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 13:14:51 (NZT):
Full SQL Query: "select * from FissionAllNew where E = 'Ni' and E2 in ('S') order by MeV desc"
6 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2MeV
1079noneNi58b28bMg24b12bS34b16b-16.362901
1155rightNi61f28fAl27f13bS34b16b-17.092887
1081noneNi58b28bMg26b12bS32b16b-17.998084
1110noneNi60b28bMg26b12bS34b16b-18.326305
1080noneNi58b28bMg25f12fS33f16f-20.449538
1119rightNi60b28bAl27f13bS33f16f-20.689942

All Nuclides Appearing in Results Table:

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHz
262412bbMg23.98504169700198.251660643278.26048586014SPN50.0000null0.000078.700018337.1513nullnullnullnullnull
272512ffMg24.98583697600205.581949722808.22327798891SPN50.0000null0.000010.13002360.29695/2+-0.85533000000.1990000000nullnull
282612bbMg25.98259296800216.674811754458.33364660594SPN50.0000null0.000011.17002602.6179nullnullnullnullnull
292713fbAl26.98153853000224.945768328178.33132475290SPN50.0000null0.0000100.000082300585/2+3.64070000000.14660000001170.0000104.227
343216bbS31.97207117440271.772991001508.49290596880SPN50.0000null0.000095.0000332.5396nullnullnullnullnull
353316ffS32.97145890980280.414398968678.49740602935SPN50.0000null0.00000.76002.66null3/2+0.6432500000-0.0678000000nullnull
363416bbS33.96786700400291.831325829678.58327428911SPN50.0000null0.00004.220014.77nullnullnullnullnullnull
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