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 26-Jul-2022 12:25:03 (NZT):
Full SQL Query: "select * from FissionAll where E = 'Xe' and E1 = 'C' order by MeV desc limit 1000"
2 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2MeV
589noneXe124b54bC12b6bCd112b48b3.055300
623noneXe126b54bC12b6bCd114b48b0.558000

All Nuclides Appearing in Results Table: (5)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
15126bbC12.0000000000092.159043079567.67992025663SPN50.0000null0.000098.8900197.783032nullnullnullnullnullnull
16011248bbCd111.90276388300956.984628025278.54450560737SPN50.0000null0.000024.07000.036105nullnullnullnullnullnullnull
16211448bbCd113.90336499000972.566874184178.53128837004SPN50.0000null0.000028.86000.04329nullnullnullnullnullnullnull
18912454bbXe123.905891588001046.230231620308.43734057758UPN22.2553KK2.86400.0961nullnullnullnullnullnullnullnull
19012654bbXe125.904296794001063.857947117708.44331704062SPN50.0000null0.00000.0900nullnullnullnullnullnullnullnull

All Elements Appearing in Results Table: (3)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
6CCarbon21412.01114675.31466382343002.55153.9464727722600.11407102004600Diamagneticnull-0.00001400000
48CdCadmium512112.4342016112.99817594.2210401.690233616865014972300.15nullDiamagneticnull-0.00001990000
54XeXenon518131.3000410822254.24478161.3165.12.60833099.45.9null0.00565158.32nullnullDiamagneticnull-0.00000002540