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 19-Aug-2020 08:13:41 (NZT):
Full SQL Query: "select * from FissionAll where E = 'Cs' order by MeV desc"
2 rows were found.
.
Results Table:

idneutrinoEAnBorFZaBorFE1A1nBorF1Z1aBorF1E2A2nBorF2Z2aBorF2MeV
641rightCs137f55bnu0b0bBa137f56f1.173681
640rightCs133f55bO17f8fCd116b48b0.881191

All Nuclides Appearing in Results Table:

idAZnBorFaBorFEAMUBEBENSUSLHLRDMDEMeVpcaNCrustppmNCrustppmNSolarSPMDEQRCPTInova_MHz
29300bbnu0.000000000000.000000000000.00000000000SPN50.0000null0.00000.000000nullnullnullnullnull
19178ffO16.99913175650131.758574968117.75050440989SPN50.0000null0.00000.0370170.57null5/2+-1.8935430000-0.02560000000.061050.227
14811648bbCd115.90476315000987.406669990038.51212646543UPN19.49162 b-2.80907.58000.01137nullnullnullnullnullnull
18113355fbCs132.905451961001118.497190924308.40975331522SPN50.0000null0.0000100.00003null7/2+2.5778000000-0.0034300000269.000052.465
18213755fbCs136.907089000001149.256646218508.38873464393UPN1.5092g or b-0.66170.00000null7/2+2.83740000000.0480000000nullnull
18813756ffBa136.905827140001149.649728248308.39160385583SPN50.0000null0.000011.320048.11null3/2+0.93750000000.24500000004.410044.452