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 09-Dec-2020 01:45:59 (NZT):

Full SQL Query: "select * from TwoToTwoAll where (neutrino = 'left' or neutrino = 'right') and (E1 in ('Li', 'D') and E2 in ('Li', 'D') ) order by MeV desc "

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
19224	right	305	Li	6	b	3	f	Li	7	f	3	b	H	1	f	1	b	C	12	b	6	b	21.709395
26563	right	307	Li	7	f	3	b	Li	7	f	3	b	H	1	f	1	b	C	13	f	6	f	19.403948
26564	right	306	Li	7	f	3	b	Li	7	f	3	b	D	2	b	1	f	C	12	b	6	b	16.681190
26566	right	1382	Li	7	f	3	b	Li	7	f	3	b	He	4	b	2	b	B	10	b	5	f	15.339839
26565	right	1383	Li	7	f	3	b	Li	7	f	3	b	He	3	f	2	f	B	11	f	5	b	6.217717
4286	right	1	D	2	b	1	f	D	2	b	1	f	H	1	f	1	b	He	3	f	2	f	4.051062
1212528	left	261818	D	2	b	1	f	D	2	b	1	f	n*	1	f	0	f	T	3	f	1	b	3.250700
19226	right	1381	Li	6	b	3	f	Li	7	f	3	b	He	3	f	2	f	B	10	b	5	f	2.013884
1212539	left	261829	Li	6	b	3	f	Li	6	b	3	f	T	3	f	1	b	Be	9	f	4	f	1.878600

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
3	1	0	f	f	n*	1.00866491582	0.00000000000	0.00000000000	UPN	-4.6070	null	0.0000	100.0000	null	null	1/2+	-1.9130427000	null	null	null	-18.32471830
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
6	3	1	f	b	T	3.01604928199	8.48111224352	2.82703741451	SYN	1.0906	B-	0.0186	0.0000	0	null	1/2+	2.9789624600	null	6897.0000	426.656	28.53498650
7	3	2	f	f	He	3.01602932265	7.71737084564	2.57245694855	SPN	50.0000	null	0.0000	0.0001	null	35	1/2+	-2.1276253100	null	null	null	-20.37894730
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
9	6	3	b	f	Li	6.01512288742	31.99263760101	5.33210626683	SPN	50.0000	null	0.0000	7.4200	1.484	null	1+	0.8220430000	-0.0008060000	3.5800	58.864	3.93712700
10	7	3	f	b	Li	7.01600343666	39.24349793516	5.60621399074	SPN	50.0000	null	0.0000	92.5800	18.516	null	3/2-	3.2564070000	-0.0400000000	1540.0000	155.455	10.39770400
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
13	10	5	b	f	B	10.01293686200	64.74858891927	6.47485889193	SPN	50.0000	null	0.0000	19.6000	1.96	null	3+	1.8004636000	0.0845000000	22.0000	42.975	2.87467955
14	11	5	f	b	B	11.00930516600	76.20258012611	6.92750728419	SPN	50.0000	null	0.0000	80.4000	8.04	null	3/2-	2.6883780000	0.0405900000	754.0000	128.286	8.58470700
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
16	13	6	f	f	C	13.00335483521	97.10512005305	7.46962461947	SPN	50.0000	null	0.0000	1.1100	2.22	37	1/2-	0.7023690000	null	1.0000	100.589	6.72828600

All Elements Appearing in Results Table: (6)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	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	-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	-0.00000000105
3	Li	Lithium	2	1	6.94174	167	12.97521	453.69	1615	0.98	59.6	1	3	11815	535	11	85	3570	20	null	Paramagnetic	0.00000137000
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	-0.00002328000
5	B	Boron	2	13	10.81402	87	4.39594	2348	4273	2.04	26.7	3	5	32826.7	2460	0	27	1030	10	null	Diamagnetic	-0.00002140000
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	-0.00001400000