Intensity Modulated Proton Therapy Backgrounder
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Five Common Particles
The Five Common Particles The world around you consists of only three particles: protons, neutrons, and electrons. Protons and neutrons form the nuclei of atoms, and electrons glue everything together and create chemicals and materials. Along with the photon and the neutrino, these particles are essentially the only ones that exist in our solar system, because all the other subatomic particles have half-lives of typically 10-9 second or less, and vanish almost the instant they are created by nuclear reactions in the Sun, etc. Particles interact via the four fundamental forces of nature. Some basic properties of these forces are summarized below. (Other aspects of the fundamental forces are also discussed in the Summary of Particle Physics document on this web site.) Force Range Common Particles It Affects Conserved Quantity gravity infinite neutron, proton, electron, neutrino, photon mass-energy electromagnetic infinite proton, electron, photon charge -14 strong nuclear force ≈ 10 m neutron, proton baryon number -15 weak nuclear force ≈ 10 m neutron, proton, electron, neutrino lepton number Every particle in nature has specific values of all four of the conserved quantities associated with each force. The values for the five common particles are: Particle Rest Mass1 Charge2 Baryon # Lepton # proton 938.3 MeV/c2 +1 e +1 0 neutron 939.6 MeV/c2 0 +1 0 electron 0.511 MeV/c2 -1 e 0 +1 neutrino ≈ 1 eV/c2 0 0 +1 photon 0 eV/c2 0 0 0 1) MeV = mega-electron-volt = 106 eV. It is customary in particle physics to measure the mass of a particle in terms of how much energy it would represent if it were converted via E = mc2. -
Proton Stereotactic Body Radiation Therapy for Liver Metastases— Results of 5-Year Experience for 81 Hepatic Lesions
1760 Original Article Proton stereotactic body radiation therapy for liver metastases— results of 5-year experience for 81 hepatic lesions Alex R. Coffman1, Daniel C. Sufficool2, Joseph I. Kang1, Chung-Tsen Hsueh3, Sasha Swenson4, Patrick Q. McGee4, Gayathri Nagaraj3, Baldev Patyal1, Mark E. Reeves5, Jerry D. Slater1, Gary Y. Yang1 1Department of Radiation Oncology, Loma Linda University Medical Center, Loma Linda, CA, USA; 2Department of Radiation Oncology, Kettering Health Network, Kettering, OH, USA; 3Department of Medical Oncology, Loma Linda University Medical Center, Loma Linda, CA, USA; 4Loma Linda University School of Medicine, Loma Linda, CA, USA; 5Department of Surgical Oncology, Loma Linda University Medical Center, Loma Linda, CA, USA Contributions: (I) Conception and design: GY Yang; (II) Administrative support: B Patyal, JD Slater, GY Yang; (III) Provision of study materials or patients: CT Hsueh, G Nagaraj, ME Reeves; (IV) Collection and assembly of data: AR Coffman, GY Yang; (V) Data analysis and interpretation: AR Coffman, GY Yang; (VI) Manuscript writing: All authors; (VII) Final approval of manuscript: All authors. Correspondence to: Alex R. Coffman, MD. Department of Radiation Oncology, Loma Linda University Medical Center, 11234 Anderson Street, Suite B121, Loma Linda, CA 92354, USA. Email: [email protected]. Background: To report on our institutional experience using Proton stereotactic body radiation therapy (SBRT) for patients with liver metastases. Methods: All patients with liver metastases treated with Proton SBRT between September 2012 and December 2017 were retrospectively analyzed. Local control (LC) and overall survival (OS) were estimated using the Kaplan-Meier method calculated from the time of completion of Proton SBRT. LC was defined according to Response Evaluation Criteria in Solid Tumors (RECIST) guidelines (version 1.1). -
An Analysis of Vertebral Body Growth After Proton Beam Therapy for Pediatric Cancer
