The BMV project : axion search with a pulsed magnet Status of the experiment Rémy Battesti Laboratoire National des Champs Magnétiques Pulsés Université.

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Transcription de la présentation:

The BMV project : axion search with a pulsed magnet Status of the experiment Rémy Battesti Laboratoire National des Champs Magnétiques Pulsés Université Paul Sabatier, CNRS Toulouse, France

The Biréfringence Magnétique du Vide project Laboratoire des Collisions Agrégats et Réactivité, Toulouse : B. Pinto da Souza (Ph-D student), C. Robilliard, J. Vigué, C. Rizzo. Laboratoire National des Champs Magnétiques Pulsés, Toulouse : S. Batut (Ph-D student), R. Battesti, O. Portugall, G. Rikken Laboratoire des Matériaux Avancés -VIRGO, Lyon : P. Ganau, A. Remillieux, C. Michel, L. Pinard, J-M. Mackowski. Astrophysical consequences Centre d’Etudes Spatiales du Rayonnement, Toulouse : G.F. Bignami, JF Olive

Photodiode Analysing prism Cavity mirrors (T~5-10 ppm) Polarising prism B0B0 laser Pulsed magnet Principle of the experiment

Experimental Challenge Relevant parameters : F = Finesse of the Optical Cavity L = Length of the Magnet = Laser Wavelength B = Magnetic Field and  s = Sensitivity QED Vacuum ellipticity : Reference experiment : PVLAS  B²L = 25 T²m  F =  modulation frequency 0.6 Hz  Ψs = /Hz 1/2 (arXiv:hep-ex/ )

The pulsed magnet

Magnetic field labs in Europe

One of the highest field in the world 77,3 T Generator 24 kV,14 MJ 65 kA current limitation

B1B1 B2B2 B I I  X coil geometry Goal : Transverse magnetic field B²L > 30 T²m B²L/I² = 2,5×10 -7 T²m/A² Design of the pulsed magnet : X-coil B(mT) B(mT) z(m)

Magnet prototype 25 cm G10 - copper wire - cool at liquid nitrogen temperature - cost ~ €

X coil Winding (5 hours) Test at liquid nitrogen temperature

Imax = A Vmax= V Bmax = 14,3 T B²Lmax = 28 T²m Last results

The cavity mirrors

Clean environments for our VIRGO mirrors Class 10 Class 1 Class 10 Class 100 Class 1  mounting the mirrors in barrels Class 10  inserting the mirror in the chamber Class 100  for the people to stand (fully equipped) (= 1 particle > 0.3  m per ft 3 )

Référence Original diffusion  12 mm (2002) Diffusion after 1st manipulation  12 mm (2004) Diffusion after cleaning  12 mm (2004) Diffusion after last manipulation  12 mm (2005) C02011/2 concave 8 m, incidence 0°, 1064 nm 8 ppm2500 ppm69 ppm67 ppm C02011/3 concave 8 m, incidence 0°,1064 nm 25 ppm3000 ppm120 ppm125 ppm C02011/5 concave 8 m, incidence 0°,1064 nm 15 ppm4200 ppm2300 ppm2100 ppm C02011/6 concave 8 m, incidence 0°,1064 nm 30 ppm4000 ppm75 ppm80 ppm Miroirs après Montage et Démontage sur la cavité réalisé en Novembre 2005 great improvement !

Clean room at LNCMP Set-up starting February 06

50 cm 2 m 2 m 90 polarizer mirror analyzer Cavity set-up Xcoil+ cryostat Xcoil+ cryostat

Sensitivity

 S sensitivity We can reasonably expect Ellipticity modulated at frequency 2 b > 100 Hz PVLAS BMV time (ms) ellipticity Realistic estimation (with PVLAS results) Ph-D thesis G. Ruoso  S ~ /√Hz Shot noise

Conclusion Goal for 2006 :  B²L = 30 T²m  finesse =  Ψs = /Hz 1/2 Magnet is ready Mirrors of the cavity have been tested Our sensitivity is sufficient Build the experiment and take the first datas Parameters :

Conclusion Goal for 2007 : m a (eV) M a (GeV) Brookhaven, 1993 BMV

Perspectives  25 T over 1.5 m  finesse QED effect Feasability study for Mega Gauss generator at LNCMP destructive coil : 300 T over 10 cm photoregeneration experiment Astrophysical observations : GLAST telescope 2007 PRL 94, , 2005 and PRL 95, ,2005