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 25-Mar-2023 12:04:10 (NZT):

Full SQL Query: "select * from FissionAll where E = 'Au' and MEV < 10 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
1652	none	Au	197	f	79	b	He	4	b	2	b	Ir	193	f	77	b	0.623200
1653	none	Au	197	f	79	b	B	11	f	5	b	W	186	b	74	b	2.707900

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
277	186	74	b	b	W	185.95436521500	1485.83804616380	7.98837659228	SPN	50.0000	null	0.0000	28.4100	0.355125	null	null	null	null	null	null	null
289	193	77	f	b	Ir	192.96292382400	1532.01635887860	7.93790859523	SPN	50.0000	null	0.0000	62.7000	0.000627	null	3/2+	0.1630000000	0.7510000000	null	null	0.52270000
296	197	79	f	b	Au	196.96657011400	1559.33954143160	7.91542914432	SPN	50.0000	null	0.0000	100.0000	0.004	null	3/2+	0.1452000000	0.5470000000	null	null	0.47306000

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
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	null	-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	null	-0.00002140000
74	W	Tungsten	6	6	183.84152	193	9.55021	3695	5828	2.36	78.6	6	2	1700	19250	20	170	132	1.25	null	Paramagnetic	null	0.00008840000
77	Ir	Iridium	6	9	192.21637	180	8.48637	2739	4701	2.2	151	8	2	1600	22650	21	150	131	0.001	null	Paramagnetic	null	0.00003770000
79	Au	Gold	6	11	196.96655	174	10.20552	1337.33	3129	2.54	222.8	5	2	1980	19300	45	320	129.1	0.004	null	Diamagnetic	null	-0.00003440000