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 18-Feb-2020 03:19:38 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H') and E2 in ('Ni', 'Fe' ) 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
43	left	43	H	1	f	1	b	Ni	61	f	28	f	He	4	b	2	b	Fe	58	b	26	b	2.793553
46	right	1081	H	1	f	1	b	Ni	64	b	28	b	He	4	b	2	b	Ni	61	f	28	f	1.985939
37	left	35	H	1	f	1	b	Fe	57	f	26	f	He	4	b	2	b	Cr	54	b	24	b	1.618007
38	right	1076	H	1	f	1	b	Fe	57	f	26	f	He	4	b	2	b	Fe	54	b	26	b	0.926831
44	right	1079	H	1	f	1	b	Ni	61	f	28	f	He	4	b	2	b	Ni	58	b	28	b	0.865352
42	left	40	H	1	f	1	b	Ni	60	b	28	b	He	4	b	2	b	Fe	57	f	26	f	0.569145
39	none	83	H	1	f	1	b	Fe	58	b	26	b	He	4	b	2	b	Mn	55	f	25	b	0.409900
45	none	90	H	1	f	1	b	Ni	62	b	28	b	He	4	b	2	b	Co	59	f	27	b	0.351200

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
7	4	2	b	b	He	4.0026030	7.4652	SPN	50.0000	null	0.0000	99.9999	null	275200
62	54	24	b	b	Cr	53.9388790	9.1257	SPN	50.0000	null	0.0000	2.3800	2.4276	null
63	55	25	f	b	Mn	54.9380540	9.1205	SPN	50.0000	null	0.0000	100.0000	950	null
64	54	26	b	b	Fe	53.9396210	9.1129	SPN	50.0000	null	0.0000	5.8200	3276.66	72
66	57	26	f	f	Fe	56.9353940	9.1272	SPN	50.0000	null	0.0000	2.1900	1232.97	28
67	58	26	b	b	Fe	57.9332720	9.1431	SPN	50.0000	null	0.0000	0.3300	185.79	null
68	59	27	f	b	Co	58.9331900	9.1262	SPN	50.0000	null	0.0000	100.0000	25	null
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