cancers Article An Analysis of Vertebral Body Growth after Proton Beam Therapy for Pediatric Cancer Keiichiro Baba 1, Masashi Mizumoto 1,* , Yoshiko Oshiro 1,2, Shosei Shimizu 1 , Masatoshi Nakamura 1, Yuichi Hiroshima 1 , Takashi Iizumi 1, Takashi Saito 1, Haruko Numajiri 1, Kei Nakai 1 , Hitoshi Ishikawa 1,3, Toshiyuki Okumura 1, Kazushi Maruo 4 and Hideyuki Sakurai 1 1 Proton Medical Research Center, Department of Radiation Oncology, University of Tsukuba Hospital, Tsukuba, Ibaraki 305-8576, Japan; [email protected] (K.B.); [email protected] (Y.O.); [email protected] (S.S.); [email protected] (M.N.); [email protected] (Y.H.); [email protected] (T.I.); [email protected] (T.S.); [email protected] (H.N.); [email protected] (K.N.); [email protected] (H.I.); [email protected] (T.O.); [email protected] (H.S.) 2 Department of Radiation Oncology, Tsukuba Medical Center Hospital, Tsukuba, Ibaraki 305-8558, Japan 3 National Institutes for Quantum and Radiological Science and Technology, QST Hospital, Chiba 263-8555, Japan 4 Department of Clinical Trial and Clinical Epidemiology, Faculty of Medicine, University of Tsukuba, Tsukuba, Ibaraki 305-8575, Japan; [email protected] * Correspondence: [email protected]; Tel.: +81-29-853-7100; Fax: +81-29-853-7102 Simple Summary: Radiotherapy has a key role in treatment of pediatric cancer and has greatly improved survival in recent years. However, vertebrae are often included in the irradiated area, and this may affect growth after treatment. -
Particle Accelerators and Detectors for Medical Diagnostics and Therapy Arxiv:1601.06820V1 [Physics.Med-Ph] 25 Jan 2016
Particle Accelerators and Detectors for medical Diagnostics and Therapy Habilitationsschrift zur Erlangung der Venia docendi an der Philosophisch-naturwissenschaftlichen Fakult¨at der Universit¨atBern arXiv:1601.06820v1 [physics.med-ph] 25 Jan 2016 vorgelegt von Dr. Saverio Braccini Laboratorium f¨urHochenenergiephysik L'aspetto pi`uentusiasmante della scienza `eche essa incoraggia l'uomo a insistere nei suoi sogni. Guglielmo Marconi Preface This Habilitation is based on selected publications, which represent my major sci- entific contributions as an experimental physicist to the field of particle accelerators and detectors applied to medical diagnostics and therapy. They are reprinted in Part II of this work to be considered for the Habilitation and they cover original achievements and relevant aspects for the present and future of medical applications of particle physics. The text reported in Part I is aimed at putting my scientific work into its con- text and perspective, to comment on recent developments and, in particular, on my contributions to the advances in accelerators and detectors for cancer hadrontherapy and for the production of radioisotopes. Dr. Saverio Braccini Bern, 25.4.2013 i ii Contents Introduction 1 I 5 1 Particle Accelerators and Detectors applied to Medicine 7 2 Particle Accelerators for medical Diagnostics and Therapy 23 2.1 Linacs and Cyclinacs for Hadrontherapy . 23 2.2 The new Bern Cyclotron Laboratory and its Research Beam Line . 39 3 Particle Detectors for medical Applications of Ion Beams 49 3.1 Segmented Ionization Chambers for Beam Monitoring in Hadrontherapy 49 3.2 Proton Radiography with nuclear Emulsion Films . 62 3.3 A Beam Monitor Detector based on doped Silica Fibres . -
Proton Therapy ACKNOWLEDGEMENTS
AMERICAN BRAIN TUMOR ASSOCIATION Proton Therapy ACKNOWLEDGEMENTS ABOUT THE AMERICAN BRAIN TUMOR ASSOCIATION Founded in 1973, the American Brain Tumor Association (ABTA) was the first national nonprofit organization dedicated solely to brain tumor research. For over 40 years, the Chicago-based ABTA has been providing comprehensive resources that support the complex needs of brain tumor patients and caregivers, as well as the critical funding of research in the pursuit of breakthroughs in brain tumor diagnosis, treatment and care. To learn more about the ABTA, visit www.abta.org. We gratefully acknowledge Anita Mahajan, Director of International Development, MD Anderson Proton Therapy Center, director, Pediatric Radiation Oncology, co-section head of Pediatric and CNS Radiation Oncology, The University of Texas MD Anderson Cancer Center; Kevin S. Oh, MD, Department of Radiation Oncology, Massachusetts General Hospital; and Sridhar Nimmagadda, PhD, assistant professor of Radiology, Medicine and Oncology, Johns Hopkins