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 11:46:46 (NZT):

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

23 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
150962	none	48919	Mg	25	f	12	f	Si	29	f	14	f	He	4	b	2	b	Cr	50	b	24	b	12.740000
160246	none	48934	Mg	26	b	12	b	Si	30	b	14	b	He	4	b	2	b	Cr	52	b	24	b	12.328300
160230	none	48915	Mg	26	b	12	b	Si	28	b	14	b	He	4	b	2	b	Cr	50	b	24	b	10.119800
160243	none	48933	Mg	26	b	12	b	Si	30	b	14	b	H	1	f	1	b	Mn	55	f	25	b	9.755500
141647	none	48927	Mg	24	b	12	b	Si	30	b	14	b	He	4	b	2	b	Cr	50	b	24	b	9.456500
150964	none	48921	Mg	25	f	12	f	Si	29	f	14	f	O	16	b	8	b	Ar	38	b	18	b	4.369600
150963	none	48920	Mg	25	f	12	f	Si	29	f	14	f	C	12	b	6	b	Ca	42	b	20	b	3.449300
150966	none	48923	Mg	25	f	12	f	Si	29	f	14	f	Mg	24	b	12	b	Si	30	b	14	b	3.283500
150971	none	48930	Mg	25	f	12	f	Si	30	b	14	b	He	3	f	2	f	Cr	52	b	24	b	2.847600
150967	none	48924	Mg	25	f	12	f	Si	29	f	14	f	Mg	26	b	12	b	Si	28	b	14	b	2.620300
160237	none	48925	Mg	26	b	12	b	Si	29	f	14	f	He	3	f	2	f	Cr	52	b	24	b	2.364100
150965	none	48922	Mg	25	f	12	f	Si	29	f	14	f	Ne	20	b	10	b	S	34	b	16	b	1.885300
160232	none	48917	Mg	26	b	12	b	Si	28	b	14	b	O	16	b	8	b	Ar	38	b	18	b	1.749300
150957	none	48914	Mg	25	f	12	f	Si	28	b	14	b	Mg	24	b	12	b	Si	29	f	14	f	1.146700
141649	none	48929	Mg	24	b	12	b	Si	30	b	14	b	O	16	b	8	b	Ar	38	b	18	b	1.086100
160231	none	48916	Mg	26	b	12	b	Si	28	b	14	b	C	12	b	6	b	Ca	42	b	20	b	0.829000
160247	none	48935	Mg	26	b	12	b	Si	30	b	14	b	C	12	b	6	b	Ca	44	b	20	b	0.802900
150973	none	48931	Mg	25	f	12	f	Si	30	b	14	b	C	12	b	6	b	Ca	43	f	20	f	0.764800
160233	none	48918	Mg	26	b	12	b	Si	28	b	14	b	Mg	24	b	12	b	Si	30	b	14	b	0.663200
150954	none	48913	Mg	25	f	12	f	Si	28	b	14	b	He	3	f	2	f	Cr	50	b	24	b	0.639000
150976	none	48932	Mg	25	f	12	f	Si	30	b	14	b	Mg	26	b	12	b	Si	29	f	14	f	0.483400
160239	none	48926	Mg	26	b	12	b	Si	29	f	14	f	C	12	b	6	b	Ca	43	f	20	f	0.281300
141648	none	48928	Mg	24	b	12	b	Si	30	b	14	b	C	12	b	6	b	Ca	42	b	20	b	0.165800

All Nuclides Appearing in Results Table (20):

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
6	3	2	f	f	He	3.0160300	3.0941	SPN	50.0000	null	0.0000	0.0001	null	35
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
22	20	10	b	b	Ne	19.9924420	8.4234	SPN	50.0000	null	0.0000	90.9200	null	1548
26	24	12	b	b	Mg	23.9850450	8.6518	SPN	50.0000	null	0.0000	78.7000	18337.1	513
27	25	12	f	f	Mg	24.9858400	8.5990	SPN	50.0000	null	0.0000	10.1300	2360.29	69
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
40	38	18	b	b	Ar	37.9627250	8.9851	SPN	50.0000	null	0.0000	0.0630	null	null
46	42	20	b	b	Ca	41.9586280	8.9890	SPN	50.0000	null	0.0000	0.6400	265.6	null
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
59	50	24	b	b	Cr	49.9460510	9.0764	SPN	50.0000	null	0.0000	4.3100	4.3962	null
60	52	24	b	b	Cr	51.9405140	9.1370	SPN	50.0000	null	0.0000	83.7600	85.4352	null
63	55	25	f	b	Mn	54.9380540	9.1205	SPN	50.0000	null	0.0000	100.0000	950	null