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-Sep-2021 06:27:36 (NZT):

Full SQL Query: "select * from TwoToTwoAll where neutrino = 'none' and (E1 in ('N') and E2 in ('Fe' ) and E3 in ('Si', 'O') ) order by MeV desc limit 1000"

8 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
66509	none	21239	N	14	b	7	f	Fe	57	f	26	f	O	16	b	8	b	Mn	55	f	25	b	5.278800
66519	none	21244	N	14	b	7	f	Fe	57	f	26	f	Si	30	b	14	b	K	41	f	19	b	2.831700
66479	none	21210	N	14	b	7	f	Fe	54	b	26	b	Si	29	f	14	f	K	39	f	19	b	2.475900
75814	none	21213	N	15	f	7	b	Fe	54	b	26	b	Si	30	b	14	b	K	39	f	19	b	2.099600
75822	none	21234	N	15	f	7	b	Fe	56	b	26	b	O	16	b	8	b	Mn	55	f	25	b	1.929100
66477	none	21209	N	14	b	7	f	Fe	54	b	26	b	Si	28	b	14	b	K	40	b	19	f	1.795900
75811	none	21212	N	15	f	7	b	Fe	54	b	26	b	Si	28	b	14	b	K	41	f	19	b	0.900800
66497	none	21230	N	14	b	7	f	Fe	56	b	26	b	Si	30	b	14	b	K	40	b	19	f	0.377300

All Nuclides Appearing in Results Table: (13)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
18	14	7	b	f	N	14.00307400446	104.65546585700	7.47539041836	SPN	50.0000	null	0.0000	99.6300	18.9297	1105	1+	0.4035730000	0.0204400000	null	null	1.93377980
19	15	7	f	b	N	15.00010889894	115.48853180891	7.69923545393	SPN	50.0000	null	0.0000	0.3700	0.0703	null	1/2-	-0.2830569000	null	0.0220	40.547	-2.71261890
20	16	8	b	b	O	15.99491461960	127.61572713267	7.97598294579	SPN	50.0000	null	0.0000	99.7590	459888.99	9592	null	null	null	null	null	null
33	28	14	b	b	Si	27.97692653499	236.53056909801	8.44752032493	SPN	50.0000	null	0.0000	92.2100	260032.2	653	null	null	null	null	null	null
34	29	14	f	f	Si	28.97649466525	245.00394027528	8.44841173363	SPN	50.0000	null	0.0000	4.7000	13254	34	1/2+	-0.5550520000	null	2.0900	79.468	-5.31903000
35	30	14	b	b	Si	29.97377013600	255.61291079491	8.52043035983	SPN	50.0000	null	0.0000	3.0900	8713.8	23	null	null	null	null	null	null
46	39	19	f	b	K	38.96370648661	333.71525878127	8.55680150721	SPN	50.0000	null	0.0000	93.1000	19457.9	null	3/2+	0.3914700000	0.0585000000	null	null	1.25006120
47	40	19	b	f	K	39.96399816600	341.51464804390	8.53786620110	UPN	9.0969	B- or K or B+	1.5050	0.0118	2.4662	null	4-	-1.2979700000	-0.0730000000	null	null	-1.55428600
48	41	19	f	b	K	40.96182525796	351.60978653214	8.57584845200	SPN	50.0000	null	0.0000	6.8800	1437.92	null	3/2+	0.2148720000	0.0711000000	null	null	0.68614062
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

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	MagVolSus
7	N	Nitrogen	2	15	14.00693	56	11196.58705	63.05	77.36	3.04	7	3	7	64360	1.251	null	0.026583	1040	19	960	Diamagnetic	-0.00000000680
8	O	Oxygen	2	16	15.99938	48	11196.20378	54.8	90.2	3.44	141	2	8	84078	1.429	null	0.02658	919	461000	10400	Paramagnetic	0.00000190772
14	Si	Silicon	3	14	28.08561	111	12.05391	1687	3173	1.9	133.6	4	14	257923	2330	0.001	150	710	282000	650	Diamagnetic	-0.00000373000
19	K	Potassium	4	1	39.09811	243	45.67536	336.53	1032	0.82	48.4	1	19	476063	856	14	100	757	20900	null	Paramagnetic	0.00000574000
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	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	null