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 Fission tables created from Dr Parkhomov's two spreadsheets, the latest of which includes the effects of neutrinos

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 table ("FissionAll" "TwoToTwoAll" and "FusionAll" respectively).

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.

New Feature (1): In the checkbox, you may indicate which of the three tables you want effectively included. The resulting query is only on FussionAll but it uses the new field "neutrino" (setable to "left" and/or "none" and/or "right") to effectively select "FusionEoL" and/or "Fussion" and/or "FussionEoR".

New Feature (2): 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 if its A number is even; if odd a Fermion (thus nBorF = 'b' or 'f'). The atom itself is considered a Boson if its number of neutrons (A - Z) is even; if odd a Fermion (thus aBorF = 'b' or 'f').

The above extra parameters can be used either passively by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively by the New Feature (3) of selecting 'b only', 'f only' or 'either' in the boxes below.

Input used for this run on 08-Feb-2020 06:19:46 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('H', 'D') and E2 in ('Ni' ) order by MeV desc limit 100"

10 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
361	left	51	D	2	b	1	f	Ni	58	b	28	b	Ni	60	b	28	b	17.382613
362	left	53	D	2	b	1	f	Ni	60	b	28	b	Ni	62	b	28	b	15.406914
366	right	28	D	2	b	1	f	Ni	64	b	28	b	Zn	66	b	30	b	14.916013
363	none	792	D	2	b	1	f	Ni	61	f	28	f	Cu	63	f	29	b	14.490300
364	left	55	D	2	b	1	f	Ni	62	b	28	b	Ni	64	b	28	b	13.495489
365	right	27	D	2	b	1	f	Ni	62	b	28	b	Zn	64	b	30	b	12.390733
71	left	54	H	1	f	1	b	Ni	61	f	28	f	Ni	62	b	28	b	9.807703
73	none	794	H	1	f	1	b	Ni	64	b	28	b	Cu	65	f	29	b	7.450100
70	left	52	H	1	f	1	b	Ni	60	b	28	b	Ni	61	f	28	f	7.041166
72	none	793	H	1	f	1	b	Ni	62	b	28	b	Cu	63	f	29	b	6.124600

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar
3	1	1	f	b	H	1.0078250	0.7824	SPN	50.0000	null	0.0000	99.9850	1399.79	705700
4	2	1	b	f	D	2.0141020	1.5034	SPN	50.0000	null	0.0000	0.0150	0.21	23
70	58	28	b	b	Ni	57.9353420	9.1098	SPN	50.0000	null	0.0000	67.8800	57.0192	49
71	60	28	b	b	Ni	59.9307830	9.1460	SPN	50.0000	null	0.0000	26.2300	22.0332	null
72	61	28	f	f	Ni	60.9310490	9.1243	SPN	50.0000	null	0.0000	1.1900	0.9996	null
73	62	28	b	b	Ni	61.9283450	9.1479	SPN	50.0000	null	0.0000	3.6600	3.0744	null
74	64	28	b	b	Ni	63.9279590	9.1199	SPN	50.0000	null	0.0000	1.0800	0.9072	null
75	63	29	f	b	Cu	62.9295950	9.1124	SPN	50.0000	null	0.0000	69.0900	41.454	null
76	65	29	f	b	Cu	64.9277860	9.1063	SPN	50.0000	null	0.0000	30.9100	18.546	null
77	64	30	b	b	Zn	63.9291450	9.1027	SPN	50.0000	null	0.0000	48.8900	34.223	null
78	66	30	b	b	Zn	65.9260480	9.1151	SPN	50.0000	null	0.0000	27.8100	19.467	null