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 03-Sep-2024 21:43:20 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('D', 'Pd') and E2 in ('D', 'Pd') and E4 in ('Ag') 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
5837	right	65	D	2	b	1	f	Pd	108	b	46	b	H	1	f	1	b	Ag	109	f	47	b	5.120417
5801	right	63	D	2	b	1	f	Pd	106	b	46	b	H	1	f	1	b	Ag	107	f	47	b	4.198238
955724	left	190201	Pd	102	b	46	b	Pd	105	f	46	f	Ru	100	b	44	b	Ag	107	f	47	b	1.481078
964003	right	303067	Pd	105	f	46	f	Pd	110	b	46	b	Pd	106	b	46	b	Ag	109	f	47	b	1.155047
959536	left	190204	Pd	104	b	46	b	Pd	105	f	46	f	Ru	100	b	44	b	Ag	109	f	47	b	0.447119
963961	left	190207	Pd	105	f	46	f	Pd	105	f	46	f	Ru	101	f	44	f	Ag	109	f	47	b	0.428489
963986	right	303058	Pd	105	f	46	f	Pd	108	b	46	b	Pd	106	b	46	b	Ag	107	f	47	b	0.363281
963985	right	303059	Pd	105	f	46	f	Pd	108	b	46	b	Pd	104	b	46	b	Ag	109	f	47	b	0.279446
955733	left	190210	Pd	102	b	46	b	Pd	108	b	46	b	Ru	101	f	44	f	Ag	109	f	47	b	0.037262

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
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
142	100	44	b	b	Ru	99.90421045200	861.91344729911	8.61913447299	SPN	50.0000	null	0.0000	12.6200	0.0001262	null	null	null	null	null	null	null
143	101	44	f	f	Ru	100.90557307500	868.71525865745	8.60114117483	SPN	50.0000	null	0.0000	17.0700	0.0001707	null	5/2+	-0.7180000000	0.4600000000	null	null	-1.37200000
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
152	108	46	b	b	Pd	107.90389180500	925.21429404707	8.56679901895	SPN	50.0000	null	0.0000	26.7100	0.0040065	null	null	null	null	null	null	null
153	110	46	b	b	Pd	109.90517286800	940.16316504488	8.54693786404	SPN	50.0000	null	0.0000	11.8100	0.0017715	null	null	null	null	null	null	null
154	107	47	f	b	Ag	106.90509153100	915.24333570460	8.55367603462	SPN	50.0000	null	0.0000	51.8200	0.038865	null	1/2-	-0.1135200000	null	null	null	-1.08891800
155	109	47	f	b	Ag	108.90475577300	931.69826630231	8.54769051653	SPN	50.0000	null	0.0000	48.1800	0.036135	null	1/2-	-0.1305100000	null	null	null	-1.25190000

All Elements Appearing in Results Table: (4)

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
44	Ru	Ruthenium	5	8	101.03531	178	8.16777	2607	4423	2.2	101.3	8	3	2747	12370	14	120	238	0.001	null	Paramagnetic	null	0.00006700000
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
47	Ag	Silver	5	11	107.86844	165	10.28298	1234.93	2435	1.93	125.6	4	3	3361	10490	62	430	235	0.075	null	Diamagnetic	null	-0.00002380000