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 00:57:38 (NZT):

Full SQL Query: "select * from FusionAllNewPlus where E = 'Th' and A = 232 limit 1000"

2 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
434	left	n*	1	f	0	f	Pa	231	f	91	b	1760.58666595	Th	232	b	90	b	1766.63537252	6.048707
1195	left	D	2	b	1	f	Th	230	b	90	b	1758.08383806	Th	232	b	90	b	1766.63537252	8.551534

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
3	1	0	f	f	n*	1.00866491582	0.00000000000	0.00000000000	UPN	-4.6070	null	0.0000	100.0000	null	null	1/2+	-1.9130427000	null	null	null	-18.32471830
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
312	230	90	b	b	Th	230.03313235800	1755.07739054050	7.63077126322	UPN	4.8773	A	4.4384	null	null	null	null	null	null	null	null	null
313	232	90	b	b	Th	232.03805368900	1766.63537252370	7.61480764019	UPN	10.1480	A or SF	4.0830	100.0000	9.6	null	null	null	null	null	null	null
314	231	91	f	b	Pa	231.03588257500	1759.80433254050	7.61820057377	UPN	4.5153	A	4.5990	100.0000	null	null	3/2-	1.9900000000	-1.7200000000	null	null	6.42000000

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
90	Th	Thorium	7	4	232.03877	null	19.79173	2023	5093	1.3	null	4	4	2780	11724	6.7	54	118	9.6	null	Paramagnetic	null	0.00008400000
91	Pa	Protactinium	7	5	231.03588	null	15.03160	1845	4273	1.5	null	5	1	568	15370	5.6	47	99.1	null	null	Paramagnetic	null	0.00049950000