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-Apr-2022 20:54:36 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('B') and E2 in ('W') order by MeV desc limit 100"

3 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
2214	left	1030	B	10	b	5	f	W	186	b	74	b	Pt	196	b	78	b	2.140575
2215	right	528	B	10	b	5	f	W	186	b	74	b	Hg	196	b	80	b	1.357185
2213	left	1029	B	10	b	5	f	W	184	b	74	b	Pt	194	b	78	b	1.042344

All Nuclides Appearing in Results Table: (6)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
13	10	5	b	f	B	10.01293686200	64.74858891927	6.47485889193	SPN	50.0000	null	0.0000	19.6000	1.96	null	3+	1.8004636000	0.0845000000	22.0000	42.975	2.87467955
276	184	74	b	b	W	183.95093326000	1472.89271887610	8.00485173302	SPN	50.0000	null	0.0000	30.6400	0.383	null	null	null	null	null	null	null
277	186	74	b	b	W	185.95436521500	1485.83804616380	7.98837659228	SPN	50.0000	null	0.0000	28.4100	0.355125	null	null	null	null	null	null	null
292	194	78	b	b	Pt	193.96268352700	1539.52894772410	7.93571622538	SPN	50.0000	null	0.0000	32.9000	0.001645	null	null	null	null	null	null	null
294	196	78	b	b	Pt	195.96495467500	1553.55556015470	7.92630387834	SPN	50.0000	null	0.0000	25.3000	0.001265	null	null	null	null	null	null	null
297	196	80	b	b	Hg	195.96583344400	1551.17232499070	7.91414451526	SPN	50.0000	null	0.0000	0.1460	0.0001241	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
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
74	W	Tungsten	6	6	183.84152	193	9.55021	3695	5828	2.36	78.6	6	2	1700	19250	20	170	132	1.25	null	Paramagnetic	null	0.00008840000
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
80	Hg	Mercury	6	12	200.60902	171	14.82260	234.32	629.88	2	0	4	3	3300	13534	1	8.3	139.5	0.085	null	Diamagnetic	null	-0.00002840000