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 28-Jul-2022 04:34:20 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('D') and E2 in ('Pd' ) and E4 in ('Cr') order by MeV desc limit 1000"

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
5836	right	95702	D	2	b	1	f	Pd	106	b	46	b	Cr	54	b	24	b	Cr	54	b	24	b	36.834997
5800	right	95700	D	2	b	1	f	Pd	105	f	46	f	Cr	53	f	24	f	Cr	54	b	24	b	36.525741
5760	right	95697	D	2	b	1	f	Pd	104	b	46	b	Cr	52	b	24	b	Cr	54	b	24	b	35.647342
5709	right	95692	D	2	b	1	f	Pd	102	b	46	b	Cr	52	b	24	b	Cr	52	b	24	b	35.409811
5761	right	95696	D	2	b	1	f	Pd	104	b	46	b	Cr	53	f	24	f	Cr	53	f	24	f	33.869119
5704	left	357	D	2	b	1	f	Pd	102	b	46	b	Ti	50	b	22	b	Cr	54	b	24	b	32.949743
5707	none	561	D	2	b	1	f	Pd	102	b	46	b	V	51	f	23	b	Cr	53	f	24	f	32.055500
5708	right	95694	D	2	b	1	f	Pd	102	b	46	b	Cr	50	b	24	b	Cr	54	b	24	b	31.775121
5706	none	560	D	2	b	1	f	Pd	102	b	46	b	V	50	b	23	f	Cr	54	b	24	b	30.737400

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
5	2	1	b	f	D	2.01410177811	2.22411411070	1.11205705535	SPN	50.0000	null	0.0000	0.0150	0.21	23	1+	0.8574382310	0.0028600000	0.0082	61.403	4.10662920
61	50	22	b	b	Ti	49.94478583900	437.77469116518	8.75549382330	SPN	50.0000	null	0.0000	5.3400	299.04	null	null	null	null	null	null	null
62	50	23	b	f	V	49.94715584500	434.78471059568	8.69569421191	UPN	17.1461	B+ or B-	2.2050	0.2400	0.288	null	6+	3.3442000000	0.2100000000	null	null	2.67065000
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
64	50	24	b	b	Cr	49.94604144300	435.04043633398	8.70080872668	SPN	50.0000	null	0.0000	4.3100	4.3962	null	null	null	null	null	null	null
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
66	53	24	f	f	Cr	52.94064696100	464.27862663436	8.75997408744	SPN	50.0000	null	0.0000	9.5500	9.741	null	3/2-	-0.4743100000	-0.1500000000	null	null	-1.51518000
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
147	102	46	b	b	Pd	101.90563205800	875.16673646882	8.58006604381	SPN	50.0000	null	0.0000	0.9600	0.000144	null	null	null	null	null	null	null
148	104	46	b	b	Pd	103.90403040100	892.80084481188	8.58462350781	SPN	50.0000	null	0.0000	10.9700	0.0016455	null	null	null	null	null	null	null
149	105	46	f	f	Pd	104.90507948700	899.89471410910	8.57042584866	SPN	50.0000	null	0.0000	22.2300	0.0033345	null	5/2+	-0.6420000000	0.6600000000	null	null	-1.23000000
150	106	46	b	b	Pd	105.90348029300	909.45544121998	8.57976831340	SPN	50.0000	null	0.0000	27.3300	0.0040995	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	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
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
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
46	Pd	Palladium	5	10	106.44101	169	8.85312	1828	3236	2.2	53.7	4	3	3177	12023	10	72	240	0.015	null	Paramagnetic	null	0.00078990000