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 20-Jan-2022 04:17:52 (NZT):

Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E1 in ('H', 'B', 'C', 'O') and E2 in ('Nb') ) 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
2332	none	744	B	11	f	5	b	Nb	93	f	41	b	Pd	104	b	46	b	10.959000
114	none	740	H	1	f	1	b	Nb	93	f	41	b	Mo	94	b	42	b	8.481300

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
4	1	1	f	b	H	1.00782503224	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700	1/2+	2.7928473510	null	5700.0000	400.000	26.75222080
14	11	5	f	b	B	11.00930516600	76.20258012611	6.92750728419	SPN	50.0000	null	0.0000	80.4000	8.04	null	3/2-	2.6883780000	0.0405900000	754.0000	128.286	8.58470700
128	93	41	f	b	Nb	92.90637316100	805.74828761906	8.66396008193	SPN	50.0000	null	0.0000	100.0000	20	null	9/2+	6.1630000000	-0.3200000000	2740.0000	97.904	6.56740000
130	94	42	b	b	Mo	93.90508359200	814.23826738693	8.66210922752	SPN	50.0000	null	0.0000	9.0600	0.10872	null	null	null	null	null	null	null
148	104	46	b	b	Pd	103.90403040100	892.80084481188	8.58462350781	SPN	50.0000	null	0.0000	10.9700	0.0016455	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (5)

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
5	B	Boron	2	13	10.81402	87	4.39594	2348	4273	2.04	26.7	3	5	32826.7	2460	0	27	1030	10	null	Diamagnetic	null	-0.00002140000
41	Nb	Niobium	5	5	92.90602	198	10.84084	2750	5017	1.6	86.1	5	7	12100	8570	6.7	54	265	20	null	Paramagnetic	null	0.00023700000
42	Mo	Molybdenum	5	6	95.21689	190	9.26234	2896	4912	2.16	71.9	6	30	154500	10280	20	139	251	1.2	null	Paramagnetic	null	0.00012030000
46	Pd	Palladium	5	10	106.44101	169	8.85312	1828	3236	2.2	53.7	4	3	3177	12023	10	72	240	0.015	null	Paramagnetic	null	0.00078990000