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 04:42:29 (NZT):

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

5 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
5649	left	371	D	2	b	1	f	Pd	102	b	46	b	He	4	b	2	b	Ru	100	b	44	b	12.499721
5711	left	398	D	2	b	1	f	Pd	104	b	46	b	He	4	b	2	b	Ru	102	b	44	b	10.562214
5802	left	419	D	2	b	1	f	Pd	106	b	46	b	He	4	b	2	b	Ru	104	b	44	b	8.540871
5839	right	2827	D	2	b	1	f	Pd	108	b	46	b	Be	9	f	4	f	Ru	101	f	44	f	1.598438
5765	right	2826	D	2	b	1	f	Pd	105	f	46	f	Be	9	f	4	f	Ru	98	b	44	b	0.983652

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
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
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
11	9	4	f	f	Be	9.01218306600	58.16199207030	6.46244356337	SPN	50.0000	null	0.0000	100.0000	2.8	null	3/2-	-1.1774300000	0.0529000000	78.8000	56.207	-3.75066000
140	98	44	b	b	Ru	97.90528671300	844.76874235291	8.62008920768	SPN	50.0000	null	0.0000	1.8700	0.0000187	null	null	null	null	null	null	null
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
144	102	44	b	b	Ru	101.90434030000	877.93466854616	8.60720263281	SPN	50.0000	null	0.0000	31.6100	0.0003161	null	null	null	null	null	null	null
145	104	44	b	b	Ru	103.90542536000	893.06611522785	8.58717418488	SPN	50.0000	null	0.0000	18.5700	0.0001857	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
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

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
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
4	Be	Beryllium	2	2	9.01219	112	4.87672	1560	2743	1.57	0	2	4	21006.6	1848	25	190	1820	2.8	null	Diamagnetic	null	-0.00002328000
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