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-May-2022 11:52:28 (NZT):

Full SQL Query: "select * from TwoToTwoAll where E1 in ('H', 'W') and E2 in ('Ni', 'N') order by MeV desc limit 100"

6 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
5	none	14	H	1	f	1	b	N	15	f	7	b	He	4	b	2	b	C	12	b	6	b	4.964900
43	left	43	H	1	f	1	b	Ni	61	f	28	f	He	4	b	2	b	Fe	58	b	26	b	2.793553
46	right	1081	H	1	f	1	b	Ni	64	b	28	b	He	4	b	2	b	Ni	61	f	28	f	1.985939
44	right	1079	H	1	f	1	b	Ni	61	f	28	f	He	4	b	2	b	Ni	58	b	28	b	0.865352
42	left	40	H	1	f	1	b	Ni	60	b	28	b	He	4	b	2	b	Fe	57	f	26	f	0.569145
45	none	90	H	1	f	1	b	Ni	62	b	28	b	He	4	b	2	b	Co	59	f	27	b	0.351200

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
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
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
73	58	26	b	b	Fe	57.93327373800	509.93751006707	8.79202603564	SPN	50.0000	null	0.0000	0.3300	185.79	null	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
77	58	28	b	b	Ni	57.93534178000	506.44647384250	8.73183575591	SPN	50.0000	null	0.0000	67.8800	57.0192	49	null	null	null	null	null	null
79	60	28	b	b	Ni	59.93078525600	526.83302405250	8.78055040087	SPN	50.0000	null	0.0000	26.2300	22.0332	null	null	null	null	null	null	null
80	61	28	f	f	Ni	60.93105494500	534.65289723880	8.76480159408	SPN	50.0000	null	0.0000	1.1900	0.9996	null	3/2-	-0.7496500000	0.1620000000	null	null	-2.39477000
81	62	28	b	b	Ni	61.92834487100	545.24840277495	8.79432907702	SPN	50.0000	null	0.0000	3.6600	3.0744	null	null	null	null	null	null	null
82	64	28	b	b	Ni	63.92796634100	561.74317524830	8.77723711325	SPN	50.0000	null	0.0000	1.0800	0.9072	null	null	null	null	null	null	null

All Elements Appearing in Results Table: (7)

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
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	null	-0.00000000680
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
28	Ni	Nickel	4	10	58.72843	149	6.59277	1728	3186	1.91	112	4	28	1039668	8908	14	91	445	84	null	Ferromagnetic	631	null