San José State University |
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the Stability of Neutrons within Nuclei as Opposed to the Instability of Free Neutrons is Due to Their Being Paired with Protons |
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A previous study made the case that the stability of neutrons within nuclei can be explained by the nuclear strong force between nucleons being an attraction between like nucleons and a repulsion between like nucleons. There is overwhelming evidence for this from the data on nuclear binding energies. See Strong Force. In contrast the conventional theory of nuclear structure holds that all nucleons are attracted to each other.
Some nuclides are beta ray (electron) emitters. This suggests that such beta emission is associated with a nuclide having a neutron which is not paired with a proton. The following is a list of the pure beta emitters and their half-lives.
The Pure Beta Emitting Nuclides and Their Half Lives | |||||
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Nuclide | Number of Protons | Number of Neutrons | Half-Life (seconds) | Is there a neutron not paired with a proton? | Is there a neutron not paired with a neutron? |
cu-66 | 29 | 37 | 0.035 | Yes | Yes |
pb-209 | 82 | 127 | 1.37 | Yes | No |
pr-145 | 59 | 86 | 2.47 | Yes | Yes |
te-127 | 52 | 75 | 3.85 | Yes | No |
sn-121 | 50 | 71 | 10.8 | Yes | Yes |
ni-66 | 28 | 38 | 22.7 | Yes | No |
y-90 | 39 | 51 | 25.2 | Yes | Yes |
bi-210 | 83 | 127 | 50.4 | Yes | Yes |
er-169 | 68 | 101 | 92.9 | Yes | Yes |
pr-143 | 59 | 86 | 133 | Yes | No |
p-32 | 15 | 17 | 140 | Yes | Yes |
sr-89 | 38 | 51 | 497 | Yes | Yes |
y-91 | 39 | 52 | 576 | Yes | No |
w-188 | 74 | 114 | 684 | Yes | No |
w-188 | 74 | 114 | 684 | Yes | No |
s-35 | 16 | 19 | 864 | Yes | No |
sn-123 | 50 | 73 | 1270 | Yes | No |
ca-45 | 20 | 25 | 1600 | Yes | No |
bk-249 | 97 | 152 | 3160 | Yes | Yes |
ru-106 | 44 | 62 | 3600 | Yes | No |
tm-171 | 69 | 102 | 6840 | Yes | Yes |
pm-147 | 61 | 86 | 9360 | Yes | Yes |
kr-85 | 36 | 49 | 38900 | Yes | Yes |
h-3 | 1 | 2 | 44300 | Yes | Yes |
cd-113m | 48 | 65 | 50800 | Yes | Yes |
pu-241 | 94 | 147 | 51800 | Yes | Yes |
sr-90 | 38 | 52 | 104000 | Yes | No |
ar-42 | 18 | 24 | 118440 | Yes | No |
sm-151 | 62 | 89 | 324000 | Yes | Yes |
ni-63 | 28 | 35 | 361000 | Yes | Yes |
si-32 | 14 | 18 | 620000 | Yes | No |
ar-39 | 18 | 21 | 969000 | Yes | Yes |
c-14 | 6 | 8 | 2060000 | Yes | No |
tc-99 | 43 | 56 | 756000000 | Yes | No |
se-79 | 34 | 45 | 2340000000 | Yes | Yes |
be-10 | 4 | 6 | 5400000000 | Yes | No |
cs-135 | 55 | 80 | 8280000000 | Yes | Yes |
pd-107 | 46 | 61 | 2.34×1010 | Yes | Yes |
re-187 | 75 | 112 | 1.58×1014 | Yes | Yes |
in-115 | 49 | 66 | 1.58×1018 | Yes | Yes |
cd-113 | 48 | 65 | 3.35×1019 | Yes | Yes |
as-77 | 33 | 44 | NA | Yes | No |
br-83 | 35 | 48 | NA | Yes | No |
la-141 | 57 | 84 | NA | Yes | No |
cm249 | 96 | 153 | NA | Yes | No |
In no case is there beta emission without there being a neutron without a pairing with a proton. It does not matter whether the neutrons unpaired with protons are paired or unpaired with another neutron. In other words the pairing of a neutron with a proton protects it from decay but pairing with another neutron is not necessary for it to do so. The pairing of a neutron with a proton protects it from decay because the transition of the neutron into a proton would require a significant input of energy to cover the change in the interaction of the two nucleons through the nuclear strong force from the attraction of unlike nucleons to the repulsion of like nucleons.
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