Gamma-ray emission by proton beam interaction with injected Boron atoms for medical imaging. Giada Petringa - Laboratori Nazionali del Sud -

Similar documents
Radiation Quantities and Units

College Physics B - PHY2054C

Prompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research

Today, I will present the first of two lectures on neutron interactions.

neutrons in the few kev to several MeV Neutrons are generated over a wide range of energies by a variety of different processes.

Nuclear Spectroscopy: Radioactivity and Half Life

Neutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321

Physics of particles. H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School

Medical Neutron Science

Final Exam. Evaluations. From last time: Alpha radiation. Beta decay. Decay sequence of 238 U

Isotopes and Radioactive Decay

Simulations in Radiation Therapy

CHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH

Project Memorandum. N N o. = e (ρx)(µ/ρ) (1)

and have low penetrating power) Alpha particles are released through alpha decay. Beta Particles: An electron that comes from a nucleus through

Secondary Particles Produced by Hadron Therapy

Lecture PowerPoint. Chapter 31 Physics: Principles with Applications, 6 th edition Giancoli

Bhas Bapat MOL-PH Seminar October Ion Matter Interactions and Applications

Monte Carlo Simulation concerning Particle Therapy

INTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017

Interactions of Particulate Radiation with Matter. Purpose. Importance of particulate interactions

Secondary Neutron Dose Measurement for Proton Line Scanning Therapy

RADIOACTIVITY. Nature of Radioactive Emissions

Unit 08 Nuclear Structure. Unit 08 Nuclear Structure Slide 1

Using Prompt gamma ray emission to address uncertainties in proton therapy

Lecture Outlines Chapter 32. Physics, 3 rd Edition James S. Walker

Some nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle

12/1/17 OUTLINE KEY POINTS ELEMENTS WITH UNSTABLE NUCLEI Radioisotopes and Nuclear Reactions 16.2 Biological Effects of Nuclear Radiation

Neutron Dose near Spent Nuclear Fuel and HAW after the 2007 ICRP Recommendations

Radiation safety of the Danish Center for Proton Therapy (DCPT) Lars Hjorth Præstegaard Dept. of Medical Physics, Aarhus University Hospital

Nuclear Physics. AP Physics B

General Physics (PHY 2140)

Year 12 Notes Radioactivity 1/5

General Physics (PHY 2140)

Unit 3: Chemistry in Society Nuclear Chemistry Summary Notes

LET! (de / dx) 1 Gy= 1 J/kG 1Gy=100 rad. m(kg) dose rate

Atomic & Nuclear Physics

Analyzing the Sensitivity of a Hard X Ray Detector Using Monte Carlo Methods

Nuclear Physics. Chapter 43. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman

Introduction to Radiological Sciences Neutron Detectors. Theory of operation. Types of detectors Source calibration Survey for Dose

Physics of Particle Beams. Hsiao-Ming Lu, Ph.D., Jay Flanz, Ph.D., Harald Paganetti, Ph.D. Massachusetts General Hospital Harvard Medical School

Properties of the nucleus. 8.2 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus

Chapter 10. Table of Contents. Section 1 What Is Radioactivity? Section 2 Nuclear Fission and Fusion. Section 3 Nuclear Radiation Today

A Monte Carlo Study of the Relationship between the Time. Structures of Prompt Gammas and in vivo Radiation Dose in.

Dosimetry. Sanja Dolanski Babić May, 2018.

Physics (B): Physics in Context

Lecture PowerPoints. Chapter 31 Physics: Principles with Applications, 7th edition Giancoli

RADIOACTIVITY. An atom consists of protons, neutrons and electrons.

INTRODUCTION TO IONIZING RADIATION (Attix Chapter 1 p. 1-5)

ZX or X-A where X is chemical symbol of element. common unit: [unified mass unit = u] also known as [atomic mass unit = amu] or [Dalton = Da]

M. Martišíková 1,3, C. Granja 2, J. Jakůbek 2, B. Hartmann 1,3, K. Gwosch 1, P. Soukup 2 and O. Jäkel 1,3,5

Nuclear Chemistry. Nuclear Terminology

There are 82 protons in a lead nucleus. Why doesn t the lead nucleus burst apart?

