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 15-Sep-2020 02:07:16 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('He') and E2 in ('K' ) order by MeV desc"

6 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
682	left	299	He	3	f	2	f	K	41	f	19	b	Ca	44	b	20	b	20.842182
681	left	297	He	3	f	2	f	K	40	b	19	f	Ca	43	f	20	f	19.801704
680	left	295	He	3	f	2	f	K	39	f	19	b	Ca	42	b	20	b	19.669431
936	left	298	He	4	b	2	b	K	40	b	19	f	Ca	44	b	20	b	10.359148
937	none	536	He	4	b	2	b	K	41	f	19	b	Sc	45	f	21	b	7.935400
935	left	296	He	4	b	2	b	K	39	f	19	b	Ca	43	f	20	f	7.020673

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
6	3	2	f	f	He	3.01602932010	7.71737322095	2.57245774032	SPN	50.0000	null	0.0000	0.0001	null	35	1/2+	-2.1276253100	null	null	null
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
42	39	19	f	b	K	38.96370648640	333.71525897689	8.55680151223	SPN	50.0000	null	0.0000	93.1000	19457.9	null	3/2+	0.3914700000	0.0585000000	null	null
43	40	19	b	f	K	39.96399816600	341.51464804390	8.53786620110	UPN	9.0969	b- or K or b+	1.5050	0.0118	2.4662	null	4-	-1.2979700000	-0.0730000000	null	null
44	41	19	f	b	K	40.96182525790	351.60978658803	8.57584845337	SPN	50.0000	null	0.0000	6.8800	1437.92	null	3/2+	0.2148720000	0.0711000000	null	null
46	42	20	b	b	Ca	41.95861783000	361.88624105380	8.61633907271	SPN	50.0000	null	0.0000	0.6400	265.6	null	null	null	null	null	null
47	43	20	f	f	Ca	42.95876644000	369.81889864253	8.60043950331	SPN	50.0000	null	0.0000	0.1450	60.175	null	7/2-	-1.3173300000	-0.0408000000	null	null
48	44	20	b	b	Ca	43.95548156000	380.94983271058	8.65795074342	SPN	50.0000	null	0.0000	2.0600	854.9	null	null	null	null	null	null
51	45	21	f	b	Sc	44.95590828000	387.84109900019	8.61869108889	SPN	50.0000	null	0.0000	100.0000	22	null	7/2-	4.7540000000	-0.2200000000	1710.0000	97.167