پروتون، فرمیونی با اسپین ½ است و از سه کوارک ساخته میشود. دو کوارک بالا و یک کوارک پایین درون پروتون با نیروی قوی هستهای در کنار یکدیگر نگه داشته میشوند. پروتون دارای توزیع بار الکتریکی مثبت است که تقریباً به صورت نمایی کاهش مییابد و میانگین شعاع آن حدود ۰٫۸ فمتومتر است.
پروتون و نوترون ذرات درون هستهای هستند و میتوانند توسط نیروی هستهای به یکدیگر متصل شوند و هسته اتم را شکل دهند. هسته فراوانترین ایزوتوپ هیدروژن تنها از یک پروتون تشکیل شدهاست. دو ایزوتوپ دیگر هیدروژن، دارای یک یا دو نوترون هستند که به پروتون متصل شدهاند. هسته سایر اتمها از بیش از یک پروتون و تعدادی نوترون شکل گرفتهاست.
مدت زیادی نیاز بود تا مفهوم ذره هیدروژن-مانند به عنوان سازنده سایر اتمها توسعه یابد. نخست، ویلیام پروت در ۱۸۱۵ بر پایه تفسیر سادهانگارانهای از مقادیر وزن اتمی، چنین فرض کرد که همه اتمها از اتمهای هیدروژن تشکیل شدهاند. پس از آن که مقدارهای دقیقتری اندازهگیری شدند، این فرضیه رد شد.
در ۱۸۸۶، اویگن گلدشتاین پرتوهای آندی را کشف کرد و نشان داد که این پرتوها مربوط به ذرههایی با بار مثبت هستند. البته از آنجاییکه ذرات منتشر شده از گازهای مختلف، دارای نسبت بار به جرم متفاوتی بودند، شناسایی آنها با یک ذره (بر خلاف الکترون با بار منفی) امکانپذیر نبود.
پس از کشف هسته اتم توسط ارنست رادرفورد در ۱۹۱۱، آنتونیوس فندر بروک اظهار کرد که مکان هر عنصر در جدول تناوبی، متناظر با بار هسته آن است. هنری موزلی در ۱۹۱۳ این مطلب را با به کارگیری طیف پرتو ایکس به صورت تجربی تأیید کرد.
رادرفورد در ۱۹۱۷ ثابت کرد که هسته هیدروژن در هستههای دیگر نیز وجود دارد. معمولاً این نتیجه را به عنوان کشف پروتون در نظر میگیرند. رادرفورد آزمایشی انجام داد که در آن، ذرات آلفا را به هوا (که بیشتر آن نیتروژن است) شلیک نمود و آشکارگرها اثراتی از هیدروژن را به عنوان یک محصول واکنش نشان دادند. رادرفورد پس از آن که آزمایش را با نیتروژن خالص تکرار کرد و مشاهده کرد که اثرات بیشتر شدهاند، چنین نتیجه گرفت که این ذرههای هیدروژن تنها میتوانند از نیتروژن آمده باشند و بنابراین نیتروژن باید محتوی هسته هیدروژن باشد. یک هسته هیدروژن جدا شد و نیتروژن به اکسیژن-۱۷ تبدیل شد. این رخداد، نخستین واکنش هستهای گزارش شده، بود.
رادرفورد دانستهبود که هیدروژن سادهترین و سبکترین عنصر است و تحت تأثیر فرضیه پروت بود که هیدروژن واحد سازنده همه عناصر است. کشف این مطلب که هسته هیدروژن در همه هستههای دیگر وجود دارد، رادرفورد را بر آن داشت که نامی ویژه به عنوان یک ذره، به هسته هیدروژن بدهد. رادرفورد چنین پنداشت که هیدروژن به عنوان سبکترین عنصر، تنها دارای یکی از این ذرهها است و این واحد سازنده بنیادی جدید را پروتون نامید. این واژه از کلمهای یونانی به معنی نخستین، مشتق شدهبود.
پروتون آزاد (که به هیچ نوترون یا الکترونی پیوستگی ندارد) یک ذره پایدار است که تاکنون واپاشی آن مشاهده نشدهاست. پروتون آزاد در پلاسما که دمای آن به اندازهای بالا است که اجازه ترکیب پروتون با الکترون را میدهد، وجود دارد. پروتون در نوعی واپاشی هستهای نادر از برخی هستههای اتم نیز منتشر میشود. پروتون به همراه الکترون و پادنوترینو در واپاشی نوترون آزاد نیز پدید میآید.
