Bibliografías temáticas / Field-dependent specific heat C(T,H)

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Literatura académica sobre el tema "Field-dependent specific heat C(T,H)"

Autor: Grafiati
Publicado: 25 de mayo de 2024
Última modificación: 31 de julio de 2025

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Artículos de revistas sobre el tema "Field-dependent specific heat C(T,H)"

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HAGIWARA, M., H. TSUJII, C. R. ROTUNDU, et al. "FIELD-INDUCED TOMONAGA–LUTTINGER LIQUID OF A QUASI-ONE-DIMENSIONAL S = 1 ANTIFERROMAGNET." Modern Physics Letters B 21, no. 16 (2007): 965–76. http://dx.doi.org/10.1142/s0217984907013626.

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We review the results of specific-heat experiments on the S = 1 quasi-one-dimensional (quasi-1D) bond-alternating antiferromagnet Ni(C 9 H 24 N 4)( NO 2) ClO 4, alias NTENP. At low temperatures above the transition temperature of a field-induced long-range order, the magnetic specific heat (C mag ) of this compound becomes proportional to temperature (T), when a magnetic field along the spin chains exceeds the critical field H c at which the energy gap vanishes. The ratio C mag /T, which increases as the magnetic field approaches H c from above, is in good quantitative agreement with a predict
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2

KIM, J. S., J. ALWOOD, P. KUMAR, and G. R. STEWART. "SPECIFIC HEAT ANOMALY FOR H ≥ 28.5 T IN CeIrIn5." International Journal of Modern Physics B 16, no. 20n22 (2002): 3014–17. http://dx.doi.org/10.1142/s0217979202013456.

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Recently Takeuchi reported a weak, 'metamagnetic-like' increase in the magnetization around 42 T in single crystals of CeIrIn 5 for field in the c-direction. We report specific heat measurements on single crystal CeIrIn 5, H parallel c-axis, measured in the dc hybrid magnet at NHMFL in Tallahassee between 1.4 and 10 K. A clear anomaly in C/T in 35 T is observed to peak at 1.8 K, with an entropy of 6% of RIn2. This anomaly grows in size and shifts upwards in temperature (both monotonically) with increasing H until at 45 T T peak =4.1 K , with the entropy associated with the transition equal to
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3

Chauhan, Himanshu, Rohit Kumar, and G. D. Varma. "Study of anisotropy in the superconducting properties of FeTe0.55Se0.45 single crystal grown by the self-flux method." Superconductor Science and Technology 35, no. 4 (2022): 045003. http://dx.doi.org/10.1088/1361-6668/ac504d.

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Abstract We report anisotropy in the superconducting properties of FeTe0.55Se0.45 bulk single crystal synthesized via the self-flux method. We have performed magnetotransport, magnetic and heat capacity measurements on single crystals of same batch. The grown crystals have also been characterized by XRD, XPS and Raman measurements. The superconductivity at T C ∼ 14 K has been affirmed by the temperature-dependent resistivity, magnetic, and specific heat measurements. The anisotropy in the upper critical field (H C2), coherence length (ξ), and critical current density (J C) have been studied fr
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4

Kiefer, Dominik, Jens Gibmeier, and Andreas Stark. "Determination of Temperature-Dependent Elastic Constants of Steel AISI 4140 by Use of In Situ X-ray Dilatometry Experiments." Materials 13, no. 10 (2020): 2378. http://dx.doi.org/10.3390/ma13102378.

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In situ dilatometry experiments using high energy synchrotron X-ray diffraction in transmission mode were carried out at the high energy material science beamline P07@PETRAIII at DESY (Deutsches Elektronen Synchrotron) for the tempering steel AISI 4140 at defined mechanical loading. The focus of this study was on the initial tempering state ( f e r r i t e ) and the hardened state ( m a r t e n s i t e ). Lattice strains were calculated from the 2D diffraction data for different h k l planes and from those temperature-dependent lattice plane specific diffraction elastic constants ( D E C s ) w
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5

LU, JING, and LIYUAN ZHANG. "TWO-COMPONENT SUPERCONDUCTIVITY FOR DOPED FULLERENES." Modern Physics Letters B 10, no. 17 (1996): 823–29. http://dx.doi.org/10.1142/s0217984996000936.

