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 22-Aug-2021 11:54:16 (NZT):

Full SQL Query: "select * from FissionAll where neutrino = 'none' and (E2 = 'Ca' ) order by MeV desc limit 1000"

3 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
11	none	Zr	96	b	40	b	Ca	48	b	20	b	Ca	48	b	20	b	3.236000
54	none	Mo	95	f	42	f	Ti	47	f	22	f	Ca	48	b	20	b	1.489500
10	none	Zr	94	b	40	b	Ca	46	b	20	b	Ca	48	b	20	b	0.082000

All Nuclides Appearing in Results Table: (6)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
54	46	20	b	b	Ca	45.95368798800	398.76270878866	8.66875453888	SPN	50.0000	null	0.0000	0.0033	1.3695	null	null	null	null	null	null	null
55	48	20	b	b	Ca	47.95252290400	415.99015185604	8.66646149700	UPN	19.3619	2 B-	4.2740	0.1800	74.7	null	null	null	null	null	null	null
58	47	22	f	f	Ti	46.95175775200	407.06713282673	8.66100282610	SPN	50.0000	null	0.0000	7.2800	407.68	null	5/2-	-0.7881400000	0.3020000000	null	null	-1.51054000
126	94	40	b	b	Zr	93.90631252400	814.65819101258	8.66657650013	SPN	50.0000	null	0.0000	17.4000	28.71	null	null	null	null	null	null	null
127	96	40	b	b	Zr	95.90827762100	828.96988821546	8.63510300224	UPN	19.3010	2 B-	3.4000	2.8000	4.62	null	null	null	null	null	null	null
131	95	42	f	f	Mo	94.90583744200	821.60714734519	8.64849628784	SPN	50.0000	null	0.0000	15.7200	0.18864	null	5/2+	-0.9132000000	-0.0220000000	null	null	-1.75140000

All Elements Appearing in Results Table: (4)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	MagVolSus
20	Ca	Calcium	4	2	40.07586	194	25.85539	1115	1757	1	2.37	2	20	527762	1550	29	200	631	41500	null	Paramagnetic	0.00002139000
22	Ti	Titanium	4	4	47.87892	176	10.62324	1941	3560	1.54	7.6	4	22	639294	4507	2.5	22	520	5600	null	Paramagnetic	0.00018070000
40	Zr	Zirconium	5	4	91.22340	206	14.01066	2128	4682	1.33	41.1	4	6	9500	6511	2.4	23	278	165	null	Paramagnetic	0.00010900000
42	Mo	Molybdenum	5	6	95.21689	190	9.26234	2896	4912	2.16	71.9	6	30	154500	10280	20	139	251	1.2	null	Paramagnetic	0.00012030000