Two To Two 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 enables SQL commands to query the TwoToTwo (2-2) 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 and Fission and Fusion 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 TwoToTwo tables, two rules independently apply: A1 <= A2 and A3 <= A4. These rules also apply 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. Similarly with E3 and E4 on the output side, only rows whose associated mass numbers obey A3 <= A4 will appear in the results.

Input used for this run on 13-Sep-2021 23:26:27 (NZT):
Full SQL Query: "select * from TwoToTwoAll where E1 in ('H') and E2 in ('Cu' ) order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
49none97H1f1bCu65f29bHe4b2bNi62b28b4.343600
48none91H1f1bCu63f29bHe4b2bNi60b28b3.757600
47left44H1f1bCu63f29bHe4b2bCo60b27f0.941743

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
766027bfCo59.93381566700524.792546787648.74654244646SYN0.7219G, B-1.33250.00000null5+3.79900000000.4600000000nullnull3.63900000
796028bbNi59.93078525600526.833024052508.78055040087SPN50.0000null0.000026.230022.0332nullnullnullnullnullnullnull
816228bbNi61.92834487100545.248402774958.79432907702SPN50.0000null0.00003.66003.0744nullnullnullnullnullnullnull
836329fbCu62.92959723600551.370585425548.75191405437SPN50.0000null0.000069.090041.454null3/2-2.2259000000-0.2200000000365.0000106.1127.11179100
846529fbCu64.92778948700569.196667298788.75687180460SPN50.0000null0.000030.910018.546null3/2-2.3844000000-0.2040000000201.0000113.6697.60430000

All Elements Appearing in Results Table: (5)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagnetic-0.00000000223
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagnetic-0.00000000105
27CoCobalt4958.933191526.62171176832001.8863.752796602389001710042125nullFerromagneticnull
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagneticnull
29CuCopper41163.547241457.124131357.7732001.9118.44291116105892059400384.460nullDiamagnetic-0.00000963000