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 27-Mar-2025 05:06:29 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('H') and E2 in ('Tl' ) order by MeV desc limit 1000"
2 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
286none1242H1f1bTl205f81bPb206b82b7.303800
285none1241H1f1bTl203f81bPb204b82b6.601500

All Nuclides Appearing in Results Table: (5)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
311fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
28220381fbTl202.972344022001600.823033796907.88582775269SPN50.0000null0.000029.50000.25075null1/2+1.6160000000nullnullnull15.53933900
28320581fbTl204.974427237001615.024704752107.87816929147SPN50.0000null0.000070.50000.59925null1/2+1.6320000000nullnullnull15.69218600
28420482bbPb203.973043420001607.460302074607.87970736311SPN50.0000null0.00001.48000.2072nullnullnullnullnullnullnull
28520682bbPb205.974465124001622.278166777907.87513673193SPN50.0000null0.000023.60003.304nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (3)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
81TlThallium613204.3838315617.2475857717461.6219.2332878118506.7461290.85nullDiamagneticnull-0.00003560000
82PbLead614207.1771115418.26959600.6120222.3335.1456640113404.83512714nullDiamagneticnull-0.00001700000