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 22-Aug-2021 11:23:47 (NZT):

Full SQL Query: "select * from TwoToTwoAll where (E1 in ('He') and E2 in ('Tl' ) ) and nBorF1 = 'b' order by MeV desc limit 100"

11 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
19185	right	15115	He	4	b	2	b	Tl	203	f	81	b	Ne	21	f	10	f	W	186	b	74	b	24.912804
19184	right	9697	He	4	b	2	b	Tl	203	f	81	b	O	18	b	8	b	Os	189	f	76	f	16.323497
19183	right	9699	He	4	b	2	b	Tl	203	f	81	b	O	17	f	8	f	Os	190	b	76	b	16.021693
19188	right	9704	He	4	b	2	b	Tl	205	f	81	b	O	17	f	8	f	Os	192	b	76	b	15.389208
19182	none	6004	He	4	b	2	b	Tl	203	f	81	b	N	15	f	7	b	Os	192	b	76	b	12.496900
19179	right	4841	He	4	b	2	b	Tl	203	f	81	b	C	12	b	6	b	Pt	195	f	78	f	9.421125
19180	right	4840	He	4	b	2	b	Tl	203	f	81	b	C	13	f	6	f	Pt	194	b	78	b	8.169197
19187	right	4844	He	4	b	2	b	Tl	205	f	81	b	C	13	f	6	f	Pt	196	b	78	b	8.131937
19181	right	7237	He	4	b	2	b	Tl	203	f	81	b	N	14	b	7	f	Ir	193	f	77	b	7.835722
19178	none	6003	He	4	b	2	b	Tl	203	f	81	b	B	11	f	5	b	Pt	196	b	78	b	0.603600
19186	none	6027	He	4	b	2	b	Tl	205	f	81	b	B	11	f	5	b	Pt	198	b	78	b	0.214200

All Nuclides Appearing in Results Table: (20)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
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
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
18	14	7	b	f	N	14.00307400446	104.65546585700	7.47539041836	SPN	50.0000	null	0.0000	99.6300	18.9297	1105	1+	0.4035730000	0.0204400000	null	null	1.93377980
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
21	17	8	f	f	O	16.99913175664	131.75857483770	7.75050440222	SPN	50.0000	null	0.0000	0.0370	170.57	null	5/2+	-1.8935430000	-0.0256000000	0.0610	50.227	-3.62806000
22	18	8	b	b	O	17.99915961284	139.80371390688	7.76687299483	SPN	50.0000	null	0.0000	0.2040	940.44	null	null	null	null	null	null	null
25	21	10	f	f	Ne	20.99384668500	167.40127014932	7.97148905473	SPN	50.0000	null	0.0000	0.2570	null	null	3/2+	-0.6617000000	0.1020000000	null	null	-2.11308100
277	186	74	b	b	W	185.95436521500	1485.83804616380	7.98837659228	SPN	50.0000	null	0.0000	28.4100	0.355125	null	null	null	null	null	null	null
285	189	76	f	f	Os	188.95814600500	1504.96485576730	7.96277701464	SPN	50.0000	null	0.0000	16.1000	0.0002415	null	3/2-	0.6576000000	0.8600000000	null	null	2.10713000
286	190	76	b	b	Os	189.95844549600	1512.75696855950	7.96187878189	SPN	50.0000	null	0.0000	26.4000	0.000396	null	null	null	null	null	null	null
287	192	76	b	b	Os	191.96147888100	1526.07356154380	7.94829979971	SPN	50.0000	null	0.0000	41.0000	0.000615	null	null	null	null	null	null	null
289	193	77	f	b	Ir	192.96292382400	1532.01635887860	7.93790859523	SPN	50.0000	null	0.0000	62.7000	0.000627	null	3/2+	0.1630000000	0.7510000000	null	null	0.52270000
292	194	78	b	b	Pt	193.96268352700	1539.52894772410	7.93571622538	SPN	50.0000	null	0.0000	32.9000	0.001645	null	null	null	null	null	null	null
293	195	78	f	f	Pt	194.96479435300	1545.63381222760	7.92632724219	SPN	50.0000	null	0.0000	33.8000	0.00169	null	1/2-	0.6073000000	null	19.1000	85.996	5.83850000
294	196	78	b	b	Pt	195.96495467500	1553.55556015470	7.92630387834	SPN	50.0000	null	0.0000	25.3000	0.001265	null	null	null	null	null	null	null
295	198	78	b	b	Pt	197.96789673400	1566.95722279050	7.91392536763	SPN	50.0000	null	0.0000	7.2100	0.0003605	null	null	null	null	null	null	null
304	203	81	f	b	Tl	202.97234402200	1600.82303379690	7.88582775269	SPN	50.0000	null	0.0000	29.5000	0.25075	null	1/2+	1.6160000000	null	null	null	15.53933900
305	205	81	f	b	Tl	204.97442723700	1615.02470475210	7.87816929147	SPN	50.0000	null	0.0000	70.5000	0.59925	null	1/2+	1.6320000000	null	null	null	15.69218600

All Elements Appearing in Results Table: (11)

Z	E	EName	P	G	AWeight	ARadius	MolarVol	Melting	Boiling	Negativity	Affinity	Val	MxInum	MxInize	STPDensity	ElectG	ThermG	SpecHeat	ppmECrust	ppmEStellar	MagType	MagVolSus
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
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
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	-0.00000000680
8	O	Oxygen	2	16	15.99938	48	11196.20378	54.8	90.2	3.44	141	2	8	84078	1.429	null	0.02658	919	461000	10400	Paramagnetic	0.00000190772
10	Ne	Neon	2	18	20.17072	38	22411.91400	24.56	27.07	null	0	0	10	131432	0.9	null	0.0491	1030	null	1340	Diamagnetic	-0.00000000369
74	W	Tungsten	6	6	183.84152	193	9.55021	3695	5828	2.36	78.6	6	2	1700	19250	20	170	132	1.25	null	Paramagnetic	0.00008840000
76	Os	Osmium	6	8	190.32953	185	8.41794	3306	5285	2.2	106.1	8	2	1600	22610	12	88	130	0.0015	null	Paramagnetic	0.00001400000
77	Ir	Iridium	6	9	192.21637	180	8.48637	2739	4701	2.2	151	8	2	1600	22650	21	150	131	0.001	null	Paramagnetic	0.00003770000
78	Pt	Platinum	6	10	195.08590	177	9.25016	2041.4	4098	2.28	205.3	6	2	1791	21090	9.4	72	133	0.005	null	Paramagnetic	0.00025730000
81	Tl	Thallium	6	13	204.38383	156	17.24758	577	1746	1.62	19.2	3	3	2878	11850	6.7	46	129	0.85	null	Diamagnetic	-0.00003560000