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 originally created from Dr Parkhomov's spreadsheets.

To make full use of this and the other database tables, a good grasp of SQL is essential.

But note that it and Fission and Fusion is each dedicated to querying only one of two tables.

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.

You may indicate which of the three neutrino conditions to include: "left" and/or "none" and/or "right". The default condition is include all three.

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 ('b') if its A number is even; if odd a Fermion ('f'). The atom itself is considered a Boson ('b') if its number of neutrons (A - Z) is even; if odd a Fermion ('f').

These parameters can be used either passively, by observing the distributions of 'b' and 'f' in inputs and/or outputs, and/or actively, by selecting 'b only', 'f only' or 'either' in the boxes below.

NB: To avoid unnecessary duplication in all TwoToTwo tables, two rules independently apply: A1 <= A2 and A3 <= A4. These rules also apply implicitly in that, if the input side of the Core Query only involves E1 and E2, only rows whose associated mass numbers obey A1 <= A2 will appear in the results. Similarly with E3 and E4 on the output side, only rows whose associated mass numbers obey A3 <= A4 will appear in the results.

Input used for this run on 16-Dec-2021 23:26:10 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ( 'Al') and E2 in ('Cu', 'S') and E4 = 'Fe' order by MeV desc limit 1000"

10 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
166768	left	25259	Al	27	f	13	b	S	33	f	16	f	He	4	b	2	b	Fe	56	b	26	b	14.401832
166780	left	25266	Al	27	f	13	b	S	34	b	16	b	He	4	b	2	b	Fe	57	f	26	f	10.621829
167309	none	60013	Al	27	f	13	b	Cu	63	f	29	b	S	34	b	16	b	Fe	56	b	26	b	7.762100
167332	none	60039	Al	27	f	13	b	Cu	65	f	29	b	S	34	b	16	b	Fe	58	b	26	b	7.623300
167307	none	60011	Al	27	f	13	b	Cu	63	f	29	b	S	32	b	16	b	Fe	58	b	26	b	5.387800
167333	right	46726	Al	27	f	13	b	Cu	65	f	29	b	Cl	35	f	17	b	Fe	57	f	26	f	4.724532
167308	none	60012	Al	27	f	13	b	Cu	63	f	29	b	S	33	f	16	f	Fe	57	f	26	f	3.982100
166761	left	25257	Al	27	f	13	b	S	32	b	16	b	He	3	f	2	f	Fe	56	b	26	b	2.465667
166767	left	25265	Al	27	f	13	b	S	33	f	16	f	He	3	f	2	f	Fe	57	f	26	f	1.464311
166779	left	25270	Al	27	f	13	b	S	34	b	16	b	He	3	f	2	f	Fe	58	b	26	b	0.091288

All Nuclides Appearing in Results Table: (12)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
7	3	2	f	f	He	3.01602932265	7.71737084564	2.57245694855	SPN	50.0000	null	0.0000	0.0001	null	35	1/2+	-2.1276253100	null	null	null	-20.37894730
8	4	2	b	b	He	4.00260325413	28.29476455561	7.07369113890	SPN	50.0000	null	0.0000	99.9999	null	275200	null	null	null	null	null	null
32	27	13	f	b	Al	26.98153840800	224.94588197047	8.33132896187	SPN	50.0000	null	0.0000	100.0000	82300	58	5/2+	3.6407000000	0.1466000000	1170.0000	104.227	6.97627800
37	32	16	b	b	S	31.97207117443	271.77299097355	8.49290596792	SPN	50.0000	null	0.0000	95.0000	332.5	396	null	null	null	null	null	null
38	33	16	f	f	S	32.97145890985	280.41439892209	8.49740602794	SPN	50.0000	null	0.0000	0.7600	2.66	null	3/2+	0.6432500000	-0.0678000000	null	null	2.05568500
39	34	16	b	b	S	33.96786701200	291.83131837772	8.58327406993	SPN	50.0000	null	0.0000	4.2200	14.77	null	null	null	null	null	null	null
40	35	17	f	b	Cl	34.96885269400	298.20191473166	8.52005470662	SPN	50.0000	null	0.0000	75.5300	109.5185	null	3/2+	0.8217000000	-0.8170000000	null	null	2.62419910
71	56	26	b	b	Fe	55.93493561700	492.24730527224	8.79013045129	SPN	50.0000	null	0.0000	91.6600	51604.58	1169	null	null	null	null	null	null
72	57	26	f	f	Fe	56.93539213400	499.89314923521	8.77005524974	SPN	50.0000	null	0.0000	2.1900	1232.97	28	1/2-	0.0906400000	null	null	null	0.86806270
73	58	26	b	b	Fe	57.93327373800	509.93751006707	8.79202603564	SPN	50.0000	null	0.0000	0.3300	185.79	null	null	null	null	null	null	null
83	63	29	f	b	Cu	62.92959723600	551.37058542554	8.75191405437	SPN	50.0000	null	0.0000	69.0900	41.454	null	3/2-	2.2259000000	-0.2200000000	365.0000	106.112	7.11179100
84	65	29	f	b	Cu	64.92778948700	569.19666729878	8.75687180460	SPN	50.0000	null	0.0000	30.9100	18.546	null	3/2-	2.3844000000	-0.2040000000	201.0000	113.669	7.60430000

All Elements Appearing in Results Table: (6)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
2	He	Helium	1	18	4.00260	31	22423.54062	0	4.22	null	0	0	2	5250.5	0.1785	null	0.1513	5193.1	null	240000	Diamagnetic	null	-0.00000000105
13	Al	Aluminium	3	13	26.98154	118	9.99316	933.47	2792	1.61	42.5	3	13	222316	2700	38	235	904	82300	null	Paramagnetic	null	0.00002110000
16	S	Sulfur	3	16	32.05750	88	16.35587	388.36	717.87	2.58	200	6	16	337138	1960	0	0.205	705	350	440	Diamagnetic	null	-0.00001220000
17	Cl	Chlorine	3	17	35.45753	79	11032.21248	171.6	239.11	3.16	349	7	17	380760	3.214	0	0.0089	478.2	145	null	Diamagnetic	null	-0.00000002310
26	Fe	Iron	4	8	55.84731	156	7.09262	1811	3134	1.83	15.7	6	26	895161	7874	10	80	449	56300	1090	Ferromagnetic	1043	null
29	Cu	Copper	4	11	63.54724	145	7.12413	1357.77	3200	1.9	118.4	4	29	1116105	8920	59	400	384.4	60	null	Diamagnetic	null	-0.00000963000