introduction : imaging antiprotons introduction : imaging antiprotons first results of real time...

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INTRODUCTION : Imaging INTRODUCTION : Imaging antiprotons antiprotons First results of real time imaging of the high energy gamma rays coming from antiproton annihilation with the protons in the nuclei of a biological cell are presented. These results are obtained with IRIS, a patented amorphous silicon high resolution detector. We are able to demonstrate the potential for imaging the point of annihilation. The main application is the imaging of the proton-antiproton annihilation for medical purposes, e.g. cancer treatment on a biological cell level. Real Time Imaging of Antiproton Annihilation for Medical Real Time Imaging of Antiproton Annihilation for Medical Applications Applications Zlatko Dimcovski 1,3 , Sylvie Chapuy 2,3 , Michael Doser 1 , Dragan Hajdukovic 1,4 , Mimoza Ristova 3,6 , Marc Dimcovski 2 , Michael H. Holzscheiter 5 , Carl Maggiore 5 , Nicolas Rabiller 2 1 CERN, Geneva, 2 BioScan SA, Geneva, 3 University of Geneva, 4 University of Podgorica, Montenegro, 5 Pbar Labs, Santa Fe, USA, 6 PMF, University Kiril &Metodij, Skopje, Macedonia, Antiprotons beam Test object : slit in lead bricks IRIS detector IRIS & beam control systems AD experiment room AD control room IS detector for high energy gamma rays : S detector for high energy gamma rays : THE RESULTS : THE RESULTS : Gamma rays were visible within Gamma rays were visible within the slits. the slits. The slit is visible in the medial part of the image. D istribution w ith 1 cm lead bricks slit 3000 4000 5000 6000 7000 8000 9000 10000 0 10 20 30 40 50 60 70 80 90 P ixels Arbitrary un W ith beam Withoutbeam Distribution histogram. IRIS pitch size 750 µm. FWMH : ~11 mm. Lead bricks slit of ~1 cm thick THE SETUP THE SETUP Data were taken at the AD, antiproton decelerator facility at CERN. An external beam of 47.8 MeV antiprotons was deposited on a biological target. The antiprotons were delivered in pulses of approximately 3 x 10 7 particles during 200 nanoseconds at 90 seconds intervals. The high energy gamma rays, ~10 8 into 4 steradians, were produced by the proton- antiproton interaction in the biological target. The gamma rays have an energy distribution with a peak about 150 MeV. The IRIS detector was placed 50 cm away from the target, with lead shielding protection for the on-line electronics. The tests objects were slits between lead bricks, placed between the stopping point of antiprotons in the target and the detector. Transistor Photodiode D etection m atrix Electronic readout lecture Pow ersupply Data lines R aw driver O utput signal Characteristics of IRIS Characteristics of IRIS : : Based on large area pixel matrix, thin film amorphous silicon technology, Energy range : up to several hundreds MeV for gamma- rays, Dynamic visualization, High frame rate : up to 10 images per second, Active area : 20 cm x 20 cm or 41 cm x 41 cm, Pixel size : 750 µm x 750 µm, 400 µm x 400 µm down to 50 µm x 50 µm, Wide dynamic range, ADC resolution : 16 bits (65536 gray levels), IRIS-View, software package for PC for acquisition, visualization, data storage and tele-medecine. FUTURE APPLICATION : Antiprotons for cancer treatment FUTURE APPLICATION : Antiprotons for cancer treatment The biological effects of photons and particles of ordinary matter are well known and widely used in cancer therapy. Photon (x- ray) therapy has been used for almost one century. Proton cancer therapy exists worldwide and a few heavier ion therapy centers are active. Presently, production of positrons and antiprotons is a well known technique. Now, with CERN being the world leader in antiproton physics, the time has come when a study of the biological effects of antiprotons is reality. Antiprotons, as charged particles, are easy to focus with a corresponding electromagnetic optics. The annihilation phenomenon could be controlled within the 3D space of the biological target, or the human body in the future, which would be the breakthrough in radiotherapy. When the antiprotons slow down to a certain critical velocity, they annihilate, producing a variety of particles, thus making “implose” the biological cell. Thus, the annihilation could be considered as a breakthrough way for “implantation” of particle sources inside the tumour with a 3D precision. The question that follows is: what are the effects of ‘implanted’ emitters. The relatively low energy particles, created after an annihilation are expected to deposit biologically effective high LET (Linear Energy Transfer) radiation in the immediate vicinity of the annihilation point. After leaving the body, the high-energy pions, muons, and gamma-rays could be used for real time imaging. CONCLUSION : CONCLUSION : These first results are very promising. These first results are very promising. Our aim is to set-up the foundations for a cancer therapy with antiprotons. Our aim is to set-up the foundations for a cancer therapy with antiprotons. Gamma rays scintillator a-Si photodiode TFT readou t device Real time readout electronics Digital data output Electrons Visible light photons pions Antiprotons beam Tumor muons gammas at EPS 13 (European Physical Society), Bern, Switzerland, July 2005

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Page 1: INTRODUCTION : Imaging antiprotons INTRODUCTION : Imaging antiprotons First results of real time imaging of the high energy gamma rays coming from antiproton

  INTRODUCTION : Imaging antiprotonsINTRODUCTION : Imaging antiprotonsFirst results of real time imaging of the high energy gamma rays coming from antiproton annihilation with the protons in the nuclei of a biological cell are presented. These results are obtained with IRIS, a patented amorphous silicon high resolution detector. We are able to demonstrate the potential for imaging the point of annihilation.

