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 20-Mar-2025 13:42:33 (NZT):

Full SQL Query: "select * from FusionAll where E1 in ('K', 'Al', 'Si' ) and E2 in ('K', 'Al', 'Si' ) order by MeV desc limit 100"

10 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
3564	none	23	Al	27	f	13	b	Al	27	f	13	b	Fe	54	b	26	b	21.842600
3565	left	1580	Al	27	f	13	b	Si	29	f	14	f	Fe	56	b	26	b	21.511927
3566	left	1581	Al	27	f	13	b	Si	30	b	14	b	Fe	57	f	26	f	18.538598
3593	none	1079	Si	29	f	14	f	Si	29	f	14	f	Ni	58	b	28	b	16.431600
3594	left	1597	Si	29	f	14	f	Si	30	b	14	b	Co	59	f	27	b	15.893154
3609	none	1081	Si	30	b	14	b	Si	30	b	14	b	Ni	60	b	28	b	15.592300
3588	none	1080	Si	28	b	14	b	Si	30	b	14	b	Ni	58	b	28	b	14.294700
3600	left	1608	Si	29	f	14	f	K	41	f	19	b	Ge	70	b	32	b	12.993413
3608	left	1598	Si	30	b	14	b	Si	30	b	14	b	Co	60	b	27	f	12.776375
3615	left	1607	Si	30	b	14	b	K	40	b	19	f	Ge	70	b	32	b	12.474571

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
29	27	13	f	b	Al	26.98153840800	224.94588197047	8.33132896187	SPN	50.0000	null	0.0000	100.0000	82300	58	5/2+	3.6407000000	0.1466000000	1170.0000	104.227	6.97627800
30	28	14	b	b	Si	27.97692653499	236.53056909801	8.44752032493	SPN	50.0000	null	0.0000	92.2100	260032.2	653	null	null	null	null	null	null
31	29	14	f	f	Si	28.97649466525	245.00394027528	8.44841173363	SPN	50.0000	null	0.0000	4.7000	13254	34	1/2+	-0.5550520000	null	2.0900	79.468	-5.31903000
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	null
43	40	19	b	f	K	39.96399816600	341.51464804390	8.53786620110	UPN	9.0969	B- or K or B+	1.5050	0.0118	2.4662	null	4-	-1.2979700000	-0.0730000000	null	null	-1.55428600
44	41	19	f	b	K	40.96182525796	351.60978653214	8.57584845200	SPN	50.0000	null	0.0000	6.8800	1437.92	null	3/2+	0.2148720000	0.0711000000	null	null	0.68614062
64	54	26	b	b	Fe	53.93960830600	471.75254802301	8.73615829672	SPN	50.0000	null	0.0000	5.8200	3276.66	72	null	null	null	null	null	null
65	56	26	b	b	Fe	55.93493561700	492.24730527224	8.79013045129	SPN	50.0000	null	0.0000	91.6600	51604.58	1169	null	null	null	null	null	null
66	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
68	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
69	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
70	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
71	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
84	70	32	b	b	Ge	69.92424870600	610.50331931480	8.72147599021	SPN	50.0000	null	0.0000	20.5200	0.3078	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
13	Al	Aluminium	3	13	26.98154	118	9.99316	933.47	2792	1.61	42.5	3	13	222316	2700	38	235	904	82300	null	Paramagnetic	null	0.00002110000
14	Si	Silicon	3	14	28.08561	111	12.05391	1687	3173	1.9	133.6	4	14	257923	2330	0.001	150	710	282000	650	Diamagnetic	null	-0.00000373000
19	K	Potassium	4	1	39.09811	243	45.67536	336.53	1032	0.82	48.4	1	19	476063	856	14	100	757	20900	null	Paramagnetic	null	0.00000574000
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
32	Ge	Germanium	4	14	72.56952	125	13.63320	1211.4	3093	2.01	119	4	5	9020	5323	0.002	60	321.4	1.5	null	Diamagnetic	null	-0.00000798000