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In high-frequency pulsed magnets, such as kickers in particle accelerators, it is essential to reduce eddy currents that could be induced in the magnet core during excitation not to distort and attenuate the magnetic field pulse. A novel iron lamination scheme with additional interlaminar insulation is proposed for the magnet core of such pulsed magnets. A laminated steel sheet core is formed by alternately stacking thin steel and insulation sheets. For application to matched kicker magnets for accelerators, test magnets with the new and conventional iron lamination were designed, assembled, and extensively evaluated. The pulsed magnetic field waveforms of two test magnets with the new lamination successfully matched to below 0.1% over the entire pulse duration, which was significantly better than those with the conventional lamination. Among the applications of the developed high-frequency pulsed magnets, beam injection kickers for the coming next generation light sources and future colliders, where suppression of the transient stored-beam oscillation during beam injection is crucial, are considered to be promising.
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Nematicity is ubiquitous in the electronic phases of iron-based superconductors. The order parameter that characterizes the nematic phase has been investigated in momentum space, but its real-space arrangement remains largely unexplored. We use linear dichroism (LD) in a low-temperature laserphotoemission electron microscope to map out the nematic order parameter of nonmagentic FeSe and antiferromagnetic BaFe2(As0.87P0.13)2. In contrast to structural domains, which have atomic-scale domain walls, the LD patterns in both materials show peculiar sinusoidal waves of electronic nematicity with wavelengths more than 1000 times as long as the unit cell. Our findings put strong constraints on the theoretical investigation of electronic nematicity.
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Two-dimensional electron gases at oxide surfaces or interfaces show exotic ordered states of matter, like superconductivity, magnetism or spin-polarized states, and are a promising platform for alternative oxide-based electronics. Here we directly image a dense population of randomly distributed ferromagnetic domains of â¼40 nm typical sizes at room temperature at the oxygen-deficient surface of SrTiO3, a non-magnetic transparent insulator in the bulk. We use laser-based photoemission electron microscopy, an experimental technique that gives selective spin detection of the surface carriers, even in bulk insulators, with a high spatial resolution of 2.6 nm. We furthermore find that the Curie temperature in this system is as high as 900 K. These findings open perspectives for applications in nano-domain magnetism and spintronics using oxide-based devices, for instance through the nano-engineering of oxygen vacancies at surfaces or interfaces of transition-metal oxides.
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Using runway training procedure, three experiments examined effects of interrun interval (IRI) shift on serial pattern learning in rats. Series consisted of varying number of 0.045 g food pellets given in a goal box of a runway. Groups of rats were trained with 24-10-1-0 or 24-16-10-6-3-1-0 series (Experiment 1), 14-7-3-1-0 series (Experiment 2), and 18-12-6-3-1-0 or 18-7-7-7-1-0 series (Experiment 3), under either short (15-20 s) or long (5-15 min) IRI. In test phases, IRI was shifted from short to long or vice versa. Anticipation of 0 pellet was not disrupted by shortening of IRI, whereas lengthening of IRI eliminated the 0 pellet anticipation of the five- to seven-item monotonic series but did not eliminate that for the four-item series and the nonmonotonic series. These results suggest that rats learn a series with different strategies depending on IRI, pattern length, or structural complexity of a series.
Assuntos
Aprendizagem por Associação/fisiologia , Corrida/fisiologia , Aprendizagem Seriada/fisiologia , Animais , Condicionamento Operante , Masculino , Ratos , Ratos Sprague-Dawley , Recompensa , Fatores de TempoRESUMO
Two experiments using rats as subjects examined effects of item-arrangement on acquisition and extinction in serial learning. In Experiment 1, Group A received series of 16-0-16 and 1-0-1 food pellets in a runway, while Group D received 1-0-16 and 16-0-1 series. Both groups manifested a remote anticipation of the third item on Run 2, and current anticipation of the third item on Run 3. In extinction phase, resistance was greater in Group D than Group A. These results indicate that the first item signaled not only the second item, but also the third item. In Experiment 2, two of the four groups were trained with either of the following monotonic series: 0-16-0-8-0-4- 0-2-0-1 (Group M16) or 0-1-0-2-0-4-0-8-0-16 (Group M1), while the other two groups were given one of the following nonmonotonic series: 0-16-0-2-0-4-0-8-0-1 (Group NM16) or 0-1-0-8-0-4-0-2-0-16 (Group NM1). In extinction phase, Group M16 showed the least resistance. These results are discussed mainly on the basis of remote association view and structural complexity theory of serial learning.
