A, 1982KA1D, 1982KO11, 1983FE07, 1983KO1D, 1983MI1E). Other topics:(1981SE06, 1982NG01). Ground-state properties of 11Be:(1981AV02, 1982NG01,

  20. A=11Be (1990AJ01)

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    90AJ01) (See Energy Level Diagrams for 11Be) GENERAL: See also (1985AJ01) and Table 11.2 [Table of Energy Levels] (in PDF or PS). Model calculations:(1984MI1H, 1984VA06, 1986WI04). Electromagnetic transitions:(1984MI1H, 1984VA06, 1987HO1L). Complex reactions involving 11Be:(1985BO1A, 1986AV1B, 1987TR05, 1987WA09, 1988BA53, 1988RU01, 1988TA1N, 1988TR03, 1989SA10). Muon and neutrino capture and reactions:(1984KO24). Hypernuclei:(1985IK1A, 1986ME1F). Other topics:(1984MI1H, 1985AN28, 1986AN07).

  1. A=11C (1980AJ01)

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    80AJ01) (See Energy Level Diagrams for 11C) GENERAL: See also (1975AJ02) and Table 11.19 [Table of Energy Levels] (in PDF or PS). Special levels: (1976IR1B). Astrophysical questions: (1976VI1A, 1977SC1D, 1977SI1D, 1978BU1B). Special reactions: (1975HU14, 1976BE1K, 1976BU16, 1976DI01, 1976HE1H, 1976LE1F, 1976SM07, 1977AR06, 1977AS03, 1977SC1G, 1978DI1A, 1978GE1C, 1978HE1C, 1979KA07, 1979VI05). Muon and neutrino capture and reactions: (1975DO1F, 1976DO1G). Pion capture and reactions (See also

  2. A=11C (1985AJ01)

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    5AJ01) (See Energy Level Diagrams for 11C) GENERAL: See also (1980AJ01) and Table 11.17 [Table of Energy Levels] (in PDF or PS). Model calculations:(1981RA06, 1983SH38). Special states:(1981RA06). Complex reactions involving 11C:(1979BO22, 1980GR10, 1980WI1K, 1980WI1L, 1981MO20, 1982GE05, 1982LY1A, 1982RA31, 1983FR1A, 1983OL1A, 1983WI1A, 1984GR08, 1984HI1A). Electromagnetic transitions:(1978KR19). Applied work:(1979DE1H, 1982BO1N, 1982HI1H, 1982KA1R, 1982ME1C, 1982NE1D, 1982PI1H, 1982YA1C,

  3. A=11C (1990AJ01)

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    90AJ01) (See Energy Level Diagrams for 11C) GENERAL: See also (1985AJ01) and Table 11.16 [Table of Energy Levels] (PDF or PS) here. Model calculations: (1988WO04) Special states: (1985SH24, 1986AN07, 1988KW02) Astrophysical Questions: (1987RA1D) Complex reactions involving 11C:(1981AS04, 1985AR09, 1985HI1C, 1985MO08, 1986AV1B, 1986AV07, 1986BA3G, 1986HA1B, 1986HI1D, 1986UT01, 1987AR19, 1987BA38, 1987DE37, 1987NA01, 1987RI03, 1987SN01, 1987ST01, 1987YA16, 1988CA06, 1988KI05, 1988KI06, 1988SA19,

  4. A=11Li (1980AJ01)

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    80AJ01) (See the Isobar Diagram for 11Li) 11Li has been observed in the bombardment of iridium by 24 GeV protons. Its mass excess is 40.94 ± 0.08 MeV (1975TH08). The cross section for its formation is ~ 50 μb (1976TH1A). 11Li is bound: Eb for break up into 9Li + 2n and 10Li + n are 158 ± 80 and 960 ± 250 keV, respectively [see (1979AJ01) for discussions of the masses of 9Li and 10Li]. The half-life of 11Li is 8.5 ± 0.2 msec (1974RO31): it decays to neutron unstable states of 11Be [Pn =

  5. A=11Li (1985AJ01)

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    5AJ01) (See the Isobar Diagram for 11Li) GENERAL: The mass excess of 11Li is 40.94 ± 0.08 MeV (1975TH08). [(A.H. Wapstra, private communication) suggests 40.91 ± 0.11 MeV.] Using the value reported by (1975TH08) 11Li is bound with respect to 9Li + 2n by 156 ± 80 keV and with respect to 10Li + n by 966 ± 260 keV [see (1984AJ01) for the masses of 9Li and 10Li]. Systematics suggest Jπ = 1/2- for 11Lig.s.. See also (1979AZ03, 1980AZ01, 1980BO31, 1981BO1X, 1982BO1Y, 1982OG02), (1981HA2C),

