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 25-Mar-2022 11:13:29 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('HE') and E2 in ('LI') order by MeV desc limit 100"
4 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
646none612He3f2fLi7f3bB10b5f17.787800
645left273He3f2fLi6b3fBe9f4f17.670445
902none613He4b2bLi7f3bB11f5b8.665700
901none611He4b2bLi6b3fB10b5f4.461900

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
732ffHe3.016029322657.717370845642.57245694855SPN50.0000null0.00000.0001null351/2+-2.1276253100nullnullnull-20.37894730
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
963bfLi6.0151228874231.992637601015.33210626683SPN50.0000null0.00007.42001.484null1+0.8220430000-0.00080600003.580058.8643.93712700
1073fbLi7.0160034366639.243497935165.60621399074SPN50.0000null0.000092.580018.516null3/2-3.2564070000-0.04000000001540.0000155.45510.39770400
1194ffBe9.0121830660058.161992070306.46244356337SPN50.0000null0.0000100.00002.8null3/2--1.17743000000.052900000078.800056.207-3.75066000
13105bfB10.0129368620064.748588919276.47485889193SPN50.0000null0.000019.60001.96null3+1.80046360000.084500000022.000042.9752.87467955
14115fbB11.0093051660076.202580126116.92750728419SPN50.0000null0.000080.40008.04null3/2-2.68837800000.0405900000754.0000128.2868.58470700

All Elements Appearing in Results Table: (4)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagneticnull-0.00000000105
3LiLithium216.9417416712.97521453.6916150.9859.613118155351185357020nullParamagneticnull0.00000137000
4BeBeryllium229.012191124.87672156027431.5702421006.618482519018202.8nullDiamagneticnull-0.00002328000
5BBoron21310.81402874.39594234842732.0426.73532826.72460027103010nullDiamagneticnull-0.00002140000