Vacuum birefringence and dichroism signals in the PVLAS experiment Ugo Gastaldi, INFN-LNL Legnaro on behalf of the PVLAS Collaboration ICHEP’06 Moscow.

Slides:



Advertisements
Similar presentations
Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institut) HOMODYNE AND HETERODYNE READOUT OF A SIGNAL- RECYCLED GRAVITATIONAL WAVE DETECTOR.
Advertisements

Fundamentals of Photoelasticity
Lesson 17 Intro to AC & Sinusoidal Waveforms
P.-R. KettleMEG-Review February MEG Beam Line Studies  E5 Z-Branch NOW !!! NOW !!!
FARADAY ROTATION Gennady Voronov In this experiments we experimentally determine the Verdet constant of a glass rod with specification SF-59 to be rad/mT*cm.
AN ANOMALOUS CURVATURE EXPERIMENT Carol Y. Scarlett Brookhaven National Laboratory Apr. 27 th, 2006.
Polarization Techniques for Interferometer Control Peter Beyersdorf National Astronomical Observatory of Japan LSC March 2002 Advanced Configurations LIGO-G Z.
Undulator R & D Jim Clarke STFC Daresbury Laboratory, UK BAW-2 SLAC Jan 2011.
Status of g ray generation at KEK-ATF ► Introduction ► Status of the cavity R&D ► Out Look French Labs. : LAL (Orsay) in Collaboration with CELIA (Laser.
Tagger and Vacuum Chamber Assembly Procedure. Preassembly of second bottom yokes and poleshoes. a) Install special support. b) Place the second bottom.
c = km/sec I F = I 0 x (cosθ) 2.
Niels Bohr Institute Copenhagen University Eugene PolzikLECTURE 5.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
Circular Dichroism Part I. Introduction.
K. LaihemE166 collaboration LCWS06 Bangalore March 12th 2006 The E166 experiment Development of a polarized positron source for the ILC. Karim Laihem on.
X-ray Polarization as a Probe of Strong Magnetic Fields in X-ray Binaries Shane Davis (IAS) Chandra Fellows Symposium, Oct. 17, 2008.
PVLAS Day - Giuseppe Ruosowww.ts.infn.it/experiments/pvlas1 Gas measurements in the PVLAS experiment Giuseppe RUOSO INFN - Laboratori Nazionali di Legnaro.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
Status of g ray generation at KEK-ATF ► Introduction ► Status of the cavity R&D ► Out Look French Labs. : LAL (Orsay) in Collaboration with CELIA (Laser.
GWADW 2010 in Kyoto, May 19, Development for Observation and Reduction of Radiation Pressure Noise T. Mori, S. Ballmer, K. Agatsuma, S. Sakata,
HPS Test Run Setup Takashi Maruyama SLAC Heavy Photon Search Collaboration Meeting Thomas Jefferson National Accelerator Facility, May 26-27,
Status of R&D of Optical Cvities at KEK-ATF ►Introduction ►Status of the cavity R&D ►Out Look KEK, Hiroshima University LAL (Orsay) in Collaboration withCELIA.
The QED Vacuum Magnetic Birefringence (BMV) Experiment
MQXF Cold-mass Assembly and Cryostating H. Prin, D. Duarte Ramos, P. Ferracin, P. Fessia 4 th Joint HiLumi LHC-LARP Annual Meeting November 17-21, 2014.
___________________ Jürgen Schreiber, ECFA/DESY LC workshop, Amsterdam, April 1-4, 2003 BEAM ENERGY SPECTROMETER DESY – Dubna – TU Berlin Machine physicists,
Interferometer Topologies and Prepared States of Light – Quantum Noise and Squeezing Convenor: Roman Schnabel.
Book Reference : Pages To understand how we generate alternating current (A.C.) 2.To begin to appreciate some of the advantages of A.C.
Pure-state, single-photon wave-packet generation by parametric down conversion in a distributed microcavity M. G. Raymer, Jaewoo Noh* Oregon Center for.
LIPSS* and dark matter *LIght PseudoScalar boson Search K. McFarlane Hampton University 8-Mar-2006 for the LIPSS collaboration Supported by the National.
Environmental noise studies at VIRGO Environmental contributions to Virgo readout noise (C-runs) many sources identified through coherency analyses with.
Status of VIRGO Francesco Fidecaro (after Lisa Barsotti) - University and INFN Pisa – on behalf of the VIRGO collaboration Aspen - January 19 th, 2005.
