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-Apr-2022 03:50:23 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('He') and E2 in ('F' ) order by MeV desc limit 1000"

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
657	left	280	He	3	f	2	f	F	19	f	9	b	Ne	22	b	10	b	21.470941
913	none	375	He	4	b	2	b	F	19	f	9	b	Na	23	f	11	b	10.465300

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
7	3	2	f	f	He	3.01602932265	7.71737084564	2.57245694855	SPN	50.0000	null	0.0000	0.0001	null	35	1/2+	-2.1276253100	null	null	null	-20.37894730
8	4	2	b	b	He	4.00260325413	28.29476455561	7.07369113890	SPN	50.0000	null	0.0000	99.9999	null	275200	null	null	null	null	null	null
23	19	9	f	b	F	18.99840316288	147.79709630986	7.77879454262	SPN	50.0000	null	0.0000	100.0000	585	null	1/2+	2.6283210000	null	4730.0000	376.345	25.16233000
26	22	10	b	b	Ne	21.99138510900	177.76530120658	8.08024096394	SPN	50.0000	null	0.0000	8.8200	null	208	null	null	null	null	null	null
27	23	11	f	b	Na	22.98976928199	186.55918846204	8.11126906357	SPN	50.0000	null	0.0000	100.0000	23600	33	3/2+	2.2175000000	0.1040000000	525.0000	105.808	7.08085160

All Elements Appearing in Results Table: (4)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
2	He	Helium	1	18	4.00260	31	22423.54062	0	4.22	null	0	0	2	5250.5	0.1785	null	0.1513	5193.1	null	240000	Diamagnetic	null	-0.00000000105
9	F	Fluorine	2	17	18.99841	42	11201.88974	53.5	85.03	3.98	328	1	9	106434	1.696	null	0.0277	824	585	null	null	null	null
10	Ne	Neon	2	18	20.17072	38	22411.91400	24.56	27.07	null	0	0	10	131432	0.9	null	0.0491	1030	null	1340	Diamagnetic	null	-0.00000000369
11	Na	Sodium	3	1	22.98977	190	23.74977	370.87	1156	0.93	52.8	1	11	159076	968	21	140	1230	23600	null	Paramagnetic	null	0.00000850000