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1
Gravitational lensing and neutrinos
Why not look where natural lenses exist?
Proposal of an additional candidate list in point source search:1. Motivation and Theory2. Strong lenses and Galaxy clusters3. Candidate List4. Ask collaboration to reunblind 2007-2010 data next September
Internal note: ANTARES-PHYS-2012-008
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Gravitational lensing
Magnification of cosmic signals (higher fluxes)
Same geodesic for photons and neutrinos
Advantage: neutrinos not absorbed by lensed object
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Lensing geometry and Lens equation
Deflection angle:(for spheric sym.Mass distribution)
From Figure:(small angles)
Reduced deflection angle:
Lens equation:
Deflection proportional to mass andinverse proportional to min. distance
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Einstein angle and Magnification
Einstein angle:(derived from lens equation)
Magnification:(for near perfect alignment)
Both Einstein angle and Magnification are proportional to M/D_OL
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Galaxy or galaxy cluster acting as lens
Singular isothermal sphere (SIS)SIS-model takes into account the extended mass
distribution
Mass distribution(sigma=velocity
dispersion) (sigma² ~ mass)Einstein angle
Magnification
Multiple images only if source inside Einstein ring:Solutions of the lens equation: (Again Einstein angle and Magnification are proportional to M)
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Galaxy and quasar lensed by galaxy cluster
Multiple images
Magnification
Gravitational light deflection order of tenth of arcsec
Lens z=0.68
Lens mass~1014Msun
Magnification for light between 1 to 20
Field of view: arcmin => Point like for us
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Selection 1: Einstein angle Most of best studiedgalaxy clusters are also strongest gravitational lenses
Strong lensing objectsshow good constellationbetween observer,lens and source
Mass derived from strong and weak lensing
Selection:Einstein angle > 16”
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Selection 2: MassIf no info about Einstein angle
Planck selected galaxy clusters
Mass proportional to various other physical quantities like:X-ray temperature or luminositySelected only objects with M_500 > 10 * 1014 M_sun
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Selection cuts for different catalogs
Last two tables only used for crosscheckAround 50 galaxy clusters selected (remove multiple entries)
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Distance and Einstein angle distribution
Redshift between 0.15 and 0.9 Einstein angle between 16” and 55”
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Mass and mass/z distributionTake some conversion factor between M_500 and M_vir or M_x (large errors)
Einstein angle and magnification are proportional to M/z
Select only galaxy clusters with M_500 > 10 * 1014
M_sun
Select only galaxy clusters with M_500/z > 40
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Gravitational lensed neutrino source
Take into account nature of source Electromagnetic information=>potential neutrino
source Two blazars with bright flat spectrum and compact jets Both lensed by galaxy PKS 1830-211 at z=2.51, lens at z=0.89 JVASB0218+357 at z=0.94, lens at z=0.68 Both blazars are
not in gamma-ray flaring blazars paper
not in point source paper
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Final candidate list
Selection criteria: Einstein angle > 16´´ ANTARES visibility >20% M_500 > 10 * 1014 M_sun M_500/z > 40
Ten galaxy clusters +Two lensed blazars
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Discuss decisions
For the selection should we take into account:
Einstein angle? (Done) Mass, even when no lensing? (Done) Magnifications? (Not done) Nature of source? (Partially
done)
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Outlook Finalize webpage
(http://antares.in2p3.fr/internal/dokuwiki/doku.php?id=gravitationallensing)
Finalize questions and answers note Apply same candidate list search method used in
point source paper (assume E-2 spectrum) Beginning of September ask Collaboration
to reunblind 2007-2010 data Ask Juan Pablo to apply his well tested
candidate list search method Show results in Bologna
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Conclusion Gravitational lensing can increase by order of
magnitude the signal from a source. Several papers on the subject.
Selection criteria of candidate sources based on:
1. Einstein angle
2. Mass
3. Distance
=> ten galaxy cluster
Two lensed quasars with compact jets Internal note written Unblinding request for beginning of September
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Three different Gravitational lensing regimes
1.Microlensing (change in brightness of observed lensed object)
2.Weak lensing (distortion of observed lensed objects)
3.3.Strong lensing Strong lensing (multiple images and high flux magnification of observed lensed object)
Select strong lensing objects
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Magnification and Probability (arXiv:0610918v1)
Magnification up to 1012
for small misalignmentProbability very smallfor huge amplification
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Gravitational Lensing Objects:
1. Black Hole in Galactic Center
2. Galaxies (CASTLES Catalog)
3. Galaxy clusters (MCXC Catalog, etcetera)
Magnification Objects and Magnification power
If finite source of radius R_s => Galaxy clusters have magnification of 10¹²[Magnification of extended source given as Order(10)]
For near perfect alignment (is very rare):