تاکنون واپاشی خودبهخودی پروتون آزاد مشاهده نشدهاست. برای همین، پروتون به عنوان ذره پایدار در نظر گرفته میشود. البته برخی نظریههای وحدت بزرگ فیزیک ذرات پیشبینی میکنند که واپاشی پروتون با نیمعمری با مرتبه بزرگی ۱×۱۰۳۶ سال انجام میشود. هرچند که نتیجه بعضی آزمایشها حد پایینتری را برای این مقدار، پیشنهاد میدهد.
از سوی دیگر، فرایند جذب الکترون توسط پروتون و تبدیل به نوترون، فرایندی شناختهشده در فیزیک است. البته این فرایند برای پروتونهای آزاد، تنها در صورت وجود انرژی کافی انجامپذیر است. این واکنش، برگشتپذیر است و نوترون میتواند با تابش پرتو بتا به پروتون تبدیل شود که شکل متداولی از واپاشی هستهای است. در واقع، نوترون آزاد با نیمعمر میانگین ۱۵ دقیقه به این صورت واپاشی میکند.
پیوند به بیرون[ویرایش]
A proton is a subatomic particle, symbol
In the modern Standard Model of particle physics, protons are hadrons, and like neutrons, the other nucleon (particle present in atomic nuclei), are composed of three quarks. Although protons were originally considered fundamental or elementary particles, they are now known to be composed of three valence quarks: two up quarks and one down quark. The rest masses of quarks contribute only about 1% of a proton's mass, however. The remainder of a proton's mass is due to quantum chromodynamics binding energy, which includes the kinetic energy of the quarks and the energy of the gluon fields that bind the quarks together. Because protons are not fundamental particles, they possess a physical size, though not a definite one; the root mean square charge radius of a proton is about 0.84–0.87 fm or ×10−15 to 0.84×10−15 m. 0.87
At sufficiently low temperatures, free protons will bind to electrons. However, the character of such bound protons does not change, and they remain protons. A fast proton moving through matter will slow by interactions with electrons and nuclei, until it is captured by the electron cloud of an atom. The result is a protonated atom, which is a chemical compound of hydrogen. In vacuum, when free electrons are present, a sufficiently slow proton may pick up a single free electron, becoming a neutral hydrogen atom, which is chemically a free radical. Such "free hydrogen atoms" tend to react chemically with many other types of atoms at sufficiently low energies. When free hydrogen atoms react with each other, they form neutral hydrogen molecules (H2), which are the most common molecular component of molecular clouds in interstellar space.
Protons are spin-½ fermions and are composed of three valence quarks, making them baryons (a sub-type of hadrons). The two up quarks and one down quark of a proton are held together by the strong force, mediated by gluons.:21–22A modern perspective has a proton composed of the valence quarks (up, up, down), the gluons, and transitory pairs of sea quarks. Protons have an approximately exponentially decaying positive charge distribution with a mean square radius of about 0.8 fm.
Protons and neutrons are both nucleons, which may be bound together by the nuclear force to form atomic nuclei. The nucleus of the most common isotope of the hydrogen atom (with the chemical symbol "H") is a lone proton. The nuclei of the heavy hydrogen isotopes deuterium and tritium contain one proton bound to one and two neutrons, respectively. All other types of atomic nuclei are composed of two or more protons and various numbers of neutrons.
The concept of a hydrogen-like particle as a constituent of other atoms was developed over a long period. As early as 1815, William Prout proposed that all atoms are composed of hydrogen atoms (which he called "protyles"), based on a simplistic interpretation of early values of atomic weights (see Prout's hypothesis), which was disproved when more accurate values were measured.:39–42
In 1886, Eugen Goldstein discovered canal rays (also known as anode rays) and showed that they were positively charged particles (ions) produced from gases. However, since particles from different gases had different values of charge-to-mass ratio (e/m), they could not be identified with a single particle, unlike the negative electrons discovered by J. J. Thomson.
