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 10:56:59 (NZT):
Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (E1 in ('H', 'D', 'T') and E2 in ('K') ) order by MeV desc limit 1000"
20 rows were found.
.
Results Table:

idneutrinoid_subE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2E3A3nBorF3Z3aBorF3E4A4nBorF4Z4aBorF4MeV
1210735none516866T3f1bK39f19bHe4b2bAr38b18b13.446376
1210742none516873T3f1bK41f19bHe4b2bAr40b18b12.013738
4365none52D2b1fK40b19fHe4b2bAr38b18b11.906400
1210738none516869T3f1bK40b19fn*1f0fCa42b20b11.889850
1210741none516872T3f1bK41f19bn*1f0fCa43f20f9.724126
1210734none516865T3f1bK39f19bH1f1bK41f19b9.411144
4362none51D2b1fK40b19fH1f1bK41f19b7.871100
1210731none516862T3f1bK39f19bC12b6bSi30b14b5.591087
4358none48D2b1fK39f19bH1f1bK40b19f5.573100
4366none53D2b1fK40b19fC12b6bSi30b14b4.051100
22none55H1f1bK41f19bHe4b2bAr38b18b4.035200
1210739none516870T3f1bK40b19fD2b1fK41f19b3.838015
1210737none516868T3f1bK40b19fC13f6fSi30b14b2.740715
1210733none516864T3f1bK39f19bO16b8bMg26b12b2.102641
1210732none516863T3f1bK39f19bD2b1fK40b19f1.540019
1210740none516871T3f1bK40b19fHe3f2fAr40b18b1.530704
18none47H1f1bK39f19bHe4b2bAr36b18b1.292900
4361none49D2b1fK39f19bC12b6bSi29f14f1.234200
4367none54D2b1fK40b19fO16b8bMg26b12b0.562600
1210736none516867T3f1bK40b19fBe9f4fS34b16b0.005848

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
732ffHe3.016029322657.717370845642.57245694855SPN50.0000null0.00000.0001null351/2+-2.1276253100nullnullnull-20.37894730
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
1194ffBe9.0121830660058.161992070306.46244356337SPN50.0000null0.0000100.00002.8null3/2--1.17743000000.052900000078.800056.207-3.75066000
15126bbC12.0000000000092.159043079567.67992025663SPN50.0000null0.000098.8900197.783032nullnullnullnullnullnull
16136ffC13.0033548352197.105120053057.46962461947SPN50.0000null0.00001.11002.22371/2-0.7023690000null1.0000100.5896.72828600
20168bbO15.99491461960127.615727132677.97598294579SPN50.0000null0.000099.7590459888.999592nullnullnullnullnullnull
302612bbMg25.98259297100216.674808959968.33364649846SPN50.0000null0.000011.17002602.6179nullnullnullnullnullnull
342914ffSi28.97649466525245.003940275288.44841173363SPN50.0000null0.00004.700013254341/2+-0.5550520000null2.090079.468-5.31903000
353014bbSi29.97377013600255.612910794918.52043035983SPN50.0000null0.00003.09008713.823nullnullnullnullnullnull
393416bbS33.96786701200291.831318377728.58327406993SPN50.0000null0.00004.220014.77nullnullnullnullnullnullnull
433618bbAr35.96754510500306.708680027418.51968555632SPN50.0000null0.00000.3370null77nullnullnullnullnullnull
443818bbAr37.96273210400327.334137109588.61405623973SPN50.0000null0.00000.0630nullnullnullnullnullnullnullnull
454018bbAr39.96238312378343.801384130298.59503460326SPN50.0000null0.000099.6000nullnullnullnullnullnullnullnull
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
514220bbCa41.95861782800361.886242916798.61633911707SPN50.0000null0.00000.6400265.6nullnullnullnullnullnullnull
524320ffCa42.95876643000369.818907957478.60043971994SPN50.0000null0.00000.145060.175null7/2--1.3173300000-0.0408000000nullnull-1.80306900

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
4BeBeryllium229.012191124.87672156027431.5702421006.618482519018202.8nullDiamagneticnull-0.00002328000
6CCarbon21412.01114675.31466382343002.55153.9464727722600.11407102004600Diamagneticnull-0.00001400000
8OOxygen21615.999384811196.2037854.890.23.4414128840781.429null0.0265891946100010400Paramagneticnull0.00000190772
12MgMagnesium3224.3095514513.9870892313631.310212189368173823160102023300580Paramagneticnull0.00001200000
14SiSilicon31428.0856111112.05391168731731.9133.641425792323300.001150710282000650Diamagneticnull-0.00000373000
16SSulfur31632.057508816.35587388.36717.872.58200616337138196000.205705350440Diamagneticnull-0.00001220000
18ArArgon31839.947667122392.1870083.887.3null02184270661.784null0.01772520.33nullnullDiamagneticnull-0.00000001070
19KPotassium4139.0981124345.67536336.5310320.8248.41194760638561410075720900nullParamagneticnull0.00000574000
20CaCalcium4240.0758619425.855391115175712.3722052776215502920063141500nullParamagneticnull0.00002139000