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 02-Oct-2024 06:58:04 (NZT):
Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (E1 in ('H', '') and E2 in ('Ni', 'Li', 'Zn', 'O', 'N' ) ) order by MeV desc limit 100"
8 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
2none5H1f1bLi7f3bHe4b2bHe4b2b17.348100
5none14H1f1bN15f7bHe4b2bC12b6b4.964900
1none2H1f1bLi6b3fHe3f2fHe4b2b4.022200
7none21H1f1bO18b8bHe4b2bN15f7b3.981200
55none103H1f1bZn68b30bHe4b2bCu65f29b2.143400
51none98H1f1bZn66b30bHe4b2bCu63f29b1.560300
6none18H1f1bO17f8fHe4b2bN14b7f1.037700
45none90H1f1bNi62b28bHe4b2bCo59f27b0.351200

All Nuclides Appearing in Results Table: (16)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
732ffHe3.016029322657.717370845642.57245694855SPN50.0000null0.00000.0001null351/2+-2.1276253100nullnullnull-20.37894730
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
963bfLi6.0151228874231.992637601015.33210626683SPN50.0000null0.00007.42001.484null1+0.8220430000-0.00080600003.580058.8643.93712700
1073fbLi7.0160034366639.243497935165.60621399074SPN50.0000null0.000092.580018.516null3/2-3.2564070000-0.04000000001540.0000155.45510.39770400
15126bbC12.0000000000092.159043079567.67992025663SPN50.0000null0.000098.8900197.783032nullnullnullnullnullnull
18147bfN14.00307400446104.655465857007.47539041836SPN50.0000null0.000099.630018.929711051+0.40357300000.0204400000nullnull1.93377980
19157fbN15.00010889894115.488531808917.69923545393SPN50.0000null0.00000.37000.0703null1/2--0.2830569000null0.022040.547-2.71261890
21178ffO16.99913175664131.758574837707.75050440222SPN50.0000null0.00000.0370170.57null5/2+-1.8935430000-0.02560000000.061050.227-3.62806000
22188bbO17.99915961284139.803713906887.76687299483SPN50.0000null0.00000.2040940.44nullnullnullnullnullnullnull
755927fbCo58.93319365600517.300859547928.76781117878SPN50.0000null0.0000100.000025null7/2-4.61500000000.42000000001570.000094.9086.33200000
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
866630bbZn65.92603370400578.120922765878.75940792070SPN50.0000null0.000027.810019.467nullnullnullnullnullnullnull
886830bbZn67.92484429100595.371028158908.75545629645SPN50.0000null0.000018.570012.999nullnullnullnullnullnullnull

All Elements Appearing in Results Table: (10)

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
6CCarbon21412.01114675.31466382343002.55153.9464727722600.11407102004600Diamagneticnull-0.00001400000
7NNitrogen21514.006935611196.5870563.0577.363.04737643601.251null0.026583104019960Diamagneticnull-0.00000000680
8OOxygen21615.999384811196.2037854.890.23.4414128840781.429null0.0265891946100010400Paramagneticnull0.00000190772
27CoCobalt4958.933191526.62171176832001.8863.752796602389001710042125nullFerromagnetic1394null
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagnetic631null
29CuCopper41163.547241457.124131357.7732001.9118.44291116105892059400384.460nullDiamagneticnull-0.00000963000
30ZnZinc41265.386881429.15783692.6811801.65022117910071401712038870nullDiamagneticnull-0.00001580000