SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals

Similar documents
SIFS... SOAR Integral Field Spectrograph

UV/Optical/IR Astronomy Part 2: Spectroscopy

Gemini 8m Telescopes Instrument Science Requirements. R. McGonegal Controls Group. January 27, 1996

GLAO instrument specifications and sensitivities. Yosuke Minowa

An integral eld spectrograph for the 4-m European Solar Telescope

Observational Astronomy

GMT Instruments and AO. GMT Science Meeting - March

Conceptual design for the High Resolution Optical Spectrograph on the Thirty-Meter Telescope: a new concept for a ground-based highresolution

Performance Comparison of Spectrometers Featuring On-Axis and Off-Axis Grating Rotation

Improving the Collection Efficiency of Raman Scattering

MS260i 1/4 M IMAGING SPECTROGRAPHS

High Resolution Optical Spectroscopy in the ELT Era. Cynthia S. Froning University of Texas at Austin May 25, 2016

ABSTRACT 1. INTRODUCTION

Preliminary Characterization Results: Fiber-Coupled, Multi-channel, Hyperspectral Spectrographs

DESIGN NOTE: DIFFRACTION EFFECTS

Oriel MS260i TM 1/4 m Imaging Spectrograph

Properties of a Detector

arxiv: v1 [astro-ph.im] 26 Mar 2012

SpectraPro 2150 Monochromators and Spectrographs

SPECTRAL SCANNER. Recycling

Science Detectors for E-ELT Instruments. Mark Casali

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Grating and Filter Specification Document

!!! DELIVERABLE!D60.2!

Better Imaging with a Schmidt-Czerny-Turner Spectrograph

The Field Camera Unit for WSO/UV

Padova and Asiago Observatories

Information for users of the SOAR Goodman Spectrograph Multi-Object Slit (MOS) mode. César Briceño and Sean Points

New opportunities of freeform gratings using diamond machining

GPI INSTRUMENT PAGES

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan

Basic spectrometer types

erosita mirror calibration:

VATTSpec Instructions Rev. 10/23/2015

The ASTRI SST-2M Illuminator

Multi-fibers connectors systems for FOCCoS-PFS-Subaru

Nonlinearity in the Detector used in the Subaru Telescope High Dispersion Spectrograph

TriVista. Universal Raman Solution

Image Slicer for the Subaru Telescope High Dispersion Spectrograph

Cascaded holographic spectrographs for astronomical applications

SLICING THE UNIVERSE CCDs for MUSE

CFHT and Subaru Wide Field Camera

Descriptions for Each Test

Development of different kind of IFU prototypes for the OPTIMOS-EVE study for the E-ELT

The Photonic TIGER: a multicore fiber-fed spectrograph

Development of four-dimensional imaging spectrometers (4D-IS)

ZIMPOL-3: a powerful solar polarimeter

Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region

UltraGraph Optics Design

TIRCAM2 (TIFR Near Infrared Imaging Camera - 3.6m Devasthal Optical Telescope (DOT)

Presented by Jerry Hubbell Lake of the Woods Observatory (MPC I24) President, Rappahannock Astronomy Club

MEGARA Spectrograph Optics

Radiometric Solar Telescope (RaST) The case for a Radiometric Solar Imager,

The DSI for Autostar Suite

Southern African Large Telescope. RSS CCD Geometry

Chasing Faint Objects

Commissioning of Thomson Scattering on the Pegasus Toroidal Experiment

Non-adaptive Wavefront Control

Astro 500 A500/L-20 1

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the

Performance of the HgCdTe Detector for MOSFIRE, an Imager and Multi-Object Spectrometer for Keck Observatory

Simulation team in Vienna. Joao Alves, Werner Zeilinger, Rainer Köhler, Michael Mach

Optical Design of the SuMIRe PFS Spectrograph

Flux Calibration Monitoring: WFC3/IR G102 and G141 Grisms

MEGARA FOCAL PLANE SUBSYSTEMS

a simple optical imager

BEAM HALO OBSERVATION BY CORONAGRAPH

Scaling relations for telescopes, spectrographs, and reimaging instruments

Interpixel crosstalk in a 3D-integrated active pixel sensor for x-ray detection

COS Near-UV Flat Fields and High S/N Determination from SMOV Data

Phase-2 Preparation Tool

QE65000 Spectrometer. Scientific-Grade Spectroscopy in a Small Footprint. now with. Spectrometers