Assuntos
Extinção Psicológica/fisiologia , Reforço Psicológico , Aprendizagem Seriada/fisiologia , Animais , Masculino , Ratos , Ratos Sprague-DawleyRESUMO
Investigation of the non-equilibrium dynamics after an impulsive impact provides insights into couplings among various excitations. A two-temperature model (TTM) is often a starting point to understand the coupled dynamics of electrons and lattice vibrations: the optical pulse primarily raises the electronic temperature T(el) while leaving the lattice temperature T(l) low; subsequently the hot electrons heat up the lattice until T(el) = T(l) is reached. This temporal hierarchy owes to the assumption that the electron-electron scattering rate is much larger than the electron-phonon scattering rate. We report herein that the TTM scheme is seriously invalidated in semimetal graphite. Time-resolved photoemission spectroscopy (TrPES) of graphite reveals that fingerprints of coupled optical phonons (COPs) occur from the initial moments where T(el) is still not definable. Our study shows that ultrafast-and-efficient phonon generations occur beyond the TTM scheme, presumably associated to the long duration of the non-thermal electrons in graphite.
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We report the characterization of a quasi-phase-matched second-harmonic generation device in LiTaO(3) that has a periodically domain-inverted region and a proton-exchanged channel waveguide. A blue-light power of 2.4 mW was obtained at a 424-nm wavelength. The observed temperature bandwidth for FWHM power is approximately 3 degrees C-cm, which is three times wider than that in a similar device in LiNbO(3). It is also shown that diffraction-limited focusing of the generated blue light may be obtained.
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We have demonstrated, for the first time to our knowledge, periodic poling of a 2-mm-thick near-stoichiometric LiTaO(3) substrate and its operation in a nanosecond optical parametric oscillator. Because the coercive field of stoichiometric LiTaO(3) is ~2 kV/mm , which is approximately one tenth that of the conventional congruent field, periodic poling of thicker stoichiometric substrates was successfully performed by means of an electric-field poling process at room temperature. The performance of a parametric oscillator with a 1-mm-thick sample was compared with that of the oscillator with the periodically poled congruent oscillator. The stoichiometric device exhibited better performance.
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The first known demonstration of tunable terahertz-wave generation by difference-frequency generation of dual signal-wave quasi-phase-matched optical parametric oscillation was performed with periodically poled LiNbO(3) (PPLN) with a series of gratings. An organic ionic salt, 4-dimethylamino-N-methyl-4-stilbazolium-tosylate (DAST), was used as a nonlinear crystal. A compact terahertz-wave source resulted, and changing the temperature of the PPLN permitted the wavelength to be varied from 120 to 160 microm. The wavelength could be tuned from 100 to 700 microm by proper selection of combinations of periodically poled gratings.
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ZBP-89 is a Krüppel-type zinc finger protein that binds to the gastrin EGF response element (gERE). Sp1 binds to the same DNA element and transactivates gastrin promoter activity, whereas ZBP-89 competes for Sp1 binding and prevents EGF induction. Both transcription factors mediate growth factor signals originating from the EGF receptor and thus were studied in normal and neoplastic tissues or cell lines. When compared to normal tissue from the same patient, ZBP-89 protein expression was increased in neoplastic tissue from the stomach antrum and in malignant cell lines. RT-PCR analysis of ZBP-89 mRNA correlated with protein overexpression. Immunocytochemical studies confirmed that ZBP-89 expression is elevated in neoplastic tissue and chronic gastritis, whereas Sp1 expression was nearly unchanged. These results suggest that the transcription factor ZBP-89, like Sp1, may be a marker for neoplastic transformation in some gastric cancers.
