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 30-Apr-2022 01:52:56 (NZT):
Full SQL Query: "select * from TwoToTwoAll where E1 in ('Li','H','B','Cl') and E2 in ('Cu' ) and E3 in ('Al') order by MeV desc limit 100"
9 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
39767right27135B10b5fCu65f29bAl27f13bTi48b22b10.471851
39731right27133B10b5fCu63f29bAl27f13bTi46b22b7.792874
48537right27136B11f5bCu65f29bAl27f13bTi49f22f7.162252
39730left6337B10b5fCu63f29bAl27f13bCa46b20b6.809224
39766left6349B10b5fCu65f29bAl27f13bCa48b20b6.359312
19994right26920Li6b3fCu65f29bAl27f13bCa44b20b5.483700
48510right27134B11f5bCu63f29bAl27f13bTi47f22f5.222881
27475right26919Li7f3bCu63f29bAl27f13bCa43f20f4.922940
19963right26918Li6b3fCu63f29bAl27f13bCa42b20b4.245744

All Nuclides Appearing in Results Table: (16)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
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
13105bfB10.0129368620064.748588919276.47485889193SPN50.0000null0.000019.60001.96null3+1.80046360000.084500000022.000042.9752.87467955
14115fbB11.0093051660076.202580126116.92750728419SPN50.0000null0.000080.40008.04null3/2-2.68837800000.0405900000754.0000128.2868.58470700
322713fbAl26.98153840800224.945881970478.33132896187SPN50.0000null0.0000100.000082300585/2+3.64070000000.14660000001170.0000104.2276.97627800
514220bbCa41.95861782800361.886242916798.61633911707SPN50.0000null0.00000.6400265.6nullnullnullnullnullnullnull
524320ffCa42.95876643000369.818907957478.60043971994SPN50.0000null0.00000.145060.175null7/2--1.3173300000-0.0408000000nullnull-1.80306900
534420bbCa43.95548154300380.949848545988.65795110332SPN50.0000null0.00002.0600854.9nullnullnullnullnullnullnull
544620bbCa45.95368798800398.762708788668.66875453888SPN50.0000null0.00000.00331.3695nullnullnullnullnullnullnull
554820bbCa47.95252290400415.990151856048.66646149700UPN19.36192 B-4.27400.180074.7nullnullnullnullnullnullnull
574622bbTi45.95262685600398.186480413828.65622783508SPN50.0000null0.00007.9300444.08nullnullnullnullnullnullnull
584722ffTi46.95175775200407.067132826738.66100282610SPN50.0000null0.00007.2800407.68null5/2--0.78814000000.3020000000nullnull-1.51054000
594822bbTi47.94794093200418.693565990568.72278262480SPN50.0000null0.000073.94004140.64nullnullnullnullnullnullnull
604922ffTi48.94786462700426.835730627328.71093327811SPN50.0000null0.00005.5100308.56null7/2--1.10370000000.2470000000nullnull-1.51095000
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: (6)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
3LiLithium216.9417416712.97521453.6916150.9859.613118155351185357020nullParamagneticnull0.00000137000
5BBoron21310.81402874.39594234842732.0426.73532826.72460027103010nullDiamagneticnull-0.00002140000
13AlAluminium31326.981541189.99316933.4727921.6142.531322231627003823590482300nullParamagneticnull0.00002110000
20CaCalcium4240.0758619425.855391115175712.3722052776215502920063141500nullParamagneticnull0.00002139000
22TiTitanium4447.8789217610.62324194135601.547.642263929445072.5225205600nullParamagneticnull0.00018070000
29CuCopper41163.547241457.124131357.7732001.9118.44291116105892059400384.460nullDiamagneticnull-0.00000963000