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 04-Oct-2021 10:04:08 (NZT):

Full SQL Query: "select * from FissionAll where neutrino = 'none' and (E = 'Bi' ) 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
1731	none	Bi	209	f	83	b	B	11	f	5	b	Pt	198	b	78	b	3.336600
1730	none	Bi	209	f	83	b	He	4	b	2	b	Tl	205	f	81	b	3.122400

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
8	4	2	b	b	He	4.00260325413	28.29476455561	7.07369113890	SPN	50.0000	null	0.0000	99.9999	null	275200	null	null	null	null	null	null
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
295	198	78	b	b	Pt	197.96789673400	1566.95722279050	7.91392536763	SPN	50.0000	null	0.0000	7.2100	0.0003605	null	null	null	null	null	null	null
305	205	81	f	b	Tl	204.97442723700	1615.02470475210	7.87816929147	SPN	50.0000	null	0.0000	70.5000	0.59925	null	1/2+	1.6320000000	null	null	null	15.69218600
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	MagVolSus
2	He	Helium	1	18	4.00260	31	22423.54062	0	4.22	null	0	0	2	5250.5	0.1785	null	0.1513	5193.1	null	240000	Diamagnetic	-0.00000000105
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	-0.00002140000
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	0.00025730000
81	Tl	Thallium	6	13	204.38383	156	17.24758	577	1746	1.62	19.2	3	3	2878	11850	6.7	46	129	0.85	null	Diamagnetic	-0.00003560000
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	-0.00017000000