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 12-May-2021 13:21:47 (NZT):

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

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
589437	none	235896	Cu	63	f	29	b	Cu	65	f	29	b	Ni	62	b	28	b	Zn	66	b	30	b	2.783300
599596	none	235899	Cu	65	f	29	b	Cu	65	f	29	b	Ni	62	b	28	b	Zn	68	b	30	b	2.200200
589432	none	235891	Cu	63	f	29	b	Cu	63	f	29	b	Ni	60	b	28	b	Zn	66	b	30	b	2.197400
589436	none	235895	Cu	63	f	29	b	Cu	65	f	29	b	Ni	60	b	28	b	Zn	68	b	30	b	1.614300
589434	none	235892	Cu	63	f	29	b	Cu	63	f	29	b	Ni	62	b	28	b	Zn	64	b	30	b	1.583500
599597	none	235900	Cu	65	f	29	b	Cu	65	f	29	b	Ni	64	b	28	b	Zn	66	b	30	b	1.457800
589435	none	235894	Cu	63	f	29	b	Cu	65	f	29	b	Fe	56	b	26	b	Ge	72	b	32	b	0.341900
589433	left	110182	Cu	63	f	29	b	Cu	63	f	29	b	Ni	61	f	28	f	Cu	65	f	29	b	0.330682
589438	none	235897	Cu	63	f	29	b	Cu	65	f	29	b	Ni	64	b	28	b	Zn	64	b	30	b	0.258000
599595	none	235898	Cu	65	f	29	b	Cu	65	f	29	b	Fe	58	b	26	b	Ge	72	b	32	b	0.203100

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
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
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
79	60	28	b	b	Ni	59.93078525600	526.83302405250	8.78055040087	SPN	50.0000	null	0.0000	26.2300	22.0332	null	null	null	null	null	null	null
80	61	28	f	f	Ni	60.93105494500	534.65289723880	8.76480159408	SPN	50.0000	null	0.0000	1.1900	0.9996	null	3/2-	-0.7496500000	0.1620000000	null	null	-2.39477000
81	62	28	b	b	Ni	61.92834487100	545.24840277495	8.79432907702	SPN	50.0000	null	0.0000	3.6600	3.0744	null	null	null	null	null	null	null
82	64	28	b	b	Ni	63.92796634100	561.74317524830	8.77723711325	SPN	50.0000	null	0.0000	1.0800	0.9072	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
85	64	30	b	b	Zn	63.92914177200	559.08360111230	8.73568126738	SPN	50.0000	null	0.0000	48.8900	34.223	null	null	null	null	null	null	null
86	66	30	b	b	Zn	65.92603370400	578.12092276587	8.75940792070	SPN	50.0000	null	0.0000	27.8100	19.467	null	null	null	null	null	null	null
88	68	30	b	b	Zn	67.92484429100	595.37102815890	8.75545629645	SPN	50.0000	null	0.0000	18.5700	12.999	null	null	null	null	null	null	null
93	72	32	b	b	Ge	71.92207582600	628.66951864558	8.73152109230	SPN	50.0000	null	0.0000	27.4300	0.41145	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (5)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	MagVolSus
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	null
28	Ni	Nickel	4	10	58.72843	149	6.59277	1728	3186	1.91	112	4	28	1039668	8908	14	91	445	84	null	Ferromagnetic	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	-0.00000963000
30	Zn	Zinc	4	12	65.38688	142	9.15783	692.68	1180	1.65	0	2	21	179100	7140	17	120	388	70	null	Diamagnetic	-0.00001580000
32	Ge	Germanium	4	14	72.56952	125	13.63320	1211.4	3093	2.01	119	4	5	9020	5323	0.002	60	321.4	1.5	null	Diamagnetic	-0.00000798000