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Kinetic Energy of Emerging Neutrons Produced by Photodisintegration in a Medical Linear Accelerator ARTÍCULO DE INVESTIGACIÓN Vol. 34, No. 2, Agosto 2013, pp. 125-130 Kinetic Energy of Emerging Neutrons Produced by Photodisintegration in a Medical Linear Accelerator U. Reyes∗ ABSTRACT ∗ M. Sosa When a gamma photon interacts with a target nucleus a nuclear ∗ J. Bernal reaction can be generated, producing as a consequence the expulsion ∗ T. Córdova of particles from the atomic nucleus, this process is called ∗∗ F. Mesa photodisintegration. For this work, are of interest nuclear reactions of photodisintegration in which neutrons are ejected due to the ∗ Department of Physical interaction of photons with atomic nuclei of different materials in a Engineering, Division of linear accelerator for medical use. In this paper, the kinetic energy of Science and Engineering, photoneutrons produced by interactions with atomic nuclei of 184W, University of Guanajuato, 63Cu, 27Al and 12C, which are some of the materials that constitute Leon, Gto., Mexico. the head of a medical linear accelerator, is calculated. Also, the nuclei ∗∗ Polytechnic University of present in the construction materials of the room and the maze of the Victoria, Ciudad Victoria, accelerator, such as, 23Na, 40Ca and 28Si, as also in the human body, 2H, Tam., Mexico. 14N and 16O, are considered. It derives an exact theoretical expression, which has a linear dependence of the energy of the produced neutrons relative to the incident photon energy. It is found that, in the majority of cases, just photons with energies above 10 MV contribute to the production of neutrons. The values calculated from the expression obtained in this work are in good agreement with those reported in the literature, that are obtained by other approaches. Keywords: photoneutrons, kinetic energy, linear accelerator, photodisintegration. 126 Revista Mexicana de Ingeniería Biomédica · volumen 34 · número 2 · Agosto, 2013 Correspondencia: RESUMEN M. Sosa Cuando un fotón gamma interactúa con un núcleo blanco una Loma del Bosque 103, Lomas reacción nuclear puede ser generada, produciendo como consecuencia del Campestre 37150 León, la expulsión de partículas del núcleo atómico, este proceso se denomina Guanajuato México fotodesintegración. Para este trabajo, son de interés las reacciones Correo electrónico: nucleares de fotodesintegración en las que los neutrones son expulsados modesto@fisica.ugto.mx debido a la interacción de los fotones con los núcleos atómicos de diferentes materiales en un acelerador lineal para uso médico. En este trabajo, la energía cinética de fotoneutrones producidos por la Fecha de recepción: interacción con los núcleos atómicos de 184W, 63Cu, 27Al y 12C, que son 29 de Noviembre de 2012 algunos de los materiales que constituyen el cabezal de un acelerador Fecha de aceptación: lineal médico, es calculada. Además, los núcleos presentes en los 15 de Mayo de 2013 materiales de construcción de la sala y el laberinto del acelerador, como por ejemplo, 23Na, 40Ca y 28Si, como también en el cuerpo humano, 2H, 14N y 16O, son considerados. Se obtiene una expresión exacta teórica, la cual tiene una dependencia lineal de la energía de los neutrones producidos en relación a la energía del fotón incidente. Se ha encontrado que, en la mayoría de los casos, sólo los fotones con energías por encima de 10 MV contribuyen a la producción de neutrones. Los valores calculados a partir de la expresión obtenida en este trabajo están en buen acuerdo con los reportados en la literatura, los cuales se obtienen mediante otros métodos. Palabras clave: fotoneutrones, energía cinética, acelerador lineal, fotodesintegración. INTRODUCTION you want to analyze the spectrum of neutrons produced in a medical linear accelerator. The The energies binding the nucleons inside the neutrons released by this type of nuclear nucleus are very large. However, when particles reactions are known as photoneutrons. such as neutrons, protons, alpha particles, or Linear accelerators are a modern tool widely high energy photons collide with atomic nuclei, used in medicine for radiotherapy treatments. In they can produce changes within it. During these recent years, the accelerators have replaced the interactions can occur several events: sometimes use of 60Co sources, when required irradiation is the incident particle enters the nucleus, where it with high-energy photons. An advantage thereof remains, while a second particle, or many more, is that there is a controlled radiation emitter, are expelled. In other cases, the incident particle unlike a radioactive source having a constant can get to fracture the nucleus into several parts, rate of emission. However, when a linac is used or simply can bounce in an elastic collision. The in the photon mode, contamination arises due stability of the atomic nuclei is measured in to neutrons produced by photodisintegration, terms of the energy of the incident