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 11-Mar-2020 15:01:51 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H') and E2 in ('Zn', 'N' ) 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
5	none	14	H	1	f	1	b	N	15	f	7	b	He	4	b	2	b	C	12	b	6	b	4.964900
52	left	52	H	1	f	1	b	Zn	67	f	30	f	He	4	b	2	b	Ni	64	b	28	b	4.109754
56	right	1087	H	1	f	1	b	Zn	70	b	30	b	He	4	b	2	b	Zn	67	f	30	f	3.186635
50	left	46	H	1	f	1	b	Zn	64	b	30	b	He	4	b	2	b	Ni	61	f	28	f	3.090699
53	right	1085	H	1	f	1	b	Zn	67	f	30	f	He	4	b	2	b	Zn	64	b	30	b	3.004994
55	none	103	H	1	f	1	b	Zn	68	b	30	b	He	4	b	2	b	Cu	65	f	29	b	2.143400
51	none	98	H	1	f	1	b	Zn	66	b	30	b	He	4	b	2	b	Cu	63	f	29	b	1.560300
54	right	4206	H	1	f	1	b	Zn	67	f	30	f	C	12	b	6	b	Fe	56	b	26	b	0.039121

All Nuclides Appearing in Results Table (14):

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
13	12	6	b	b	C	12.0000000	8.0714	SPN	50.0000	null	0.0000	98.8900	197.78	3032
17	15	7	f	b	N	15.0001080	8.0647	SPN	50.0000	null	0.0000	0.3700	0.0703	null
65	56	26	b	b	Fe	55.9349320	9.1537	SPN	50.0000	null	0.0000	91.6600	51604.58	1169
72	61	28	f	f	Ni	60.9310490	9.1243	SPN	50.0000	null	0.0000	1.1900	0.9996	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
79	67	30	f	f	Zn	66.9271490	9.0842	SPN	50.0000	null	0.0000	4.1100	2.877	null
80	68	30	b	b	Zn	67.9248650	9.1006	SPN	50.0000	null	0.0000	18.5700	12.999	null
81	70	30	b	b	Zn	69.9253480	9.0648	SPN	50.0000	null	0.0000	0.6200	0.434	null