Fission Reactions - data provided by Dr. Alexander Parkhomov
Conceived by R. W. Greenyer and coded by P. W. Power for the Martin Fleischmann Memorial Project

Version 5.0, Sep 28, 2019

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This program ("Fission.php") enables SQL commands to query the Fission tables created from Dr Parkhomov's spreadsheets.

To make full use of this and the other database tables, a good grasp of SQL is essential.

But note that it, TwoToTwo and Fusion is each dedicated to querying only one of two tables.

The "universal" program All Tables can accept full SQL commands that query any of the 12 "Parkhomov" tables, together with the "ElementProperties", "Nuclides", "RadioNuclides" and "Atomic Radii" tables as well.

You may indicate which of the three neutrino conditions to include: "left" and/or "none" and/or "right". The default condition is include all three.

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 ('b') if its A number is even; if odd a Fermion ('f'). The atom itself is considered a Boson ('b') if its number of neutrons (A - Z) is even; if odd a Fermion ('f').

These parameters can be used either passively, by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively, by selecting 'b only', 'f only' or 'either' in the boxes below.

NB: To avoid unnecessary duplication in the Fission tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly, in that, if the ouput side of the Core Query only involves E1 and E2, only rows for which their associated mass numbers obey the rule that A1 <= A2 will be included in the results

Input used for this run on 23-Aug-2020 13:32:14 (NZT):
Full SQL Query: "select * from FissionAllNew where E = 'Ni' and E2 in ('P') order by MeV desc"
3 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2MeV
1156rightNi61f28fSi30b14bP31f15b-15.347826
1120rightNi60b28bSi29f14fP31f15b-18.136924
1082noneNi58b28bAl27f13bP31f15b-18.590874

All Nuclides Appearing in Results Table:

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHz
292713fbAl26.98153853000224.945768328178.33132475290SPN50.0000null0.0000100.000082300585/2+3.64070000000.14660000001170.0000104.227
312914ffSi28.97649466490245.003940601318.44841174487SPN50.0000null0.00004.700013254341/2+-0.5550520000null2.090079.468
323014bbSi29.97377013600255.612910794918.52043035983SPN50.0000null0.00003.09008713.823nullnullnullnullnull
333115fbP30.97376199842262.909244456198.48094336955SPN50.0000null0.0000100.00001050null1/2+1.1309250000null377.0000161.923
705828bbNi57.93534241000506.445887001088.73182563795SPN50.0000null0.000067.880057.019249nullnullnullnullnull
716028bbNi59.93078588000526.832442800038.78054071333SPN50.0000null0.000026.230022.0332nullnullnullnullnullnull
726128ffNi60.93105557000534.652315054858.76479205008SPN50.0000null0.00001.19000.9996null3/2--0.74965000000.1620000000nullnull