Results for user from Brno, Czechia
Version 4.0, P W Power May 31, 2019
Fusion Reactions | Fission Reactions | Two To Two Reactions | All Tables
Cascades | CascadesAll | Tables in Detail | All Results | Notes | Downloads
To make full use of this and the other database tables, a good grasp of SQL is essential.
But note that it, TwoToTwo and Fission is each dedicated to querying only one table ("FissionAll" "TwoToTwoAll" and "FusionAll" respectively).
The "universal" program All Tables can accept full SQL commands that query any and all of the now 9 "Parkhomov" tables together with the "Selected Isotopes" and "Periodic" tables as well.
New Feature (1): In the checkbox, you may indicate which of the three tables you want effectively included. The resulting query is only on FussionAll but it uses the new field "neutrino" (setable to "left" and/or "none" and/or "right") to effectively select "FusionEoL" and/or "Fussion" and/or "FussionEoR".
New Feature (2): In all the above tables except the Periodic, each atom, in either the input or the output, as well as its 'A' and 'Z' numbers now also has a 'nBorF' ('nuclear Boson or Fermion') and a 'aBorF' ('atomic Boson or Fermion') parameter associated with it.
An atom's nucleus is considered a Boson if its A number is even; if odd a Fermion (thus nBorF = 'b' or 'f'). The atom itself is considered a Boson if its number of neutrons (A - Z) is even; if odd a Fermion (thus aBorF = 'b' or 'f').
The above extra parameters can be used either passively by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively by the New Feature (3) of selecting 'b only', 'f only' or 'either' in the boxes below.
| id | neutrino | id_sub | E1 | A1 | nBorF1 | Z1 | aBorF1 | E2 | A2 | nBorF2 | Z2 | aBorF2 | E | A | nBorF | Z | aBorF | MeV |
| 767 | none | 872 | He | 3 | f | 2 | f | Pd | 105 | f | 46 | f | Cd | 108 | b | 48 | b | 15.528000 |
| 771 | right | 192 | He | 3 | f | 2 | f | Pd | 110 | b | 46 | b | In | 113 | f | 49 | b | 15.136777 |
| 770 | none | 876 | He | 3 | f | 2 | f | Pd | 110 | b | 46 | b | Cd | 113 | f | 48 | f | 14.829400 |
| 769 | none | 874 | He | 3 | f | 2 | f | Pd | 108 | b | 46 | b | Cd | 111 | f | 48 | f | 14.382300 |
| 766 | left | 350 | He | 3 | f | 2 | f | Pd | 104 | b | 46 | b | Ag | 107 | f | 47 | b | 13.618446 |
| 768 | left | 352 | He | 3 | f | 2 | f | Pd | 106 | b | 46 | b | Ag | 109 | f | 47 | b | 13.534611 |
| 1028 | none | 875 | He | 4 | b | 2 | b | Pd | 108 | b | 46 | b | Cd | 112 | b | 48 | b | 3.430700 |
| 1029 | none | 877 | He | 4 | b | 2 | b | Pd | 110 | b | 46 | b | Cd | 114 | b | 48 | b | 3.291000 |
| 1027 | none | 873 | He | 4 | b | 2 | b | Pd | 106 | b | 46 | b | Cd | 110 | b | 48 | b | 2.638900 |
| 1026 | left | 351 | He | 4 | b | 2 | b | Pd | 105 | f | 46 | f | Ag | 109 | f | 47 | b | 2.368791 |
| 1025 | none | 871 | He | 4 | b | 2 | b | Pd | 104 | b | 46 | b | Cd | 108 | b | 48 | b | 2.014800 |
| 1024 | none | 870 | He | 4 | b | 2 | b | Pd | 102 | b | 46 | b | Cd | 106 | b | 48 | b | 1.483900 |