Following the discovery of the atomic nucleus by Ernest Rutherford in 1911, Antonius van den Broek proposed that the place of each element in the periodic table (its atomic number) is equal to its nuclear charge. This was confirmed experimentally by Henry Moseley in 1913 using X-ray spectra.
In 1917 (in experiments reported in 1919), Rutherford proved that the hydrogen nucleus is present in other nuclei, a result usually described as the discovery of protons. Rutherford had earlier learned to produce hydrogen nuclei as a type of radiation produced as a product of the impact of alpha particles on nitrogen gas, and recognize them by their unique penetration signature in air and their appearance in scintillation detectors. These experiments were begun when Rutherford had noticed that, when alpha particles were shot into air (mostly nitrogen), his scintillation detectors showed the signatures of typical hydrogen nuclei as a product. After experimentation Rutherford traced the reaction to the nitrogen in air, and found that when alphas were produced into pure nitrogen gas, the effect was larger. Rutherford determined that this hydrogen could have come only from the nitrogen, and therefore nitrogen must contain hydrogen nuclei. One hydrogen nucleus was being knocked off by the impact of the alpha particle, producing oxygen-17 in the process. This was the first reported nuclear reaction, 14N + α → 17O + p. (This reaction would later be observed happening directly in a cloud chamber in 1925).
Rutherford knew hydrogen to be the simplest and lightest element and was influenced by Prout's hypothesis that hydrogen was the building block of all elements. Discovery that the hydrogen nucleus is present in all other nuclei as an elementary particle, led Rutherford to give the hydrogen nucleus a special name as a particle, since he suspected that hydrogen, the lightest element, contained only one of these particles. He named this new fundamental building block of the nucleus the proton, after the neuter singular of the Greek word for "first", πρῶτον. However, Rutherford also had in mind the word protyle as used by Prout. Rutherford spoke at the British Association for the Advancement of Science at its Cardiff meeting beginning 24 August 1920. Rutherford was asked by Oliver Lodge for a new name for the positive hydrogen nucleus to avoid confusion with the neutral hydrogen atom. He initially suggested both proton and prouton (after Prout). Rutherford later reported that the meeting had accepted his suggestion that the hydrogen nucleus be named the "proton", following Prout's word "protyle". The first use of the word "proton" in the scientific literature appeared in 1920.
The free proton (a proton not bound to nucleons or electrons) is a stable particle that has not been observed to break down spontaneously to other particles. Free protons are found naturally in a number of situations in which energies or temperatures are high enough to separate them from electrons, for which they have some affinity. Free protons exist in plasmas in which temperatures are too high to allow them to combine with electrons. Free protons of high energy and velocity make up 90% of cosmic rays, which propagate in vacuum for interstellar distances. Free protons are emitted directly from atomic nuclei in some rare types of radioactive decay. Protons also result (along with electrons and antineutrinos) from the radioactive decay of free neutrons, which are unstable.
The spontaneous decay of free protons has never been observed, and protons are therefore considered stable particles according to the Standard Model. However, some grand unified theories (GUTs) of particle physics predict that proton decay should take place with lifetimes between 1031 to 1036 years and experimental searches have established lower bounds on the mean lifetime of a proton for various assumed decay products.
Experiments at the Super-Kamiokande detector in Japan gave lower limits for proton mean lifetime of ×1033 years for decay to an 6.6antimuon and a neutral pion, and ×1033 years for decay to a 8.2positron and a neutral pion. Another experiment at the Sudbury Neutrino Observatory in Canada searched for gamma rays resulting from residual nuclei resulting from the decay of a proton from oxygen-16. This experiment was designed to detect decay to any product, and established a lower limit to a proton lifetime of ×1029 years. 2.1
However, protons are known to transform into neutrons through the process of electron capture (also called inverse beta decay). For free protons, this process does not occur spontaneously but only when energy is supplied. The equation is:
The process is reversible; neutrons can convert back to protons through beta decay, a common form of radioactive decay. In fact, a free neutron decays this way, with a mean lifetime of about 15 minutes.
