1
A Bright Source Defocusing Op4c for the IXO NFI Richard Willingale The PSF of the IXO op/cs is specified as 5 arc seconds Half Power Diameter. With a focal length of 20 m this translates to 0.485 mm in the focal plane and therefore the large collec/ng area provided by the mirrors, 3 m 2 at 1 keV, is focused into a very small area on the detector. For bright sources the Narrow Field Imager (a TES array) will be severely count rate limited because each pixel cannot be read out fast enough. It will not be possible to use the NFI on IXO for many astrophysically important bright X‐ray sources. The radial surface brightness with and without the BSDO Radial packing of square pores • The MCP must be slumped to a radius of curvature of R=240 mm to defocus the beam of X‐rays from the IXO main mirror. Such slumping has already been demonstrated on the Bepi Columbo MIXS plates. • If the filter wheel is at a distance of 200 mm from the focal plane the MCP must have a diameter of 36 mm to accommodate the full beam. •For high efficiency the ra/o of the length of the channels to the width must be ~100. Plates with this l/d have been manufactured. The channel walls must be coated with Iridium to provide high reflectivity. This has already been successfully achieved and tested. The open fraction of the plates is 0.58 and the low energy efficiency will be close to this value. • The alignment of the channels in current plates is 1‐2 arc minutes which is more than adequate for this applica/on. The Problem Verifica4on of the basic design by ray‐tracing Defocus the telescope when observing bright sources so that the counts are spread over the detector. The central area of the NFI with small pixels and the best spectral resolu/on is expected to be 2.5 by 2.5 arc minutes equivalent to 14.5 by 14.5 mm. We want to defocus the telescope so that the PSF covers a significant frac/on of this area as evenly as possible. This can be achieved using a square pore Micro Channel Plate (MCP) mounted in the filter wheel in front of the NFI. The Solu4on The Astrophysics We will be able to use the NFI on IXO for the observa/on of ma]er under extreme condi/ons using very bright sources to produce /me resolved spectra with excellent signal to noise and an energy resolu/on of ~3 eV. • Cataclysmic variables – variable accre/on onto a white dwarf in all its manifesta/ons • Bright X‐ray pulsars - finding the neutron star equa/on of state • Low/High Mass X‐ray Binaries – high resolu/on spectra of accre/on onto a neutron star or black hole • Magnetars ‐ Sob Gamma Ray Repeaters – systems dominated by very strong magne/c fields A radially packed square pore MCP from the Bepi Columbo MIXS instrument The mul4‐fibre structure in the MCP Square pores in a single mul4‐fibre Predicted performance of the Bright Source Defocusing Op/c • At low energies ~1 keV the BSDO u/lizes ~38% of the mirror area giving an effec/ve area of ~1.2 m 2 • The surface brightness ra/o is 180 so sources ~200 /mes brighter can be observed using the BSDO • At high energies ~6.4 keV the BSDO u/lizes ~26 % of the mirror area giving an effec/ve area of ~0.24 m 2 • The surface brightness ra/o at ~6.4 keV is 73 Geometry of defocusing Accommoda/on • The MCP op/c is a disk of glass diameter ~36 mm, thickness ~1mm, full of microscopic holes with a mass of just a few grams • It can be accommodated in the filter wheel like any other thin filter • The alignment/posi/oning for this applica/on is not cri/cal. Small /lts/shibs make li]le difference to the defocused distribu/on

A Bright Source Defocusing Opc for the IXO NFI...willingale_aas_poster.ppt Author: Randall Smith Created Date: 1/12/2009 2:36:45 PM

  • Upload
    others

  • View
    0

  • Download
    0

Embed Size (px)

Citation preview

Page 1: A Bright Source Defocusing Opc for the IXO NFI...willingale_aas_poster.ppt Author: Randall Smith Created Date: 1/12/2009 2:36:45 PM

