William Fuller Brown Jr. | |
---|---|
Born | Lyon Mountain, New York, United States | September 21, 1904
Died | 1983 (aged 78–79) |
Alma mater | Cornell University, Columbia University |
Known for | Micromagnetics |
Awards | Fulbright scholar, IEEE Fellow, Meritorious Civilian Service Award |
Scientific career | |
Fields | magnetism |
Institutions | Princeton University, Naval Ordnance Laboratory, Sun Oil Company, 3M Company, University of Minnesota |
Thesis | The variation of the internal friction and elastic constants with magnetization in iron (1937) |
Doctoral advisor | Shirley Leon Quimby |
William Fuller Brown Jr. (21 September 1904 – 12 December 1983) was an American physicist and electrical engineer who developed the theory of micromagnetics, a continuum theory of ferromagnetism that has had numerous applications in physics and engineering. He published three books: Magnetostatic Principles in Ferromagnetism, [1] Micromagnetics, [2] and Magnetoelastic Interactions. [3]
William Fuller Brown Jr. was born in Lyon Mountain, New York on September 21, 1904 to William Fuller Brown and Mary Emily Williams, daughter of Hon. Andrew Williams. [4] [5] [6] An early interest in electromagnetism was stimulated by a toy motor but "destimulated" by high school and college physics courses. [7] He graduated from Cornell University with a BA in English in 1925 and began teaching at Carolina Academy, a private high school in Raleigh, North Carolina. Teaching general science "restimulated" his interest in physics. [7]
In 1927, Brown enrolled in Columbia University. With S. L. Quimby as his doctoral advisor, he wrote a dissertation on the effect of magnetization on the elastic properties of iron. On August 17, 1936 he was married to Nancy Shannon Johnson. [6] He received his PhD in physics in 1937. [7]
In 1938 Brown was appointed assistant professor of physics at Princeton University. It was during this period that he developed micromagnetics. In 1941, he went to the U.S. Naval Ordnance Laboratory, where he headed a team that was working on methods to protect ships against magnetic mines. He developed novel methods for degaussing ships and instrumentation for measuring magnetic fields and the magnetic properties of steels. For his work he was awarded the Meritorious Civilian Service Award by the U.S. Navy. [6]
From 1946 to 1955, Brown worked in Newton Square, Pennsylvania as a research physicist at the Sun Oil Company, investigating dielectric and ferromagnetic phenomena. In 1955 he moved to Minnesota and worked with the 3M Company as a senior research physicist, where there was a strong interest in ferromagnetic single-domain particles. [6]
In 1957 Brown became a professor of electrical engineering at the University of Minnesota. He remained in this position until he became emeritus in 1973, aside from 1962 (when he was a Fulbright scholar at the Weizmann Institute in Rehovot, Israel) and 1963–1964 (when he was guest professor at the Max Planck Institute for Metals Research in Stuttgart). [6] He died in St. Paul, Minnesota in 1983. [8]
At the time of Brown's graduation from Cornell, the theory for magnetic domains was not very developed. Richard Becker and Werner Döring, in their book Ferromagnetismus, [9] emphasized internal stresses. Brown realized that the most important factor, magnetostatic forces, were "totally ignored". He was strongly influenced by the 1935 paper of Lev Landau and Evgeny Lifshitz, which developed a one-dimensional continuous model for domain wall motion. In 1938 W. C. Elmore published a paper that discussed a three-dimensional generalization of the Landau-Lifshitz theory, but did not attempt to derive the equations. Brown set out to do this. [10]
Brown published his equations in 1940 and applied them to the approach to saturation of magnetization curves. [11] He later said that "nobody paid any attention to them for 16 years", [7] although Charles Kittel said that it was one of the "starting points" for his review of ferromagnetism in 1946. [12]
In 1967, Brown received an A. Cressy Morrison Award from the New York Academy of Sciences. In 1968 he was elected Fellow of the IEEE and in 1974 was made an Honorary Life Member of the IEEE Magnetics Society. He was also elected Fellow of the American Physical Society in 1938 [13] and the American Association for the Advancement of Science. [6]
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: CS1 maint: location missing publisher (link)Ferromagnetism is a property of certain materials that results in a significant, observable magnetic permeability, and in many cases, a significant magnetic coercivity, allowing the material to form a permanent magnet. Ferromagnetic materials are noticeably attracted to a magnet, which is a consequence of their substantial magnetic permeability.
