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 14:57:16 (NZT):

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

14 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
63	right	1091	H	1	f	1	b	Ge	73	f	32	f	He	4	b	2	b	Ge	70	b	32	b	3.916927
62	left	63	H	1	f	1	b	Ge	73	f	32	f	He	4	b	2	b	Zn	70	b	30	b	3.012454
72	right	1093	H	1	f	1	b	Ge	76	b	32	b	He	4	b	2	b	Ge	73	f	32	f	3.001268
65	right	8800	H	1	f	1	b	Ge	73	f	32	f	O	16	b	8	b	Fe	58	b	26	b	2.792613
64	right	4216	H	1	f	1	b	Ge	73	f	32	f	C	12	b	6	b	Ni	62	b	28	b	2.645437
60	left	54	H	1	f	1	b	Ge	70	b	32	b	He	4	b	2	b	Zn	67	f	30	f	2.282163
69	right	28816	H	1	f	1	b	Ge	73	f	32	f	Si	30	b	14	b	Ca	44	b	20	b	1.801504
61	none	120	H	1	f	1	b	Ge	72	b	32	b	He	4	b	2	b	Ga	69	f	31	b	1.510900
71	none	126	H	1	f	1	b	Ge	74	b	32	b	He	4	b	2	b	Ga	71	f	31	b	1.427000
66	right	20989	H	1	f	1	b	Ge	73	f	32	f	Mg	24	b	12	b	Ti	50	b	22	b	1.257511
70	right	37364	H	1	f	1	b	Ge	73	f	32	f	S	34	b	16	b	Ar	40	b	18	b	0.871872
67	right	20987	H	1	f	1	b	Ge	73	f	32	f	Mg	26	b	12	b	Ti	48	b	22	b	0.601739
68	right	28817	H	1	f	1	b	Ge	73	f	32	f	Si	28	b	14	b	Ca	46	b	20	b	0.530014
73	right	28826	H	1	f	1	b	Ge	76	b	32	b	Si	29	f	14	f	Ca	48	b	20	b	0.308323

All Nuclides Appearing in Results Table (27):

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
18	16	8	b	b	O	15.9949150	8.3674	SPN	50.0000	null	0.0000	99.7590	459888.99	9592
26	24	12	b	b	Mg	23.9850450	8.6518	SPN	50.0000	null	0.0000	78.7000	18337.1	513
28	26	12	b	b	Mg	25.9825910	8.6951	SPN	50.0000	null	0.0000	11.1700	2602.61	79
30	28	14	b	b	Si	27.9769270	8.8390	SPN	50.0000	null	0.0000	92.2100	260032.2	653
31	29	14	f	f	Si	28.9764910	8.8265	SPN	50.0000	null	0.0000	4.7000	13254	34
32	30	14	b	b	Si	29.9737610	8.8861	SPN	50.0000	null	0.0000	3.0900	8713.8	23
36	34	16	b	b	S	33.9678650	8.9518	SPN	50.0000	null	0.0000	4.2200	14.77	null
41	40	18	b	b	Ar	39.9623840	8.9474	SPN	50.0000	null	0.0000	99.6000	null	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
54	48	22	b	b	Ti	47.9479480	9.0815	SPN	50.0000	null	0.0000	73.9400	4140.64	null
56	50	22	b	b	Ti	49.9447900	9.0999	SPN	50.0000	null	0.0000	5.3400	299.04	null
67	58	26	b	b	Fe	57.9332720	9.1431	SPN	50.0000	null	0.0000	0.3300	185.79	null
73	62	28	b	b	Ni	61.9283450	9.1479	SPN	50.0000	null	0.0000	3.6600	3.0744	null
79	67	30	f	f	Zn	66.9271490	9.0842	SPN	50.0000	null	0.0000	4.1100	2.877	null
81	70	30	b	b	Zn	69.9253480	9.0648	SPN	50.0000	null	0.0000	0.6200	0.434	null
82	69	31	f	b	Ga	68.9256820	9.0747	SPN	50.0000	null	0.0000	60.4000	11.476	null
83	71	31	f	b	Ga	70.9248400	9.0575	SPN	50.0000	null	0.0000	39.6000	7.524	null
84	70	32	b	b	Ge	69.9243770	9.0777	SPN	50.0000	null	0.0000	20.5200	0.3078	null
85	72	32	b	b	Ge	71.9220820	9.0794	SPN	50.0000	null	0.0000	27.4300	0.41145	null
86	73	32	f	f	Ge	72.9233600	9.0493	SPN	50.0000	null	0.0000	7.7600	0.1164	null
87	74	32	b	b	Ge	73.9211500	9.0639	SPN	50.0000	null	0.0000	36.5400	0.5481	null
88	76	32	b	b	Ge	75.9213600	9.0352	UPN	21.2553	2 b-	2.0390	7.6700	0.11505	null