Spyros Manolopoulos

Dr. Spyros Manolopoulos

1. School of Physics, University of Warwick, Coventry, CV4 7AL, UK
+2
orcid

Research Focus & Metrics

Academic Career Length

32Years (1995-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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22 September 2008 in Medical Physics
Verified
Journal Article
Closed access
EPE. Pappas
E. Pappas
TMT. G. Maris
T. G. Maris
FZF. Zacharopoulou
F. Zacharopoulou
APA. Papadakis
A. Papadakis
SMSpyros Manolopoulos
Spyros Manolopoulos
CWC. Wojnecki
C. Wojnecki

1 May 2014 in Physics in Medicine & Biology
Verified
Journal Article
Closed access
GPG Poludniowski
G Poludniowski
Nigel M. AllinsonNigel M. Allinson
Nigel M. Allinson
TAT Anaxagoras
T Anaxagoras
MEM Esposito
M Esposito
SGS Green
S Green
PEPhilip M evans
Philip M evans
Despite the early recognition of the potential of proton imaging to assist proton therapy (Cormack 1963 J. Appl. Phys. 34 2722), the modality is still removed from clinical practice, with various approaches in development. For proton-counting radiography applications such as computed tomography (CT), the water-equivalent-path-length that each proton has travelled through an imaged object must be inferred. Typically, scintillator-based technology has been used in various energy/range telescope designs. Here we propose a very different alternative of using radiation-hard CMOS active pixel sensor technology. The ability of such a sensor to resolve the passage of individual protons in a therapy beam has not been previously shown. Here, such capability is demonstrated using a 36 MeV cyclotron beam (University of Birmingham Cyclotron, Birmingham, UK) and a 200 MeV clinical radiotherapy beam (iThemba LABS, Cape Town, SA). The feasibility of tracking individual protons through multiple CMOS layers is also demonstrated using a two-layer stack of sensors. The chief advantages of this solution are the spatial discrimination of events intrinsic to pixelated sensors, combined with the potential provision of information on both the range and residual energy of a proton. The challenges in developing a practical system are discussed.

1 March 2003 in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Journal Article
Closed access
RTR Turchetta
R Turchetta
MFM French
M French
SMSpyros Manolopoulos
Spyros Manolopoulos
MTM Tyndel
M Tyndel
PAP Allport
P Allport
MRM Raymond
M Raymond

1 August 2005 in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Journal Article
Closed access
HSHoward Stone
Howard Stone
MTM.G. Tucker
M.G. Tucker
YGY. Le Godec
Y. Le Godec
FMF.M. Méducin
F.M. Méducin
ECE.R. Cope
E.R. Cope
MDM.T. Dove
M.T. Dove

1 June 1999 in IEEE Transactions on Nuclear Science
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Journal Article
Closed access
RIR. Irsigler
R. Irsigler
JAJ. Andersson
J. Andersson
JAJ. Alverbro
J. Alverbro
JBJ. Borglind
J. Borglind
CFC. Frojdh
C. Frojdh
KSK. Smith
K. Smith

25 October 2016 in Medical Physics
Verified
Journal Article
Open access
PDF file
JTJ. T. Taylor
J. T. Taylor
GPG. Poludniowski
G. Poludniowski
TPT. Price
T. Price
CWC. Waltham
C. Waltham
PAP. P. Allport
P. P. Allport
NAN. M. Allinson
N. M. Allinson
Purpose: Radiography and tomography using proton beams promise benefit to image guidance and treatment planning for proton therapy. A novel proton tracking detector is described and experimental demonstrations at a therapy facility are reported. A new type of proton CT reconstructing relative “scattering power” rather than “stopping power” is also demonstrated. Notably, this new type of imaging does not require the measurement of the residual energies of the protons.Methods: A large area, silicon microstrip tracker with high spatial and temporal resolution has been developed by the Proton Radiotherapy Verification and Dosimetry Applications consortium and commissioned using beams of protons at iThemba LABS, Medical Radiation Department, South Africa. The tracker comprises twelve planes of silicon developed using technology from high energy physics with each plane having an active area of ∼10 × 10 cm segmented into 2048 microstrips. The tracker is organized into four separate units each containing three detectors at 60° to one another creating an x‐u‐v coordinate system. Pairs of tracking units are used to reconstruct vertices for protons entering and exiting a phantom containing tissue equivalent inserts. By measuring the position and direction of each proton before and after the phantom, the nonlinear path for each proton through an object can be reconstructed.Results: Experimental results are reported for tracking the path of protons with initial energies of 125 and 191 MeV. A spherical phantom of 75 mm diameter was imaged by positioning it between the entrance and exit detectors of the tracker. Positions and directions of individual protons were used to create angular distributions and 2D fluence maps of the beam. These results were acquired for 36 equally spaced projections spanning 180°, allowing, for the first time, an experimental CT image based upon the relative scattering power of protons to be reconstructed.Conclusions: Successful tracking of protons through a thick target (phantom) has demonstrated that the tracker discussed in this paper can provide the precise directional information needed to perform proton radiography and tomography. When synchronized with a range telescope, this could enable the reconstruction of proton CT images of stopping power. Furthermore, by measuring the deflection of many protons through a phantom, it was demonstrated that it is possible to reconstruct a new kind of CT image (scattering power) based upon this tracking information alone.