Quarks and the mass of a proton
In quantum chromodynamics, the modern theory of the nuclear force, most of the mass of protons and neutrons is explained by special relativity. The mass of a proton is about 80–100 times greater than the sum of the rest masses of the quarks that make it up, while the gluons have zero rest mass. The extra energy of the quarks and gluons in a region within a proton, as compared to the rest energy of the quarks alone in the QCD vacuum, accounts for almost 99% of the mass. The rest mass of a proton is, thus, the invariant mass of the system of moving quarks and gluons that make up the particle, and, in such systems, even the energy of massless particles is still measured as part of the rest mass of the system.
Two terms are used in referring to the mass of the quarks that make up protons: current quark mass refers to the mass of a quark by itself, while constituent quark mass refers to the current quark mass plus the mass of the gluon particle field surrounding the quark.:285–286 :150–151 These masses typically have very different values. As noted, most of a proton's mass comes from the gluons that bind the current quarks together, rather than from the quarks themselves. While gluons are inherently massless, they possess energy—to be more specific, quantum chromodynamics binding energy (QCBE)—and it is this that contributes so greatly to the overall mass of protons (see mass in special relativity). A proton has a mass of approximately 938 MeV/c2, of which the rest mass of its three valence quarks contributes only about 9.4 MeV/c2; much of the remainder can be attributed to the gluons' QCBE.
The internal dynamics of protons are complicated, because they are determined by the quarks' exchanging gluons, and interacting with various vacuum condensates. Lattice QCD provides a way of calculating the mass of a proton directly from the theory to any accuracy, in principle. The most recent calculations claim that the mass is determined to better than 4% accuracy, even to 1% accuracy (see Figure S5 in Dürr et al.). These claims are still controversial, because the calculations cannot yet be done with quarks as light as they are in the real world. This means that the predictions are found by a process of extrapolation, which can introduce systematic errors. It is hard to tell whether these errors are controlled properly, because the quantities that are compared to experiment are the masses of the hadrons, which are known in advance.
These recent calculations are performed by massive supercomputers, and, as noted by Boffi and Pasquini: "a detailed description of the nucleon structure is still missing because ... long-distance behavior requires a nonperturbative and/or numerical treatment..." More conceptual approaches to the structure of protons are: the topological soliton approach originally due to Tony Skyrme and the more accurate AdS/QCD approach that extends it to include a string theory of gluons, various QCD-inspired models like the bag model and the constituent quark model, which were popular in the 1980s, and the SVZ sum rules, which allow for rough approximate mass calculations. These methods do not have the same accuracy as the more brute-force lattice QCD methods, at least not yet.
The problem of defining a radius for an atomic nucleus (proton) is similar to the problem of atomic radius, in that neither atoms nor their nuclei have definite boundaries. However, the nucleus can be modeled as a sphere of positive charge for the interpretation of electron scattering experiments: because there is no definite boundary to the nucleus, the electrons "see" a range of cross-sections, for which a mean can be taken. The qualification of "rms" (for "root mean square") arises because it is the nuclear cross-section, proportional to the square of the radius, which is determining for electron scattering.
The internationally accepted value of a proton's charge radius is fm (see 0.8768 orders of magnitude for comparison to other sizes). This value is based on measurements involving a proton and an electron (namely, electron scattering measurements and complex calculation involving scattering cross section based on Rosenbluth equation for momentum-transfer cross section), and studies of the atomic energy levels of hydrogen and deuterium.
However, in 2010 an international research team published a proton charge radius measurement via the Lamb shift in muonic hydrogen (an exotic atom made of a proton and a negatively charged muon). Their measurement of the root-mean-square charge radius of a proton is "84(67) fm, which differs by 5.0 0.841standard deviations from the CODATA value of ". 0.8768(69) fm In January 2013, an updated value for the charge radius of a proton—87(39) fm—was published. The precision was improved by 1.7 times, increasing the significance of the discrepancy to 7σ. 0.840
The international research team that obtained this result at the Paul Scherrer Institut in Villigen includes scientists from the Max Planck Institute of Quantum Optics, Ludwig-Maximilians-Universität, the Institut für Strahlwerkzeuge of Universität Stuttgart, and the University of Coimbra, Portugal. The team is now attempting to explain the discrepancy, and re-examining the results of both previous high-precision measurements and complex calculations involving scattering cross section. If no errors are found in the measurements or calculations, it could be necessary to re-examine the world's most precise and best-tested fundamental theory: quantum electrodynamics. The proton radius remains a puzzle as of 2017.  Perhaps the discrepancy is due to new physics, or the explanation may be an ordinary physics effect that has been missed.