Overview installation of Polarized Target 14th Crystal Ball Meeting
HD target.
1 Preparation for the 3 He Injection Test 11/2007 MIT/BATES D. Dutta*, H. Gao, M. Busch, Q. Ye, X. Qian, W. Zheng, X. Zhu ( Duke University) ASU, BU, Caltech,
Modern Optics PHY485F/1485F Robin Marjoribanks McLennan Physics 1104C
Radius To use a Compton polarimeter, the possible range of the backscattered photons’ energy should be calculated. Applying the laws of conservation of.
Low-frequency nuclear spin maser and search for atomic EDM of 129 Xe A. Yoshimi RIKEN SPIN /10/11-16 Trieste, ITALY Collaborator : K. Asahi (Professor,
1 Options for low energy spin manipulation Ken Moffeit, SLAC 2009 Linear Collider Workshop of the Americas 29 September to 3 October 2009 K. Moffeit, D.
1 CERN, 27 January 2009A. Lindner Ultra-light Particles beyond the Standard Model: Laboratory Experiments.
BNL - 21 Oct Recent Results From the PVLAS Experiment and Future Perspectives Guido Zavattini on behalf of the PVLAS collaboration Università di.
1 The Virgo noise budget Romain Gouaty For the Virgo collaboration GWADW 2006, Isola d’Elba.
Magnet vacuum vessel w/radiation shield and cold mass in place Magnet leads (left) and the three cryocoolers on the top of the spectrometer solenoid service.
A users viewpoint: absorption spectroscopy at a synchrotron Frithjof Nolting.
1 Yuri Shestakov Budker Institute of Nuclear Physics Novosibirsk, Russia Tagging system of almost-real photons for photonuclear experiments at VEPP-3 Moscow,
The status of VIRGO Edwige Tournefier (LAPP-Annecy ) for the VIRGO Collaboration HEP2005, 21st- 27th July 2005 The VIRGO experiment and detection of.
1 Collaboration Meeting 33 - Glasgow 26 th June 2012 Design Layout Andrew Moss for Alan Grant, STFC.
LIGHT PSEUDOSCALAR BOSONS, PVLAS AND DOUBLE PULSAR J Marco Roncadelli, INFN – Pavia (Italy)
22 October 2005MICE Meeting at RAL1 Tracker Solenoid Overview Michael A. Green Lawrence Berkeley Laboratory MICE Collaboration Meeting 22 October 2005.
November 19, 2008 SLAC Linear Collider Department Slide 1 ILC Superconducting Quadrupole Characterization J. C. Sheppard, Cherrill Spencer, et al. SLAC.
Results and perspectives of the solar axion search with the CAST experiment Esther Ferrer Ribas IRFU/CEA-Saclay For the CAST Collaboration Rencontres de.
Kerr Effect-based Measurement of the Electric Field
Compton Experiment at ATF DR 2009 Summary and Plan ATF2 Project Meeting 15-Dec-2009 T. Omori (KEK) for collaborators.
A liner in the Corrector package A Cu liner has been inserted in the gap between the CBT and the coil aperture of all the corrector package elements (see.
Spoke section of the ESS linac: - the Spoke cryomodules - the cryogenic distribution system P. DUTHIL (CNRS-IN2P3 IPN Orsay / Division Accélérateurs) on.
Stereo Collab Meeting | CEA Saclay July-2015 Conclusions.
SuperB Meeting XVII May 28 – June 2, 2011 IR design status 1 IR Design Status and Update M. Sullivan For M. Boscolo, K. Bertsche, E. Paoloni, S. Bettoni,
Ion Accelerator Activities at VECC
Arun Saini, N. Solyak Fermi National Accelerator Laboratory
X-ray telescope: D. Greenwald, R. Kotthaus, G. Lutz
Progress toward squeeze injection in Enhanced LIGO
INSTALLATION SEQUENCE
M. Boscolo, K. Bertsche, E. Paoloni, S. Bettoni,
Status of the TESLA Magnet Package and Vibrations at TTF
Electricity from Magnetism
Emidio Gabrielli Helsinki Institute of Physics
ERL accelerator review. Parameters for a Compton source
Strong Coupling of a Spin Ensemble to a Superconducting Resonator
PROGRESS TOWARDS AN OPEN MIDPLANE SEPARATION DIPOLE
Marco Roncadelli, INFN – Pavia (Italy)
Measurement of Parity-Violation in the N→△ Transition During Qweak
Presentation transcript:

