Fusion 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 ("Fusion.php") enables SQL commands to query the Fusion tables originally 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 Fission 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 all Fusion tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies implicitly in that, if the input side of the Core Query only involves E1 and E2, only rows whose associated mass numbers obey A1 <= A2 will appear in the results

Input used for this run on 17-Apr-2022 19:58:02 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('C') and E2 in ('F') order by MeV desc limit 100"

2 rows were found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E	A	nBorF	Z	aBorF	MeV
2506	right	531	C	13	f	6	f	F	19	f	9	b	S	32	b	16	b	27.651400
2410	none	380	C	12	b	6	b	F	19	f	9	b	P	31	f	15	b	22.953900

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
15	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032	null	null	null	null	null	null
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
23	19	9	f	b	F	18.99840316288	147.79709630986	7.77879454262	SPN	50.0000	null	0.0000	100.0000	585	null	1/2+	2.6283210000	null	4730.0000	376.345	25.16233000
36	31	15	f	b	P	30.97376199863	262.90924426058	8.48094336324	SPN	50.0000	null	0.0000	100.0000	1050	null	1/2+	1.1309250000	null	377.0000	161.923	10.83940000
37	32	16	b	b	S	31.97207117443	271.77299097355	8.49290596792	SPN	50.0000	null	0.0000	95.0000	332.5	396	null	null	null	null	null	null

All Elements Appearing in Results Table: (4)

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
9	F	Fluorine	2	17	18.99841	42	11201.88974	53.5	85.03	3.98	328	1	9	106434	1.696	null	0.0277	824	585	null	null	null	null
15	P	Phosphorus	3	15	30.97376	98	16.99054	317.3	553.6	2.19	72	5	15	296195	1823	10	0.236	769.7	1050	null	Diamagnetic	null	-0.00002060000
16	S	Sulfur	3	16	32.05750	88	16.35587	388.36	717.87	2.58	200	6	16	337138	1960	0	0.205	705	350	440	Diamagnetic	null	-0.00001220000