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 26-Jan-2022 11:13:20 (NZT):

Full SQL Query: "select * from FissionAllNewPlus where E = 'Au' and E1 = 'C' and MeV > 1.0 order by MeV desc limit 100"

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
7712	right	Au	197	f	79	b	1559.33954143	C	14	b	6	b	W	183	f	74	f	1571.54549440	12.205953
7711	right	Au	197	f	79	b	1559.33954143	C	13	f	6	f	W	184	b	74	b	1570.78017234	11.440631

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
17	14	6	b	b	C	14.00324198843	105.28132315081	7.52009451077	UPN	3.7581	B-	0.1565	0.0000	0	null	3-	0.8200000000	null	null	null	null
275	183	74	f	f	W	182.95022450000	1465.48183783830	8.00809747453	SPN	50.0000	null	0.0000	14.4000	0.18	null	1/2-	0.1173900000	null	null	null	1.12824070
276	184	74	b	b	W	183.95093326000	1472.89271887610	8.00485173302	SPN	50.0000	null	0.0000	30.6400	0.383	null	null	null	null	null	null	null
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: (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
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
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
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