University, for their review of this edition of this publication. This publication is not intended as a substitute for professional medical advice and does not provide advice on treatments or conditions for individual patients. All health and treatment decisions must be made in consultation with your physician(s), utilizing your specific medical information. Inclusion in this publication is not a recommendation of any product, treatment, physician or hospital. COPYRIGHT © 2015 ABTA REPRODUCTION WITHOUT PRIOR WRITTEN PERMISSION IS PROHIBITED AMERICAN BRAIN TUMOR ASSOCIATION Proton Therapy INTRODUCTION Brain tumors are highly variable in their treatment and prognosis. Many are benign and treated conservatively, while others are malignant and require aggressive combinations of surgery, radiation and chemotherapy. -
Key Words: 1. Proton: Found Inside the Nucleus of an Atom, Have a Positive Charge 2. Electron: Found in Rings Orbiting the Nucle
Nucleus development Particle Charge Mass This experiment allowed Rutherford to replace the plum pudding Electron -1 0 model with the nuclear model – the Proton +1 1 atom was mainly empty space with a small positively charged nucleus Neutron 0 1 Element All the same type of atom Alpha particle scattering Geiger and Key words: Marsden 1. Proton: Found inside the nucleus of an atom, have a positive charge Compound fired positively-charged alpha More than one type 2. Electron: Found in rings orbiting the nucleus, have a negative charge particles at gold foil. This showed of atom chemically that the mas of an atom was 3. Neutrons: Found in the nucleus of an atom, have no charge bonded together concentrated in the centre, it was 4. Nucleus: The centre of an atom, made up of protons and neutrons positively charged too 5. Mass number: The mass of the atom, made up of protons and neutrons Mixture Plum pudding 6. Atomic number: The number of protons in an atom More than one type After the electron 7. Element: All the same type of atom chemically bonded together of element or was discovered, 8. Compound: More than one type of atom chemically bonded together compound not chemically bound Thomson created the 9. Mixture: More than one type of element or compound not chemically together plum pudding model – bound together the atom was a ball of 10. Electron Shell: A ring surrounding the nucleus containing the positive charge with negative electrons electrons scattered in it Position in the Periodic Rules for electron shells: Table: 1. -
Detection of a Strange Particle
10 extraordinary papers Within days, Watson and Crick had built a identify the full set of codons was completed in forensics, and research into more-futuristic new model of DNA from metal parts. Wilkins by 1966, with Har Gobind Khorana contributing applications, such as DNA-based computing, immediately accepted that it was correct. It the sequences of bases in several codons from is well advanced. was agreed between the two groups that they his experiments with synthetic polynucleotides Paradoxically, Watson and Crick’s iconic would publish three papers simultaneously in (see go.nature.com/2hebk3k). structure has also made it possible to recog- Nature, with the King’s researchers comment- With Fred Sanger and colleagues’ publica- nize the shortcomings of the central dogma, ing on the fit of Watson and Crick’s structure tion16 of an efficient method for sequencing with the discovery of small RNAs that can reg- to the experimental data, and Franklin and DNA in 1977, the way was open for the com- ulate gene expression, and of environmental Gosling publishing Photograph 51 for the plete reading of the genetic information in factors that induce heritable epigenetic first time7,8. any species. The task was completed for the change. No doubt, the concept of the double The Cambridge pair acknowledged in their human genome by 2003, another milestone helix will continue to underpin discoveries in paper that they knew of “the general nature in the history of DNA. biology for decades to come. of the unpublished experimental results and Watson devoted most of the rest of his ideas” of the King’s workers, but it wasn’t until career to education and scientific administra- Georgina Ferry is a science writer based in The Double Helix, Watson’s explosive account tion as head of the Cold Spring Harbor Labo- Oxford, UK. -
