Fig.1 Schematic representation of Hall Effect in a conductor. The theory of the Hall effect is discussed in Omar, Sections 4.10, 5.19, 6.8, Hutchison and Baird, the Physics of Engineering Solids, Section 11.6, and Kittel, Elementary Solid State Physics, pp. Observation of Quantum Hall effect in an ultra-thin (Bi 0.53Sb 0.47) 2Te 3 film Wenqin Zou,1,a) Wei Wang,2,a) Xufeng Kou,3 Murong Lang,3 Yabin Fan,3 Eun Sang Choi,4 Alexei V. Fedorov,5 Kejie Wang,2 Liang He,2,3,b) Yongbing Xu,2,b) and Kang. 1.1 The simple theory of the Hall effect Consider a conducting slab as shown in Fig. The Hall effect was discovered in 1879 by Edwin Herbert Hall while he was 4, with a magnetic field H in the z direction perpendicular to contacts 1, 2 and 3, 4. The Hall effect was discovered by Dr. Edwin Hall in 1879 while he was a doctoral candidate at Johns Hopkins University in Baltimore. Hall was attempting to verify the theory of electron flow proposed by Kelvin some 30 years earlier. A sharp switching behaviour can be seen in the Hall resistivity at low temperatures, which is a signature of the anomalous Hall effect. suggestions for smooth experimenting and completion of the observation table. hall effect experiment observation table and calculation Hall Effect Experiment and 10 Viva Questions. It is illustrated in Fig. Note the values of I X, V 1, V 2 in the table – 1 and calculate V H. Repeat the experiment for different values of I X by increasing its value in equal intervals of 0.25 mA. This experiment attempts to measure the constant of proportional-ity between these two variables for two different materials: bismuth and silver. from Hall Effect measurements, which are a basic tool for the determination of mobilities. The Hall effect data taken at different temperatures is shown in the Fig. The effect was discovered by E.H. Hall in 1879. L. Wang3,b) 1National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing 210093, People’s Republic of China Using the ... Table 3: Measurements of the Hall voltage with 1.0 mA running through the film as a function of magnetic field for both Bismuth and Silver. Faculty in-charge will take second round to check the observation table of each group and sign one or two observations. 166-167. Hall Effect Experiment and Viva Questions: In the hall effect experiment, we determine the hall voltage and hall coefficient. The Hall Effect is the production of a voltage difference (the Hall voltage) across an electrical conductor, transverse to an electric current in the conductor and a magnetic field perpendicular to the current. Figure 1: Geometry of fields and sample in Hall effect experiment. Hall effect in silver Objects of the experiment g Validation of the proportionality of the Hall voltage and the magnetic flux density. In order to remove the possible contribution of the orbital MR from the Hall data, the measured Hall data is anti-symmetrized. Better references for the purpose of our experiment are Azároff and Brophy, Electronic If the magnetic field is applied along negative z-axis, the Lorentz force moves the charge carriers (say electrons) toward the y-direction. 1 with length L in the x direction, width w in the y direction and thickness t in the z direction. The current was increased in 0.05 20.1. Consider a simple crystal mounted as in the Fig. The Hall Effect The Hall effect was first observed by an American scientist, E.H.Hall, in 1879. 1: Hall Effect schematically: Inside a charge carrying metallic g Determining the polarity of the charge carriers. 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