2009 METALS, SUPERCONDUCTORS...Magnetic torque experim<strong>en</strong>ts on the magnetic-field-induced organicsuperconductor λ-(BETS) 2 FeCl 4Layered organic superconductors have upper critical fieldsexceeding the theoretical Pauli limit for superconductivitywh<strong>en</strong> the magnetic field is applied parallel to the layers.Theory predicts th<strong>en</strong> the possibility of a Fulde-Ferrel-Larkin-Ovchinnikov (FFLO) superconducting state[Fulde and Ferrel, Phys. Rev. 135, A550 (1964);Larkin and Ovchinnikov, Sov. Phys. JETP 20, 762(1965)]. Besi<strong>des</strong> κ-(BEDT-TTF) 2 Cu(NCS) 2 , the two dim<strong>en</strong>sionalfield-induced superconductor λ-(BETS) 2 FeCl 4 ,where BETS is bis(ethyl<strong>en</strong>edithio)tetrasel<strong>en</strong>afulval<strong>en</strong>e, is acandidate which fulfils all necessary conditions. Wh<strong>en</strong> themagnetic field is applied parallel to the metallic layers, asuperconducting phase appears above 17 T below 1 K.In our first experim<strong>en</strong>t we focused on the critical field at17 T. Figure 98 shows torque data tak<strong>en</strong> at differ<strong>en</strong>t temperaturesduring field sweeps. Surprisingly, a broad kinklikeanomaly appears only above 22 T indicating the transitioninto the field-induced superconducting state. Below200 mK a pronounced hysteresis appears. The experim<strong>en</strong>tsshow no evid<strong>en</strong>ce for additional phase transitions withinthe superconducting state. The phase diagram clearly differsfrom that reported by Uji et al. A misalignm<strong>en</strong>t of thesample can be ruled out. A possible explanation may befound in the rather rapid cooling conditions in our experim<strong>en</strong>twhich is known to cause anion-disorder effects in 1Dorganic superconductors. The result stimulates further experim<strong>en</strong>tsunder more controlled experim<strong>en</strong>tal conditions.This field-induced superconductivity is well understoodin the framework of the Fischer theory, based on theJaccarino-Peter effect. Uji et al. reported possible FFLOstates at the two critical fields based on dip structures inthe resistivity [Uji et al., Phys. Rev. Lett. 97, 157001(2006) and refer<strong>en</strong>ces therein]. This motivated us to lookfor a thermodynamic phase transition betwe<strong>en</strong> the homog<strong>en</strong>eoussuperconducting phase and the FFLO states bymeans of magnetic torque experim<strong>en</strong>ts using a capacitancecantilever technique. The probe was equipped with a rotator,which allowed us to align the layers parallel to the fielddirection with a precision of 0.001 ◦ . Single crystals of λ-(BETS) 2 FeCl 4 were grown by the standard electrochemicaloxidation technique.Figure 98: Magnet torque of λ-(BETS) 2 FeCl 4 is plotted as afunction of field at differ<strong>en</strong>t temperatures.I. SheikinR. Lortz (The Hong Kong University of Sci<strong>en</strong>ce and Technology, Kowloon, Hong Kong), Y. Nakazawa ( University ofOsaka, Osaka, Japan), B. Zhou, A. Kobayashi, H. Kobayashi (Nihon University, Tokyo, Japan)71
METALS, SUPERCONDUCTORS... 2009Temperature and magnetic field dep<strong>en</strong>d<strong>en</strong>ce of domain wall width and periodof Condon domain structure in AgDiamagnetic instability of electron gas in normal metals underquantizing magnetic field and low temperature is a resultof strong electron correlations induced by the magneticfield. It gives rise to a phase transition with formation ofcomplex domain patterns (Condon domains).hysteresis in magnetization curves, exist<strong>en</strong>ce of persist<strong>en</strong>tcurr<strong>en</strong>ts which results in a discontinuity of magnetic inductionalong the interface boundaries of regular domainpatterns. Still, there remain op<strong>en</strong> fundam<strong>en</strong>tal questionsrelated to the formation of Condon domain phase. As anexample, the important information about the size of thedomains, the domain wall width and surface <strong>en</strong>ergy of theinterface boundaries is still lacking. In our studies [N. Logoboyand W. Joss, Solid State Comm. 149, 2007 (2009)]we offer a way to calculate the expected values of domainwall width and period of the domain structure by means ofmeasurem<strong>en</strong>t of the value of the jump of magnetic inductionat the domain wall δB (figure 99 and figure 100).Figure 99: Temperature dep<strong>en</strong>d<strong>en</strong>ce of the DW width δ (a) andperiod of the domain structure D (b) at the conditions of the experim<strong>en</strong>t[Kramer et al., Phys. Rev. Lett. 95, 267209 (2005)].The solid lines correspond to the theory, the circles are calculatedfrom the temperature dep<strong>en</strong>d<strong>en</strong>ce of the measured jump of magneticinduction at the interface boundaries.The diamagnetic phase transition has received rec<strong>en</strong>tlymuch att<strong>en</strong>tion due to a number of unusual ph<strong>en</strong>om<strong>en</strong>a forthe physics of diamagnetism, e.g. formation of complexbranch structures, strong dep<strong>en</strong>d<strong>en</strong>ce of magnetic phase diagramson Fermi-surface topology, pres<strong>en</strong>ce of diamagneticFigure 100: Magneticfield dep<strong>en</strong>d<strong>en</strong>ce of the DW width δ (a)and period of the domain structure D (b) at the conditions of theexperim<strong>en</strong>t [Kramer et al., Phys. Rev. Lett. 95, 267209 (2005)].The solid lines correspond to the theory, the circles are calculatedfrom the temperature dep<strong>en</strong>d<strong>en</strong>ce of the measured jump of magneticinduction at the interface boundaries.W. JossN. Logoboy (The Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem, Israel and The Instituteof Superconductivity, Departm<strong>en</strong>t of Physics, Bar-Ilan University, Ramat-Gan, Israel)72
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LABORATOIRE NATIONAL DES CHAMPS MAG
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TABLE OF CONTENTSPreface 1Carbon Al
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Coexistence of closed orbit and qua
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2009PrefaceDear Reader,You have bef
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2009 CARBON ALLOTROPESInvestigation
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2009 CARBON ALLOTROPESPropagative L
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2009 CARBON ALLOTROPESEdge fingerpr
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2009 CARBON ALLOTROPESObservation o
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2009 CARBON ALLOTROPESImproving gra
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2009 CARBON ALLOTROPESHow perfect c
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2009 CARBON ALLOTROPESTuning the el
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2009 CARBON ALLOTROPESElectric fiel
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- Page 84 and 85: 2009 MAGNETIC SYSTEMSY b 3+ → Er
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- Page 108 and 109: 2009 APPLIED SUPERCONDUCTIVITYMagne
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 PROPOSALSProposals for Magnet
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2009 PROPOSALSSpin-Jahn-Teller effe
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2009 PROPOSALSQuantum Oscillations
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2009 PROPOSALSThermoelectric tensor
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2009 PROPOSALSDr. EscoffierCyclotro
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2009 PROPOSALSHigh field magnetotra
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2009 THESESPhD Theses 20091. Nanot
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2009 PUBLICATIONS[21] O. Drachenko,
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2009 PUBLICATIONS[75] S. Nowak, T.
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Contributors of the LNCMI to the Pr
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Institut Jean Lamour, Nancy : 68Ins
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Lawrence Berkeley National Laborato