The Low Temperature Heat Capacity of Ni(CH3COO)2:4H20

The heat capacity of Ni(CH3COO)2:4H2O has been measured between 0.43 and 10.73K revealing a Schottky anomaly. An octahedral crystal field with axial and rhombic distortions plus spin-orbit interaction split the triplet ground state completely, the upper components lying 3.52K and 8.06K above the low...

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Hauptverfasser: Polgar,L. G, Friedberg,S. A
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Friedberg,S. A
description The heat capacity of Ni(CH3COO)2:4H2O has been measured between 0.43 and 10.73K revealing a Schottky anomaly. An octahedral crystal field with axial and rhombic distortions plus spin-orbit interaction split the triplet ground state completely, the upper components lying 3.52K and 8.06K above the lowest. The lattice contribution to C(p) is estimated. Comparison of the ground state splittings with those inferred from magnetic susceptibility data suggests the presence of a small interaction between Ni(++) ions. This is described by an antiferromagnetic molecular field coefficient A/k=+0.08K which may be largely of dipolar origin. (Author)
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An octahedral crystal field with axial and rhombic distortions plus spin-orbit interaction split the triplet ground state completely, the upper components lying 3.52K and 8.06K above the lowest. The lattice contribution to C(p) is estimated. Comparison of the ground state splittings with those inferred from magnetic susceptibility data suggests the presence of a small interaction between Ni(++) ions. This is described by an antiferromagnetic molecular field coefficient A/k=+0.08K which may be largely of dipolar origin. (Author)</description><language>eng</language><subject>ACETATES ; CRYOGENICS ; CRYSTAL DEFECTS ; HYDRATES ; LIGAND FIELDS ; MAGNETIC PROPERTIES ; MOLECULAR ENERGY LEVELS ; MOLECULAR FIELD THEORY ; NICKEL COMPOUNDS ; NICKEL(II) IONS ; Solid State Physics ; SPECIFIC HEAT ; SPIN ORBIT INTERACTIONS</subject><creationdate>1972</creationdate><rights>APPROVED FOR PUBLIC RELEASE</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,780,885,27567,27568</link.rule.ids><linktorsrc>$$Uhttps://apps.dtic.mil/sti/citations/AD0746113$$EView_record_in_DTIC$$FView_record_in_$$GDTIC$$Hfree_for_read</linktorsrc></links><search><creatorcontrib>Polgar,L. G</creatorcontrib><creatorcontrib>Friedberg,S. 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A</creatorcontrib><creatorcontrib>CARNEGIE-MELLON UNIV PITTSBURGH PA DEPT OF PHYSICS</creatorcontrib><collection>DTIC Technical Reports</collection><collection>DTIC STINET</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Polgar,L. G</au><au>Friedberg,S. A</au><aucorp>CARNEGIE-MELLON UNIV PITTSBURGH PA DEPT OF PHYSICS</aucorp><format>book</format><genre>unknown</genre><ristype>RPRT</ristype><btitle>The Low Temperature Heat Capacity of Ni(CH3COO)2:4H20</btitle><date>1972-05-15</date><risdate>1972</risdate><abstract>The heat capacity of Ni(CH3COO)2:4H2O has been measured between 0.43 and 10.73K revealing a Schottky anomaly. An octahedral crystal field with axial and rhombic distortions plus spin-orbit interaction split the triplet ground state completely, the upper components lying 3.52K and 8.06K above the lowest. The lattice contribution to C(p) is estimated. Comparison of the ground state splittings with those inferred from magnetic susceptibility data suggests the presence of a small interaction between Ni(++) ions. This is described by an antiferromagnetic molecular field coefficient A/k=+0.08K which may be largely of dipolar origin. (Author)</abstract><oa>free_for_read</oa></addata></record>
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subjects ACETATES
CRYOGENICS
CRYSTAL DEFECTS
HYDRATES
LIGAND FIELDS
MAGNETIC PROPERTIES
MOLECULAR ENERGY LEVELS
MOLECULAR FIELD THEORY
NICKEL COMPOUNDS
NICKEL(II) IONS
Solid State Physics
SPECIFIC HEAT
SPIN ORBIT INTERACTIONS
title The Low Temperature Heat Capacity of Ni(CH3COO)2:4H20
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