The radius is linked to the form factor and momentum transfer cross section. The atomic form factor G modifies the cross section corresponding to point-like proton.
The atomic form factor is related to the wave function density of the target:
The form factor can be split in electric and magnetic form factors. These can be further written as linear combinations of Dirac and Pauli form factors.
Interaction of free protons with ordinary matter
Although protons have affinity for oppositely charged electrons, this is a relatively low-energy interaction and so free protons must lose sufficient velocity (and kinetic energy) in order to become closely associated and bound to electrons. High energy protons, in traversing ordinary matter, lose energy by collisions with atomic nuclei, and by ionization of atoms (removing electrons) until they are slowed sufficiently to be captured by the electron cloud in a normal atom.
However, in such an association with an electron, the character of the bound proton is not changed, and it remains a proton. The attraction of low-energy free protons to any electrons present in normal matter (such as the electrons in normal atoms) causes free protons to stop and to form a new chemical bond with an atom. Such a bond happens at any sufficiently "cold" temperature (i.e., comparable to temperatures at the surface of the Sun) and with any type of atom. Thus, in interaction with any type of normal (non-plasma) matter, low-velocity free protons are attracted to electrons in any atom or molecule with which they come in contact, causing the proton and molecule to combine. Such molecules are then said to be "protonated", and chemically they often, as a result, become so-called Bronsted acids.
Proton in chemistry
In chemistry, the number of protons in the nucleus of an atom is known as the atomic number, which determines the chemical element to which the atom belongs. For example, the atomic number of chlorine is 17; this means that each chlorine atom has 17 protons and that all atoms with 17 protons are chlorine atoms. The chemical properties of each atom are determined by the number of (negatively charged) electrons, which for neutral atoms is equal to the number of (positive) protons so that the total charge is zero. For example, a neutral chlorine atom has 17 protons and 17 electrons, whereas a Cl− anion has 17 protons and 18 electrons for a total charge of −1.
All atoms of a given element are not necessarily identical, however, as the number of neutrons may vary to form different isotopes, and energy levels may differ forming different nuclear isomers. For example, there are two stable isotopes of chlorine: 35
In chemistry, the term proton refers to the hydrogen ion, H+
The transfer of H+
Proton nuclear magnetic resonance (NMR)
Also in chemistry, the term "proton NMR" refers to the observation of hydrogen-1 nuclei in (mostly organic) molecules by nuclear magnetic resonance. This method uses the spin of the proton, which has the value one-half. The name refers to examination of protons as they occur in protium (hydrogen-1 atoms) in compounds, and does not imply that free protons exist in the compound being studied.
Protons also have extrasolar origin from galactic cosmic rays, where they make up about 90% of the total particle flux. These protons often have higher energy than solar wind protons, and their intensity is far more uniform and less variable than protons coming from the Sun, the production of which is heavily affected by solar proton events such as coronal mass ejections.
Research has been performed on the dose-rate effects of protons, as typically found in space travel, on human health. To be more specific, there are hopes to identify what specific chromosomes are damaged, and to define the damage, during cancer development from proton exposure. Another study looks into determining "the effects of exposure to proton irradiation on neurochemical and behavioral endpoints, including dopaminergic functioning, amphetamine-induced conditioned taste aversion learning, and spatial learning and memory as measured by the Morris water maze. Electrical charging of a spacecraft due to interplanetary proton bombardment has also been proposed for study. There are many more studies that pertain to space travel, including galactic cosmic rays and their possible health effects, and solar proton event exposure.
CPT-symmetry puts strong constraints on the relative properties of particles and antiparticles and, therefore, is open to stringent tests. For example, the charges of a proton and antiproton must sum to exactly zero. This equality has been tested to one part in . The equality of their masses has also been tested to better than one part in 108. By holding antiprotons in a 108Penning trap, the equality of the charge to mass ratio of protons and antiprotons has been tested to one part in ×109. 6 The magnetic moment of antiprotons has been measured with error of ×10−3 nuclear 8Bohr magnetons, and is found to be equal and opposite to that of a proton.