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 29-Oct-2025 10:41:11 (NZT):

Full SQL Query: "select * from FusionAllNewPlus where E1 in ('W', 'Ar') and E2 in ('Ni', 'Li', 'Al', 'B', 'N' ) order by MeV desc limit 100"

3 rows were found.

Results Table:

id	neutrino	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	BEin	E	A	nBorF	Z	aBorF	BEout	MeV
7494	none	Ar	40	b	18	b	Ni	64	b	28	b	905.54455938	Pd	104	b	46	b	892.80084481	-12.743715
7493	none	Ar	40	b	18	b	Ni	62	b	28	b	889.04978691	Pd	102	b	46	b	875.16673647	-13.883050
7462	none	Ar	38	b	18	b	Ni	64	b	28	b	889.07731236	Pd	102	b	46	b	875.16673647	-13.910576

All Nuclides Appearing in Results Table: (6)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
40	38	18	b	b	Ar	37.96273210400	327.33413710958	8.61405623973	SPN	50.0000	null	0.0000	0.0630	null	null	null	null	null	null	null	null
41	40	18	b	b	Ar	39.96238312378	343.80138413029	8.59503460326	SPN	50.0000	null	0.0000	99.6000	null	null	null	null	null	null	null	null
73	62	28	b	b	Ni	61.92834487100	545.24840277495	8.79432907702	SPN	50.0000	null	0.0000	3.6600	3.0744	null	null	null	null	null	null	null
74	64	28	b	b	Ni	63.92796634100	561.74317524830	8.77723711325	SPN	50.0000	null	0.0000	1.0800	0.9072	null	null	null	null	null	null	null
133	102	46	b	b	Pd	101.90563205800	875.16673646882	8.58006604381	SPN	50.0000	null	0.0000	0.9600	0.000144	null	null	null	null	null	null	null
134	104	46	b	b	Pd	103.90403040100	892.80084481188	8.58462350781	SPN	50.0000	null	0.0000	10.9700	0.0016455	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
18	Ar	Argon	3	18	39.94766	71	22392.18700	83.8	87.3	null	0	2	18	427066	1.784	null	0.01772	520.33	null	null	Diamagnetic	null	-0.00000001070
28	Ni	Nickel	4	10	58.72843	149	6.59277	1728	3186	1.91	112	4	28	1039668	8908	14	91	445	84	null	Ferromagnetic	631	null
46	Pd	Palladium	5	10	106.44101	169	8.85312	1828	3236	2.2	53.7	4	3	3177	12023	10	72	240	0.015	null	Paramagnetic	null	0.00078990000