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-Jan-2022 04:07:43 (NZT):
Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E1 in ('H', 'Li', 'O') and E2 in ('Nb') ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
1529none743Li7f3bNb93f41bRu100b44b17.703000
1215none742Li6b3fNb93f41bRu99f44f14.033900
114none740H1f1bNb93f41bMo94b42b8.481300

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
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
1289341fbNb92.90637316100805.748287619068.66396008193SPN50.0000null0.0000100.000020null9/2+6.1630000000-0.32000000002740.000097.9046.56740000
1309442bbMo93.90508359200814.238267386938.66210922752SPN50.0000null0.00009.06000.10872nullnullnullnullnullnullnull
1419944ffRu98.90593027800852.240352163768.60848840569SPN50.0000null0.000012.72000.0001272null5/2+-0.64100000000.0790000000nullnull-1.22800000
14210044bbRu99.90421045200861.913447299118.61913447299SPN50.0000null0.000012.62000.0001262nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (5)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
3LiLithium216.9417416712.97521453.6916150.9859.613118155351185357020nullParamagneticnull0.00000137000
41NbNiobium5592.9060219810.84084275050171.686.1571210085706.75426520nullParamagneticnull0.00023700000
42MoMolybdenum5695.216891909.26234289649122.1671.963015450010280201392511.2nullParamagneticnull0.00012030000
44RuRuthenium58101.035311788.16777260744232.2101.383274712370141202380.001nullParamagneticnull0.00006700000