(19)
(11) EP 3 554 199 A8

(12) CORRECTED EUROPEAN PATENT APPLICATION
Note: Bibliography reflects the latest situation

(15) Correction information:
Corrected version no 1 (W1 A1)

(48) Corrigendum issued on:
08.01.2020 Bulletin 2020/02

(43) Date of publication:
16.10.2019 Bulletin 2019/42

(21) Application number: 18167210.6

(22) Date of filing: 13.04.2018
(51) International Patent Classification (IPC): 
H05H 9/00(2006.01)
H05H 7/00(2006.01)
(84) Designated Contracting States:
AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR
Designated Extension States:
BA ME
Designated Validation States:
KH MA MD TN

(71) Applicants:
  • ADAM S.A.
    1217 Meyrin (CH)
  • Università degli studi di Bergamo
    24129 Bergamo (IT)

(72) Inventors:
  • CALDARA, Michele
    CH-1202 Geneve (CH)
  • GALIZZI, Francesco
    I-24016 San Pellegrino Terme (IT)
  • JEFF, Adam
    F-01210 Ferney Voltaire (FR)

(74) Representative: Vanzini, Christian et al
Jacobacci & Partners S.p.A. Corso Emilia 8
10152 Torino
10152 Torino (IT)

   


(54) BEAM ENERGY MEASUREMENT SYSTEM


(57) A time-of-flight (TOF) measurement system for measuring energy of a pulsed hadron beam, wherein each pulse of the beam is structured into a series of bunches (B) of charged particles, said bunches being repeated according to a repetition rate of the order of magnitude of radiofrequency. The system comprises
a first detector (1), a second detector (2) and a third detector (3) arranged along a beam path (10), each of the detectors being configured to detect the passage of a bunch (B) of charged particles and provide an output signal (vPP,1, vPP,2, vPP,3) dependent on phase of the detected bunch (B), wherein the second detector (2) is spaced apart from the first detector (1) by a first distance (L12) and wherein the third detector (3) is spaced apart from the second detector (2) by a second distance (L23), wherein the first distance is set out in such a way as that time of flight (t12) of the bunch (B) from the first detector (1) to the second detector (2) is approximately equal to, or lower than a repetition period (TRFQ) of the bunches (B), and wherein the second distance is set out in such a way as that time of flight (T23) of the bunch (B) from the second detector (2) to the third detector (3) is greater than a multiple of the repetition period (TRFQ) of the bunches (B), and
a processing unit (7) configured to
a) calculate phase shifts (Δϕ12, Δϕ13, Δϕ23) between the output signals (vPP,1, vPP,2, vPP,3) of the detectors (1, 2, 3), and
b) calculate energy (E) of the pulse based on the calculated phase shifts.