  6. A=12Be (1975AJ02)

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    75AJ02) (See the Isobar Diagram for 12Be) GENERAL: See also (1968AJ02) and Table 12.1 [Table of Energy Levels] (in PDF or PS). Special reactions: (1965GI10, 1969AR13, 1971AR02, 1972VO06, 1973KO1D). General review: (1974CE1A). Theoretical papers: (1971DO1F, 1972ST1C, 1973WI15, 1974IR04, 1974MA1E). Mass of 12Be: The Q-value of the 14C(18O, 20Ne)12Be reaction [-15.77 ± 0.05 MeV] (1974BA15) leads to an atomic mass excess of 25.05 ± 0.05 MeV; that for the 7Li(7Li, 2p)12Be reaction [Q = -9.71 ±

  7. A=12Be (1985AJ01)

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    85AJ01) (See Energy Level Diagrams for 12Be) GENERAL: See also (1980AJ01) and Table 12.1 [Table of Energy Levels] (in PDF or PS). Theoretical papers:(1979KO29, 1981AV02, 1981SE06, 1982NG01, 1983ANZQ, 1983MI1E, 1984VA06). Hypernuclei:(1980GA1P, 1982IK1A, 1982KA1D, 1982PO1C, 1983BR1E, 1983DO1B, 1983MI1E, 1984DO04). Other topics:(1983OL1A, 1983WI1A, 1984HI1A). Mass of 12Be: The Q-value of the 10Be(t, p) reaction (-4809 ± 15 keV) (1978AL29) leads to an atomic mass excess of 25077 ± 15 keV for

  8. A=12Be (1990AJ01)

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    90AJ01) (See Energy Level Diagrams for 12Be) GENERAL: See also (1985AJ01) and Table 12.1 [Table of Energy Levels] (in PDF or PS) here. General theoretical papers: (1984FR13, 1985AN28, 1985BA51, 1985WI1B, 1986WI04, 1987BL18, 1987GI1C, 1987SA15, 1987YA16, 1988RU01, SU88C, 1989BE03). Hypernuclei: (1984IW1B, 1984YA04, 1985BE31, 1985GA1C, 1985IK1A, 1985WA1N, 1985YA01, 1985YA07, 1986BA1W, 1986BI1G, 1986DO1B, 1986GA14, 1986GA33, 1986GA1H, 1986HA26, 1986MA1J, 1986ME1F, 1986MI1N, 1986PO1H, 1986YA1T,

  9. A=12C (1975AJ02)

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    75AJ02) (See Energy Level Diagrams for 12C) GENERAL: See also (1968AJ02) and Table 12.8 [Table of Energy Levels] (in PDF or PS). Shell model: (1967SV1A, 1968BA1L, 1968DR1B, 1968FA1B, 1968FU1B, 1968GO01, 1968GU1C, 1968HA11, 1968RO1G, 1969GU1E, 1969GU03, 1969IK1A, 1969LA26, 1969MO1F, 1969SA1A, 1969SV1A, 1969WA06, 1969WO05, 1970AR21, 1970BE26, 1970BO33, 1970BO1J, 1970CO1H, 1970DE1F, 1970DO1A, 1970EI06, 1970GI11, 1970GU11, 1970KH01, 1970KO04, 1970KR1D, 1970LO1C, 1970RE1G, 1970RU1A, 1970RY1A,

  10. A=12C (1980AJ01)

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    0AJ01) (See Energy Level Diagrams for 12C) GENERAL: See also (1975AJ02) and Table 12.7 [Table of Energy Levels] (in PDF or PS). Shell model: (1974BO1P, 1975BI05, 1975BO27, 1975FR06, 1975GI1C, 1975MU13, 1975WA30, 1976BA24, 1977CA02, 1977CA08, 1977GR02, 1977JA14, 1978FU13, 1978MU04, 1978SV01, 1979LO1F). Collective and deformed models: (1974BO1P, 1975BO27, 1975KI21, 1975LE14, 1975MC15, 1975SO07, 1976GL1C, 1976PA25, 1977CA08, 1977TH03, 1977UE01, 1977VI03, 1979MA1J). Cluster and alpha particle