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 25-Mar-2023 12:04:10 (NZT):
Full SQL Query: "select * from FissionAll where E = 'Au' and MEV < 10 limit 1000"
2 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2MeV
1652noneAu197f79bHe4b2bIr193f77b0.623200
1653noneAu197f79bB11f5bW186b74b2.707900

All Nuclides Appearing in Results Table: (5)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
14115fbB11.0093051660076.202580126116.92750728419SPN50.0000null0.000080.40008.04null3/2-2.68837800000.0405900000754.0000128.2868.58470700
27718674bbW185.954365215001485.838046163807.98837659228SPN50.0000null0.000028.41000.355125nullnullnullnullnullnullnull
28919377fbIr192.962923824001532.016358878607.93790859523SPN50.0000null0.000062.70000.000627null3/2+0.16300000000.7510000000nullnull0.52270000
29619779fbAu196.966570114001559.339541431607.91542914432SPN50.0000null0.0000100.00000.004null3/2+0.14520000000.5470000000nullnull0.47306000

All Elements Appearing in Results Table: (5)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagneticnull-0.00000000105
5BBoron21310.81402874.39594234842732.0426.73532826.72460027103010nullDiamagneticnull-0.00002140000
74WTungsten66183.841521939.55021369558282.3678.662170019250201701321.25nullParamagneticnull0.00008840000
77IrIridium69192.216371808.48637273947012.215182160022650211501310.001nullParamagneticnull0.00003770000
79AuGold611196.9665517410.205521337.3331292.54222.85219801930045320129.10.004nullDiamagneticnull-0.00003440000