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

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 23-Aug-2020 13:02:08 (NZT):

Full SQL Query: "select * from FissionAllNew where E = 'Ni' and E2 in ('Mn') order by MeV desc"

4 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
1061	left	Ni	58	b	28	b	He	3	f	2	f	Mn	55	f	25	b	-17.447653
1131	none	Ni	61	f	28	f	Li	6	b	3	f	Mn	55	f	25	b	-20.596483
1193	right	Ni	64	b	28	b	Be	9	f	4	f	Mn	55	f	25	b	-20.735208
1162	none	Ni	62	b	28	b	Li	7	f	3	b	Mn	55	f	25	b	-23.941246

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz
6	3	2	f	f	He	3.01602932010	7.71737322095	2.57245774032	SPN	50.0000	null	0.0000	0.0001	null	35	1/2+	-2.1276253100	null	null	null
8	6	3	b	f	Li	6.01512288740	31.99263761964	5.33210626994	SPN	50.0000	null	0.0000	7.4200	1.484	null	1+	0.8220430000	-0.0008060000	3.5800	58.864
9	7	3	f	b	Li	7.01600343660	39.24349799105	5.60621399872	SPN	50.0000	null	0.0000	92.5800	18.516	null	3/2-	3.2564070000	-0.0400000000	1540.0000	155.455
10	9	4	f	f	Be	9.01218306500	58.16199300180	6.46244366687	SPN	50.0000	null	0.0000	100.0000	2.8	null	3/2-	-1.1774300000	0.0529000000	78.8000	56.207
63	55	25	f	b	Mn	54.93804391000	482.06319440408	8.76478535280	SPN	50.0000	null	0.0000	100.0000	950	null	5/2-	3.4669000000	0.3300000000	994.0000	98.980
70	58	28	b	b	Ni	57.93534241000	506.44588700108	8.73182563795	SPN	50.0000	null	0.0000	67.8800	57.0192	49	null	null	null	null	null
72	61	28	f	f	Ni	60.93105557000	534.65231505485	8.76479205008	SPN	50.0000	null	0.0000	1.1900	0.9996	null	3/2-	-0.7496500000	0.1620000000	null	null
73	62	28	b	b	Ni	61.92834537000	545.24793795928	8.79432157999	SPN	50.0000	null	0.0000	3.6600	3.0744	null	null	null	null	null	null
74	64	28	b	b	Ni	63.92796682000	561.74272906251	8.77723014160	SPN	50.0000	null	0.0000	1.0800	0.9072	null	null	null	null	null	null