Two To Two 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 enables SQL commands to query the TwoToTwo (2-2) 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.

It replaces its orginal (and rather misnamed) version "FissionFusion.php".

But note that it and Fission and Fusion is each dedicated to querying only one table ("TwoToTwo", "Fission" and "Fusion" 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 TwoToTwoAll but it uses the new field "neutrino" (setable to "left" and/or "none" and/or "right") to effectively select "TwoToTwoEoL" and/or "TwoToTwo" and/or "TwoToTwoEoR".

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 19-Feb-2020 01:20:27 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H') and E2 in ('W' ) and E3 in ('Ca') and E4 in ('Ba') order by MeV desc limit 100"

8 rows were found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E3	A3	nBorF3	Z3	aBorF3	E4	A4	nBorF4	Z4	aBorF4	MeV
3686	right	61609	H	1	f	1	b	W	183	f	74	f	Ca	48	b	20	b	Ba	136	b	56	b	94.446044
3704	right	61612	H	1	f	1	b	W	184	b	74	b	Ca	48	b	20	b	Ba	137	f	56	f	93.980297
3684	right	61611	H	1	f	1	b	W	183	f	74	f	Ca	46	b	20	b	Ba	138	b	56	b	92.605411
3659	right	61605	H	1	f	1	b	W	182	b	74	b	Ca	48	b	20	b	Ba	135	f	56	f	91.437318
3658	right	61607	H	1	f	1	b	W	182	b	74	b	Ca	46	b	20	b	Ba	137	f	56	f	90.211472
3627	right	61599	H	1	f	1	b	W	180	b	74	b	Ca	46	b	20	b	Ba	135	f	56	f	89.000529
3626	right	61601	H	1	f	1	b	W	180	b	74	b	Ca	44	b	20	b	Ba	137	f	56	f	87.332223
3625	right	61602	H	1	f	1	b	W	180	b	74	b	Ca	43	f	20	f	Ba	138	b	56	b	84.779930

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
47	43	20	f	f	Ca	42.9587800	8.9643	SPN	50.0000	null	0.0000	0.1450	60.175	null
48	44	20	b	b	Ca	43.9554900	9.0137	SPN	50.0000	null	0.0000	2.0600	854.9	null
49	46	20	b	b	Ca	45.9536890	9.0092	SPN	50.0000	null	0.0000	0.0033	1.3695	null
50	48	20	b	b	Ca	47.9523630	8.9958	UPN	19.3619	2 b-	4.2740	0.1800	74.7	null
186	135	56	f	f	Ba	134.9055700	8.7229	SPN	50.0000	null	0.0000	6.5900	28.0075	null
187	136	56	b	b	Ba	135.9043600	8.7264	SPN	50.0000	null	0.0000	7.8100	33.1925	null
188	137	56	f	f	Ba	136.9055600	8.7135	SPN	50.0000	null	0.0000	11.3200	48.11	null
189	138	56	b	b	Ba	137.9050100	8.7126	SPN	50.0000	null	0.0000	71.6600	304.555	null
252	180	74	b	b	W	179.9469800	8.3458	UPN	18.2555	a	2.5090	0.1400	0.00175	null
253	182	74	b	b	W	181.9482700	8.3361	SPN	50.0000	null	0.0000	26.4100	0.330125	null
254	183	74	f	f	W	182.9502900	8.3244	SPN	50.0000	null	0.0000	14.4000	0.18	null
255	184	74	b	b	W	183.9509900	8.3195	SPN	50.0000	null	0.0000	30.6400	0.383	null