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The combining mechanism of the itinerant carrier pair and the local carrier pair (two-component model) is considered for doped fullerenes. The superconducting transition temperature T c , penetration depth λ, coherent length ξ, thermodynamic critical field H c and specific heat jump ΔC/T c are calculated and there is overall consistency between the calculations and the experiments for both alkali-metal-doped fullerenes ( Na 3 C 60, K 3 C 60, Rb 3 C 60 and RbCs 2 C 60) and alkaline-earth doped fullerenes ( Ba 6 C 60).
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6

MA, Y. L., and X. X. DAI. "PHENOMENOLOGICAL IMPLICATIONS OF HIGH-Tc SUPERCONDUCTIVITY." International Journal of Modern Physics B 06, no. 14 (1992): 2499–519. http://dx.doi.org/10.1142/s0217979292001250.

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We develop a phenomenological model for high-T c superconductors. Some main features are emerging in copper oxides: characteristic quasi two-dimensional Cu-O planes, strong correlation of antiferromagnetism, existence of a vortex lattice structure, and observation of a small coherence length and a large penetration depth. These features indicate that the superconductive pair is reasonably constrained to a small volume in real space and may be conceived of as a string-carrying vortex, and therefore can be well simulated by the dual phenomenological local boson fields [Formula: see text] and Φ.
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7

Gouda, Kaiki, and Takashi Nishioka. "Angular-field magnetic phase diagram of b-plane at 4 K of YAlGe-type TbAlGe with zigzag-chain." Journal of Physics: Conference Series 2164, no. 1 (2022): 012072. http://dx.doi.org/10.1088/1742-6596/2164/1/012072.

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Abstract Orthorhombic YAlGe-type TbAlGe is expected to have an interesting magnetic anisotropy due to zigzag chains of the Tb ions. We have grown the single crystal for the first time and measured the AC magnetic susceptibility and specific heat from 1.3 K to 60 K, and the vector magnetization for the b-plane up to 7 T at 4 K. The specific heat and AC magnetic susceptibility indicate that there are two antiferromagnetic transitions at T N1 = 38 K and TN2 = 7.6 K, where the transition at T N2 is first-order like. The magnetization curve at 4 K for the a-axis shows a large hysteresis, and metama
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8

Volkova, Olga S., Abdellali Hadj-Azzem, Gyorgy Remenyi, et al. "Magnetic Phase Diagram of van der Waals Antiferromagnet TbTe3." Materials 15, no. 24 (2022): 8772. http://dx.doi.org/10.3390/ma15248772.

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Terbium tritelluride, TbTe3, orders antiferromagnetically in three steps at TN1 = 6.7 K, TN2 = 5.7 K, and TN3 = 5.4 K, preceded by a correlation hump in magnetic susceptibility at T* ~8 K. Combining thermodynamic, i.e., specific heat Cp and magnetization M, and transport, i.e., resistance R, measurements we established the boundaries of two commensurate and one charge density wave modulated phases in a magnetic field oriented along principal crystallographic axes. Based on these measurements, the magnetic phase diagrams of TbTe3 at H‖a, H‖b and H‖c were constructed.
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9

Suyama, Masahiro, Sunseng Pyon, Yasuhiro Iijima, Satoshi Awaji, and Tsuyoshi Tamegai. "Trapping a magnetic field of 17.89 T in stacked coated conductors by suppression of flux jumps." Superconductor Science and Technology 35, no. 2 (2022): 02LT01. http://dx.doi.org/10.1088/1361-6668/ac4560.

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Abstract We have successfully trapped a field of 17.89 T at 6.5 K at the center of a compact coated-conductor (CC) stacks (13 × 12 × 11.7 mm3) within 75 min by suppressing flux jumps. The CC stack consists of 200 sheets of EuBa2Cu3O7 CCs with BaHfO3 nanorods to increase the critical current density at high fields and low temperatures. To enhance thermomagnetic stability, the central 50 CCs are coated with 1 µm thick Pb with large specific heat at low temperatures. Numerical calculations based on the actual J c–H characteristics reproduces the trapped field quantitatively. New directions for ac
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10

Fonseca Jr., J. G., and P. S. Schneider. "COMPARATIVE ANALYSIS OF THE IAPWS-IF97 FORMULATION PERFORMANCE FOR THERMODYNAMIC PROPERTIES OF WATER ON A RANKINE CYCLE." Revista de Engenharia Térmica 3, no. 1 (2004): 52. http://dx.doi.org/10.5380/reterm.v3i1.3488.