Wavelength Calibration Accuracy of the First-Order CCD Modes Using the E1 Aperture

SONG Stellar Observations Network Group. The prototype

Guide to Processing Spectra Using the BASS Software

OmegaCAM calibrations for KiDS

Cerro Tololo Inter-American Observatory. CHIRON manual. A. Tokovinin Version 2. May 25, 2011 (manual.pdf)

6. Very low level processing (radiometric calibration)

Mini Workshop Interferometry. ESO Vitacura, 28 January Presentation by Sébastien Morel (MIDI Instrument Scientist, Paranal Observatory)

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist)

Basic spectrometer types

Instruction Manual for HyperScan Spectrometer

Fastest high definition Raman imaging. Fastest Laser Raman Microscope RAMAN

Astrophysical Techniques Optical/IR photometry and spectroscopy. Danny Steeghs

Telescopes and their configurations. Quick review at the GO level

F/48 Slit Spectroscopy

Light gathering Power: Magnification with eyepiece:

Astr 535 Class Notes Fall

Historical. McPherson 15 Mount

CCD reductions techniques

IBIL setup operation manual for SynerJY software version

Order Overlap. A single wavelength constructively interferes in several directions A given direction can receive multiple wavelengths.

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

LAMOST-HiRes. Fengshan - September 4, A Fiber-Fed High Resolution Echelle Spectrograph for LAMOST. Frank Grupp Slide 1

CCD User s Guide SBIG ST7E CCD camera and Macintosh ibook control computer with Meade flip mirror assembly mounted on LX200

Instructions for the Experiment

Observation Data. Optical Images

metcon meteorologieconsultgmbh, Instruments for Atmospheric Research W1aa_Feb_2017_1.doc 1 -

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak

You, too, can make useful and beautiful astronomical images at Mees: Lesson 1

Specifications. Offers the best spatial resolution for multi-stripe spectroscopy. Provides the user the choice of either high accuracy slit mechanism

Transcription:

Published on SOAR (http://www.ctio.noao.edu/soar) Home > SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals SOAR is issuing a call for proposals for science verification with SIFS, the SOAR Integral Field Unit Spectrograph, for 4 nights in 2017A (May 11&12 and July 7&8, 2017). The deadline for proposal submission is April 17, 2017. The proposals will be evaluated by the SIFS Team. The observations will be conducted by Luciano Fraga (<lfraga at lna.br>), who will be also responsible for the data reduction of all science and standards data collected on this SV. Technical questions and the SV proposals should be submitted to Luciano as well. The SIFS final products are wavelength calibrated data-cubes. PIs with observed proposals will receive their data-cubes one month after the end of SIFS SV. PIs are expected to provide feedback within two months after the data delivered. There is no proprietary period for SV data. In order to include a wide range of science cases, we expect that proposals for this SV be limited to a total observing time not exceeding 3 hrs. The proposal will consist of a cover page with the science team and affiliations, followed by a scientific justification of maximum one page (11 pt) and a Technical Justification section with the requested setup for SIFS (see below), target information and approximate exposure time. Proposals will be evaluated on the basis of their science cases and overall feasibility; additional objectives are to demonstrate a range of science projects and to include investigators from all members of the SOAR consortium. SIFS is an instrument developed and constructed in Brazil for the 4.1-m SOAR telescope by the Laboratório Nacional de Astrofísica (LNA/MCTIC) in collaboration with the Instituto de Astronomia, Geofísica e Ciências Atmosféricas, Universidade de São Paulo (Institute of Astronomy, Geophysics and Atmospheric Sciences of the University of São Paulo, IAG/USP). The instrument consists of three subsystems: a fore-optics module mounted at the optical Nasmyth focus, a 14-m long optical fiber bundle and a bench spectrograph. The fore-optics re-images the telescope focal plane onto the input of the integral field unit (IFU) in two interchangeable magnifications: 0.15 arcsec/fiber or 0.30 arcsec/fiber, which produces a field of view of 7.5 x 3.9 arcsec 2 and 15 x 7.8 arcsec 2, respectively. The IFU is a two-dimensional array of 1300 microlens ( lenslets ) and optical fibers arranged into a 50-by-26 matrix. The optical fibers in the IFU output are aligned as a pseudo slit at the bench spectrograph entrance. The spectrograph has a set of interchangeable Volume Phase Holographic (VPH) gratings (from 700 to 3000 l/mm) mounted in a rotation stage where is also mounted the camera and the detector. The combination of gratings and

