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 15-Dec-2024 02:08:59 (NZT):
Full SQL Query: "select * from FusionAll where E in ('U') order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
3921right757T3f1bTh232b90bU235f92f9.619799
900none1185He3f2fTh232b90bU235f92f9.601800
1415left709Li6b3fTh232b90bU238b92b2.400462

All Nuclides Appearing in Results Table: (6)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
631fbT3.016049281998.481112243522.82703741451SYN1.0906B-0.01860.00000null1/2+2.9789624600null6897.0000426.65628.53498650
732ffHe3.016029322657.717370845642.57245694855SPN50.0000null0.00000.0001null351/2+-2.1276253100nullnullnull-20.37894730
963bfLi6.0151228874231.992637601015.33210626683SPN50.0000null0.00007.42001.484null1+0.8220430000-0.00080600003.580058.8643.93712700
31323290bbTh232.038053689001766.635372523707.61480764019UPN10.1480A or SF4.0830100.00009.6nullnullnullnullnullnullnull
31723592ffU235.043928190001783.811902194507.59068894551UPN8.8476A or SF4.67900.72000.01944null7/2--0.38000000004.9360000000nullnull-0.52000000
31923892bbU238.050786996001801.636224155507.56990010149UPN9.6504A or SF or 2 B-4.270099.27452.6804115nullnullnull13.9000000000nullnullnull

All Elements Appearing in Results Table: (5)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagneticnull-0.00000000105
3LiLithium216.9417416712.97521453.6916150.9859.613118155351185357020nullParamagneticnull0.00000137000
90ThThorium74232.03877null19.79173202350931.3null442780117246.7541189.6nullParamagneticnull0.00008400000
92UUranium76238.02891null12.49500140842001.38null621420190503.6271162.7nullParamagneticnull0.00041100000