Relevant bibliographies by topics / Spin-frustrated Pyrochlores

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Academic literature on the topic 'Spin-frustrated Pyrochlores'

Author: Grafiati
Published: 4 June 2021
Last updated: 7 September 2023

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Journal articles on the topic "Spin-frustrated Pyrochlores"

1

Boldrin, D., and A. S. Wills. "Anomalous Hall Effect in Geometrically Frustrated Magnets." Advances in Condensed Matter Physics 2012 (2012): 1–12. http://dx.doi.org/10.1155/2012/615295.

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Geometrically frustrated conducting magnets display extraordinarily large anomalous Hall effects (AHEs) that could be used to realise materials required for the emerging field of spintronics. While the intrinsic Berry phase developed in collinear ferromagnets is well explained through the effects of spin-orbit interactions within the Karplus and Luttinger model, its origins in frustrated magnets are not. The direct space mechanism based on spin chirality that was originally applied to the pyrochlore Nd2Mo2O7appears unsatisfactory. Recently, an orbital description based on the Aharonov-Bohm eff
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2

Gardner, J. S., G. Ehlers, S. T. Bramwell, and B. D. Gaulin. "Spin dynamics in geometrically frustrated antiferromagnetic pyrochlores." Journal of Physics: Condensed Matter 16, no. 11 (2004): S643—S651. http://dx.doi.org/10.1088/0953-8984/16/11/011.

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3

Bonville, P. "Spin fluctuations in the magnetic phase of frustrated pyrochlores: Evidence and controversy." Journal of Physics: Conference Series 217 (March 1, 2010): 012119. http://dx.doi.org/10.1088/1742-6596/217/1/012119.

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4

Nandi, S., Y. M. Jana, D. Swarnakar, J. Alam, P. Bag, and R. Nath. "Magnetization process and specific heat properties of geometrically frustrated pyrochlores R 2 FeSbO 7 (R 3+ = Dy, Y) and spin-ice magnetic phase in Dy 2 FeSbO 7." Journal of Alloys and Compounds 714 (August 2017): 318–30. http://dx.doi.org/10.1016/j.jallcom.2017.04.160.

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5

Ueda, Hiroaki, Jun-Ichi Yamaura, Hiroyuki Mitamura, et al. "spin systems on frustrated pyrochlore lattice." Journal of Magnetism and Magnetic Materials 310, no. 2 (2007): 1275–79. http://dx.doi.org/10.1016/j.jmmm.2006.10.436.

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6

Petit, Sylvain, Solène Guitteny, Julien Robert, et al. "Spin dynamics in highly frustrated pyrochlore magnets." EPJ Web of Conferences 83 (2015): 03012. http://dx.doi.org/10.1051/epjconf/20158303012.

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7

Gaulin, B. D., J. N. Reimers, T. E. Mason, J. E. Greedan, and Z. Tun. "Spin freezing in the geometrically frustrated pyrochlore antiferromagnetTb2Mo2O7." Physical Review Letters 69, no. 22 (1992): 3244–47. http://dx.doi.org/10.1103/physrevlett.69.3244.

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8

Zheng, Yanzhen, Arkady Ellern, and Paul Kögerler. "A spin-frustrated cobalt(II) carbonate pyrochlore network." Acta Crystallographica Section C Crystal Structure Communications 67, no. 11 (2011): i56—i58. http://dx.doi.org/10.1107/s0108270111043605.

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9

Bramwell, S. T. "Spin Ice State in Frustrated Magnetic Pyrochlore Materials." Science 294, no. 5546 (2001): 1495–501. http://dx.doi.org/10.1126/science.1064761.

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10

Sheetal, A. Elghandour, R. Klingeler, and C. S. Yadav. "Field induced spin freezing and low temperature heat capacity of disordered pyrochlore oxide Ho2Zr2O7." Journal of Physics: Condensed Matter 34, no. 24 (2022): 245801. http://dx.doi.org/10.1088/1361-648x/ac5fd8.

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Abstract Spin ice materials are the model systems that have a zero-point entropy as T → 0 K, owing to the frozen disordered states. Here, we chemically alter the well-known spin ice Ho2Ti2O7 by replacing Ti sites with isovalent but larger Zr ion. Unlike the Ho2Ti2O7 which is a pyrochlore material, Ho2Zr2O7 crystallizes in disordered pyrochlore structure. We have performed detailed structural, ac magnetic susceptibility and heat capacity studies on Ho2Zr2O7 to investigate the interplay of structural disorder and frustrated interactions. The zero-field ground state exhibits large magnetic suscep
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