Magnetic Domains in Thin Films by the Faraday Effect

Abstract

LETTERS TO X=0.78 mm FIG. 2. Cathode-ray display of two of the three hyperfine components of the 7 = 0->1 transition of HI at 0.778-mm wavelength. The line to the left is the F = 5/2 -• > 7/2 component, and the one to the right is the F = 5/2 -> 3/2 component. These two components observed on the same scope trace are 163.3 Mc/sec apart. The klystron mode would not cover all three components in a single sweep.

The magneto-optical properties of annealed Co96Pt4 nanowire arrays

“…The results presented here prove that a modest anneal at 300°C can enhance the FRA in a nanowire assembly by a factor of 38%. The standard theory of the Faraday effect 16,17 demonstrates that, for a given sample thickness, the FRA is proportional to the saturation magnetization, but Fig. 4͑b͒ shows that M s remains constant within experimental error over the temperature interval up to 400°C.…”

A Magneto-Optic Apparatus for the Dynamic Study of Ferromagnetic Surface Domains

“…(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25)(26)(27)) and (II-40a), we see that the transmission 2 factors are primarily proportional to rkm . Obviously, then, any increase in r km will result in an increase in the transmission factors at a given contrast ratio.…”

“…At this point wi will introduce the contrast ratio, Re, which we will define as the ratio of the transmission factor in State II to the transmission factor in State I, i.e., T2 R T -- (11)(12)(13)(14)(15)(16)(17)(18)(19) c TI…”

“…(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24)(25) n plotted at a wavelength X = 4910 Pd, and T is the white light transmission. It is apparent, then, that the condition of maximum contrast may differ considerably from the most desirable operating point since the characteristics for determining the transmission parameters can vary from specimen to specimen.…”

Vergleich neuer Speicherelemente für elektronische Rechenmaschinen/ Comparison of new storage devices for electronic computers

“…Sie beträgt normalerweise nur wenige Grad (schlechtes L: O-Verhältnis), kann jedoch durch hellere Lichtquellen und durch Bedampfen der Probe mit einer dielektrischen Schicht auf etwa den 5 fachen Wert vergrößert werden [117], [120]. Liegen die Magnetisierungsvektoren parallel zur Schichtoberfläche, so gelangt Schrägbeleuchtung zur Anwendung [114], [115]. Hartmagnetische Filme (ζ.…”