The main application is the imaging of the proton-antiproton annihilation for medical purposes, e.g. cancer treatment on a biological cell level.

Real Time Imaging of Antiproton Annihilation for Medical ApplicationsReal Time Imaging of Antiproton Annihilation for Medical ApplicationsZlatko Dimcovski1,3, Sylvie Chapuy2,3, Michael Doser1, Dragan Hajdukovic1,4, Mimoza Ristova3,6,

Marc Dimcovski2, Michael H. Holzscheiter5, Carl Maggiore5, Nicolas Rabiller2

1CERN, Geneva, 2BioScan SA, Geneva, 3University of Geneva, 4University of Podgorica, Montenegro, 5Pbar Labs, Santa Fe, USA, 6PMF, University Kiril &Metodij, Skopje, Macedonia,

Antiprotons beam

Test object : slit in lead bricks

IRIS detector

IRIS & beam control systems

AD experiment room AD control room

IRIS detector for high energy gamma rays :IRIS detector for high energy gamma rays :

THE RESULTS : THE RESULTS : Gamma rays were visible within the slits.Gamma rays were visible within the slits.

The slit is visible in the medial part of the image.

Distribution with 1 cm lead bricks slit

3000

4000

5000

6000

7000

8000

9000

10000

0 10 20 30 40 50 60 70 80 90Pixels

Arb

itra

ry u

nit

s

With beam

Without beam

Distribution histogram.IRIS pitch size 750 µm.

FWMH : ~11 mm.

Lead bricks slit of ~1 cm thick

THE SETUPTHE SETUPData were taken at the AD, antiproton decelerator facility at CERN.  An external beam of 47.8 MeV antiprotons was deposited on a biological target.  The antiprotons were delivered in pulses of approximately 3 x 107 particles during 200 nanoseconds at 90 seconds intervals. The high energy gamma rays, ~108 into 4 steradians, were produced by the proton-antiproton interaction in the biological target. The gamma rays have an energy distribution with a peak about 150 MeV. The IRIS detector was placed 50 cm away from the target, with lead shielding protection for the on-line electronics.

The tests objects were slits between lead bricks, placed between the stopping point of antiprotons in the target and the detector.

Transistor

Photodiode

Detection matrix

Electronic readout lecture

Power supply Data lines

Ra

w d

riv

er

Output signal

Characteristics of IRISCharacteristics of IRIS :: Based on large area pixel matrix, thin film amorphous silicon technology,

Energy range : up to several hundreds MeV for gamma-rays,

Dynamic visualization,

High frame rate : up to 10 images per second,

Active area : 20 cm x 20 cm or 41 cm x 41 cm,

Pixel size : 750 µm x 750 µm, 400 µm x 400 µm

down to 50 µm x 50 µm,

Wide dynamic range,

ADC resolution : 16 bits (65536 gray levels),

IRIS-View, software package for PC for acquisition,

visualization, data storage and tele-medecine.

FUTURE APPLICATION : Antiprotons for cancer treatmentFUTURE APPLICATION : Antiprotons for cancer treatmentThe biological effects of photons and particles of ordinary matter are well known and widely used in cancer therapy. Photon (x-ray) therapy has been used for almost one century. Proton cancer therapy exists worldwide and a few heavier ion therapy centers are active.

Presently, production of positrons and antiprotons is a well known technique. Now, with CERN being the world leader in antiproton physics, the time has come when a study of the biological effects of antiprotons is reality.

Antiprotons, as charged particles, are easy to focus with a corresponding electromagnetic optics. The annihilation phenomenon could be controlled within the 3D space of the biological target, or the human body in the future, which would be the breakthrough in radiotherapy. When the antiprotons slow down to a certain critical velocity, they annihilate, producing a variety of particles, thus making “implose” the biological cell.

Thus, the annihilation could be considered as a breakthrough way for “implantation” of particle sources inside the tumour with a 3D precision. The question that follows is: what are the effects of ‘implanted’ emitters.

The relatively low energy particles, created after an annihilation are expected to deposit biologically effective high LET (Linear Energy Transfer) radiation in the immediate vicinity of the annihilation point. After leaving the body, the high-energy pions, muons, and gamma-rays could be used for real time imaging.

CONCLUSION : CONCLUSION : These first results are very promising.These first results are very promising.Our aim is to set-up the foundations for a cancer therapy with antiprotons. Our aim is to set-up the foundations for a cancer therapy with antiprotons.

Gamma rays

scintillator

a-Si photodiode TFT

readout device

Real time readout electronics

Digital data output

Electrons

Visible light

photons

pions

Antiprotons beam

Tumor

muons

gammas

Presented at EPS 13 (European Physical Society), Bern, Switzerland, July 2005