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 17-Mar-2022 10:59:45 (NZT):
Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (E1 in ('H', 'D', 'T') and E2 in ('Ca') ) order by MeV desc limit 1000"
18 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
1210747none516878T3f1bCa40b20bHe4b2bK39f19b11.477198
1210746none516877T3f1bCa40b20bH1f1bCa42b20b11.350515
1210750none516881T3f1bCa42b20bH1f1bCa44b20b10.583895
1210753none516884T3f1bCa43f20fn*1f0fSc45f21b9.543416
1210751none516882T3f1bCa42b20bHe4b2bK41f19b9.537827
1210754none516885T3f1bCa44b20bH1f1bCa46b20b9.338487
4380none59D2b1fCa43f20fH1f1bCa44b20b8.911600
1210755none516886T3f1bCa46b20bH1f1bCa48b20b8.896028
4381none60D2b1fCa43f20fHe4b2bK41f19b7.865500
4374none57D2b1fCa42b20bH1f1bCa43f20f5.705400
4376none58D2b1fCa42b20bHe4b2bK40b19f5.699800
1210752none516883T3f1bCa43f20fD2b1fCa44b20b4.878494
1210743none516874T3f1bCa40b20bC12b6bP31f15b4.541293
1210745none516876T3f1bCa40b20bO16b8bAl27f13b2.038368
1210748none516879T3f1bCa42b20bD2b1fCa43f20f1.672291
1210744none516875T3f1bCa40b20bN15f7bSi28b14b1.493444
1210749none516880T3f1bCa42b20bN15f7bSi30b14b0.752906
23none56H1f1bCa42b20bHe4b2bK39f19b0.126700

All Nuclides Appearing in Results Table: (22)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
310ffn*1.008664915820.000000000000.00000000000UPN-4.6070null0.0000100.0000nullnull1/2+-1.9130427000nullnullnull-18.32471830
411fbH1.007825032240.000000000000.00000000000SPN50.0000null0.000099.98501399.797057001/2+2.7928473510null5700.0000400.00026.75222080
521bfD2.014101778112.224114110701.11205705535SPN50.0000null0.00000.01500.21231+0.85743823100.00286000000.008261.4034.10662920
631fbT3.016049281998.481112243522.82703741451SYN1.0906B-0.01860.00000null1/2+2.9789624600null6897.0000426.65628.53498650
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
15126bbC12.0000000000092.159043079567.67992025663SPN50.0000null0.000098.8900197.783032nullnullnullnullnullnull
19157fbN15.00010889894115.488531808917.69923545393SPN50.0000null0.00000.37000.0703null1/2--0.2830569000null0.022040.547-2.71261890
20168bbO15.99491461960127.615727132677.97598294579SPN50.0000null0.000099.7590459888.999592nullnullnullnullnullnull
322713fbAl26.98153840800224.945881970478.33132896187SPN50.0000null0.0000100.000082300585/2+3.64070000000.14660000001170.0000104.2276.97627800
332814bbSi27.97692653499236.530569098018.44752032493SPN50.0000null0.000092.2100260032.2653nullnullnullnullnullnull
353014bbSi29.97377013600255.612910794918.52043035983SPN50.0000null0.00003.09008713.823nullnullnullnullnullnull
363115fbP30.97376199863262.909244260588.48094336324SPN50.0000null0.0000100.00001050null1/2+1.1309250000null377.0000161.92310.83940000
463919fbK38.96370648661333.715258781278.55680150721SPN50.0000null0.000093.100019457.9null3/2+0.39147000000.0585000000nullnull1.25006120
474019bfK39.96399816600341.514648043908.53786620110UPN9.0969B- or K or B+1.50500.01182.4662null4--1.2979700000-0.0730000000nullnull-1.55428600
484119fbK40.96182525796351.609786532148.57584845200SPN50.0000null0.00006.88001437.92null3/2+0.21487200000.0711000000nullnull0.68614062
494020bbCa39.96259086500342.043207541018.55108018853SPN50.0000null0.000096.970040242.5560nullnullnullnullnullnull
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
564521fbSc44.95590750300387.841822771298.61870717270SPN50.0000null0.0000100.000022null7/2-4.7540000000-0.22000000001710.000097.1676.50880000

All Elements Appearing in Results Table: (11)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
1HHydrogen111.007985311212.1902114.0120.282.272.81113120.0899null0.1805143001400739000Diamagneticnull-0.00000000223
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagneticnull-0.00000000105
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
13AlAluminium31326.981541189.99316933.4727921.6142.531322231627003823590482300nullParamagneticnull0.00002110000
14SiSilicon31428.0856111112.05391168731731.9133.641425792323300.001150710282000650Diamagneticnull-0.00000373000
15PPhosphorus31530.973769816.99054317.3553.62.19725152961951823100.236769.71050nullDiamagneticnull-0.00002060000
19KPotassium4139.0981124345.67536336.5310320.8248.41194760638561410075720900nullParamagneticnull0.00000574000
20CaCalcium4240.0758619425.855391115175712.3722052776215502920063141500nullParamagneticnull0.00002139000
21ScScandium4344.9959218415.07401181431031.3618.132158216329851.81656722nullParamagneticnull0.00026270000