Giant magnetoresistance (GMR) is a quantum mechanical magnetoresistance effect observed in multilayers composed of alternating ferromagnetic and non-magnetic conductive layers. The 2007 Nobel Prize in Physics was awarded to Albert Fert and Peter Grünberg for the discovery of GMR, which also sets the foundation for the study of spintronics.
A magnon is a quasiparticle, a collective excitation of the spin structure of an electron in a crystal lattice. In the equivalent wave picture of quantum mechanics, a magnon can be viewed as a quantized spin wave. Magnons carry a fixed amount of energy and lattice momentum, and are spin-1, indicating they obey boson behavior.
In the physical theory of spin glass magnetization, the Ruderman–Kittel–Kasuya–Yosida (RKKY) interaction models the coupling of nuclear magnetic moments or localized inner d- or f-shell electron spins through conduction electrons. It is named after Malvin Ruderman, Charles Kittel, Tadao Kasuya, and Kei Yosida, the physicists who first proposed and developed the model.
Magnetostatics is the study of magnetic fields in systems where the currents are steady. It is the magnetic analogue of electrostatics, where the charges are stationary. The magnetization need not be static; the equations of magnetostatics can be used to predict fast magnetic switching events that occur on time scales of nanoseconds or less. Magnetostatics is even a good approximation when the currents are not static – as long as the currents do not alternate rapidly. Magnetostatics is widely used in applications of micromagnetics such as models of magnetic storage devices as in computer memory.
Ferromagnetic resonance, or FMR, is coupling between an electromagnetic wave and the magnetization of a medium through which it passes. This coupling induces a significant loss of power of the wave. The power is absorbed by the precessing magnetization of the material and lost as heat. For this coupling to occur, the frequency of the incident wave must be equal to the precession frequency of the magnetization and the polarization of the wave must match the orientation of the magnetization.
Micromagnetics is a field of physics dealing with the prediction of magnetic behaviors at sub-micrometer length scales. The length scales considered are large enough for the atomic structure of the material to be ignored, yet small enough to resolve magnetic structures such as domain walls or vortices.
Spin pumping is the dynamical generation of pure spin current by the coherent precession of magnetic moments, which can efficiently inject spin from a magnetic material into an adjacent non-magnetic material. The non-magnetic material usually hosts the spin Hall effect that can convert the injected spin current into a charge voltage easy to detect. A spin pumping experiment typically requires electromagnetic irradiation to induce magnetic resonance, which converts energy and angular momenta from electromagnetic waves to magnetic dynamics and then to electrons, enabling the electronic detection of electromagnetic waves. The device operation of spin pumping can be regarded as the spintronic analog of a battery.
A magnetic domain is a region within a magnetic material in which the magnetization is in a uniform direction. This means that the individual magnetic moments of the atoms are aligned with one another and they point in the same direction. When cooled below a temperature called the Curie temperature, the magnetization of a piece of ferromagnetic material spontaneously divides into many small regions called magnetic domains. The magnetization within each domain points in a uniform direction, but the magnetization of different domains may point in different directions. Magnetic domain structure is responsible for the magnetic behavior of ferromagnetic materials like iron, nickel, cobalt and their alloys, and ferrimagnetic materials like ferrite. This includes the formation of permanent magnets and the attraction of ferromagnetic materials to a magnetic field. The regions separating magnetic domains are called domain walls, where the magnetization rotates coherently from the direction in one domain to that in the next domain. The study of magnetic domains is called micromagnetics.
Spin-polarized scanning tunneling microscopy (SP-STM) is a type of scanning tunneling microscope (STM) that can provide detailed information of magnetic phenomena on the single-atom scale additional to the atomic topography gained with STM. SP-STM opened a novel approach to static and dynamic magnetic processes as precise investigations of domain walls in ferromagnetic and antiferromagnetic systems, as well as thermal and current-induced switching of nanomagnetic particles.
In condensed matter physics, magnetic anisotropy describes how an object's magnetic properties can be different depending on direction. In the simplest case, there is no preferential direction for an object's magnetic moment. It will respond to an applied magnetic field in the same way, regardless of which direction the field is applied. This is known as magnetic isotropy. In contrast, magnetically anisotropic materials will be easier or harder to magnetize depending on which way the object is rotated.
