Fusion 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 ("Fusion.php") enables SQL commands to query the Fusion tables originally 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 Fission 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 all Fusion tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly in that, if the input side of the Core Query only involves E1 and E2, only rows whose associated mass numbers obey A1 <= A2 will appear in the results

Input used for this run on 20-Dec-2021 05:21:04 (NZT):
Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E1= 'Si' and E2 = 'Si' ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
3593none1079Si29f14fSi29f14fNi58b28b16.431600
3609none1081Si30b14bSi30b14bNi60b28b15.592300
3588none1080Si28b14bSi30b14bNi58b28b14.294700

All Nuclides Appearing in Results Table: (5)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
332814bbSi27.97692653499236.530569098018.44752032493SPN50.0000null0.000092.2100260032.2653nullnullnullnullnullnull
342914ffSi28.97649466525245.003940275288.44841173363SPN50.0000null0.00004.700013254341/2+-0.5550520000null2.090079.468-5.31903000
353014bbSi29.97377013600255.612910794918.52043035983SPN50.0000null0.00003.09008713.823nullnullnullnullnullnull
775828bbNi57.93534178000506.446473842508.73183575591SPN50.0000null0.000067.880057.019249nullnullnullnullnullnull
796028bbNi59.93078525600526.833024052508.78055040087SPN50.0000null0.000026.230022.0332nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (2)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
14SiSilicon31428.0856111112.05391168731731.9133.641425792323300.001150710282000650Diamagneticnull-0.00000373000
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagnetic631null