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-Sep-2020 02:05:58 (NZT):
Full SQL Query: "select * from FusionAll where E1 in ('He') and E2 in ('Cl' ) order by MeV desc"
6 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2EAnBorFZaBorFMeV
673left290He3f2fCl35f17bAr38b18b20.641911
674left291He3f2fCl37f17bAr40b18b18.203260
676right172He3f2fCl37f17bCa40b20b18.012299
675none257He3f2fCl37f17bK40b19f16.690500
929none256He4b2bCl35f17bK39f19b7.213500
930none258He4b2bCl37f17bK41f19b6.207500

All Nuclides Appearing in Results Table:

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHz
632ffHe3.016029320107.717373220952.57245774032SPN50.0000null0.00000.0001null351/2+-2.1276253100nullnullnull
742bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnull
373517fbCl34.96885268200298.201925909598.52005502599SPN50.0000null0.000075.5300109.5185null3/2+0.8217000000-0.8170000000nullnull
383717fbCl36.96590260200317.092082636398.57005628747SPN50.0000null0.000024.470035.4815null3/2+0.6840000000-0.0644000000nullnull
403818bbAr37.96273211000327.334131520618.61405609265SPN50.0000null0.00000.0630nullnullnullnullnullnullnull
414018bbAr39.96238312370343.801384204818.59503460512SPN50.0000null0.000099.6000nullnullnullnullnullnullnull
423919fbK38.96370648640333.715258976898.55680151223SPN50.0000null0.000093.100019457.9null3/2+0.39147000000.0585000000nullnull
434019bfK39.96399816600341.514648043908.53786620110UPN9.0969b- or K or b+1.50500.01182.4662null4--1.2979700000-0.0730000000nullnull
444119fbK40.96182525790351.609786588038.57584845337SPN50.0000null0.00006.88001437.92null3/2+0.21487200000.0711000000nullnull
454020bbCa39.96259086300342.043209404008.55108023510SPN50.0000null0.000096.970040242.5560nullnullnullnullnull