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 18-Dec-2021 00:54:10 (NZT):
Full SQL Query: "select * from FissionAllNewPlus where neutrino = 'none' and (E='D' ) order by MeV desc limit 101"
2 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFBEinE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2BEoutMeV
4noneD2b1f2.22411411n*1f0fH1f1b0.00000000-2.224114
5noneD2b1f2.22411411H1f1bn*1f0f0.00000000-2.224114

All Nuclides Appearing in Results Table: (3)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
310ffn*1.008664915820.000000000000.00000000000UPN-4.6070null0.0000100.0000nullnull1/2+-1.9130427000nullnullnull-18.32471830
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
521bfD2.014101778112.224114110701.11205705535SPN50.0000null0.00000.01500.21231+0.85743823100.00286000000.008261.4034.10662920

All Elements Appearing in Results Table: (1)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223