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 | Overview | Select LENR Events


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 29-Jun-2023 09:55:05 (NZT):
Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (A1 = 16 and E2 in ('Pd', 'Ag') and E3 in ('Fe') ) order by MeV desc limit 100"
9 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
83701none28058O16b8bAg107f47bFe58b26bCu65f29b36.167100
83610none27926O16b8bPd106b46bFe58b26bNi64b28b34.357200
83510none27780O16b8bPd104b46bFe58b26bNi62b28b34.333000
83459none27619O16b8bPd102b46bFe56b26bNi62b28b34.072200
83564none27852O16b8bPd105f46fFe57f26fNi64b28b33.721900
83462none27621O16b8bPd102b46bFe58b26bNi60b28b33.347500
83508none27779O16b8bPd104b46bFe56b26bNi64b28b33.146300
83460none27620O16b8bPd102b46bFe57f26fNi61f28f31.123100
83458none27617O16b8bPd102b46bFe54b26bNi64b28b30.064000

All Nuclides Appearing in Results Table: (15)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
20168bbO15.99491461960127.615727132677.97598294579SPN50.0000null0.000099.7590459888.999592nullnullnullnullnullnull
705426bbFe53.93960830600471.752548023018.73615829672SPN50.0000null0.00005.82003276.6672nullnullnullnullnullnull
715626bbFe55.93493561700492.247305272248.79013045129SPN50.0000null0.000091.660051604.581169nullnullnullnullnullnull
725726ffFe56.93539213400499.893149235218.77005524974SPN50.0000null0.00002.19001232.97281/2-0.0906400000nullnullnull0.86806270
735826bbFe57.93327373800509.937510067078.79202603564SPN50.0000null0.00000.3300185.79nullnullnullnullnullnullnull
796028bbNi59.93078525600526.833024052508.78055040087SPN50.0000null0.000026.230022.0332nullnullnullnullnullnullnull
806128ffNi60.93105494500534.652897238808.76480159408SPN50.0000null0.00001.19000.9996null3/2--0.74965000000.1620000000nullnull-2.39477000
816228bbNi61.92834487100545.248402774958.79432907702SPN50.0000null0.00003.66003.0744nullnullnullnullnullnullnull
826428bbNi63.92796634100561.743175248308.77723711325SPN50.0000null0.00001.08000.9072nullnullnullnullnullnullnull
846529fbCu64.92778948700569.196667298788.75687180460SPN50.0000null0.000030.910018.546null3/2-2.3844000000-0.2040000000201.0000113.6697.60430000
14710246bbPd101.90563205800875.166736468828.58006604381SPN50.0000null0.00000.96000.000144nullnullnullnullnullnullnull
14810446bbPd103.90403040100892.800844811888.58462350781SPN50.0000null0.000010.97000.0016455nullnullnullnullnullnullnull
14910546ffPd104.90507948700899.894714109108.57042584866SPN50.0000null0.000022.23000.0033345null5/2+-0.64200000000.6600000000nullnull-1.23000000
15010646bbPd105.90348029300909.455441219988.57976831340SPN50.0000null0.000027.33000.0040995nullnullnullnullnullnullnull
15410747fbAg106.90509153100915.243335704608.55367603462SPN50.0000null0.000051.82000.038865null1/2--0.1135200000nullnullnull-1.08891800

All Elements Appearing in Results Table: (6)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
8OOxygen21615.999384811196.2037854.890.23.4414128840781.429null0.0265891946100010400Paramagneticnull0.00000190772
26FeIron4855.847311567.09262181131341.8315.762689516178741080449563001090Ferromagnetic1043null
28NiNickel41058.728431496.59277172831861.9111242810396688908149144584nullFerromagnetic631null
29CuCopper41163.547241457.124131357.7732001.9118.44291116105892059400384.460nullDiamagneticnull-0.00000963000
46PdPalladium510106.441011698.85312182832362.253.74331771202310722400.015nullParamagneticnull0.00078990000
47AgSilver511107.8684416510.282981234.9324351.93125.643336110490624302350.075nullDiamagneticnull-0.00002380000