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 09-Apr-2020 21:11:05 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and E1 in ('N') and E2 in ('Al') order by MeV desc limit 100"

16 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
75429	none	20869	N	15	f	7	b	Al	27	f	13	b	He	4	b	2	b	Ar	38	b	18	b	15.197300
65927	none	20858	N	14	b	7	f	Al	27	f	13	b	H	1	f	1	b	K	40	b	19	f	12.057300
75424	none	20867	N	15	f	7	b	Al	27	f	13	b	H	1	f	1	b	K	41	f	19	b	11.162100
65936	none	20863	N	14	b	7	f	Al	27	f	13	b	C	12	b	6	b	Si	29	f	14	f	7.718400
75430	none	20870	N	15	f	7	b	Al	27	f	13	b	C	12	b	6	b	Si	30	b	14	b	7.342000
65929	none	20859	N	14	b	7	f	Al	27	f	13	b	D	2	b	1	f	K	39	f	19	b	6.484100
65930	none	20860	N	14	b	7	f	Al	27	f	13	b	He	3	f	2	f	Ar	38	b	18	b	5.609500
65937	none	20864	N	14	b	7	f	Al	27	f	13	b	C	13	f	6	f	Si	28	b	14	b	4.188000
75433	none	20872	N	15	f	7	b	Al	27	f	13	b	O	16	b	8	b	Mg	26	b	12	b	3.853600
65939	none	20865	N	14	b	7	f	Al	27	f	13	b	O	16	b	8	b	Mg	25	f	12	f	3.746500
75426	none	20868	N	15	f	7	b	Al	27	f	13	b	D	2	b	1	f	K	40	b	19	f	3.291000
1212432	none	518563	N	15	f	7	b	Al	27	f	13	b	T	3	f	1	b	K	39	f	19	b	1.750950
75431	none	20871	N	15	f	7	b	Al	27	f	13	b	C	13	f	6	f	Si	29	f	14	f	1.674800
65932	none	20861	N	14	b	7	f	Al	27	f	13	b	Li	6	b	3	f	Cl	35	f	17	b	0.741500
65940	none	20866	N	14	b	7	f	Al	27	f	13	b	O	17	f	8	f	Mg	24	b	12	b	0.557000
65934	none	20862	N	14	b	7	f	Al	27	f	13	b	Be	9	f	4	f	S	32	b	16	b	0.481600

All Nuclides Appearing in Results Table (26):

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
4	2	1	b	f	D	2.0141020	1.5034	SPN	50.0000	null	0.0000	0.0150	0.21	23
5	3	1	f	b	T	3.0160492	8.4810	SYN	1.0906	b-	0.0186	0.0000	0	null
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
8	6	3	b	f	Li	6.0151260	5.7231	SPN	50.0000	null	0.0000	7.4200	1.484	null
10	9	4	f	f	Be	9.0121860	6.8101	SPN	50.0000	null	0.0000	100.0000	2.8	null
13	12	6	b	b	C	12.0000000	8.0714	SPN	50.0000	null	0.0000	98.8900	197.78	3032
14	13	6	f	f	C	13.0033540	7.8311	SPN	50.0000	null	0.0000	1.1100	2.22	37
16	14	7	b	f	N	14.0032420	7.8557	SPN	50.0000	null	0.0000	99.6300	18.9297	1105
17	15	7	f	b	N	15.0001080	8.0647	SPN	50.0000	null	0.0000	0.3700	0.0703	null
18	16	8	b	b	O	15.9949150	8.3674	SPN	50.0000	null	0.0000	99.7590	459888.99	9592
19	17	8	f	f	O	16.9991340	8.1188	SPN	50.0000	null	0.0000	0.0370	170.57	null
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
29	27	13	f	b	Al	26.9815350	8.7084	SPN	50.0000	null	0.0000	100.0000	82300	58
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
34	32	16	b	b	S	31.9720740	8.8843	SPN	50.0000	null	0.0000	95.0000	332.5	396
37	35	17	f	b	Cl	34.9688550	8.9003	SPN	50.0000	null	0.0000	75.5300	109.5185	null
40	38	18	b	b	Ar	37.9627250	8.9851	SPN	50.0000	null	0.0000	0.0630	null	null
42	39	19	f	b	K	38.9637140	8.9381	SPN	50.0000	null	0.0000	93.1000	19457.9	null
43	40	19	b	f	K	39.9640080	8.9095	UPN	9.0969	b- or K or b+	1.5050	0.0118	2.4662	null
44	41	19	f	b	K	40.9618350	8.9385	SPN	50.0000	null	0.0000	6.8800	1437.92	null