Vacuum birefringence and dichroism signals in the PVLAS experiment Ugo Gastaldi, INFN-LNL Legnaro on behalf of the PVLAS Collaboration ICHEP’06 Moscow Introduction DYCHROISMPRL96,110406(2006) vacuum B induced rotation BIREFRINGENCEQCD-06 and ICHEP-06 vacuum B induced ellipticity Ellipticity measurements PHASE and AMPLITUDE calibrations with gases VACUUM Measurements Outcome VACUUM BIREFRINGENCE has OPPOSITE SIGN of He, Ne,… Birefringence m= meV M= GeV 0++ boson responsible??? Prospects CONFIRM LIGHT BOSON INTERPRETATION by REGENERATION measurements REDUCE NOISE INCREASE DUTY CYCLE PRECISE MEASUREMENTS OF m by changing magnet length

PVLAS Collaboration (Trieste, Pisa, Legnaro, Frascati, Ferrara) : from left to right E.Polacco, E.Milotti, E.Zavattini, R.Cimino, G.Cantatore, S.Marigo, U.Gastaldi, G.Petrucci and A.Zanetti standing G.Zavattini, M.Karuza, G.Ruoso, G.DiDomenico and F.DellaValle seated (S.Carusotto, G.Raiteri and P.Temnikov are not in the picture)

PVLAS EXPERIMENT SITE MAGNET ELLIPSOMETER Fabry-Perot CAVITY MODULATIONS FINESSE ELLIPTICITY CONTROLS OPERATIONS

PVLAS site: two opposite walls of the square pit support the concrete beam (with turntable and cryostat on top) pit floor and pit walls rest on separate foundations

PVLAS top optical bench resting on 4 granite pillars that surround the (rotating) cryostat (with superconducting magnet inside)

Ne run1049_1

N 2 run1110_0

He run1161_0

Ne run1187_0

Run 807_1 Vacuum IR light

run945_5V Vacuum IR light

Run 1101_0 Vacuum Green light

run1137_0 Vacuum Green light

Run 1166_0 Vacuum Green light

run1167_0 Vacuum Green light

November 2005: N 2 +Ne + Vacuum

November 2005: N 2 +He + Vacuum

PVLAS: Vacuum, N 2 and Ne ellipticity phases of runs

PVLAS 1064nm light ISOELLIPTICITY and ISOROTATION curves in (m,M) plane

Physics outcome DICHROISM(IR) amplitude circa (published in PRL2006) ELLIPTICITY(IR) amplitude circa , phase opposite to CME(He, Ne) ELLIPTICITY(Gr) amplitude amplitude circa , phase opposite to CME(He, Ne) If effects observed truly generated mostly by quantum vacuum effects and not by apparatus If microscopic interpretation in terms of existence of ultralight bosons coupled to two photons valid If ultralight bosons have spin zero and only one sort present Phase opposite to CME(noble gases) tells bosons are scalars 0++ m= meV M= GeV

PVLAS oasis in desert of (m,1/M) plane main question: oasis or mirage???

