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 26-Apr-2022 09:57:33 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('H', 'D') and E2 in ('Co' ) order by MeV desc limit 100"
5 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
360none285D2b1fCo60b27fNi62b28b18.222800
359none278D2b1fCo59f27bNi61f28f15.130300
69none284H1f1bCo60b27fNi61f28f9.857100
68none277H1f1bCo59f27bNi60b28b9.531000
67left50H1f1bCo59f27bCo60b27f6.715143

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
521bfD2.014101778112.224114110701.11205705535SPN50.0000null0.00000.01500.21231+0.85743823100.00286000000.008261.4034.10662920
755927fbCo58.93319365600517.300859547928.76781117878SPN50.0000null0.0000100.000025null7/2-4.61500000000.42000000001570.000094.9086.33200000
766027bfCo59.93381566700524.792546787648.74654244646SYN0.7219G, B-1.33250.00000null5+3.79900000000.4600000000nullnull3.63900000
796028bbNi59.93078525600526.833024052508.78055040087SPN50.0000null0.000026.230022.0332nullnullnullnullnullnullnull
806128ffNi60.93105494500534.652897238808.76480159408SPN50.0000null0.00001.19000.9996null3/2--0.74965000000.1620000000nullnull-2.39477000
816228bbNi61.92834487100545.248402774958.79432907702SPN50.0000null0.00003.66003.0744nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (3)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
27CoCobalt4958.933191526.62171176832001.8863.752796602389001710042125nullFerromagnetic1394null
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagnetic631null