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 17-Apr-2022 22:01:36 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('C') and E2 in ('Ti') order by MeV desc limit 100"

12 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
2542	none	1207	C	13	f	6	f	Ti	47	f	22	f	Ni	60	b	28	b	22.662300
2544	none	1211	C	13	f	6	f	Ti	49	f	22	f	Ni	62	b	28	b	21.308900
2540	left	1067	C	13	f	6	f	Ti	46	b	22	b	Co	59	f	27	b	21.235273
2541	left	1069	C	13	f	6	f	Ti	47	f	22	f	Co	60	b	27	f	19.846415
2543	none	1209	C	13	f	6	f	Ti	48	b	22	b	Ni	61	f	28	f	18.865600
2440	left	1068	C	12	b	6	b	Ti	47	f	22	f	Co	59	f	27	b	17.295984
2545	right	541	C	13	f	6	f	Ti	50	b	22	b	Cu	63	f	29	b	17.278282
2439	none	1206	C	12	b	6	b	Ti	46	b	22	b	Ni	58	b	28	b	16.106500
2442	none	1208	C	12	b	6	b	Ti	48	b	22	b	Ni	60	b	28	b	15.989100
2443	none	1210	C	12	b	6	b	Ti	49	f	22	f	Ni	61	f	28	f	15.665900
2444	none	1212	C	12	b	6	b	Ti	50	b	22	b	Ni	62	b	28	b	15.318400
2441	left	1070	C	12	b	6	b	Ti	48	b	22	b	Co	60	b	27	f	13.173192

All Nuclides Appearing in Results Table: (14)

id	A	Z	nBorF	aBorF	E	AMU	BE	BEN	SUS	LHL	RDM	DEMeV	pcaNCrust	ppmNCrust	ppmNSolar	SP	MD	EQ	RCPT	Inova_MHz	MagGR
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
57	46	22	b	b	Ti	45.95262685600	398.18648041382	8.65622783508	SPN	50.0000	null	0.0000	7.9300	444.08	null	null	null	null	null	null	null
58	47	22	f	f	Ti	46.95175775200	407.06713282673	8.66100282610	SPN	50.0000	null	0.0000	7.2800	407.68	null	5/2-	-0.7881400000	0.3020000000	null	null	-1.51054000
59	48	22	b	b	Ti	47.94794093200	418.69356599056	8.72278262480	SPN	50.0000	null	0.0000	73.9400	4140.64	null	null	null	null	null	null	null
60	49	22	f	f	Ti	48.94786462700	426.83573062732	8.71093327811	SPN	50.0000	null	0.0000	5.5100	308.56	null	7/2-	-1.1037000000	0.2470000000	null	null	-1.51095000
61	50	22	b	b	Ti	49.94478583900	437.77469116518	8.75549382330	SPN	50.0000	null	0.0000	5.3400	299.04	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
76	60	27	b	f	Co	59.93381566700	524.79254678764	8.74654244646	SYN	0.7219	G, B-	1.3325	0.0000	0	null	5+	3.7990000000	0.4600000000	null	null	3.63900000
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
83	63	29	f	b	Cu	62.92959723600	551.37058542554	8.75191405437	SPN	50.0000	null	0.0000	69.0900	41.454	null	3/2-	2.2259000000	-0.2200000000	365.0000	106.112	7.11179100

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
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
22	Ti	Titanium	4	4	47.87892	176	10.62324	1941	3560	1.54	7.6	4	22	639294	4507	2.5	22	520	5600	null	Paramagnetic	null	0.00018070000
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
29	Cu	Copper	4	11	63.54724	145	7.12413	1357.77	3200	1.9	118.4	4	29	1116105	8920	59	400	384.4	60	null	Diamagnetic	null	-0.00000963000