Available beams

The table below lists ion beams which were extracted from the cyclotron:

Cyklotron K= 90 – 160
Ion	Energy min [MeV]	Energy max [MeV]	Energy max [MeV/nucl.]	Intensity of the extracted beam [nA]	Intensity of the extracted beam [pnA]	Intensity of the extracted beam [p/s]
¹⁰B⁺²	51	55	5.5	45	9.0	5.6 10⁺¹⁰
¹¹B⁺²	40	50	4.5	50	10.0	6.3 10⁺¹⁰
¹²C⁺²	38	50	4.2	100	16.7	1.0 10⁺¹¹
¹²C⁺³	53	92	7.7	220	36.7	2.3 10⁺¹¹
¹³C⁺³		90	6.9	90	16
¹⁴N⁺²	32	50	3.6	240	34.3	2.1 10⁺¹¹
¹⁴N⁺³	57	91	6.5	1500	214.3	1.3 10⁺¹²
¹⁵N⁺³		43	2.9	50	7.1
¹⁶O⁺³	46	80	5.0	400	50.0	3.1 10⁺¹¹
¹⁶O⁺⁴	80	120	7.5	650	81.3	5.1 10⁺¹¹
¹⁸O⁺⁴	100	120	6.7	2000	250.0	1.6 10⁺¹²
¹⁹F⁺³	50	66	3.5	10	1.1	6.9 10⁺⁹
²⁰Ne⁺³	45	68	3.4	300	30.0	1.9 10⁺¹¹
²⁰Ne⁺⁴	68	115	5.8	1300	130.0	8.1 10⁺¹¹
²⁰Ne⁺⁵	130	160	8.0	120	12.0	7.5 10⁺¹¹
²²Ne⁺³	44	55	2.5	260	26.0	1.6 10⁺¹¹
²⁴Mg⁺⁴		77	3.2	120	10
³²S⁺⁵	79	110	3.4	50	3.1	2.0 10⁺¹⁰
³²S⁺⁶	120^()*	150	4.7	70	4.4	2.7 10⁺¹⁰
³²S⁺⁷	120^()*	225	7.0	50	3.1	2.0 10⁺¹⁰
⁴⁰Ar⁺⁶	90^()*	132	3.7	100	5.6	3.6 10⁺¹⁰
⁴⁰Ar⁺⁷	130^()*	164	4.1	35	1.9	1.2 10⁺¹⁰
⁴⁰Ar⁺⁸	180^()*	200	5.0	40	2.2	1.4 10⁺¹⁰

(*) estimation, no experimental data

²⁰Ne⁺⁴ accelerated ion on the 2nd harmonic
²²Ne⁺³ accelerated ion on the 3rd harmonic

Remark:

Intensities shown in this table depend on the beam energy. This is due to the conditions of the extraction – the radius of the extraction and the fringing field geometry associated with the orbit trajectories. The most intense beams are obtained for the maximum energy of a given charge state. Decrease of energy results in an inevitable loss of the intensity due to changing the one-turn extraction mode to the multiturn one.

Intensity on the target position should reach 50-90% of the listed values, depending on the experimental configuration, collimators used, etc.