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 06-Mar-2020 11:38:19 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and E1 in ('Si') and E2 in ('Si' ) order by MeV desc"

7 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
186367	none	63027	Si	29	f	14	f	Si	29	f	14	f	He	4	b	2	b	Fe	54	b	26	b	10.021000
196207	none	63033	Si	30	b	14	b	Si	30	b	14	b	He	4	b	2	b	Fe	56	b	26	b	9.302800
176274	none	63031	Si	28	b	14	b	Si	30	b	14	b	He	4	b	2	b	Fe	54	b	26	b	7.884200
196205	none	63032	Si	30	b	14	b	Si	30	b	14	b	H	1	f	1	b	Co	59	f	27	b	6.061200
186370	none	63030	Si	29	f	14	f	Si	29	f	14	f	Si	28	b	14	b	Si	30	b	14	b	2.136800
186368	none	63028	Si	29	f	14	f	Si	29	f	14	f	C	12	b	6	b	Ti	46	b	22	b	0.325100
186369	none	63029	Si	29	f	14	f	Si	29	f	14	f	Mg	24	b	12	b	S	34	b	16	b	0.067100

All Nuclides Appearing in Results Table (12):

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
26	24	12	b	b	Mg	23.9850450	8.6518	SPN	50.0000	null	0.0000	78.7000	18337.1	513
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
52	46	22	b	b	Ti	45.9526330	9.0306	SPN	50.0000	null	0.0000	7.9300	444.08	null
64	54	26	b	b	Fe	53.9396210	9.1129	SPN	50.0000	null	0.0000	5.8200	3276.66	72
65	56	26	b	b	Fe	55.9349320	9.1537	SPN	50.0000	null	0.0000	91.6600	51604.58	1169
68	59	27	f	b	Co	58.9331900	9.1262	SPN	50.0000	null	0.0000	100.0000	25	null