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 07-Feb-2024 05:22:06 (NZT):

Full SQL Query: "select * from FissionAll where E = 'Bi' and MeV > 10 order by MeV desc limit 1000"

2 rows were found.

Results Table:

id	neutrino	E	A	nBorF	Z	aBorF	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	MeV
1733	right	Bi	209	f	83	b	O	17	f	8	f	Os	192	b	76	b	18.511580
1732	right	Bi	209	f	83	b	C	13	f	6	f	Pt	196	b	78	b	11.254310

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
16	13	6	f	f	C	13.00335483521	97.10512005305	7.46962461947	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589	6.72828600
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
287	192	76	b	b	Os	191.96147888100	1526.07356154380	7.94829979971	SPN	50.0000	null	0.0000	41.0000	0.000615	null	null	null	null	null	null	null
294	196	78	b	b	Pt	195.96495467500	1553.55556015470	7.92630387834	SPN	50.0000	null	0.0000	25.3000	0.001265	null	null	null	null	null	null	null
310	209	83	f	b	Bi	208.98039851900	1640.18217043150	7.84776158101	UPN	19.2788	A	3.1370	100.0000	0.0085	null	9/2-	4.0920000000	-0.5160000000	777.0000	64.277	4.37470000

All Elements Appearing in Results Table: (5)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
6	C	Carbon	2	14	12.01114	67	5.31466	3823	4300	2.55	153.9	4	6	47277	2260	0.1	140	710	200	4600	Diamagnetic	null	-0.00001400000
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
76	Os	Osmium	6	8	190.32953	185	8.41794	3306	5285	2.2	106.1	8	2	1600	22610	12	88	130	0.0015	null	Paramagnetic	null	0.00001400000
78	Pt	Platinum	6	10	195.08590	177	9.25016	2041.4	4098	2.28	205.3	6	2	1791	21090	9.4	72	133	0.005	null	Paramagnetic	null	0.00025730000
83	Bi	Bismuth	6	15	208.98042	143	21.36814	544.4	1837	2.02	91.2	5	6	8520	9780	0.77	8	122	0.0085	null	Diamagnetic	null	-0.00017000000