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 14-Apr-2022 23:21:03 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('D') and E2 in ('S' ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
316left20D2b1fS32b16bS34b16b17.056590
317none955D2b1fS33f16fCl35f17b15.563400
318right9D2b1fS34b16bAr36b18b13.431211

All Nuclides Appearing in Results Table: (6)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
521bfD2.014101778112.224114110701.11205705535SPN50.0000null0.00000.01500.21231+0.85743823100.00286000000.008261.4034.10662920
373216bbS31.97207117443271.772990973558.49290596792SPN50.0000null0.000095.0000332.5396nullnullnullnullnullnull
383316ffS32.97145890985280.414398922098.49740602794SPN50.0000null0.00000.76002.66null3/2+0.6432500000-0.0678000000nullnull2.05568500
393416bbS33.96786701200291.831318377728.58327406993SPN50.0000null0.00004.220014.77nullnullnullnullnullnullnull
403517fbCl34.96885269400298.201914731668.52005470662SPN50.0000null0.000075.5300109.5185null3/2+0.8217000000-0.8170000000nullnull2.62419910
433618bbAr35.96754510500306.708680027418.51968555632SPN50.0000null0.00000.3370null77nullnullnullnullnullnull

All Elements Appearing in Results Table: (4)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
16SSulfur31632.057508816.35587388.36717.872.58200616337138196000.205705350440Diamagneticnull-0.00001220000
17ClChlorine31735.457537911032.21248171.6239.113.163497173807603.21400.0089478.2145nullDiamagneticnull-0.00000002310
18ArArgon31839.947667122392.1870083.887.3null02184270661.784null0.01772520.33nullnullDiamagneticnull-0.00000001070