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

Fusion Reactions | Fission Reactions | Two To Two Reactions | All Tables
CascadesAll | Cascades4 | Cascades5Lite | Cascades5 | All Results
Show Element Data | Tables in Detail | Downloads | Notes


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 15-Sep-2020 01:03:33 (NZT):
Full SQL Query: "select * from TwoToTwoAll where (E4 in ('F' ) ) and nBorF1 = 'b' order by MeV desc"
18 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
38469none11720B10b5fB10b5fH1f1bF19f9b18.302000
38490none11741B10b5fC13f6fHe4b2bF19f9b14.237900
19263none6102Li6b3fO17f8fHe4b2bF19f9b12.344200
19248none6080Li6b3fN14b7fH1f1bF19f9b11.306500
38477none11724B10b5fB11f5bD2b1fF19f9b9.070000
38567none11824B10b5fNe21f10fC12b6bF19f9b7.808700
4308right6D2b1fO18b8bH1f1bF19f9b6.550261
4316none27D2b1fNe21f10fHe4b2bF19f9b6.467400
38619none11883B10b5fMg25f12fO16b8bF19f9b5.085000
65829none20758N14b7fO17f8fC12b6bF19f9b3.699000
65872none20801N14b7fNe21f10fO16b8bF19f9b3.512700
19253none6088Li6b3fN15f7bD2b1fF19f9b2.540200
38580none11839B10b5fNe22b10bC13f6fF19f9b2.389300
19320none6170Li6b3fMg25f12fC12b6bF19f9b2.385600
38534none11788B10b5fO18b8bBe9f4fF19f9b1.404700
38594none11851B10b5fNa23f11bN14b7fF19f9b0.992000
95705right12469O18b8bO18b8bO17f8fF19f9b0.727491
65839none20766N14b7fO18b8bC13f6fF19f9b0.599000

All Nuclides Appearing in Results Table:

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHz
311fbH1.007825032230.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.000
421bfD2.014101778122.224114101381.11205705069SPN50.0000null0.00000.01500.21231+0.85743823100.00286000000.008261.403
742bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnull
863bfLi6.0151228874031.992637619645.33210626994SPN50.0000null0.00007.42001.484null1+0.8220430000-0.00080600003.580058.864
1094ffBe9.0121830650058.161993001806.46244366687SPN50.0000null0.0000100.00002.8null3/2--1.17743000000.052900000078.800056.207
11105bfB10.0129369500064.748506947776.47485069478SPN50.0000null0.000019.60001.96null3+1.80046360000.084500000022.000042.975
12115fbB11.0093053600076.202399416216.92749085602SPN50.0000null0.000080.40008.04null3/2-2.68837800000.0405900000754.0000128.286
13126bbC12.0000000000092.159043079567.67992025663SPN50.0000null0.000098.8900197.783032nullnullnullnullnull
14136ffC13.0033548350797.105120183467.46962462950SPN50.0000null0.00001.11002.22371/2-0.7023690000null1.0000100.589
16147bfN14.00307400443104.655465884947.47539042035SPN50.0000null0.000099.630018.929711051+0.40357300000.0204400000nullnull
17157fbN15.00010889888115.488531864807.69923545765SPN50.0000null0.00000.37000.0703null1/2--0.2830569000null0.022040.547
18168bbO15.99491461957127.615727160617.97598294754SPN50.0000null0.000099.7590459888.999592nullnullnullnullnull
19178ffO16.99913175650131.758574968117.75050440989SPN50.0000null0.00000.0370170.57null5/2+-1.8935430000-0.02560000000.061050.227
20188bbO17.99915961286139.803713888247.76687299379SPN50.0000null0.00000.2040940.44nullnullnullnullnullnull
21199fbF18.99840316273147.797096449597.77879454998SPN50.0000null0.0000100.0000585null1/2+2.6283210000null4730.0000376.345
232110ffNe20.99384668500167.401270149327.97148905473SPN50.0000null0.00000.2570nullnull3/2+-0.66170000000.1020000000nullnull
242210bbNe21.99138511400177.765296549118.08024075223SPN50.0000null0.00008.8200null208nullnullnullnullnull
252311fbNa22.98976928200186.559188452728.11126906316SPN50.0000null0.0000100.000023600333/2+2.21750000000.1040000000525.0000105.808
272512ffMg24.98583697600205.581949722808.22327798891SPN50.0000null0.000010.13002360.29695/2+-0.85533000000.1990000000nullnull