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Citation counts use data from CrossRef as provided by the publishers of the citing articles.
❖ 2005 and later content is hosted outside of PROLA.
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Rebecca Lippmann Kung, Peter Kung, and Cedric Linder
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Physics education research increasingly makes use of video data for analysis of student learning and teaching practice. Collection of these data is conceptually simple but execution is often fraught with costly and time-consuming complications. This pragmatic paper discusses the development of systems to record and permanently archive audio and video data in real-time. We focus on a system based upon consumer video DVD recorders, but also give an overview of other technologies and detail issues common to all systems. We detail common yet unexpected complications, particularly with regard to sound quality and compatibility with transcription software. Information specific to fixed and transportable systems, other technology options, and generic and specific equipment recommendations are given in supplemental appendices
Phys. Rev. ST Phys. Educ. Res. 1, 010105 (2005)
Cited 0 times
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M. Grayson, L. B. Rigal, D. C. Schmadel, H. D. Drew, and P.-J. Kung
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We measure the temperature and frequency dependence of the complex Hall angle for normal state YBa2Cu3O7 films from dc to far-infrared frequencies (20–250 cm-1) using a new modulated polarization technique. We determine that the functional dependence of the Hall angle on scattering does not fit the expected Lorentzian response. We find spectral evidence supporting models of the Hall effect where the scattering ΓH is linear in T, suggesting that a single relaxation rate, linear in temperature, governs transport in the cuprates.
Phys. Rev. Lett. 89, 037003 (2002)
Cited 13 times
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J. Černe, M. Grayson, D. C. Schmadel, G. S. Jenkins, H. D. Drew, R. Hughes, A. Dabkowski, J. S. Preston, and P.-J. Kung
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Infrared ( 20–120 and 900–1100 cm-1) Faraday rotation and circular dichroism are measured in high- Tc superconductors using sensitive polarization modulation techniques. Optimally doped YBa2Cu3O7 thin films are studied at temperatures in the range ( 15<T<300 K) and magnetic fields up to 8 T. At 1000 cm-1 the Hall conductivity σxy varies strongly with temperature in contrast to the longitudinal conductivity σxx which is nearly independent of temperature. The Hall scattering rate γH has a T2 temperature dependence but, unlike a Fermi liquid, depends only weakly on frequency. The experiment puts severe constraints on theories of transport in the normal state of high- Tc superconductors.
Phys. Rev. Lett. 84, 3418 (2000)
Cited 17 times
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Hung-chi Lihn, Pamela Kung, Chitrlada Settakorn, Helmut Wiedemann, and David Bocek
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A bunch-length measuring method has been developed to measure the subpicosecond electron pulses generated at the Stanford University Short Intense Electron Source (SUNSHINE) facility. This method utilizes a far-infrared Michelson interferometer to measure coherent transition radiation emitted at wavelengths longer than or equal to the bunch length via optical autocorrelation. To analyze the measurement, a simple and systematic way has also been developed, which considers interference effects on the interferogram caused by the beam splitter; hence the electron bunch length can be easily obtained from the measurement. This simple, low-cost, frequency-resolved autocorrelation method demonstrates subpicosecond resolving power that cannot be achieved by existing time-resolved methods.
Phys. Rev. E 53, 6413 (1996)
Cited 11 times
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Hung-chi Lihn, Pamela Kung, Chitrlada Settakorn, Helmut Wiedemann, David Bocek, and Michael Hernandez
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Stimulated, coherent transition radiation (STR) has been observed at the Stanford SUNSHINE facility. Far-infrared light pulses of coherent transition radiation emitted from femtosecond electron bunches are recycled in a special cavity to arrive back at the radiator coincident with subsequent incoming electron bunches. This overlap enables the electrons to do work on the electromagnetic field, thus stimulating the emission of more radiated energy than would be possible without this external field. The experimental setup to observe STR via cavity detuning measurements and experimental results is discussed.
Phys. Rev. Lett. 76, 4163 (1996)
Cited 8 times
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Pamela Kung, Hung-chi Lihn, Helmut Wiedemann, and David Bocek
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An electron source has been developed at the Stanford SUNSHINE facility which can produce electron bunches as short as 50 fs (rms) with (2-4.6)×108e- per microbunch. This source consists of a 2.6 MeV rf gun with a thermionic cathode and an alpha magnet for bunch compression. Coherent transition radiation emitted at wavelengths equal to the bunch length and longer is used in a Michelson interferometer to determine the bunch length by optical autocorrelation. The experimental setup and results of bunch length measurements are described.
