Fission 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

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This program ("Fission.php") enables SQL commands to query the Fission tables 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, TwoToTwo 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 the Fission tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly, in that, if the ouput side of the Core Query only involves E1 and E2, only rows for which their associated mass numbers obey the rule that A1 <= A2 will be included in the results

Input used for this run on 25-Aug-2022 11:06:14 (NZT):
Full SQL Query: "select * from FissionAllNewPlus where E = 'U' and MeV > 1 order by MeV desc limit 100"
3 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFBEinE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2BEoutMeV
7990rightU235f92f1783.81190219He4b2bPa231f91b1788.881430515.069528
7982noneU234b92b1778.51463769He4b2bTh230b90b1783.372155104.857517
7992noneU236b92b1790.35719119He4b2bTh232b90b1794.930137084.572946

All Nuclides Appearing in Results Table: (7)

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHzMagGR
842bbHe4.0026032541328.294764555617.07369113890SPN50.0000null0.000099.9999null275200nullnullnullnullnullnull
31223090bbTh230.033132358001755.077390540507.63077126322UPN4.8773A4.4384nullnullnullnullnullnullnullnullnull
31323290bbTh232.038053689001766.635372523707.61480764019UPN10.1480A or SF4.0830100.00009.6nullnullnullnullnullnullnull
31423191fbPa231.035882575001759.804332540507.61820057377UPN4.5153A4.5990100.0000nullnull3/2-1.9900000000-1.7200000000nullnull6.42000000
31623492bbU234.040950370001778.514637689307.60048990466UPN5.3904A4.6035nullnullnullnullnullnullnullnullnull
31723592ffU235.043928190001783.811902194507.59068894551UPN8.8476A or SF4.67900.72000.01944null7/2--0.38000000004.9360000000nullnull-0.52000000
31823692bbU236.045566201001790.357191191407.58625928471UPN7.3692A4.3320nullnullnullnullnullnullnullnullnull

All Elements Appearing in Results Table: (4)

ZEENamePGAWeightARadiusMolarVolMeltingBoilingNegativityAffinityValMxInumMxInizeSTPDensityElectGThermGSpecHeatppmECrustppmEStellarMagTypeCuriePtKMagVolSus
2HeHelium1184.002603122423.5406204.22null0025250.50.1785null0.15135193.1null240000Diamagneticnull-0.00000000105
90ThThorium74232.03877null19.79173202350931.3null442780117246.7541189.6nullParamagneticnull0.00008400000
91PaProtactinium75231.03588null15.03160184542731.5null51568153705.64799.1nullnullParamagneticnull0.00049950000
92UUranium76238.02891null12.49500140842001.38null621420190503.6271162.7nullParamagneticnull0.00041100000