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UID:DSC-9707
DTSTART;TZID=Europe/Berlin:20150716T100000
SEQUENCE:1437033640
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URL:https://www.dresden-science-calendar.de/calendar/en/detail/9707
LOCATION:IFW\, Helmholtzstraße 2001069 Dresden
SUMMARY:Thota: Magneto-structural Quantum Phases and Reentrant Magnetic Beh
 avior of Few Complex Spinels 
CLASS:PUBLIC
DESCRIPTION:Speaker: Dr. Subhash  Thota\nInstitute of Speaker: Indian Insti
 tute of Technology Guwahati (IIT Guwahati)\, Indien\nTopics:\nMaterialien\
 , Physik\n Location:\n  Name: IFW (D 2E.27\, IFW Dresden\, Helmholtzstraß
 e 20)\n  Street: Helmholtzstraße 20\n  City: 01069 Dresden\n  Phone: \n  
 Fax: \nDescription: Magnetic spinels\, generally isostructural with the mi
 neral spinel MgAl2O4\, are considered as important class of materials beca
 use of their potential applications such as in microwave-wave devices\, tr
 ansformer cores\, actuators\, thermistors and magnetic recording. Such app
 lications of magnetic spinels (AB2O4) combined with the interesting physic
 s resulting from a variety of distributions of magnetic ions between the t
 etrahedral ‘A’-sites and octahedral ‘B’-sites has kept the field o
 f spinels a very active area of research for many decades. Therefore\, the
  current talk is focused on two types of spinels namely (i) Hausmannite (M
 n3O4) and (ii) Cobalt Ortho-Stannate &amp\; Titanates (Co2TiO4 &amp\; Co2S
 nO4\,) which belong to tetragonally distorted spinels and inverse-spinel f
 amily\, respectively.1-4 Special emphasis will be given to Hausmannite whi
 ch exhibits giant-atomic-displacement associated with enormous magnetocrys
 talline anisotropy\, strong magneto-dielectric coupling\, and giant magnet
 ic-entropy change at the onset of the ferrimagnetic Néel temperature. Dur
 ing the first-half of the talk\, the low-temperature magnetostructural qua
 ntum phases of Mn3O4 system will be discussed in the light of our recent e
 xperimental findings.1\,3 The second part of the talk will be focused on t
 he reentrant magnetic behavior of two inverse spinels Co2SnO4 and Co2TiO4.
  Both of these systems exhibit co-existence of longitudinal ferrimagnetic 
 order below the Néel temperature TN = 41K (for Co2SnO4) and transverse sp
 in-glass (SG) state below TSG&amp\;#8201\; =&amp\;#8201\;39.1&amp\;#8201\;
 K (Co2SnO4) resulting from the presence of non-magnetic Sn4+ ions (or Ti4+
 ) on the B sites.2\,4 The origin of ferrimagnetic ordering in both the sys
 tems is suggested to result from different magnetic moments of Co2+ on the
  A sites (3.87&amp\;#8201\;&amp\;#956\; B) and B sites (4.16&amp\;#8201\;&
 amp\;#956\; B).4 The temperature variation of ac-magnetic susceptibilities
  (&amp\;#967\;&amp\;#8242\;(T) and &amp\;#967\;&amp\;#8243\;(T))\, and ant
 iferromagnetic molecular field constants together with the exchange-consta
 nts of both the inverse spinels will be discussed. The effect of various d
 oping elements on the global magnetic structure of Co2TiO4 \, Co2SnO4 and 
 Mn3O4  will be investigated at IFW-Dresden.    References: [1] M. Kim et. 
 al\, Phys. Rev. Lett. 104\, 136402 (2010). [2] S. Thota et. al. J. Phys.: 
 Condens. Matter\, 27\, 166001 (2015) [3] F. Guillou\, et. al. Phys. Rev. B
 \, 83\, 094423\, (2011) [4] S. Thota et al. J. Appl. Phys. 113\, 203905 (2
 013)
DTSTAMP:20260427T162726Z
CREATED:20150715T075258Z
LAST-MODIFIED:20150716T080040Z
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