Fusion 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 ("Fusion.php") enables SQL commands to query the Fusion 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, TwoToTwo and Fission 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 Fusion tables, A1 is never greater than A2 in any row, i.e. A1 <= A2. This also applies 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

Input used for this run on 15-Sep-2020 09:19:52 (NZT):

Full SQL Query: "select * from FusionAll where neutrino = 'none' and (E in ('P' ) ) order by MeV desc"

11 rows were found.

Results Table:

id	neutrino	id_sub	E1	A1	nBorF1	Z1	aBorF1	E2	A2	nBorF2	Z2	aBorF2	E	A	nBorF	Z	aBorF	MeV
1969	none	770	B	10	b	5	f	Ne	21	f	10	f	P	31	f	15	b	30.762600
2651	none	839	N	14	b	7	f	O	17	f	8	f	P	31	f	15	b	26.652800
2235	none	769	B	11	f	5	b	Ne	20	b	10	b	P	31	f	15	b	26.066900
1432	none	632	Li	7	f	3	b	Mg	24	b	12	b	P	31	f	15	b	25.417700
1102	none	633	Li	6	b	3	f	Mg	25	f	12	f	P	31	f	15	b	25.339400
2410	none	380	C	12	b	6	b	F	19	f	9	b	P	31	f	15	b	22.953900
2790	none	838	N	15	f	7	b	O	16	b	8	b	P	31	f	15	b	19.803600
3708	none	1404	T	3	f	1	b	Si	28	b	14	b	P	31	f	15	b	17.897055
313	none	1044	D	2	b	1	f	Si	29	f	14	f	P	31	f	15	b	15.677000
921	none	13	He	4	b	2	b	Al	27	f	13	b	P	31	f	15	b	9.664300
30	none	1045	H	1	f	1	b	Si	30	b	14	b	P	31	f	15	b	7.287100

All Nuclides Appearing in Results Table:

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz
3	1	1	f	b	H	1.00782503223	0.00000000000	0.00000000000	SPN	50.0000	null	0.0000	99.9850	1399.79	705700	1/2+	2.7928473510	null	5700.0000	400.000
4	2	1	b	f	D	2.01410177812	2.22411410138	1.11205705069	SPN	50.0000	null	0.0000	0.0150	0.21	23	1+	0.8574382310	0.0028600000	0.0082	61.403
5	3	1	f	b	T	3.01604927790	8.48111605334	2.82703868445	SYN	1.0906	b-	0.0186	0.0000	0	null	1/2+	2.9789624600	null	6897.0000	426.656
7	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
8	6	3	b	f	Li	6.01512288740	31.99263761964	5.33210626994	SPN	50.0000	null	0.0000	7.4200	1.484	null	1+	0.8220430000	-0.0008060000	3.5800	58.864
9	7	3	f	b	Li	7.01600343660	39.24349799105	5.60621399872	SPN	50.0000	null	0.0000	92.5800	18.516	null	3/2-	3.2564070000	-0.0400000000	1540.0000	155.455
11	10	5	b	f	B	10.01293695000	64.74850694777	6.47485069478	SPN	50.0000	null	0.0000	19.6000	1.96	null	3+	1.8004636000	0.0845000000	22.0000	42.975
12	11	5	f	b	B	11.00930536000	76.20239941621	6.92749085602	SPN	50.0000	null	0.0000	80.4000	8.04	null	3/2-	2.6883780000	0.0405900000	754.0000	128.286
13	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
16	14	7	b	f	N	14.00307400443	104.65546588494	7.47539042035	SPN	50.0000	null	0.0000	99.6300	18.9297	1105	1+	0.4035730000	0.0204400000	null	null
17	15	7	f	b	N	15.00010889888	115.48853186480	7.69923545765	SPN	50.0000	null	0.0000	0.3700	0.0703	null	1/2-	-0.2830569000	null	0.0220	40.547
18	16	8	b	b	O	15.99491461957	127.61572716061	7.97598294754	SPN	50.0000	null	0.0000	99.7590	459888.99	9592	null	null	null	null	null
19	17	8	f	f	O	16.99913175650	131.75857496811	7.75050440989	SPN	50.0000	null	0.0000	0.0370	170.57	null	5/2+	-1.8935430000	-0.0256000000	0.0610	50.227
21	19	9	f	b	F	18.99840316273	147.79709644959	7.77879454998	SPN	50.0000	null	0.0000	100.0000	585	null	1/2+	2.6283210000	null	4730.0000	376.345
22	20	10	b	b	Ne	19.99244017620	160.64033816500	8.03201690825	SPN	50.0000	null	0.0000	90.9200	null	1548	null	null	null	null	null
23	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
26	24	12	b	b	Mg	23.98504169700	198.25166064327	8.26048586014	SPN	50.0000	null	0.0000	78.7000	18337.1	513	null	null	null	null	null
27	25	12	f	f	Mg	24.98583697600	205.58194972280	8.22327798891	SPN	50.0000	null	0.0000	10.1300	2360.29	69	5/2+	-0.8553300000	0.1990000000	null	null
29	27	13	f	b	Al	26.98153853000	224.94576832817	8.33132475290	SPN	50.0000	null	0.0000	100.0000	82300	58	5/2+	3.6407000000	0.1466000000	1170.0000	104.227
30	28	14	b	b	Si	27.97692653465	236.53056941472	8.44752033624	SPN	50.0000	null	0.0000	92.2100	260032.2	653	null	null	null	null	null
31	29	14	f	f	Si	28.97649466490	245.00394060131	8.44841174487	SPN	50.0000	null	0.0000	4.7000	13254	34	1/2+	-0.5550520000	null	2.0900	79.468
32	30	14	b	b	Si	29.97377013600	255.61291079491	8.52043035983	SPN	50.0000	null	0.0000	3.0900	8713.8	23	null	null	null	null	null
33	31	15	f	b	P	30.97376199842	262.90924445619	8.48094336955	SPN	50.0000	null	0.0000	100.0000	1050	null	1/2+	1.1309250000	null	377.0000	161.923