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 05-Mar-2022 06:33:32 (NZT):
Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E2 in ('Ti' ) and E in ('Fe') ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
1747none1199Be9f4fTi47f22fFe56b26b27.024500
1749none1201Be9f4fTi49f22fFe58b26b24.946300
1748none1200Be9f4fTi48b22bFe57f26f23.045200

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
1194ffBe9.0121830660058.161992070306.46244356337SPN50.0000null0.0000100.00002.8null3/2--1.17743000000.052900000078.800056.207-3.75066000
584722ffTi46.95175775200407.067132826738.66100282610SPN50.0000null0.00007.2800407.68null5/2--0.78814000000.3020000000nullnull-1.51054000
594822bbTi47.94794093200418.693565990568.72278262480SPN50.0000null0.000073.94004140.64nullnullnullnullnullnullnull
604922ffTi48.94786462700426.835730627328.71093327811SPN50.0000null0.00005.5100308.56null7/2--1.10370000000.2470000000nullnull-1.51095000
715626bbFe55.93493561700492.247305272248.79013045129SPN50.0000null0.000091.660051604.581169nullnullnullnullnullnull
725726ffFe56.93539213400499.893149235218.77005524974SPN50.0000null0.00002.19001232.97281/2-0.0906400000nullnullnull0.86806270
735826bbFe57.93327373800509.937510067078.79202603564SPN50.0000null0.00000.3300185.79nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (3)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
4BeBeryllium229.012191124.87672156027431.5702421006.618482519018202.8nullDiamagneticnull-0.00002328000
22TiTitanium4447.8789217610.62324194135601.547.642263929445072.5225205600nullParamagneticnull0.00018070000
26FeIron4855.847311567.09262181131341.8315.762689516178741080449563001090Ferromagnetic1043null