Introduction to neutron sources

INTERACTIONS OF RADIATION WITH MATTER

Radiosensitisation by nanoparticles in Proton therapy

CHAPTER 12 TEST REVIEW

Radiation and Radioactivity. PHYS 0219 Radiation and Radioactivity

Chapter 25. Nuclear Chemistry. Types of Radiation

Introduction to Accelerator Physics Part 1

β and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Final Exam Surveys New material Example of β-decay Beta decay Y + e # Y'+e +

RADIOCHEMICAL METHODS OF ANALYSIS

Measurement of secondary particle production induced by particle therapy ion beams impinging on a PMMA target

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons

Radioactive nuclei. From Last Time. Biological effects of radiation. Radioactive decay. A random process. Radioactive tracers. e r t.

III. Proton-therapytherapy. Rome SB - 2/5 1

The Case of Melting Ice

Table O: Symbols Used in Nuclear Chemistry

Interactions with Matter Photons, Electrons and Neutrons

New targets for enhancing pb nuclear fusion reaction at the PALS facility

State the position of protons, neutrons and electrons in the atom

Applied Nuclear Physics (Fall 2006) Lecture 21 (11/29/06) Detection of Nuclear Radiation: Pulse Height Spectra

CHAPTER 7 TEST REVIEW

The Feasibility of Proton Boron Capture Therapy

Applied Nuclear Physics at the NUS Physics Department

WHAT IS IONIZING RADIATION

Physics of Novel Radiation Modalities Particles and Isotopes. Todd Pawlicki, Ph.D. UC San Diego

Introduction to Ionizing Radiation

6 Neutrons and Neutron Interactions

Nuclear forces and Radioactivity. Two forces are at work inside the nucleus of an atom

Properties of the nucleus. 9.1 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus

CHARGED PARTICLE INTERACTIONS

Photonuclear Reaction Cross Sections for Gallium Isotopes. Serkan Akkoyun 1, Tuncay Bayram 2

Nuclear Physics. PHY232 Remco Zegers Room W109 cyclotron building.

Chapter 21 Nuclear Chemistry: the study of nuclear reactions

Alta Chemistry CHAPTER 25. Nuclear Chemistry: Radiation, Radioactivity & its Applications

ESTIMATION OF 90 SCATTERING COEFFICIENT IN THE SHIELDING CALCULATION OF DIAGNOSTIC X-RAY EQUIPMENT

P7 Radioactivity. Student Book answers. P7.1 Atoms and radiation. Question Answer Marks Guidance

QUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter


Nuclear Physics and Astrophysics

Queen s University PHYS 352

Particles involved proton neutron electron positron gamma ray 1

ICTP-IAEA Joint Workshop on Nuclear Data for Science and Technology: Medical Applications. 30 September - 4 October, 2013

Accelerators for Hadrontherapy -- Present & Future --

Page 1. ConcepTest Clicker Questions Chapter 32. Physics, 4 th Edition James S. Walker

PS-21 First Spring Institute say : Teaching Physical Science. Radioactivity

L 37 Modern Physics [3]

11/19/2014. Chapter 3: Interaction of Radiation with Matter in Radiology and Nuclear Medicine. Nuclide Families. Family Nuclides with Same: Example

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of?

Transcription:

Gamma-ray emission by proton beam interaction with injected Boron atoms for medical imaging Giada Petringa - Laboratori Nazionali del Sud - Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 1

high LET!! Hadrontherapy: for and against 12C-ions present some advantages over protons potential radiobiological advantages include greater RBE for killing putatively radioresistant cancer cells! Protons have been traditionally regarded as only slightly more biologically effective than photons RBE=1.1 nuclear fragmentation reactions incurred by the primary beam partially spoil the 12C superior dose distribution, depositing unwanted dose behind the target volume, as opposed to the sharp dose fall-off that characterizes protons Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 2

The Proton-Boron fusion therapy D.-K. Yoon et al, Application of proton boron fusion reaction to radiation therapy: A Monte Carlo simulation study, Applied Physics Letters 105, 223507 (2014); L. Giuffrida et al., Prompt gamma ray diagnostics and enhanced hadron-therapy using neutron-free nulcear reactions, AIP Advances (Submitted) G.A.P. Cirrone et al., First evidence of enhancement of proton biological effectiveness via p + 11 B -> 3a nuclear reaction, Nature Communication (Submitted) Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 3

The Proton-Boron fusion therapy D.-K. Yoon et al, Application of proton boron fusion reaction to radiation therapy: A Monte Carlo simulation study, Applied Physics Letters 105, 223507 (2014); L. Giuffrida et al., Prompt gamma ray diagnostics and enhanced hadron-therapy using neutron-free nulcear reactions, AIP Advances (Submitted) G.A.P. Cirrone et al., First evidence of enhancement of proton biological effectiveness via p + 11 B -> 3a nuclear reaction, Nature Communication (Submitted) Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 3

