Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal
Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained...
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E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1998 |
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| Umfang: |
9 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: Journal of low temperature physics - 1969, 110(1998) vom: Mai/Juni, Seite 1003-1011 |
| Übergeordnetes Werk: |
volume:110 ; year:1998 ; month:05/06 ; pages:1003-1011 ; extent:9 |
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NLEJ197708595 |
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| 520 | |a Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. | ||
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| 700 | 1 | |a Borowiec, M. T. |4 oth | |
| 700 | 1 | |a Dyakonov, V. P. |4 oth | |
| 700 | 1 | |a Jedrzejczak, A. |4 oth | |
| 700 | 1 | |a Markovich, V. I. |4 oth | |
| 700 | 1 | |a Pavlyuk, A. A. |4 oth | |
| 700 | 1 | |a Szymczak, H. |4 oth | |
| 700 | 1 | |a Zubov, E. E. |4 oth | |
| 700 | 1 | |a Załeski, M. |4 oth | |
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(DE-627)NLEJ197708595 DE-627 ger DE-627 rakwb eng Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal 1998 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. Springer Online Journal Archives 1860-2002 Borowiec, M. T. oth Dyakonov, V. P. oth Jedrzejczak, A. oth Markovich, V. I. oth Pavlyuk, A. A. oth Szymczak, H. oth Zubov, E. E. oth Załeski, M. oth in Journal of low temperature physics 1969 110(1998) vom: Mai/Juni, Seite 1003-1011 (DE-627)NLEJ188996001 (DE-600)2016984-X 1573-7357 nnns volume:110 year:1998 month:05/06 pages:1003-1011 extent:9 http://dx.doi.org/10.1023/A:1022308115255 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 110 1998 5/6 1003-1011 9 |
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(DE-627)NLEJ197708595 DE-627 ger DE-627 rakwb eng Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal 1998 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. Springer Online Journal Archives 1860-2002 Borowiec, M. T. oth Dyakonov, V. P. oth Jedrzejczak, A. oth Markovich, V. I. oth Pavlyuk, A. A. oth Szymczak, H. oth Zubov, E. E. oth Załeski, M. oth in Journal of low temperature physics 1969 110(1998) vom: Mai/Juni, Seite 1003-1011 (DE-627)NLEJ188996001 (DE-600)2016984-X 1573-7357 nnns volume:110 year:1998 month:05/06 pages:1003-1011 extent:9 http://dx.doi.org/10.1023/A:1022308115255 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 110 1998 5/6 1003-1011 9 |
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(DE-627)NLEJ197708595 DE-627 ger DE-627 rakwb eng Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal 1998 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. Springer Online Journal Archives 1860-2002 Borowiec, M. T. oth Dyakonov, V. P. oth Jedrzejczak, A. oth Markovich, V. I. oth Pavlyuk, A. A. oth Szymczak, H. oth Zubov, E. E. oth Załeski, M. oth in Journal of low temperature physics 1969 110(1998) vom: Mai/Juni, Seite 1003-1011 (DE-627)NLEJ188996001 (DE-600)2016984-X 1573-7357 nnns volume:110 year:1998 month:05/06 pages:1003-1011 extent:9 http://dx.doi.org/10.1023/A:1022308115255 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 110 1998 5/6 1003-1011 9 |
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(DE-627)NLEJ197708595 DE-627 ger DE-627 rakwb eng Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal 1998 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. Springer Online Journal Archives 1860-2002 Borowiec, M. T. oth Dyakonov, V. P. oth Jedrzejczak, A. oth Markovich, V. I. oth Pavlyuk, A. A. oth Szymczak, H. oth Zubov, E. E. oth Załeski, M. oth in Journal of low temperature physics 1969 110(1998) vom: Mai/Juni, Seite 1003-1011 (DE-627)NLEJ188996001 (DE-600)2016984-X 1573-7357 nnns volume:110 year:1998 month:05/06 pages:1003-1011 extent:9 http://dx.doi.org/10.1023/A:1022308115255 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 110 1998 5/6 1003-1011 9 |
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(DE-627)NLEJ197708595 DE-627 ger DE-627 rakwb eng Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal 1998 9 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. Springer Online Journal Archives 1860-2002 Borowiec, M. T. oth Dyakonov, V. P. oth Jedrzejczak, A. oth Markovich, V. I. oth Pavlyuk, A. A. oth Szymczak, H. oth Zubov, E. E. oth Załeski, M. oth in Journal of low temperature physics 1969 110(1998) vom: Mai/Juni, Seite 1003-1011 (DE-627)NLEJ188996001 (DE-600)2016984-X 1573-7357 nnns volume:110 year:1998 month:05/06 pages:1003-1011 extent:9 http://dx.doi.org/10.1023/A:1022308115255 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 110 1998 5/6 1003-1011 9 |
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Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal |
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Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. |
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Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. |
| abstract_unstemmed |
Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ197708595</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210705223106.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070527s1998 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ197708595</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Magnetic Ordering of Dy3+ Ions in RbDy(WO4)2 Single Crystal</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1998</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">9</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The specific heat C(T) of the monoclinic RbDy(WO 4 ) 2 crystal has been studied at very low temperatures 0.2≤T≤1.9 K and in magnetic fields 0≤H≤0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = − 0.798 K. The C T) dependence below Neel temperature 0.5TN<T<0.99TN ) is well described by 2D Ising model, whereas in the temperature region close above TN (1.01 TN<T< 2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN diagrams for field H ‖ a are in a reasonable agreement for simple quadratic lattice.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Borowiec, M. T.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dyakonov, V. P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jedrzejczak, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Markovich, V. I.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Pavlyuk, A. A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Szymczak, H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zubov, E. E.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Załeski, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Journal of low temperature physics</subfield><subfield code="d">1969</subfield><subfield code="g">110(1998) vom: Mai/Juni, Seite 1003-1011</subfield><subfield code="w">(DE-627)NLEJ188996001</subfield><subfield code="w">(DE-600)2016984-X</subfield><subfield code="x">1573-7357</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:110</subfield><subfield code="g">year:1998</subfield><subfield code="g">month:05/06</subfield><subfield code="g">pages:1003-1011</subfield><subfield code="g">extent:9</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://dx.doi.org/10.1023/A:1022308115255</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SOJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">110</subfield><subfield code="j">1998</subfield><subfield code="c">5/6</subfield><subfield code="h">1003-1011</subfield><subfield code="g">9</subfield></datafield></record></collection>
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