PIONEERING THERAPY for LIFE Table of Contents
PIONEERING THERAPY FOR LIFE Table of contents Key figures 20151 IBA at a glance 2 IBA is 30 years old 4 Proton therapy 6 Dosimetry 20 RadioPharma Solutions 24 Industrial 26 Human resources 28 Corporate social responsibility 30 Governance 36 Economical review 39 IFRS consolidated financial statements for the year ended December 31, 2015 73 IBA SA Annual financial statements148 General information 152 Stock market and shareholders 157 Key figures 2015 REBIT (3) / SALES & SERVICES TRENDS 12% 12 IBA is a high-technology medical 10.9% company which concentrates 10% 10 its activities on proton therapy, radiopharmacy, particle accelerators 8 8% for industry, and dosimetry. 6% IBA is the worldwide leader in 6 the proton therapy market. 4 4% Listed on the NYSE Euronext Brussels. 2 2% 1 200 employees worldwide. 0% IBA operates in two areas: “Proton 0 Therapy and Other Accelerators ” and 2010 2011 2012 2013 2014 2015 “Dosimetry”. Key figures 2015 + 22.6% 332 2015 revenue increase EUR million Backlog in Proton Therapy & Other Accelerators OPERATING RESULTS 2014 2015 Change CAGR (1) (EUR 000) (EUR 000) (EUR 000) (%) 2014/2015 Sales and services 220 577 270 357 49 780 22.60% Gross margin 96 096 113 655 18.30% REBITDA (2) 28 321 33 710 5 389 19.00% REBITDA/Sales and services 12.80% 12.50% REBIT (3) 22 932 29 553 6 621 28.90% REBIT/Sales and services 10.40% 10.90% Net profit 24 294 61 189 36 895 151.90% (1) CAGR: compound annual growth rate (2) REBITDA: recurring earnings before interest, taxes, depreciation, and amortization. -
8.1 the Neutron-To-Proton Ratio
M. Pettini: Introduction to Cosmology | Lecture 8 PRIMORDIAL NUCLEOSYNTHESIS Our discussion at the end of the previous lecture concentrated on the rela- tivistic components of the Universe, photons and leptons. Baryons (which are non-relativistic) did not figure because they make a trifling contribu- tion to the energy density. However, from t ∼ 1 s a number of nuclear reactions involving baryons took place. The end result of these reactions was to lock up most of the free neutrons into 4He nuclei and to create trace amounts of D, 3He, 7Li and 7Be. This is Primordial Nucleosynthesis, also referred to as Big Bang Nucleosynthesis (BBN). 8.1 The Neutron-to-Proton Ratio Before neutrino decoupling at around 1 MeV, neutrons and protons are kept in mutual thermal equilibrium through charged-current weak interactions: + n + e ! p +ν ¯e − p + e ! n + νe (8.1) − n ! p + e +ν ¯e While equilibrium persists, the relative number densities of neutrons and protons are given by a Boltzmann factor based on their mass difference: n ∆m c2 1:5 = exp − = exp − (8.2) p eq kT T10 where 10 ∆m = (mn − mp) = 1:29 MeV = 1:5 × 10 K (8.3) 10 and T10 is the temperature in units of 10 K. As discussed in Lecture 7.1.2, this equilibrium will be maintained so long as the timescale for the weak interactions is short compared with the timescale of the cosmic expansion (which increases the mean distance between parti- cles). In 7.2.1 we saw that the ratio of the two rates varies approximately as: Γ T 3 ' : (8.4) H 1:6 × 1010 K 1 This steep dependence on temperature can be appreciated as follows. -
Charm and Strange Quark Contributions to the Proton Structure
Report series ISSN 0284 - 2769 of SE9900247 THE SVEDBERG LABORATORY and \ DEPARTMENT OF RADIATION SCIENCES UPPSALA UNIVERSITY Box 533, S-75121 Uppsala, Sweden http://www.tsl.uu.se/ TSL/ISV-99-0204 February 1999 Charm and Strange Quark Contributions to the Proton Structure Kristel Torokoff1 Dept. of Radiation Sciences, Uppsala University, Box 535, S-751 21 Uppsala, Sweden Abstract: The possibility to have charm and strange quarks as quantum mechanical fluc- tuations in the proton wave function is investigated based on a model for non-perturbative QCD dynamics. Both hadron and parton basis are examined. A scheme for energy fluctu- ations is constructed