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 05-Sep-2021 21:25:01 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('C', 'Be') and E in ('Au' ) order by MeV desc limit 100"

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
1946	left	792	Be	9	f	4	f	Os	188	b	76	b	Au	197	f	79	b	1.494119

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
11	9	4	f	f	Be	9.01218306600	58.16199207030	6.46244356337	SPN	50.0000	null	0.0000	100.0000	2.8	null	3/2-	-1.1774300000	0.0529000000	78.8000	56.207	-3.75066000
284	188	76	b	b	Os	187.95583736100	1499.04425760990	7.97363966814	SPN	50.0000	null	0.0000	13.3000	0.0001995	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	MagVolSus
4	Be	Beryllium	2	2	9.01219	112	4.87672	1560	2743	1.57	0	2	4	21006.6	1848	25	190	1820	2.8	null	Diamagnetic	-0.00002328000
76	Os	Osmium	6	8	190.32953	185	8.41794	3306	5285	2.2	106.1	8	2	1600	22610	12	88	130	0.0015	null	Paramagnetic	0.00001400000
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	-0.00003440000