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Mise en page 1 - Laboratoire National des Champs Magnétiques ...

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2009 MAGNET DEVELOPMENT AND INSTRUMENTATIONMegagauss magnetic field g<strong>en</strong>erationThe year 2009 marks the first g<strong>en</strong>eration of a magneticfields in excess of 100 T at the Toulouse pulsed magnetfacility. The field has be<strong>en</strong> obtained with a Megagauss g<strong>en</strong>erator(1 Megagauss = 100 Tesla) making use of capacitordriv<strong>en</strong>single-turn coils to produce field pulses on a microsecondtimescale. The installation, originally developedat the Humboldt University in Berlin, betwe<strong>en</strong> 1993 and1997, has be<strong>en</strong> transferred to LNCMI-Toulouse in 2006.an improved cryostat permitting experim<strong>en</strong>ts at liquid-Hetemperature is underway.Prior to its recommissioning the g<strong>en</strong>erator has undergone amajor revision including the replacem<strong>en</strong>t of crucial compon<strong>en</strong>tsof the charge/discharge-circuit (60 kV charging supply,high-voltage switches) and the adaptation of remotecontroland security functions. In the second half of 2009the installation has be<strong>en</strong> tested at moderate charging voltagesof up to 35 kV with 80 % of the nominal capacitance(16 out of 20 capacitors available). These tests have giv<strong>en</strong>rise to the curr<strong>en</strong>t 100 T field record. The field trace isshown in figure together with a simple test measurem<strong>en</strong>t ofthe Faraday rotation in CdS sample.This technique for g<strong>en</strong>erating magnetic field is <strong>des</strong>tructive,in the s<strong>en</strong>se that the coil explo<strong>des</strong> outwards and has to bereplaced after each pulse. However, the setup can be surroundedby an absorbing material (wood) which retains coilfragm<strong>en</strong>ts, and notably prev<strong>en</strong>ts any fragm<strong>en</strong>ts bouncingback. This means that the sample, and cryostat are not <strong>des</strong>troyedduring the pulse. Replacing the coil is a simpleoperation which can be performed quickly, and without removingthe sample or cryostat. This makes this techniquesfor g<strong>en</strong>erating magnetic fields practical from the point ofview of the user since many field shots are possible per day.Indeed, operation is simpler than a classical nitrog<strong>en</strong> cooledpulsed magnet since it is not necessary to wait for the coilto cool after each shot. The price to pay however, is theextremely short pulse, with only around 1µs available fordata acquisition at the maximum of the pulse.Starting from January 2010 the g<strong>en</strong>erator will be operated atfull capacitance and initially with moderate charging voltagesnot exceeding 45 kV. This will permit the g<strong>en</strong>erationof fields in excess of 150 T with little or no risk of insulationfailure. At this point the g<strong>en</strong>erator will be used forfirst sci<strong>en</strong>tific experim<strong>en</strong>ts making use of an optical setupfor transmission measurem<strong>en</strong>ts in the mid-infrared rangethat has also be<strong>en</strong> installed in 2009. The construction ofFigure 171: (a) Magnetic field g<strong>en</strong>erated with a 12×12 mm 2 single-turncoil (inner diameter × axial l<strong>en</strong>gth) at a charging voltageof 35 kV. (b) Expanded view of the top of the magnetic field pulse.(c) Preliminary data of the Faraday rotation in a CdS sample todemonstrate the feasibility of the system for sci<strong>en</strong>tists.P.Y. Solane, F. Durantel, O. Portugall121

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