Subaru Flexibly Addressable Integral Field Spectrographs (SuFAIFS) Naoyuki Tamura (Subaru Telescope, NAOJ) J. R. Allington-Smith, G. J. Murray, “DFS” collaboration.

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Subaru Flexibly Addressable Integral Field Spectrographs (SuFAIFS) Naoyuki Tamura (Subaru Telescope, NAOJ) J. R. Allington-Smith, G. J. Murray, “DFS” collaboration (Centre for Advanced Instrumentation, Durham Univ., UK) ~ Concept of a new instrument from a collaboration recently renewed ~

Background To take “snapshots” of the universe and characterize the galaxy population at each of them, spectroscopic information is necessary. Redshift, star-forming activity, AGN activity, abundance, stellar age, etc

Background Plus integral field (i.e. 2D) spectroscopy (IFS): Spatial distribution, kinematics/dynamics, dynamical mass … Clues to knowing what they are, what’s going on & why (  physics) Nesvadba et al. (2007) HH [NII]/H  (Weijmans et al. 2009) SAURON 24h exposure with WHT of LAB-Z/SSA-22 protocluster Internal structures of galaxy main body (~10 kpc) Extended/diffuse components, halo part of a galaxy (~ kpc) (Hatch et al. 2008) Diffuse star formation in massive galaxies & cluster assembly? An SMG at z~2.5

Background (Conselice et al. 2003)(Reddy et al. 2008) What should Subaru try to address? Light-gathering power is a key for IFS. TMT should be coming with IFS & AO. SuFAIFS would be a late comer of IFS among 8-10m class telescopes … etc Little has been explored by IFS, so there should be plenty to do to understand physical process at various redshift, while coordination would be necessary.

Integral Field Spectroscopy (IFS) Deployable multi-Integral Field Units (IFUs) over an FoV OR Complete spectroscopy of a certain (usually small) part of an FoV Usually too ambitious to do an IFS over a wide area of sky. Is there any way to address targets optimally/efficiently? “Be clever” type (e.g. VLT/KMOS)“Get everything” type (e.g. VLT/MUSE)

Goal of SuFAIFS Allows a flexible selection of regions for spectroscopy among the 2D array of available spaxels on a focal plane, given a limitation in multiplicity of spectrograph(s). E.g. Number of spaxels to be routed to spectrographs = 64. Both will be in choice on SuFAIFS: “Diverse Field Spectroscopy (DFS)” Selected spaxels may be distributed to more than one spectrographs  Possibility of additional versatility to spectral domain.

“Diverse Field Spectroscopy” was proposed as an arbitrary combination of multi-IFU & complete IFS to efficiently address astronomical objects on sky. Designing & prototyping switching layer (cascading fiber switches or signal fiber switch + incoherent fiber remapping) mainly with a Rolling grant (for R&D). There are collaborations with other areas (telecom, photonics, etc) outside astronomy. Adding an idea to share a single focal plane with (existing) several spectrographs, a collaboration for instrument proposal to Subaru has recently started (ear-mid 2010). History & current status - Allington-Smith (2007, MNRAS, 376, 1099) - Murray & Allington-Smith (2009, MNRAS, 399, 209) - Poppett, Allington-Smith & Murray (2010, MNRAS, 399, 443)

Primary feed Switcher Spectrograph feed Telescope focus Spectrographs Recorded spectra Spectrograph slit Selected regions Observation control C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F C D 2 6 A E 3 7 B F Celestial Selector Murray, Allington-Smith (2009) Poppett, Allington-Smith, Murray (2010)

Focal plane array of spaxels & primary feed Switcher Components A focal plane is covered by a micro-lens array with a high filling factor. Fiber bundles (input fibers) can provide fiber connectors remote from the actual focal plane. N(input fibers) >> N(output fibers)  “Down-selection” of output fibers routed to spectrographs.

(1 x m) x n (1 x n) x m Output field: m points Input field: n 2 points nxmnxmnxmnxm nxmnxmnxmnxm nxmnxmnxmnxm nxmnxmnxmnxm nxmnxmnxmnxm nxmnxmnxmnxm n x nx1nx1nx1nx1 nx1nx1nx1nx1 nx1nx1nx1nx1 m x n x m switch made from 3 layers of n x 1 switches Any N O = m points in the field of N I = n 2 points can be routed to the output with downselection factor, F = n 2 /m Example shown: n = 6, m = 3 with contiguous field (red) so N I = 36, N O = 3, F = 6 Fibre optical switches Note: If more than one switches could not be used in cascade as above, incoherent remapping would be necessary to enhance flexibility in choice of spaxels on the focal plane.

