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 25-Nov-2023 02:03:46 (NZT):

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

7 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
186367	none	63027	Si	29	f	14	f	Si	29	f	14	f	He	4	b	2	b	Fe	54	b	26	b	10.021000
196207	none	63033	Si	30	b	14	b	Si	30	b	14	b	He	4	b	2	b	Fe	56	b	26	b	9.302800
176274	none	63031	Si	28	b	14	b	Si	30	b	14	b	He	4	b	2	b	Fe	54	b	26	b	7.884200
196205	none	63032	Si	30	b	14	b	Si	30	b	14	b	H	1	f	1	b	Co	59	f	27	b	6.061200
186370	none	63030	Si	29	f	14	f	Si	29	f	14	f	Si	28	b	14	b	Si	30	b	14	b	2.136800
186368	none	63028	Si	29	f	14	f	Si	29	f	14	f	C	12	b	6	b	Ti	46	b	22	b	0.325100
186369	none	63029	Si	29	f	14	f	Si	29	f	14	f	Mg	24	b	12	b	S	34	b	16	b	0.067100

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
4	1	1	f	b	H	1.00782503224	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700	1/2+	2.7928473510	null	5700.0000	400.000	26.75222080
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
15	12	6	b	b	C	12.00000000000	92.15904307956	7.67992025663	SPN	50.0000	null	0.0000	98.8900	197.78	3032	null	null	null	null	null	null
28	24	12	b	b	Mg	23.98504169700	198.25166064327	8.26048586014	SPN	50.0000	null	0.0000	78.7000	18337.1	513	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
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
57	46	22	b	b	Ti	45.95262685600	398.18648041382	8.65622783508	SPN	50.0000	null	0.0000	7.9300	444.08	null	null	null	null	null	null	null
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
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

All Elements Appearing in Results Table: (9)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	CuriePtK	MagVolSus
1	H	Hydrogen	1	1	1.00798	53	11212.19021	14.01	20.28	2.2	72.8	1	1	1312	0.0899	null	0.1805	14300	1400	739000	Diamagnetic	null	-0.00000000223
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
6	C	Carbon	2	14	12.01114	67	5.31466	3823	4300	2.55	153.9	4	6	47277	2260	0.1	140	710	200	4600	Diamagnetic	null	-0.00001400000
12	Mg	Magnesium	3	2	24.30955	145	13.98708	923	1363	1.31	0	2	12	189368	1738	23	160	1020	23300	580	Paramagnetic	null	0.00001200000
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	null	-0.00000373000
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
22	Ti	Titanium	4	4	47.87892	176	10.62324	1941	3560	1.54	7.6	4	22	639294	4507	2.5	22	520	5600	null	Paramagnetic	null	0.00018070000
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