The Proton-Boron fusion therapy D.-K. Yoon et al, Application of proton boron fusion reaction to radiation therapy: A Monte Carlo simulation study, Applied Physics Letters 105, 223507 (2014); L. Giuffrida et al., Prompt gamma ray diagnostics and enhanced hadron-therapy using neutron-free nulcear reactions, AIP Advances (Submitted) G.A.P. Cirrone et al., First evidence of enhancement of proton biological effectiveness via p + 11B -> 3a nuclear reaction, Nature Communication (Submitted) Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 3

The Proton-Boron fusion therapy Many experimental evidences show that it proceeds predominantly by a sequential decay through the ground or first excited states of 8 Be: M. C. Spraker et al, The 11B(p,a)8Be => a + a and the 11B(a,a)11B Reactions at Energies Below 5.4 MeV, J Fusion Energy (2012) Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 4

Gamma prompt from proton-boron fusion reaction D. -K. Yoon et al, Application of proton boron fusion reaction ti radiation therapy: A Monte Carlo simulation study Applied Physics Letters 105, 223507 (2014); 1. Gamma prompt from the proton boron fusion reaction 2. Boron target at its nominal density of 2.08 gr/cm 3 3. The background contribute from the main components of the biological tissue Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 5

Gamma prompt from proton-boron fusion reaction Investigation main aim: Investigate the configuration proposed Verifying its real feasibility Propose a new approach still maintaining the therapeutical Boron role Experimental run Talys simulation code Copper atoms Patent submitted Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 6

Experimental run @ LNS - INFN Experimental set-up GEM series model 70220-S zero degree experimental hall 62 MeV protons beam Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 7

Experimental run @ LNS - INFN Experimental set-up GEM series model 70220-S Target The Boron targets consisted of two Mylar cylinders, filled with a pressed 11 B and 10 B powder. Resulted density was measured to be 1.15 gr/cm 3. Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 7

11B and 10B spectrum Fixed the acquisition time at 500 sec, each spectra has been normalized for the incident beam current Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 8

11B and 10B spectrum Fixed the acquisition time at 500 sec, each spectra has been normalized for the incident beam current Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 8

11B and 10B spectrum 429 KeV 718 KeV Talys -1.6 1.022 MeV 1.430 MeV Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 9

Talys validation code In order to validate the code, the gamma yield, obtained by the simulation, has been compared to the intensity of each line experimentally measured The percentage ratio of the integral calculated as each peak for the two isotopes has been compared Two data sets show inconsistencies smaller than 15% Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 10

Gamma rays emission in a typical concentration the gamma-prompts levels emitted from p- 11 B interaction, are the same generated by the interaction of protons with the main constituents of the Human body => 12 C and 16 O Gamma rays energies by proton interaction with major elements in human tissues B. Kozlovsky et al., Astrophysics J., Suppl. Ser. 141. (2002) Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 11

Gamma rays emission in a typical concentration Is the boron concentration sufficient? a typical concentration of B nuclei that can reach a tumor, ensuring the minimal cell toxicity, is the order of 10-5 g/cm 3, four order of magnitude less than the density of carbon ions and oxygen in the human tissue (0.18 g/cm 3 and 0.65 g/cm 3 respectively) Scaling the cross section for the biological tissue density and for a typical BSH concentration, the gamma ray emission by the background are 10 3 times higher of the boron signal! Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 12

Gamma rays emission in a typical concentration Is the boron concentration sufficient? a typical concentration of B nuclei that can reach a tumor, ensuring the minimal cell toxicity, is the order of 10-5 g/cm 3, four order of magnitude less than the density of carbon ions and oxygen in the human tissue (0.18 g/cm 3 and 0.65 g/cm 3 respectively) Scaling the cross section for the biological tissue density and for a typical BSH concentration, the gamma ray emission by the background are 10 3 times higher of the boron signal! Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 12

The copper atoms for the imaging In order to improve the imaging capabilities, still maintaining the Boron therapeutic role, we propose to use the atoms of natural Copper bound by a dipyrromethene BodiPy to boron atoms Nuclear Reaction 1320 KeV peak A good candidate for the gamma prompt imaging! Goal! ATSM BodiPy Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 13

Thank you for your attention! Giada Petringa Topical Seminar on Innovative Particle and Radiation Detector - 2016 14