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 24-Jan-2024 11:31:55 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('N') and E2 in ('N' ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
2648none722N14b7fN14b7fSi28b14b27.532200
2649none723N14b7fN15f7bSi29f14f25.019000
2789none724N15f7bN15f7bSi30b14b24.642700

All Nuclides Appearing in Results Table: (5)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
18147bfN14.00307400446104.655465857007.47539041836SPN50.0000null0.000099.630018.929711051+0.40357300000.0204400000nullnull1.93377980
19157fbN15.00010889894115.488531808917.69923545393SPN50.0000null0.00000.37000.0703null1/2--0.2830569000null0.022040.547-2.71261890
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

All Elements Appearing in Results Table: (2)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
7NNitrogen21514.006935611196.5870563.0577.363.04737643601.251null0.026583104019960Diamagneticnull-0.00000000680
14SiSilicon31428.0856111112.05391168731731.9133.641425792323300.001150710282000650Diamagneticnull-0.00000373000