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 23-May-2024 00:32:30 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('fe') and E2 in ('fe' ) order by MeV desc limit 100"

9 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
494078	none	194264	Fe	54	b	26	b	Fe	58	b	26	b	Fe	56	b	26	b	Fe	56	b	26	b	2.821500
513089	none	194262	Fe	57	f	26	f	Fe	57	f	26	f	Fe	56	b	26	b	Fe	58	b	26	b	2.407000
494076	left	88526	Fe	54	b	26	b	Fe	57	f	26	f	Mn	55	f	25	b	Fe	56	b	26	b	1.890004
513087	none	194260	Fe	57	f	26	f	Fe	57	f	26	f	Cr	52	b	24	b	Ni	62	b	28	b	1.796900
494077	none	194263	Fe	54	b	26	b	Fe	58	b	26	b	Cr	52	b	24	b	Ni	60	b	28	b	1.486700
494075	left	88527	Fe	54	b	26	b	Fe	57	f	26	f	Cr	52	b	24	b	Co	59	f	27	b	1.221191
513088	none	194261	Fe	57	f	26	f	Fe	57	f	26	f	Cr	54	b	24	b	Ni	60	b	28	b	1.048900
513090	right	119438	Fe	57	f	26	f	Fe	58	b	26	b	Fe	56	b	26	b	Co	59	f	27	b	0.506731
494074	left	88528	Fe	54	b	26	b	Fe	57	f	26	f	V	51	f	23	b	Ni	60	b	28	b	0.236602

All Nuclides Appearing in Results Table: (11)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
63	51	23	f	b	V	50.94395686700	445.83562743748	8.74187504779	SPN	50.0000	null	0.0000	99.7600	119.712	null	7/2-	5.1464000000	-0.0430000000	2160.0000	101.212	7.04551390
65	52	24	b	b	Cr	51.94050499200	456.33978299176	8.77576505753	SPN	50.0000	null	0.0000	83.7600	85.4352	null	null	null	null	null	null	null
67	54	24	b	b	Cr	53.93887801200	473.99747956583	8.77773110307	SPN	50.0000	null	0.0000	2.3800	2.4276	null	null	null	null	null	null	null
69	55	25	f	b	Mn	54.93804317200	482.06388184689	8.76479785176	SPN	50.0000	null	0.0000	100.0000	950	null	5/2-	3.4669000000	0.3300000000	994.0000	98.980	6.64525453
70	54	26	b	b	Fe	53.93960830600	471.75254802301	8.73615829672	SPN	50.0000	null	0.0000	5.8200	3276.66	72	null	null	null	null	null	null
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
75	59	27	f	b	Co	58.93319365600	517.30085954792	8.76781117878	SPN	50.0000	null	0.0000	100.0000	25	null	7/2-	4.6150000000	0.4200000000	1570.0000	94.908	6.33200000
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
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

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
23	V	Vanadium	4	5	50.94159	171	8.33741	2183	3680	1.63	50.6	5	23	699144	6110	5	31	489	120	null	Paramagnetic	null	0.00038370000
24	Cr	Chromium	4	6	51.99763	166	7.28258	2180	2944	1.66	64.3	6	24	761733	7140	7.9	94	448	102	null	Antiferromagnetic	null	0.00031770000
25	Mn	Manganese	4	7	54.93805	161	7.35449	1519	2334	1.55	0	7	25	827067	7470	0.62	7.8	479	950	null	Paramagnetic	null	0.00090387000
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
27	Co	Cobalt	4	9	58.93319	152	6.62171	1768	3200	1.88	63.7	5	27	966023	8900	17	100	421	25	null	Ferromagnetic	1394	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	631	null