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The present paper presents the computational implementation of the industrial
formulation of the thermodynamic properties of water at liquid and
steam phases, proposed by the International Association for the Properties
of Water and Steam, known as IAPWS-IF97. The validity field extends over
to temperatures T between 0ºC and 800°C, for pressures p up to 100 MPa.
Temperature T, specific volume v, specific enthalpy h, specific entropy s,
specific heat at constant pressure cp and constant volume cv, besides saturation
pressure ps, are calculated having a pair of
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Tesis sobre el tema "Field-dependent specific heat C(T,H)"

1

Umugabe, Gilbert. "Enhanced magnetoelastic coupling in bulk magnetoelectric composites prepared by Laser Heated Pedestal Growth." Electronic Thesis or Diss., Sorbonne université, 2019. http://www.theses.fr/2019SORUS502.

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Dans la recherche de matériaux magnétoélectriques (ME) présentant des performances ME élevées, nous étudions dans cette thèse certains mécanismes fondamentaux qui conduit au renforcement du couplage magnéto-élastique dans les composites MEs. Notre étude porte sur les composites particulaires 0-3 composés de phase magnétostrictive (MS) de CFO imbibée dans des matrices ferroélectriques (FE) suivantes : à base de Pb PZT, PMNPT et leur alternative sans plomb KNN et BTO. Nous démontrons que la technique Laser Heated Pedestal Growth (LHPG) peut être utilisé pour synthétiser des échantillons massives
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Capítulos de libros sobre el tema "Field-dependent specific heat C(T,H)"

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Bohren, Craig F., and Bruce A. Albrecht. "Specific Heats and Enthalpy." In Atmospheric Thermodynamics, 2nd ed. Oxford University PressOxford, 2023. http://dx.doi.org/10.1093/oso/9780198872702.003.0003.

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Abstract Thermodynamics is based on impossible processes (adiabatic, reversible, isothermal) and nonexistent entities (perfect insulation, ideal gases) but must pass tests of consistency and agreement with experiment. ∂U/∂T defines a heat capacity C at constant volume or pressure per unit mass, volume, or mole number. C requires an equation of state U(p,V), either from microscopic theory or macroscopic measurements. A reversible adiabatic process (Q = 0) undergone by an ideal gas yields the Poisson relations between any two variables, for example, pressure and volume. pV is constant in isother
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Actas de conferencias sobre el tema "Field-dependent specific heat C(T,H)"

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Muñoz, David. "New strategies in proprioception’s analysis for newer theories about sensorimotor control." In Systems & Design 2017. Universitat Politècnica València, 2017. http://dx.doi.org/10.4995/sd2017.2017.6903.

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Abstract Human’s motion and its mechanisms had become interesting in the last years, where the medecine’s field search for rehabilitation methods for handicapped persons. Other fields, like sport sciences, professional or military world, search to distinguish profiles and ways to train them with specific purposes. Besides, recent findings in neuroscience try to describe these mechanisms from an organic point of view. Until now, different researchs had given a model about control motor that describes how the union between the senses’s information allows adaptable movements. One of this sense is
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Informes sobre el tema "Field-dependent specific heat C(T,H)"

1

Shen, Gianetto, and Tyson. L52342 Development of Procedure for Low-Constraint Toughness Testing Using a Single-Specimen Technique. Pipeline Research Council International, Inc. (PRCI), 2011. http://dx.doi.org/10.55274/r0010687.

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Pipelines from remote frontier regions are increasingly required to have adequate resistance to large deformations such as that caused by ground movement. In response to this, �strain-based design"� has been developed to enable assessment of imperfections at applied strains beyond yield. In addition, it is proposed to take advantage of the increased apparent toughness of pipe under low constraint, such as girth weld imperfections under axial tension, compared with the high-constraint toughness measured in conventional tests such as ASTM E1290 [1]. Application of low-constraint testing has been
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