User Facilities
FRIB offers fast, stopped, and reaccelerated rare-isotope beams from the FRIB linear accelerator (linac), produced from a primary beam that impinges on a target.
FRIB also offers stable and long-lived radioactive beams that may be run at ReA3, ReA6, or the stopped beam area in stand-alone mode (that is, not coupled to the FRIB linac).
FRIB primary beams
Being developed for PAC4 Epoch3a call for proposals
(updated 1 June 2026)
The beam list defines the isotopes and their maximum beam intensity for the primary beam that the FRIB linac can deliver on target. These intensities cannot be achieved for all requested rare isotope beams, specifically for rare isotope beams of rigidity close to the primary beams when the primary beam intensity will be limited to values significantly below the listed value.
| Isotope | Energy (MeV/u) | Beam current on FRIB target (particle nA) |
|---|---|---|
| 16O | 165 | 11364 |
| 16O | 300 | 1563 |
| 18O | 165 | 10101 |
| 18O | 250 | 1667 |
| 20Ne | 175 | 8571 |
| 20Ne | 300 | 1250 |
| 22Ne | 175 | 7792 |
| 22Ne | 250 | 1364 |
| 28Si | 255 | 4202 |
| 28Si | 300 | 1845 |
| 30Si | 255 | 3922 |
| 36Ar | 255 | 3268 |
| 36Ar | 300 | 1435 |
| 40Ar | 255 | 2941 |
| 40Ca | 255 | 2941 |
| 40Ca | 300 | 1292 |
| 48Ca | 240 | 2604 |
| 58Ni | 250 | 2759 |
| 64Ni | 235 | 2660 |
| 64Zn | 250 | 2500 |
| 70Zn | 230 | 2484 |
| 70Ge | 246 | 2033 |
| 76Ge | 228 | 1847 |
| 82Se | 227 | 2149 |
| 78Kr | 247 | 2076 |
| 86Kr | 228 | 2040 |
| 92Mo | 238 | 594 |
| 124Xe | 240 | 1008 |
| 144Sm | 222 | 1251 |
| 195Pt | 190 | 540 |
| 198Pt | 188 | 537 |
| 208Pb | 188 | 1151 |
| 209Bi | 188 | 1018 |
| 232Th | 181 | 476 |
| 238U | 177 | 1187 |
| 238U | 193 | 501 |
*pps = pnA x 6.25 x 109
pps = particles per second
pnA = particle nanoampere
Rare isotope beam rates
Rare isotope beam rates used in proposals must be calculated by an FRIB beam scientist.
An approximate estimate for PAC4 can be obtained from the calculator. The estimates available on the web-based calculator assume optimal conditions and are only intended to provide a rough indication of experiment feasibility. Actual rates will likely be less. Rates above 1E8 pps will require a detailed evaluation of primary beam and fragment power deposition and may not be possible.
For further information on how rates are calculated, please review this tutorial: LISE++ tutorial: Making 64Cr
Demonstrated and available (updated 29 May 2026)
| Isotope | Energy (MeV/u) | Beam current on FRIB target (particle nA) |
|---|---|---|
| 16O | 160 | 7813 |
| 18O | 160 | 6944 |
| 22Ne | 170 | 5348 |
| 22Ne | 260 | 1748 |
| 28Si | 255 | 2801 |
| 28Si | 300 | 1190 |
| 36Ar | 250 | 2222 |
| 36Ar | 300 | 926 |
| 40Ar | 255 | 1961 |
| 40Ca | 250 | 2000 |
| 40Ca | 300 | 833 |
| 48Ca | 240 | 1736 |
| 58Ni | 250 | 1379 |
| 64Ni | 235 | 1330 |
| 64Zn | 250 | 1250 |
| 70Zn | 230 | 1242 |
| 70Ge | 246 | 1161 |
| 76Ge | 228 | 1154 |
| 78Kr | 247 | 1038 |
| 86Kr | 228 | 1020 |
| 82Se | 227 | 1074 |
| 92Mo | 238 | 228 |
| 124Xe | 240 | 672 |
| 144Sm | 222 | 626 |
| 195Pt | 190 | 186 |
| 198Pt | 188 | 185 |
| 208Pb | 188 | 511 |
| 209Bi | 188 | 509 |
| 238U | 177 | 475 |
| 238U | 193 | 435 |
*pps = pnA x 6.25 x 109
pps = particles per second
pnA = particle nanoampere
Beam list for stand-alone operation at ReA3, ReA6, or Stopped Beam Area
The PDF list below includes stable and long-lived radioactive beams that may be run at ReA3, ReA6, or the stopped beam area in stand-alone mode (that is, not coupled to the FRIB linac).
Please note that beams of long-lived and rare stable isotopes are subject to proven extraction from the ion source and availability of material at the time of the experiment.
Beam rate calculator
The beam rate calculator provides a preliminary estimate based on optimal conditions, offering a general indication of experiment feasibility.