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Ion Sources Accelerators Available Beams

Ion Sources

NEOMAFIOS

An external ECR ion source using 10 GHz microwaves and a permanent-magnet (NdFeB) mirror field. It supplies beams to the AVF cyclotron. It is used for generating light ions, offering stable operation and ease of handling.

NEOMAFIOS external ECR ion source

Fig. NEOMAFIOS.

ECR ion source
RF frequency10 GHz
Mirror magnetPermanent magnet (Fe–Nd–B)
Vacuum chamberDiameter 67 mm, length 170 mm
Pumping speed520 l/s
Extraction voltage5–50 kV
Available ionsp, d, He, Li–Mg, Ar

HIPIS

A polarized ion source developed to generate high-intensity, high-polarization proton and deuteron beams.

HIPIS polarized ion source

Fig. HIPIS.

High-intensity polarized ion source
DissociatorRF (13.6 MHz, 300 W), nozzle (20 K+N2), Skimmer (Diameter: 4 mm)
SextupolePermanent magnet (Nd–B–Fe, NEOMAX-35H)
RF transition unitTwo weak-field and two strong-field RF transition units
ECR ionizerRF (52.45 GHz, 200 W) + Solenoid + N2
Extraction voltage5–20 kV
Ion supplypol-p, pol-d

SCECR

A superconducting ECR (Electron Cyclotron Resonance) ion source using 18 GHz microwaves to efficiently generate high charge-state ions. The superconducting magnets provide strong, stable fields, enabling high-intensity beams across elements from light to medium-heavy.

SCECR superconducting ECR ion source

Fig. SCECR.

Superconducting ECR ion source
RF frequency18 GHz
Magnet systemSuperconducting coils (mirror magnetic field) + permanent magnet hexapole
Typical extraction voltage5–30 kV
Available ions (examples)He–Ar, Kr, Xe (light to medium-heavy elements)

Accelerators

K140 AVF Cyclotron

K140 AVF Cyclotron
Magnet
Pole diameter3300 mm
Pole gap206–347 mm
Isomagnetic field1.6 T
Extraction radius1000 mm
Trim coils16 pairs
Valley coils3 pairs
Weight400 tons
Acceleration system
Dee electrodeDouble type with 87° spanning angle
ResonatorCoaxial; movable shorting plate
Frequency18–36 MHz
Maximum accelerating voltage60 kV
Harmonics1, 2, 3, 6
ExtractionElectrostatic deflector

K400 Ring Cyclotron

K400 Ring Cyclotron
Magnet
Sector magnets6
Pole gap60 mm
Maximum field1.75 T
Trim coils36 pairs
Injection radius2 m
Extraction radius4 m
Weight2200 tons
Acceleration
Single-gap cavities3
Frequency30–52 MHz
Harmonics6, 10
Maximum accelerating voltage500 kV
RF power250 kW / cavity
Flat-top cavity
Single-gap1
FT harmonic3
Frequency90–156 MHz

Old K140 AVF Cyclotron

Old K140 AVF Cyclotron
Magnet
Pole diameter3300 mm
Pole gap206–347 mm
Isomagnetic field1.6 T
Extraction radius1000 mm
Trim coils16 pairs
Valley coils3–5 pairs
Weight400 tons
Acceleration system
Dee electrodeSingle type with 180° spanning angle
ResonatorCoaxial; movable shorting plate
Frequency6–19 MHz
Maximum accelerating voltage60 kV
Harmonics1, 3
ExtractionElectrostatic deflector; weak-focusing magnetic channel

Available Beams

* Black: achievements with the old AVF cyclotron (beam delivery requires acceleration tests).
* Red: achievements with the AVF cyclotron updated in 2021 (acceleration tests not required).

Ion Energy
Charge State AVF AVF+RING
AVF RING (MeV) (MeV)
1H1+1+10–80, 65100–392, 416, 230, 392
1H21+1+140
2H1+1+10–5680, 103, 140, 200
3He1+14, 25
3He2+2+45, 73, 87300, 420
4He1+10
4He2+2+38–130, 28.5210, 300, 400
6Li2+40, 45
6Li2+3+73, 82309, 360
7Li3+3+110, 150455
11B3+69
11B5+5+200900
12C4+80, 105, 110, 164
12C4+6+145600
12C5+250
12C5+6+2621200
13C5+6+178780
14N5+7+
15N6+7+220975
16O5+100–170
16O6+190
16O6+8+2861280
18O4+90, 106, 100
18O5+118, 135, 165
18O6+165, 246
18O6+8+2461080
18O7+8+3221440
19F4+100
20Ne6+/7+/8+155, 300
22Ne6+130, 190
22Ne8+10+4001760
24Mg5+140
36Ar11+(16+)4371872
40Ar8+200
40Ar11+360, 374
40Ar12+17+4862060
86Kr21+640
86Kr23+731
129Kr29+838
132Xe24+897

10-1 Mihogaoka, Ibaraki, Osaka 567-0047, Japan

Osaka University

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