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 17-Dec-2021 00:25:25 (NZT):

Full SQL Query: "select * from FusionAll where a1 in (12) and a2 in (40 ) 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
2431	left	1059	C	12	b	6	b	K	40	b	19	f	Cr	52	b	24	b	21.884524
2430	none	37	C	12	b	6	b	Ar	40	b	18	b	Cr	52	b	24	b	20.371800

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
15	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032	null	null	null	null	null	null
45	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
47	40	19	b	f	K	39.96399816600	341.51464804390	8.53786620110	UPN	9.0969	B- or K or B+	1.5050	0.0118	2.4662	null	4-	-1.2979700000	-0.0730000000	null	null	-1.55428600
65	52	24	b	b	Cr	51.94050499200	456.33978299176	8.77576505753	SPN	50.0000	null	0.0000	83.7600	85.4352	null	null	null	null	null	null	null

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
6	C	Carbon	2	14	12.01114	67	5.31466	3823	4300	2.55	153.9	4	6	47277	2260	0.1	140	710	200	4600	Diamagnetic	null	-0.00001400000
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
19	K	Potassium	4	1	39.09811	243	45.67536	336.53	1032	0.82	48.4	1	19	476063	856	14	100	757	20900	null	Paramagnetic	null	0.00000574000
24	Cr	Chromium	4	6	51.99763	166	7.28258	2180	2944	1.66	64.3	6	24	761733	7140	7.9	94	448	102	null	Antiferromagnetic	null	0.00031770000