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The main branch consists of two ions sources terminals followed by a [[Radio Frequency Quadrupole (RFQ)]] and by an Intergidigital linac [[IH linac accelerator]] resonating at 36 MHz up to the energy of 1.4 MeV/u. The main part then is operated by a classical [[linac]] of the Alvarez type which resonates at 108 MHz. Final energy adjustmnet can be performed in the last section which consists of a series of single gap resonators. This solutions was proposed in order to achieve the maximum flexibility in beam energy.▼
[[File:Part of UNILAC GSI.jpg|thumb|300px|Part of UNILAC GSI]]
The '''Universal Linear Accelerator (UNILAC)''' is a [[heavy ion]] [[linear particle accelerator|linac]] based at the [[GSI Helmholtz Centre for Heavy Ion Research]] near [[Darmstadt]], [[Germany]]. It can provide beams of accelerated [[ion]]s of elements from [[hydrogen]] to [[uranium]] with energies of 2 to 11.4 [[MeV]]/[[Dalton (unit)|Da]].<ref>{{cite journal|last=Barth|first=W.|author2=Bayer, W. |author3=Dahl, L. |author4=Groening, L. |author5=Richter, S. |author6= Yaramyshev, S. |title=Upgrade program of the high current heavy ion UNILAC as an injector for FAIR|journal=Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment|year=2007|volume=577|issue=1–2|pages=211–214|doi=10.1016/j.nima.2007.02.054|bibcode = 2007NIMPA.577..211B }}</ref>
▲The main branch consists of two
The UNILAC is used both to send beams of heavy ions to experiments and to load the [[SIS18]] Heavy-Ion Synchrotron (Schwer-Ionen-Synchrotron) with high-energy ions.
Collisions between heavy-ion beams and stationary targets can be made to generate superheavy [[transactinides
Experiments using beams from UNILAC
== See also ==
* [[GSI Helmholtz Centre for Heavy Ion Research]]
== References ==
{{reflist}}
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