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 14-Apr-2022 21:21:03 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('D') and E2 in ('Ir' ) 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
620	none	528	D	2	b	1	f	Ir	193	f	77	b	Pt	195	f	78	f	11.701400
619	left	250	D	2	b	1	f	Ir	191	f	77	b	Ir	193	f	77	b	10.872401

All Nuclides Appearing in Results Table: (4)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
5	2	1	b	f	D	2.01410177811	2.22411411070	1.11205705535	SPN	50.0000	null	0.0000	0.0150	0.21	23	1+	0.8574382310	0.0028600000	0.0082	61.403	4.10662920
288	191	77	f	b	Ir	190.96059152700	1518.04670639500	7.94788851516	SPN	50.0000	null	0.0000	37.3000	0.000373	null	3/2+	0.1502000000	0.8160000000	null	null	0.48120000
289	193	77	f	b	Ir	192.96292382400	1532.01635887860	7.93790859523	SPN	50.0000	null	0.0000	62.7000	0.000627	null	3/2+	0.1630000000	0.7510000000	null	null	0.52270000
293	195	78	f	f	Pt	194.96479435300	1545.63381222760	7.92632724219	SPN	50.0000	null	0.0000	33.8000	0.00169	null	1/2-	0.6073000000	null	19.1000	85.996	5.83850000

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
77	Ir	Iridium	6	9	192.21637	180	8.48637	2739	4701	2.2	151	8	2	1600	22650	21	150	131	0.001	null	Paramagnetic	null	0.00003770000
78	Pt	Platinum	6	10	195.08590	177	9.25016	2041.4	4098	2.28	205.3	6	2	1791	21090	9.4	72	133	0.005	null	Paramagnetic	null	0.00025730000