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 11-Sep-2020 05:53:48 (NZT):

Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E1 in ('He') and E2 in ('Ti' ) ) and nBorF1 = 'b' order by MeV desc limit 100"

4 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
947	none	1192	He	4	b	2	b	Ti	48	b	22	b	Cr	52	b	24	b	9.349400
948	none	1194	He	4	b	2	b	Ti	49	f	22	f	Cr	53	f	24	f	9.146300
945	none	1190	He	4	b	2	b	Ti	46	b	22	b	Cr	50	b	24	b	8.555800
949	none	1196	He	4	b	2	b	Ti	50	b	22	b	Cr	54	b	24	b	7.930700

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz
7	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
52	46	22	b	b	Ti	45.95262772000	398.18567560272	8.65621033919	SPN	50.0000	null	0.0000	7.9300	444.08	null	null	null	null	null	null
54	48	22	b	b	Ti	47.94794198000	418.69258978450	8.72276228718	SPN	50.0000	null	0.0000	73.9400	4140.64	null	null	null	null	null	null
55	49	22	f	f	Ti	48.94786568000	426.83474976378	8.71091326049	SPN	50.0000	null	0.0000	5.5100	308.56	null	7/2-	-1.1037000000	0.2470000000	null	null
56	50	22	b	b	Ti	49.94478689000	437.77371216463	8.75547424329	SPN	50.0000	null	0.0000	5.3400	299.04	null	null	null	null	null	null
59	50	24	b	b	Cr	49.94604183000	435.04007584568	8.70080151691	SPN	50.0000	null	0.0000	4.3100	4.3962	null	null	null	null	null	null
60	52	24	b	b	Cr	51.94050623000	456.33862980178	8.77574288080	SPN	50.0000	null	0.0000	83.7600	85.4352	null	null	null	null	null	null
61	53	24	f	f	Cr	52.94064815000	464.27751908759	8.75995319033	SPN	50.0000	null	0.0000	9.5500	9.741	null	3/2-	-0.4743100000	-0.1500000000	null	null
62	54	24	b	b	Cr	53.93887916000	473.99641021034	8.77771130019	SPN	50.0000	null	0.0000	2.3800	2.4276	null	null	null	null	null	null