LOW LEVEL RF S YSTEM OF THE LIGHT P ROTON THERAPY LINAC D. Soriano Guillen G. De Michele S. Benedetti Y. Ivanisenko M. Cerv AVO -ADAM Meyrin Switzerland

2025-05-02 0 0 606.37KB 4 页 10玖币
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LOW LEVEL RF SYSTEM OF THE LIGHT PROTON THERAPY LINAC
D. Soriano Guillen, G. De Michele, S. Benedetti, Y. Ivanisenko, M. Cerv, AVO-ADAM, Meyrin,
Switzerland
Abstract
The LIGHT (Linac for Image-Guided Hadron Ther-
apy) project was initiated to develop a modular proton ac-
celerator delivering beam with energies up to 230 MeV for
cancer therapy. The machine consists of three different
kinds of accelerating structures: RFQ (Radio-Frequency
Quadrupole), SCDTL (Side Coupled Drift Tube Linac) and
CCL (Coupled Cavity Linac). These accelerating struc-
tures operate at 750 MHz (RFQ) and 3 GHz (SCDTL,
CCL). The accelerator RF signals are generated, distrib-
uted, and controlled by a Low-Level RF (LLRF) system.
The LIGHT LLRF system is based on a commercially
available solution from Instrumentation Technologies with
project specific customization. This LLRF system features
high amplitude and phase stability, monitoring of the RF
signals from the RF network and the accelerating structures
at 200 Hz, RF pulse shaping over real-time interface inte-
grated, RF breakdown detection, and thermal resonance
frequency correction feedback. The LLRF system control
is integrated in a Front-End Controller (FEC) which con-
nects it to the LIGHT control system. In this contribution
we present the main features of the AVO LLRF system, its
operation and performance.
INTRODUCTION
AVO-ADAM designed and is currently commissioning
the LIGHT (Linac for Image Guided Hadron Therapy) pro-
ton cancer therapy LINAC [1], which is a modular normal
conducting RF accelerator fed by 4 Inductive Output
Tubes (IOTs) and 13 klystrons grouped in 14 power sta-
tions. At each power station the RF power can be modu-
lated independently every pulse. The pulse repetition rate
is 200 Hz allowing accurate dose delivery within tumour
volume and longitudinal layer switching on a pulse-to-
pulse basis, given the low emittance of the proton beam.
These features of the LIGHT LINAC are key to have im-
age-guided adaptative radiation therapy with protons [1].
The modular structure of the LIGHT system consists of:
A proton source injecting 40 keV protons with cur-
rents up to 300 uA and pulses up to 20 us at 200 Hz
repetition rate.
an RFQ (Radio Frequency Quadrupole) with a reso-
nant frequency of 749.48 MHz accelerating the pro-
tons up to 5 MeV. This is the fourth sub-harmonic of
the 2997.92 MHz LINAC frequency. The RFQ is fed
by an IOT powering system driven by the first LLRF
unit. Several signals are monitored in the LLRF from
the RFQ system: 4 probe signals from the RFQ cavity
and 4 pairs of directional couplers (forward and re-
flected power) in the RF network.
Four SCDTL (Side Coupled Drift Tube LINAC) struc-
tures powered by two klystrons at the main LIGHT fre-
quency of 2997.92 MHz. Passing through the four
SCDTL cavities, the beam will accelerate to 37.5
MeV. A SCDTL RF unit consists of a LLRF driving
power to a Modulator Klystron System (MKS) that
amplifies the 5 microseconds duration RF pulses to
MW levels. From each SCDTL RF unit, the associated
LLRF receives 4 probe signals (2 per cavity) and 3
pairs of directional couplers (forward and reflected)
signals in the RF network. The power is split from
main line and there is a coupler on each branch before
the SCDTL cavities.
Fifteen CCL (Coupled Cavity LINAC) structures pow-
ered by eleven klystrons at 2997.92 MHz, bringing the
beam energy up to 230 MeV. Four CCL RF units split
power between two CCL cavities and the other six are
fed directly from the MKS. In the first case, the asso-
ciated LLRF receives 4 probe signals (2 per cavity)
and 3 pairs of directional couplers (forward and re-
flected) signals in the RF network (as in the SCDTL
case); and in the latter case only 2 probe signals from
the cavity and 2 pairs of directional couplers are re-
ceived.
Figure 1 shows a schematic view of the LIGHT LINAC
design. The three types of RF accelerating cavities are
highlighted with the final energy at each section. The RF
peak power required for the RFQ, SCDTL and CCL units
is 400 kW, 8 MW and 45 MW respectively [2].
Figure 1: LIGHT system schematic with expected beam
energy reached after each type of RF accelerating cavity
section.
The LIGHT beam production system is currently be-
ing commissioned at AVO-ADAM Daresbury integration
site (DIS) in UK.
LLRF SYSTEM DESCRIPTION
Each high-power RF unit is fed by a LLRF device, which
makes a total of 14 LLRF units for the whole LIGHT
LINAC. The LLRF system has been built and delivered by
Instrumentation Technologies [2] and on top of the LLRF
device units, its composed of a Reference Master
________________________________________
d.soriano@avo-adam.com
摘要:

LOWLEVELRFSYSTEMOFTHELIGHTPROTONTHERAPYLINACD.SorianoGuillen†,G.DeMichele,S.Benedetti,Y.Ivanisenko,M.Cerv,AVO-ADAM,Meyrin,SwitzerlandAbstractTheLIGHT(LinacforImage-GuidedHadronTher-apy)projectwasinitiatedtodevelopamodularprotonac-celeratordeliveringbeamwithenergiesupto230MeVforcancertherapy.Themachi...

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