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 02-Mar-2023 15:06:07 (NZT):

Full SQL Query: "select * from FissionAllNewPlus where (E = 'Al' and E1 in ('B') ) and nBorF = 'f' order by MeV desc limit 1000"

2 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	BEin	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	BEout	MeV
254	none	Al	27	f	13	b	224.94588197	B	11	f	5	b	O	16	b	8	b	203.81830726	-21.127575
253	none	Al	27	f	13	b	224.94588197	B	10	b	5	f	O	17	f	8	f	196.50716376	-28.438718

All Nuclides Appearing in Results Table: (5)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
13	10	5	b	f	B	10.01293686200	64.74858891927	6.47485889193	SPN	50.0000	null	0.0000	19.6000	1.96	null	3+	1.8004636000	0.0845000000	22.0000	42.975	2.87467955
14	11	5	f	b	B	11.00930516600	76.20258012611	6.92750728419	SPN	50.0000	null	0.0000	80.4000	8.04	null	3/2-	2.6883780000	0.0405900000	754.0000	128.286	8.58470700
20	16	8	b	b	O	15.99491461960	127.61572713267	7.97598294579	SPN	50.0000	null	0.0000	99.7590	459888.99	9592	null	null	null	null	null	null
21	17	8	f	f	O	16.99913175664	131.75857483770	7.75050440222	SPN	50.0000	null	0.0000	0.0370	170.57	null	5/2+	-1.8935430000	-0.0256000000	0.0610	50.227	-3.62806000
32	27	13	f	b	Al	26.98153840800	224.94588197047	8.33132896187	SPN	50.0000	null	0.0000	100.0000	82300	58	5/2+	3.6407000000	0.1466000000	1170.0000	104.227	6.97627800

All Elements Appearing in Results Table: (3)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
5	B	Boron	2	13	10.81402	87	4.39594	2348	4273	2.04	26.7	3	5	32826.7	2460	0	27	1030	10	null	Diamagnetic	null	-0.00002140000
8	O	Oxygen	2	16	15.99938	48	11196.20378	54.8	90.2	3.44	141	2	8	84078	1.429	null	0.02658	919	461000	10400	Paramagnetic	null	0.00000190772
13	Al	Aluminium	3	13	26.98154	118	9.99316	933.47	2792	1.61	42.5	3	13	222316	2700	38	235	904	82300	null	Paramagnetic	null	0.00002110000