Assuntos
Proteínas de Ligação a DNA/genética , Neoplasias Gástricas/genética , Dedos de Zinco , Células Cultivadas , Humanos , Imuno-Histoquímica , Fator de Transcrição Sp1/metabolismo , Neoplasias Gástricas/metabolismo , Células Tumorais CultivadasRESUMO
In recent years widely tunable terahertz- (THz-) wave generation from LiNbO(3) optical parametric oscillators (OPO's) has been successfully demonstrated by use of the prism output-coupler method. However, there remains a problem of large absorption loss for generated terahertz waves inside the crystal, so we investigated the cryogenic characteristics of the OPO. We achieved 125-times-higher THz-wave output and 32% reduction of the generation threshold by cooling the crystal to 78 K. This scheme also provides direct loss measurement at THz frequency, and we found that the THz-wave enhancement mechanism is improvement of the gain as well as the reduction of the absorption coefficient.
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Greater than 6-microm-oscillation was demonstrated by means of optical parametric oscillation with periodically poled LiNbO3 (PPLN). The interaction length and thickness were 40 mm and 500 microm. The pump source used was a Q-switched Nd:YAG laser with a pulse duration of 120 ns and a repetition rate of 1 kHz. The tuning ranges of the idler waves were 6.57-6.56, 6.22-6.12, and 6.06-5.94 microm for PPLN wafers of 20-, 21.3-, and 22-microm periods, respectively.
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A new alignment method for Helmholtz coils is proposed. This method is based on a probe, whose axis is the same as the alignment axis. This probe includes one magnetic sensor, whose position is slightly shifted from the probe axis, and which is set perpendicular to the axis. Using this probe, the tilt and shift of the magnetic centre of Helmholtz coils can be aligned to within an order of 0.1 mrad and 0.1 mm, respectively. Moreover, by this method, effects of terrestrial magnetism and tilt of the magnetic sensor can be removed from the measurement. This alignment method is presented along with an estimate of the alignment accuracy of the SPring-8 linac injector.
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Among nonlinear materials, the organic ionic salt crystal 4-dimethylamino- N -methyl-4-stilbazolium-tosylate (DAST) is known for its large nonlinearity. We generated a coherent terahertz (THz) wave, using DAST, from the difference frequency between two oscillating wavelengths of an electronically tuned Ti:sapphire laser. In LiNbO(3), LiTaO(3), KTiOPO(4), and GaP crystals, THz-wave generation was not observed under the same experimental conditions. This result proves the high efficiency of DAST crystals for generation of difference-frequency THz waves.
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Monitoring by means of blood and urine analysis for methanol was successfully applied in 32 male workers who were exposed to methyl methacrylate (MMA) monomer at 6 ppm as a geometric mean and at 112 ppm as the maximum. Measurement of time-weighted average (TWA) intensity of the vapor exposure was successfully conducted with a diffusive sampler with activated carbon cloth as an adsorbent. Methanol concentrations in whole blood, serum, and urine samples were measured by headspace gas chromatography. The methanol concentrations in the three biological samples collected at the end of 8-h workshifts related linearly with the TWA MMA vapor concentrations, with correlation coefficients of 0.8-0.9. Quantitative evaluation of MMA in vapor and of methanol in urine suggests that only 1.5% of MMA inhaled will be excreted in urine as methanol. There were no significant clinical symptoms or abnormal hematological or serum biochemical findings at this exposure level, except that some workers complained throat irritation and frequent cough and sputa. The results indicate that biological monitoring by analysis for methanol is sensitive enough to detect MMA exposure at levels at which no serious health effects are to be expected.