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 22-Dec-2022 06:18:04 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('Fe', 'S') and E2 in ('Na', 'Cl', 'H', 'O', 'Si' ) order by MeV desc limit 1000"

One row was found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E	A	nBorF	Z	aBorF	MeV
3633	left	1624	S	33	f	16	f	Cl	37	f	17	b	Ge	70	b	32	b	12.090795

All Nuclides Appearing in Results Table: (3)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
38	33	16	f	f	S	32.97145890985	280.41439892209	8.49740602794	SPN	50.0000	null	0.0000	0.7600	2.66	null	3/2+	0.6432500000	-0.0678000000	null	null	2.05568500
42	37	17	f	b	Cl	36.96590258400	317.09209940329	8.57005674063	SPN	50.0000	null	0.0000	24.4700	35.4815	null	3/2+	0.6840000000	-0.0644000000	null	null	2.18436880
92	70	32	b	b	Ge	69.92424870600	610.50331931480	8.72147599021	SPN	50.0000	null	0.0000	20.5200	0.3078	null	null	null	null	null	null	null

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
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
17	Cl	Chlorine	3	17	35.45753	79	11032.21248	171.6	239.11	3.16	349	7	17	380760	3.214	0	0.0089	478.2	145	null	Diamagnetic	null	-0.00000002310
32	Ge	Germanium	4	14	72.56952	125	13.63320	1211.4	3093	2.01	119	4	5	9020	5323	0.002	60	321.4	1.5	null	Diamagnetic	null	-0.00000798000