Phys. Rev. Lett. 73, 967 (1994)
Cited 48 times
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P. J. Kung, M. P. Maley, M. E. McHenry, J. O. Willis, M. Murakami, and S. Tanaka
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Magnetic hysteresis, flux pinning, and flux creep in melt-powder-melt-growth processed YBa2Cu3O7 (Y 1:2:3) containing nominal 0, 25, and 40 mol % concentration of Y2BaCuO5 (Y 2:1:1) inclusions were investigated. The strong pinning due to 2:1:1-phase precipitates in these samples allows for characterization of the hysteretic response as a function of pinning-site concentration over a large portion of magnetic-field–temperature space. We have found the following: (i) The curves of effective pinning energy Ueff versus current density J reveal a diverging behavior of Ueff(J) in the low-J regime. This supports the existence of a vortex-glass state, and is a signature of a vanishing resistance as the current density approaches zero. (ii) Both the Ueff and the J values obtained from magnetic hysteresis loops were observed to increase with Y 2:1:1 concentration. The appearance of the butterfly-shaped (or ‘‘fishtail’’) hysteresis loops indicates a Jc that is an increasing function of H (or B). Moreover, it has been demonstrated that the additional pinning leads to an increase in Ueff in an H-T region in which the butterfly is developed. The derived effective pinning energy is fit, from the instantaneous experimental relaxation data, to the relation, Ueff(J,T,H)=Ui[G(T)/Hn](Ji/J)μ, where Ui is the scale of the activation energy, G(T) =[1-(T/Tx)2]m, and Tx is close in value to Tirr(H) (the irreversibility line of the material). This description breaks down in the vicinity of the ‘‘butterfly’’ peak. We observed two power-law regimes of J dependence of Ueff which have μ values that agree qualitatively with the theoretical predictions (=7/9 and 3/2) for a three-dimensional flux-line lattice.
Phys. Rev. B 48, 13922 (1993)
Cited 38 times
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K. E. Sickafus, J. O. Willis, P. J. Kung, W. B. Wilson, D. M. Parkin, M. P. Maley, F. W. Clinard, C. J. Salgado, R. P. Dye, and K. M. Hubbard
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The critical current density Jc in Y0.9Gd0.1Ba2Cu3O7-x was found to increase relative to the unirradiated value following neutron irradiations in a mixed-spectrum reactor (total neutron fluences ranged between 1×1017 and 2×1018 n/cm2). Additional neutron irradiations of structurally similar GdBa2Cu3O7-x were carried out in either a highly thermalized or a pure fast-neutron environment (in the same reactor). This was done to determine whether enhancements in Jc are to be attributed to defects arising from interactions with thermal neutrons (En∼0.025 eV) or with fast neutrons (En>0.1 MeV). Magnetic-hysteresis measurements on these samples indicate that flux pinning (and thereby Jc) is enhanced by fast-neutron irradition, but not by thermal-neutron irradiation. On the other hand, the critical temperature Tc is significantly altered by exposure both to thermal and fast neutrons. It is proposed that thermal neutrons induce the formation of Frenkel pair defects on the rare-earth sublattice, but that these point defects do not serve as effective flux-pinning centers.
Phys. Rev. B 46, 11862 (1992)
Cited 1 times
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P. J. Kung, M. P. Maley, M. E. McHenry, J. O. Willis, J. Y. Coulter, M. Murakami, and S. Tanaka
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Magnetic hysteresis and flux creep characteristics in melt-powder-melt-growth YBa2Cu3O7 with Y2BaCuO5 inclusions were measured between 5 and 80 K for magnetic fields up to 5 T. The critical magnetization current densities which were calculated using the Bean model and the sample dimension show a weak dependence on magnetic field. The Jc values are of the order of 104 A/cm2 at 60 K over the investigated field range. The magnetic relaxation rate Q=-dM/d lnt first drops monotonically with increasing temperatures and then gradually saturates, which is similar to the behavior of the initial magnetization M0 versus temperature. The normalized relaxation rate S=d lnM/d lnt, plotted as a function of temperature, shows a maximum at around 30 K, and the corresponding values of S and T at the maximum are field dependent. A scaling relationship Ueff(J,H)=UiG(T)F(J/Ji)/H0.55, where G(T)=1-(T/Tx)2, F(J/Ji)∼(J/Ji)-n, and Ui and Ji are scaling constants, is proposed to fit the creep data from which a universal curve is attained. The characteristic temperature Tx for the scaling function G(T) is determined from the irreversibility line. The current-dependent behavior of Ueff obtained from this work agrees qualitatively with the result predicted by the theory of collective flux creep and suggests a vortex-glass state at low current density.
Phys. Rev. B 46, 6427 (1992)
Cited 33 times
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M. P. Maley, P. J. Kung, J. Y. Coulter, W. L. Carter, G. N. Riley, and M. E. McHenry
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We have measured the dependence of the transport critical current density on magnetic field and temperature of a high-Jc Bi-Sr-Ca-Cu-O/Ag tape sample. At low temperature, Jc>104 A/cm2 extending to high fields as previously reported by several groups. For T>20 K and with the applied field parallel to the c axis Jc declines precipitously with increasing field and temperature, reflecting the properties of intragranular pinning. The variation of Jc with the angle between B and the tape normal is consistent with a two-dimensional model of the vortex lattice. Independent determination of Jc by magnetic hysteresis measurement shows rough agreement with transport Jc’s at low fields but falls below by a factor that increases with increasing field and temperature. This can be accounted for by a model for thermally activated flux motion.
Phys. Rev. B 45, 7566 (1992)
Cited 32 times
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