Gallium manganese arsenide, chemical formula (Ga,Mn)As is a magnetic semiconductor. It is based on the world's second most commonly used semiconductor, gallium arsenide,, and readily compatible with existing semiconductor technologies. Differently from other dilute magnetic semiconductors, such as the majority of those based on II-VI semiconductors, it is not paramagnetic but ferromagnetic, and hence exhibits hysteretic magnetization behavior. This memory effect is of importance for the creation of persistent devices. In (Ga,Mn)As, the manganese atoms provide a magnetic moment, and each also acts as an acceptor, making it a p-type material. The presence of carriers allows the material to be used for spin-polarized currents. In contrast, many other ferromagnetic magnetic semiconductors are strongly insulating and so do not possess free carriers. (Ga,Mn)As is therefore a candidate material for spintronic devices but it is likely to remain only a testbed for basic research as its Curie temperature could only be raised up to approximatelly 200 K.
In physics, the Landau–Lifshitz–Gilbert equation, named for Lev Landau, Evgeny Lifshitz, and T. L. Gilbert, is a name used for a differential equation describing the dynamics of magnetization M in a solid. It is a modified version by Gilbert of the original equation of Landau and Lifshitz. The LLG equation is similar to the Bloch equation, but they differ in the form of the damping term. The LLG equation describes a more general scenario of magnetization dynamics beyond the simple Larmor precession. In particular, the effective field driving the precessional motion of M is not restricted to real magnetic fields; it incorporates a wide range of mechanisms including magnetic anisotropy, exchange interaction, and so on.
Discovered only as recently as 2006 by C.D. Stanciu and F. Hansteen and published in Physical Review Letters, this effect is generally called all-optical magnetization reversal. This magnetization reversal technique refers to a method of reversing magnetization in a magnet simply by circularly polarized light and where the magnetization direction is controlled by the light helicity. In particular, the direction of the angular momentum of the photons would set the magnetization direction without the need of an external magnetic field. In fact, this process could be seen as similar to magnetization reversal by spin injection. The only difference is that now, the angular momentum is supplied by the circularly polarized photons instead of the polarized electrons.
In its most general form, the magnetoelectric effect (ME) denotes any coupling between the magnetic and the electric properties of a material. The first example of such an effect was described by Wilhelm Röntgen in 1888, who found that a dielectric material moving through an electric field would become magnetized. A material where such a coupling is intrinsically present is called a magnetoelectric.
In magnetism, single domain refers to the state of a ferromagnet in which the magnetization does not vary across the magnet. A magnetic particle that stays in a single domain state for all magnetic fields is called a single domain particle. Such particles are very small. They are also very important in a lot of applications because they have a high coercivity. They are the main source of hardness in hard magnets, the carriers of magnetic storage in tape drives, and the best recorders of the ancient Earth's magnetic field.
The demagnetizing field, also called the stray field, is the magnetic field (H-field) generated by the magnetization in a magnet. The total magnetic field in a region containing magnets is the sum of the demagnetizing fields of the magnets and the magnetic field due to any free currents or displacement currents. The term demagnetizing field reflects its tendency to act on the magnetization so as to reduce the total magnetic moment. It gives rise to shape anisotropy in ferromagnets with a single magnetic domain and to magnetic domains in larger ferromagnets.
Néel relaxation theory is a theory developed by Louis Néel in 1949 to explain time-dependent magnetic phenomena known as magnetic viscosity. It is also called Néel-Arrhenius theory, after the Arrhenius equation, and Néel-Brown theory after a more rigorous derivation by William Fuller Brown, Jr. Néel used his theory to develop a model of thermoremanent magnetization in single-domain ferromagnetic minerals that explained how these minerals could reliably record the geomagnetic field. He also modeled frequency-dependent susceptibility and alternating field demagnetization.
Anthony Schuyler Arrott was an American-born Canadian physicist, and a professor at Carnegie Institute of Technology and Simon Fraser University. He was a specialist in condensed matter physics, the physics of magnetism, and liquid crystals. He was the author of over 200 scientific papers. Arrott is the subject of the 2020 documentary Portrait, directed by Lily Ekimian and A.T. Ragheb.
In condensed matter physics, the Slater–Pauling rule states that adding an element to a metal alloy will reduce the alloy's saturation magnetization by an amount proportional to the number of valence electrons outside of the added element's d shell. Conversely, elements with a partially filled d shell will increase the magnetic moment by an amount proportional to number of missing electrons. Investigated by the physicists John C. Slater and Linus Pauling in the 1930s, the rule is a useful approximation for the magnetic properties of many transition metals.