and compared with explicit energy-momentum conservation. Resulting momentum distributions for charniand_strange quarks in the proton are derived at the start- ing scale Qo f°r the perturbative QCD evolution. Kinematical constraints are found to be important when comparing to the "intrinsic charm" model. Master of Science Thesis Linkoping University Supervisor: Gunnar Ingelman, Uppsala University 1 kuldsepp@tsl .uu.se 30-37 Contents 1 Introduction 1 2 Standard Model 3 2.1 Introductory QCD 4 2.2 Light-cone variables 5 3 Experiments 7 3.1 The HERA machine 7 3.2 Deep Inelastic Scattering 8 4 Theory 11 4.1 The Parton model 11 4.2 The structure functions 12 4.3 Perturbative QCD corrections 13 4.4 The DGLAP equations 14 5 The Edin-Ingelman Model 15 6 Heavy Quarks in the Proton Wave Function 19 6.1 Extrinsic charm 19 6.2 Intrinsic charm 20 6.3 Hadronisation 22 6.4 The El-model applied to heavy quarks -
Proton Decay at the Drip-Line Magic Number Z = 82, Corresponding to the Closure of a Major Nuclear Shell
NEWS AND VIEWS NUCLEAR PHYSICS-------------------------------- case since it has one proton more than the Proton decay at the drip-line magic number Z = 82, corresponding to the closure of a major nuclear shell. In Philip Woods fact the observed proton decay comes from an excited intruder state configura WHAT determines whether a nuclear ton decay half-life measurements can be tion formed by the promotion of a proton species exists? For nuclear scientists the used to explore nuclear shell structures in from below the Z=82 shell closure. This answer to this poser is that the species this twilight zone of nuclear existence. decay transition was used to provide should live long enough to be identified The proton drip-line sounds an inter unique information on the quantum mix and its properties studied. This still begs esting place to visit. So how do we get ing between normal and intruder state the fundamental scientific question of there? The answer is an old one: fusion. configurations in the daughter nucleus. what the ultimate boundaries to nuclear In this case, the fusion of heavy nuclei Following the serendipitous discovery existence are. Work by Davids et al. 1 at produces highly neutron-deficient com of nuclear proton decay4 from an excited Argonne National Laboratory in the pound nuclei, which rapidly de-excite by state in 1970, and the first example of United States has pinpointed the remotest boiling off particles and gamma-rays, leav ground-state proton decay5 in 1981, there border post to date, with the discovery of ing behind a plethora of highly unstable followed relative lulls in activity. -
Chapter 8. the Atomic Nucleus
Chapter 8. The Atomic Nucleus Notes: • Most of the material in this chapter is taken from Thornton and Rex, Chapters 12 and 13. 8.1 Nuclear Properties Atomic nuclei are composed of protons and neutrons, which are referred to as nucleons. Although both types of particles are not fundamental or elementary, they can still be considered as basic constituents for the purpose of understanding the atomic nucleus. Protons and neutrons have many characteristics in common. For example, their masses are very similar with 1.0072765 u (938.272 MeV) for the proton and 1.0086649 u (939.566 MeV) for the neutron. The symbol ‘u’ stands for the atomic mass unit defined has one twelfth of the mass of the main isotope of carbon (i.e., 12 C ), which is known to contain six protons and six neutrons in its nucleus. We thus have that 1 u = 1.66054 ×10−27 kg (8.1) = 931.49 MeV/c2 . Protons and neutrons also both have the same intrinsic spin, but different magnetic moments (see below). Their main difference, however, pertains to their electrical charges: the proton, as we know, has a charge of +e , while the neutron has none, as its name implies. Atomic nuclei are designated using the symbol A Z XN , (8.2) with Z, N and A the number of protons (atomic element number), the number of neutrons, and the atomic mass number ( A = Z + N ), respectively, while X is the chemical element symbol. It is often the case that Z and N are omitted, when there is no chance of confusion.