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 19-Aug-2020 06:44:34 (NZT):

Full SQL Query: "select * from FissionAll where neutrino = 'none' and (E = 'W' and E1 = 'Ca' ) order by MeV desc"

6 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
1475	none	W	184	b	74	b	Ca	48	b	20	b	Xe	136	b	54	b	85.144100
1462	none	W	182	b	74	b	Ca	48	b	20	b	Xe	134	b	54	b	84.308600
1448	none	W	180	b	74	b	Ca	48	b	20	b	Xe	132	b	54	b	84.258300
1447	none	W	180	b	74	b	Ca	46	b	20	b	Xe	134	b	54	b	81.871800
1461	none	W	182	b	74	b	Ca	46	b	20	b	Xe	136	b	54	b	81.375300
1446	none	W	180	b	74	b	Ca	44	b	20	b	Xe	136	b	54	b	78.496100

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
48	44	20	b	b	Ca	43.95548156000	380.94983271058	8.65795074342	SPN	50.0000	null	0.0000	2.0600	854.9	null	null	null	null	null	null
49	46	20	b	b	Ca	45.95368900000	398.76176611640	8.66873404601	SPN	50.0000	null	0.0000	0.0033	1.3695	null	null	null	null	null	null
50	48	20	b	b	Ca	47.95252276000	415.99028599123	8.66646429148	UPN	19.3619	2 b-	4.2740	0.1800	74.7	null	null	null	null	null	null
178	132	54	b	b	Xe	131.90415508560	1112.41646945910	8.42739749590	SPN	50.0000	null	0.0000	26.8900	null	null	null	null	null	null	null
179	134	54	b	b	Xe	133.90539466000	1127.40398685280	8.41346258845	SPN	50.0000	null	0.0000	10.4400	null	null	null	null	null	null	null
180	136	54	b	b	Xe	135.90721448400	1141.85100503200	8.39596327229	UPN	21.3354	2 b-	2.4620	8.8700	null	null	null	null	null	null	null
252	180	74	b	b	W	179.94671080000	1444.54156859320	8.02523093663	UPN	18.2555	a	2.5090	0.1400	0.00175	null	null	null	null	null	null
253	182	74	b	b	W	181.94820394000	1459.29289106730	8.01809280806	SPN	50.0000	null	0.0000	26.4100	0.330125	null	null	null	null	null	null
255	184	74	b	b	W	183.95093092000	1472.89489857280	8.00486357920	SPN	50.0000	null	0.0000	30.6400	0.383	null	null	null	null	null	null