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 03-Jun-2026 18:26:56 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('H') and E in ('V' ) order by MeV desc limit 100"

3 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
56	left	41	H	1	f	1	b	V	50	b	23	f	V	51	f	23	b	10.257615
55	none	1189	H	1	f	1	b	Ti	50	b	22	b	V	51	f	23	b	8.045300
53	none	1187	H	1	f	1	b	Ti	49	f	22	f	V	50	b	23	f	7.942900

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
3	1	1	f	b	H	1.00782503224	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700	1/2+	2.7928473510	null	5700.0000	400.000	26.75222080
55	49	22	f	f	Ti	48.94786462700	426.83573062732	8.71093327811	SPN	50.0000	null	0.0000	5.5100	308.56	null	7/2-	-1.1037000000	0.2470000000	null	null	-1.51095000
56	50	22	b	b	Ti	49.94478583900	437.77469116518	8.75549382330	SPN	50.0000	null	0.0000	5.3400	299.04	null	null	null	null	null	null	null
57	50	23	b	f	V	49.94715584500	434.78471059568	8.69569421191	UPN	17.1461	B+ or B-	2.2050	0.2400	0.288	null	6+	3.3442000000	0.2100000000	null	null	2.67065000
58	51	23	f	b	V	50.94395686700	445.83562743748	8.74187504779	SPN	50.0000	null	0.0000	99.7600	119.712	null	7/2-	5.1464000000	-0.0430000000	2160.0000	101.212	7.04551390

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
1	H	Hydrogen	1	1	1.00798	53	11212.19021	14.01	20.28	2.2	72.8	1	1	1312	0.0899	null	0.1805	14300	1400	739000	Diamagnetic	null	-0.00000000223
22	Ti	Titanium	4	4	47.87892	176	10.62324	1941	3560	1.54	7.6	4	22	639294	4507	2.5	22	520	5600	null	Paramagnetic	null	0.00018070000
23	V	Vanadium	4	5	50.94159	171	8.33741	2183	3680	1.63	50.6	5	23	699144	6110	5	31	489	120	null	Paramagnetic	null	0.00038370000