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 28-Jul-2022 12:59:10 (NZT):
Full SQL Query: "select * from FusionAll where A1 =16 and E2 in ('Ni', 'Li', 'Al', 'B', 'N' ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
2912left1288O16b8bAl27f13bCa43f20f16.459503
2941none814O16b8bNi64b28bKr80b36b6.046300
2940none812O16b8bNi62b28bKr78b36b2.693900

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
20168bbO15.99491461960127.615727132677.97598294579SPN50.0000null0.000099.7590459888.999592nullnullnullnullnullnull
322713fbAl26.98153840800224.945881970478.33132896187SPN50.0000null0.0000100.000082300585/2+3.64070000000.14660000001170.0000104.2276.97627800
524320ffCa42.95876643000369.818907957478.60043971994SPN50.0000null0.00000.145060.175null7/2--1.3173300000-0.0408000000nullnull-1.80306900
816228bbNi61.92834487100545.248402774958.79432907702SPN50.0000null0.00003.66003.0744nullnullnullnullnullnullnull
826428bbNi63.92796634100561.743175248308.77723711325SPN50.0000null0.00001.08000.9072nullnullnullnullnullnullnull
1077836bbKr77.92036634100675.559082366138.66101387649UPN24.9368KK2.84600.3500nullnullnullnullnullnullnullnull
1088036bbKr79.91637804800695.416328619488.69270410774SPN50.0000null0.00002.2700nullnullnullnullnullnullnullnull

All Elements Appearing in Results Table: (5)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
8OOxygen21615.999384811196.2037854.890.23.4414128840781.429null0.0265891946100010400Paramagneticnull0.00000190772
13AlAluminium31326.981541189.99316933.4727921.6142.531322231627003823590482300nullParamagneticnull0.00002110000
20CaCalcium4240.0758619425.855391115175712.3722052776215502920063141500nullParamagneticnull0.00002139000
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagnetic631null
36KrKrypton41883.800928822346.91304115.79119.93302303262003.75null0.00943248nullnullDiamagneticnull-0.00000001650