A New Method for Obtaining the Baryons Mass under the Killingbeck Plus Isotonic Oscillator Potentials

Table 4

Like Table 3, but for , , , and Ω resonances.

Baryon	Status	[42]exp	State	[43]Calc		Percent of relative error for our calculation
	⁢⁢⁢	1116	^281/2	1116	1116.05	0.004%
	⁢⁢	1560–1700	^281/2	1626.7	1647.99	5.64%–3.05%
	⁢⁢⁢	1660–1680	^281/2	1721.7	1706.84	2.82%–1.59%
	⁢⁢⁢	1685–1695	^283/2	1721.7	1706.84	1.29%–0.69%
	⁢⁢	1720–1850	^481/2	1836.6	1821.74	5.91%–1.52%
	⁢⁢	1750–1850	^281/2	1973.4	1816.04	3.77%–1.83%
	⁢⁢⁢	1815–1825	^285/2	1829.4	1866.62	2.84%–2.28%
	⁢⁢⁢	1810–1830	^485/2	1836.6	1821.74	0.64%–0.45%
	⁢⁢⁢	1850–1910	^283/2	1829.4	1866.62	0.89%–2.27%
	⁢⁢⁢	2090–2110	^217/2	—	2089.04	0.04%–0.99%
	⁢⁢⁢	2090–2140	^485/2	1995	2149.96	2.86%–0.46%
	⁢⁢	2340–2370	^289/2	—	2360.52	0.87%–0.4%
	⁢⁢⁢	1402–1410	^211/2	1657.9	1433.91	2.27%–1.69%
	⁢⁢⁢	1518–1520	^213/2	1657.9	1433.91	5.53%–5.66%
	⁢⁢⁢	1193	^281/2	1193	1193.05	0.004%
	⁢⁢	1630–1690	^281/2	1703.7	1616.12	0.05%–4.37%
	⁢⁢⁢	1665–1685	^283/2	1798.7	1783.74	7.13%–5.85%
	⁢⁢	1730–1800	^281/2	1798.7	1783.74	3.1%–0.9%
	⁢⁢⁢	1770–1780	^485/2	1913.6	1789.87	1.12%–0.55%
	⁢⁢⁢	1900–1935	^285/2	1906.4	1910.7	0.56%–1.25%
	⁢⁢	1900–1950	^283/2	1913.6	1943.62	2.29%–0.32%
	⁢⁢⁢	1383–1385	^4103/2	—	1363.67	1.39%–1.54%
	⁢⁢⁢	2025–2040	^4107/2	2085.0	2004.82	0.99%–1.72%
	⁢⁢⁢	1314–1316	^281/2	1332.6	1332.6	1.41%–1.26%
	⁢⁢	1680–1700	^281/2	—	1706.1	1.55%–0.35%
	⁢⁢	1818–1828	^283/2	1938.3	1923.39	5.79%–5.21%
	⁢⁢⁢	1531–1532	^4103/2	1511.1	1503.2	1.81%–1.87%
	⁢⁢⁢	1672–1673	^4103/2	1650.7	1643	1.73%–1.79%
	⁢⁢	2243–2261	^2103/2	—	2227.87	0.67%–1.46%

Existence is certain, and properties are at least fairly well explored. Existence ranges from very likely to certain, but further confirmation is desirable and/or quantum numbers, branching fractions, and so forth are not well determined.