ABrightSourceDefocusingOp4cfortheIXONFIRichardWillingale

ThePSFoftheIXOop/csisspecifiedas5arcsecondsHalfPowerDiameter.Withafocallengthof20mthistranslatesto0.485mminthefocalplaneandthereforethelargecollec/ngareaprovidedbythemirrors,3 m2 at 1 keV,isfocusedintoaverysmallareaonthedetector.ForbrightsourcestheNarrowFieldImager(aTESarray)willbeseverelycountratelimitedbecauseeachpixelcannotbereadoutfastenough.ItwillnotbepossibletousetheNFIonIXOformanyastrophysicallyimportantbrightX‐raysources.

TheradialsurfacebrightnesswithandwithouttheBSDO

Radialpackingofsquarepores

• TheMCPmustbeslumpedtoaradiusofcurvatureofR=240mmtodefocusthebeamofX‐raysfromtheIXOmainmirror.SuchslumpinghasalreadybeendemonstratedontheBepiColumboMIXSplates.• Ifthefilterwheelisatadistanceof200mmfromthefocalplanetheMCPmusthaveadiameterof36mmtoaccommodatethefullbeam.• Forhighefficiencythera/oofthelengthofthechannelstothewidthmustbe~100.Plateswiththisl/dhavebeenmanufactured.• The channel walls must be coated with Iridium to provide high reflectivity. This has already been successfully achieved and tested. The open fraction of the plates is 0.58 and the low energy efficiency will be close to this value. • Thealignmentofthechannelsincurrentplatesis1‐2arcminuteswhichismorethanadequateforthisapplica/on.

TheProblem

Verifica4onofthebasicdesignbyray‐tracing

Defocusthetelescopewhenobservingbrightsourcessothatthecountsarespreadoverthedetector.ThecentralareaoftheNFIwithsmallpixelsandthebestspectralresolu/onisexpectedtobe2.5by2.5arcminutesequivalentto14.5by14.5mm.WewanttodefocusthetelescopesothatthePSFcoversasignificantfrac/onofthisareaasevenlyaspossible.ThiscanbeachievedusingasquareporeMicroChannelPlate(MCP)mountedinthefilterwheelinfrontoftheNFI.

TheSolu4on

TheAstrophysics

WewillbeabletousetheNFIonIXOfortheobserva/onofma]erunderextremecondi/onsusingverybrightsourcestoproduce/meresolvedspectrawithexcellentsignaltonoiseandanenergyresolu/onof~3eV.• Cataclysmicvariables–variableaccre/onontoawhitedwarfinallitsmanifesta/ons• BrightX‐raypulsars- findingtheneutronstarequa/onofstate• Low/HighMassX‐rayBinaries–highresolu/onspectraofaccre/onontoaneutronstarorblackhole• Magnetars‐SobGammaRayRepeaters–systemsdominatedbyverystrongmagne/cfields

AradiallypackedsquareporeMCPfromtheBepiColumboMIXSinstrument

Themul4‐fibrestructureintheMCP

Squareporesinasinglemul4‐fibre

PredictedperformanceoftheBrightSourceDefocusingOp/c• Atlowenergies~1keVtheBSDOu/lizes~38%ofthemirrorareagivinganeffec/veareaof~1.2m2

• Thesurfacebrightnessra/ois180sosources~200/mesbrightercanbeobservedusingtheBSDO• Athighenergies~6.4keVtheBSDOu/lizes~26%ofthemirrorareagivinganeffec/veareaof~0.24m2

• Thesurfacebrightnessra/oat~6.4keVis73

Geometryofdefocusing

Accommoda/on• TheMCPop/cisadiskofglassdiameter~36mm,thickness~1mm,fullofmicroscopicholeswithamassofjustafewgrams• Itcanbeaccommodatedinthefilterwheellikeanyotherthinfilter• Thealignment/posi/oningforthisapplica/onisnotcri/cal.Small/lts/shibsmakeli]ledifferencetothedefocuseddistribu/on