PROSPECTS Confirm LIGHT BOSON interpretation regeneration measurements (in parallel to polarization measur.s) with permanent magnet (beeing purchased to be installed below ellipsometer) Reduce NOISE AMAGNETIC ACCESS STRUCTURE beeing installed PERMANENT MAGNETS planned in place of superconducting m. (no rotating stray field on FP mirrors and other optics elements) Improve SIGNAL Increase DUTY CICLE with permanent magnets (no cryo. constraints) Measure m accurately by changing length L of magnetized volume (in polarization and regeneration measurements)

PVLAS after June 2006 removal of Fe access structure around the vertical granite support of the top optical bench, that surrounds the cryostat

W=20 mwatt out of FP N= in FP, give photons sec-1 passing through PVLAS magnet C= conversion probability in PVLAS magnet 1m long 5.5 Tesla bosons sec-1 boson beams R=16/(4x7.5) reconversion prob. in permanent magnet 0.5m long 2 Tesla expect photons sec-1 regenerated in perm. mag

PVLAS superconducting Morpurgo magnet (assembled with vertical bore) before insertion into warm bore cryostat

Run 1092_0_2 SOM 90 Vacuum B=0

Run 1091_1 Vacuum SOM 90 B=4.35 Tesla Run 1092_0_2 Vacuum SOM 90 B=0 Tesla

B2 dependance of 2omegam signal

Run1091_0 SOM 90 Run1084_0 SOM 0

November 2005, 1ω M peak : N 2 +Ne + Vacuum

November 2005, 1ω M peak : N 2 +He + Vacuum

References Iacopini and Zavattini PL85B(1979)151 Maiani, Petronzio and Zavattini PL B175(1986)359 Raffelt and Stodolsky PR D37 (1988)1237 Cameron et al. (BFST Collab.) PR D47(1993)3707 Rizzo et al. IRPC 16 (1997) 81 and refs. therein Zavattini et al (PVLAS Collab.) PRL 96(2006) Gastaldi arXiv:hep-ex/ (2006) and refs. therein

October 2004: Ne + Vacuum

December 2004: Ne + Vacuum

May 2005: Ne + Vacuum

October 2004, 1ω M peak: Ne + Vacuum

December 2004, 1ω M peak : Ne + Vacuum

May 2005, 1ω M peak : Ne + Vacuum

B dependence: Oct. 2004, Ne 18mbar 2 ω M peak1 ω M peak B2B2 B2B2 B4B4

B dependence: Dec. 2004, Vacuum B2B2 B4B4

PVLAS 532nm and 1024nm light ISOELLIPTICITY curves in (m,M) plane

PVLAS 532 nmlight ISOELLIPTICITY and ISOROTATION curves in (m,M) plane

PVLAS 532nm and 1024nm light ISOROTATION curves in (m,M) plane

---

Regeneration scheme with TWO identical OPPOSITE GOING boson beams

Yoke of Morpurgo superconducting magnet

PVLAS Morpurgo magnet : winding of superconducting coils

PVLAS Morpurgo superconducting magnet

PVLAS superconducting Morpurgo magnet before insertion into (liquid He) cryostat

PVLAS superconducting magnet parked in vertical assembly stand

PVLAS cryostat ( with the Morpurgo superconducting magnet inside ) lowered onto the rotating table which rests onto a reinforced concrete beam supported at its extremities by the walls of the square pit of the PVLAS site at INFN-LNL in Legnaro

Top of PVLAS cryostat parked on the floor of the pit in the PVLAS site

PVLAS CRYOSTAT

PVLAS cryostat

PVLAS optical bench below magnet

PVLAS optical bench above magnet

PVLAS installation of amagnetic access structure (Al) to the top optical bench and to the cryostat (July2006)

PVLAS amagnetic access structure