particle and when the photons of the beam interact with the the Q factor of the reaction. material of the accelerator head itself as well Within the range of particles used as as with the building materials of the walls, and projectiles in nuclear reactions are the photons. finally with the patient himself. These neutrons Their ways of interaction with matter include: present a complex spectrum of energies that the photoelectric effect, pair production and depends on the energy of the incident photons, Compton effect. However, by its charge the cross section of the materials which interact neutrality, photons can also cross the electron with photons, the same energy distribution cloud to interact with atomic nuclei, producing of the photon beam and the production of nuclear reactions. Such reactions are known as thermal neutrons, as well as other possible photodisintegration reactions and are vital when mechanisms of neutron production. Meanwhile, Reyes et al. Kinetic energy of emerging neutrons produced by photodisintegration in a medical linear accelerator 127 the determination of the neutron contamination is important because the generated neutrons may interact in many cases with the patient, producing secondary charged particles that can contribute as an additional dose, which is generally not taken into account in the design of protocols for radiotherapy treatments. In Fig. 1. Schematic diagram of a photodisintegration the literature, this problem has been addressed reaction. by several authors, which raises the need to develop methods [1-6], both experimental and computational, that allow the determination of the neutron energy spectrum, and from this calculate the dose deposited. On the other hand, which is shown schematically in Figure 1. In it is known, theoretically, that the production the first scene, we have a photon with energy of neutron in photodisintegration reactions is hν which hits a nucleus of mass M, which is possible only if the energy of the incident photons at rest. Then, a recoiling nucleus with mass m exceeds the Q value of the nuclear reaction. and kinetic energy k, as also a photoneutron of Similarly, in the neutron energy spectrum, the kinetic energy kn, are ejected at angles φ and θ, neutron peak corresponding to the primary respectively. neutrons, that is, those generated by the incident photons is relatively pronounced [5]. This part of the spectrum is particularly interesting since contains fast neutrons, which are able to produce Hence, applying mass-energy conservation, secondary ionizing particles; they deliver most of we have the total neutron dose along the beam axis [7-9]. 2 2 2 hν + Mc = mnc + kn + mc + k (2) Due to the above, this paper addresses the problem of calculating the kinetic energy of from which the Q factor of the reaction is given the emerging neutrons, for which it had been by derived an exact expression, which has a linear 2 2 dependence of the photoneutrons energy with Q = Mc − (mn + m) c = kn + k − hν (3) the incident photon energy; also, such formula Then, applying conservation of momentum, one is applied to the nuclei of the various materials obtains the following equation present in a radiation room, including the " # patient. No consideration of the cross section has hν 2 p2 −2µp p cos θ−µ 2 (Q + hν) m − = 0 been made, because this last parameter is only n γ n c relevant when obtaining the energy spectrum of (4) neutrons, not their kinetic energy due to the where µ = mn . Solving Eq. (4), and doing mn+m reaction. 2 hν B = 2µpγ and D = µ 2 (Q + hν) m − c , it has " # 1/ 1 2 2 2 pn (θ) = B cos θ ± B cos θ + 4D (5) CALCULATION OF THE ENERGY 2 It has two solutions for Eq. (5),√ and both have 1 Suppose we have the following photodisintegration an average value given by pn = D ± 2 B. From reaction: the above equations, and after some algebra, yields an expression for the kinetic energy of the A A−1 1 γ + Z X → Z X + 0n (1) photoneutron, as a function of incident photon 128 Revista Mexicana de Ingeniería Biomédica · volumen 34 · número 2 · Agosto, 2013 momentum, given by MATERIAL AND METHODS 2 mn pγ The expression given by Eq. (6), to kn (pγ) = (Q + pλc) − mn + m 2 (mn + m) the output energy of the neutrons produced 2 by photodisintegration in a medical linear pγmn ± (6) accelerator has been applied to various materials 2(m + m)2 n present in the accelerator head. Specifically in where the sign ± is a consequence of the angle the head of a linac for medical use, there are at which the photoneutron emerges. nuclei of 206Pb, 207Pb, 208Pb, 180W, 182W, 183W, 184 27 63 65 54 56 57 It can be seen that Eq. (5) has two solutions W, Al, Cu, Cu, Fe, Fe and Fe, for the momentum of the photoneutron. When among others. All these elements have a nuclear considering the positive root in Eq. (5), the reaction Q factor different from each other. solution has a sinusoidal behavior shown in Furthermore, they present a different isotopic Figure 2 (dotted line).
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