camera angles gives a wide range of resolution, 4000 < R < 30000 and central wavelengths. For initial science verification, we are offering a limited selection of these combinations, listed below. Each fiber projects to 1.9 pixels on the detector array in both the spatial and spectral directions. This means that the fiber spectra on the CCD are very packed in the spatial direction (substantial crosstalk between fibers). For that reason, this instrument has an additional calibration step within the standard procedures to extract the science spectrum. The extra calibration frames are a set of 8 masked flatfield images. SIFS has a mask mechanism just in front of the microlens array used to isolate the spectrum of a set of fibers while blocking the light of other neighboring fibers. Moving this mechanism in 8 mask positions it is possible to sample all the 1300 fibers. The SIFS data reduction code simultaneously fits Gaussians to the spatial profiles of group of fibers in order to correct for the crosstalk between the fibers. This code uses as fixed parameters the width and the center position of each fiber spectrum along the dispersion axis, as measured in the masked flat-field frames. The only free parameter for the fit is the Gaussians amplitudes in the science data. The SIFS detector is a CCD231-84 from E2V, very similar to the SAM and SOI CCDs. These are thinned CCDs, unlike newer deep-depletion detectors, so there will be significant fringing in the far red. The full sensor has a format of 4096 x 4112 pixels, with pixel size of 15μm 2. The CCD is operated with a SDSU-3 Leach controller which reads the full un-binned chip in 11s with a noise of 3.9 electrons and a gain of 2.0 e-/adu. Digital saturation occurs at 65536 ADU. The image is written in a multi-extension FITS file. The basic data reduction is performed using a pipeline developed in PyRAF/MSCRED, which includes bias subtraction, flat-fielding, cosmic rays cleaning and merging the four amplifiers in a single FITS image. For this SV call we are offering only the plate scale of 0.30 arcsec/fiber (FoV of 15 x 7.8 arcsec 2 ) and the 700 l/mm grating with the preset angles listed in the table below: Grating 700l/mm Dispersion (Å/pix) Wavelength Coverage Resolution @5500Å (2 pixels) 700B 0.69 4000Å to 6800Å 4200 700M 0.69 4500Å to 7300Å 4200 700R 0.69 5000Å to 7800Å 4200 The SIFS overall system efficiency for the 700 l/mm using the Mid setup is show on the Figure below. The blue line is the efficiency measured using the standard star EG 274 (V = 11.03, DA) and the green line is for HR7950 (V=3.8, A1V). The overall efficiency in this mode is roughly 25-30% that of the Goodman spectrograph with the 930 l/mm gratings, which has a similar spectral resolution with a 0.45 arcsec slit (not allowing for slit losses, which can be significant for a narrow slit).

Radial velocity stability is not well-determined, but commissioning measurements suggest stability of a few km/sec or better during observations..

.

In the figures, we show some spectra obtained with SIFS for the galaxy NGC 3081, all with the 700 l/mm grating centered on 6000 Å, with a single 1200 s integration. The 0.30 arcsec fibers were used. In the top left we display the integrated spectrum of the galaxy. In the top right panel we show the spectrum of the nucleus (expanded scale in bottom panel) for an area of approx. 0.9" in diameter. In the lower panel we show the spectra for an area 0.9 diameter centered on fiber 39,9 (2" south of the galaxy nucleus).). In the images below we show the spatial maps of Hα and Hβ (top and bottom respectively).

Source URL: http://www.ctio.noao.edu/soar/content/soar-integral-field-spectrograph-sifs-call-science-verification-proposals