Free-space optical switches Micromirror array Microlens arrays Optical design: R. Content (Durham) Many fewer interconnections but More complex optics (Murray, Allington-Smith 2009)

Novel and efficient row/column downselection in a MEMS mirror array switching scheme

A two-layer, downselection switching architecture using the two basic switch modules: the n×n and the m×1 devices. Here, n = 8, m = 6 There are m × (n×n) modules (orange) There are n × (m×1) modules (blue) Number of inputs = n × m Number of outputs = n The rectangularity of the input dictates the downselection ratio; here 6:1 For the (n×n) modules proposed by an industrial partner, n = 1000 is feasible Similarly, there is no obstacle in principle to an (m×1) switch, where m = 1000 This technology therefore appears to be the most practical route to DFS systems with >10 6 channel counts. An alternative with less fiber interconnections Inputs: m x n Outputs: n

Remapping spaxels If fiber switches are not used in cascade … The focal plane is divided by cells, from each of which only one spaxel can be selected to be routed to a spectrograph. = “Coherent DFS”, with direct mapping & down selection.  Not optimal to observe a largely extended object (although this is intended to be a 2D spectroscopy!)If fiber switches are not used in cascade … The focal plane is divided by cells, from each of which only one spaxel can be selected to be routed to a spectrograph. = “Coherent DFS”, with direct mapping & down selection.  Not optimal to observe a largely extended object (although this is intended to be a 2D spectroscopy!) Focal plane9x1 down selection Pseudo slit

Remapping spaxels If Nx1 switches cannot be used in cascade …If Nx1 switches cannot be used in cascade … Solution Randomize input-output mapping in fiber bundle so that a large fraction of adjacent inputs can be routed to spectrograph(s). = “Incoherent DFS”, with incoherent remapping incorporated. Solution Randomize input-output mapping in fiber bundle so that a large fraction of adjacent inputs can be routed to spectrograph(s). = “Incoherent DFS”, with incoherent remapping incorporated. Focal planedown selection Slit “Randomized”

Power of incoherent remapping Remapping is very beneficial for clumpy distributions DFS is much more versatile than IFS or MOS Incoherent DFS Coherent DFS IFS (MOS) (Poppett, Allington-Smith & Murray 2010) Montecarlo realization of spaxel distribution and selection for spectroscopy: High (low) correlation index  Uniform (clumpy) Spaxel is routed to a spectrograph? Yes  Success.

Focal plane array of spaxels & primary feed Switcher Spectrograph feed & spectrographs Components Output fibers are re-organized as a slit and are input to spectrographs. Existing spectrographs? (FMOS, MOIRCS, IRCS, FOCAS …) Given a fiber-feed option can be added … E.g. SuMIRe/PFS  Better “homogeneity” & much higher multiplicity may be offered. New spectrographs?  A single focal plane can be shared.  Heterogeneous/Multi-mode spectroscopy is possible.

Focus: Ns  Assisted by MOAO? Cs  Assisted by GLAO? Spectral coverage: Fiber feed, AO assistance  (RI)zYJH? Spaxel size: AO assistance  ~0”.1? Natural seeing  ~0”.2? Preliminary specifications  Max. # of spaxels that can be routed to spectrographs cf. FMOS IRS1 & IRS2 has 400 multiplicity in total.  Available spectral resolution  Need to await for detailed design studies …

Achievement & on-going progress GMOS-IFU FMOS fiber slit FMOS fiber cable AssemblyInstallation FMOS fiber connectors Prototype of fiber bundle & IFU with an incoherent fiber re-mapping.

A single focal plane is “shared” by N(>=2) spectrographs. Flexible & optimal selections of spaxels on the focal plane will be allowed: “DFS”  MOS+multi IFU+IFS Ns/Cs focus, (RI)zYJH?  Could be assisted by MOAO/GLAO. Adding a fiber-feed option to existing spectrographs? (FMOS, MOIRCS, IRCS, FOCAS …)  Heterogeneous/multimode spectroscopy More spaxels? Better “homogeneity” on a focal plane?  Spectrographs for SuMIRe/PFS may be a possibility? Still AO-assisted in the (RI)zY band with full-depletion type CCD? R&D is on-going in Durham, exploring collaborations including other reseaerch areas (including industrial partners). Trying to wrap up technical details & scientific potentials expected by them (with instrument throughput predicted). “SuFAIFS”: Subaru Flexibly Addressable Integral Field Spectrographs Adding a new significant observing capability to the telescope Summary Main features Other details (mostly tentative) Current status & near-future plans