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Publications of the Astronomical Society of the Pacific | 2005

Hectospec, the mmt's 300 optical fiber-fed spectrograph

Daniel G. Fabricant; Robert G. Fata; John B. Roll; Edward Hertz; Nelson Caldwell; Thomas Gauron; John C. Geary; Brian A. McLeod; Andrew Szentgyorgyi; Joseph Zajac; Michael J. Kurtz; Jack Barberis; Henry Bergner; Warren R. Brown; Maureen A. Conroy; Roger Eng; Margaret J. Geller; Richard E. Goddard; Michael Honsa; Mark Mueller; Douglas J. Mink; Mark Ordway; Susan Tokarz; Deborah Freedman Woods; William F. Wyatt; Harland W. Epps; Ian P. Dell’Antonio

ABSTRACT The Hectospec is a 300 optical fiber fed spectrograph commissioned at the MMT in the spring of 2004. In the configuration pioneered by the Autofib instrument at the Anglo‐Australian Telescope, Hectospec’s fiber probes are arranged in a radial “fisherman on the pond” geometry and held in position with small magnets. A pair of high‐speed, six‐axis robots move the 300 fiber buttons between observing configurations within ∼300 s, and to an accuracy of ∼25 μm. The optical fibers run for 26 m between the MMT’s focal surface and the bench spectrograph, operating at \documentclass{aastex} \usepackage{amsbsy} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{mathrsfs} \usepackage{pifont} \usepackage{stmaryrd} \usepackage{textcomp} \usepackage{portland,xspace} \usepackage{amsmath,amsxtra} \usepackage[OT2,OT1]{fontenc} \newcommand\cyr{ \renewcommand\rmdefault{wncyr} \renewcommand\sfdefault{wncyss} \renewcommand\encodingdefault{OT2} \normalfont \selectfont} \DeclareTextFontCommand{\textc...


Proceedings of SPIE | 2012

Harps-N: the new planet hunter at TNG

Rosario Cosentino; Christophe Lovis; F. Pepe; Andrew Collier Cameron; David W. Latham; Emilio Molinari; S. Udry; Naidu Bezawada; Martin Black; Andy Born; Nicolas Buchschacher; D. Charbonneau; P. Figueira; Michel Fleury; Alberto Galli; Angus Gallie; Xiaofeng Gao; Adriano Ghedina; Carlos Gonzalez; Manuel Gonzalez; J. Guerra; David Henry; K. Horne; Ian Hughes; Dennis Kelly; Marcello Lodi; David Lunney; Charles Maire; Michel Mayor; Giusi Micela

The Telescopio Nazionale Galileo (TNG)[9] hosts, starting in April 2012, the visible spectrograph HARPS-N. It is based on the design of its predecessor working at ESOs 3.6m telescope, achieving unprecedented results on radial velocity measurements of extrasolar planetary systems. The spectrographs ultra-stable environment, in a temperature-controlled vacuum chamber, will allow measurements under 1 m/s which will enable the characterization of rocky, Earth-like planets. Enhancements from the original HARPS include better scrambling using octagonal section fibers with a shorter length, as well as a native tip-tilt system to increase image sharpness, and an integrated pipeline providing a complete set of parameters. Observations in the Kepler field will be the main goal of HARPS-N, and a substantial fraction of TNG observing time will be devoted to this follow-up. The operation process of the observatory has been updated, from scheduling constraints to telescope control system. Here we describe the entire instrument, along with the results from the first technical commissioning.


Proceedings of SPIE | 2012

The GMT-CfA, Carnegie, Catolica, Chicago Large Earth Finder (G-CLEF): a general purpose optical echelle spectrograph for the GMT with precision radial velocity capability

Andrew Szentgyorgyi; Anna Frebel; Gabor Furesz; Edward Hertz; Timothy Norton; Jacob L. Bean; Henry Bergner; Jeffrey D. Crane; Janet Evans; Ian Evans; T. Gauron; Andrés Jordán; Sang Park; Alan Uomoto; Stuart Barnes; William N. Davis; M. Eisenhower; Harland Epps; Dani Guzman; Kenneth McCracken; Mark Ordway; David Plummer; William A. Podgorski; David R. Weaver

The GMT-CfA, Carnegie, Catolica, Chicago Large Earth Finder (G-CLEF) is a fiber fed, optical echelle spectrograph that has undergone conceptual design for consideration as a first light instrument at the Giant Magellan Telescope. GCLEF has been designed to be a general-purpose echelle spectrograph with precision radial velocity (PRV) capability. We have defined the performance envelope of G-CLEF to address several of the highest science priorities in the Decadal Survey1. The spectrograph optical design is an asymmetric, two-arm, white pupil design. The asymmetric white pupil design is adopted to minimize the size of the refractive camera lenses. The spectrograph beam is nominally 300 mm, reduced to 200 mm after dispersion by the R4 echelle grating. The peak efficiency of the spectrograph is >35% and the passband is 3500-9500Å. The spectrograph is primarily fed with three sets of fibers to enable three observing modes: High-Throughput, Precision-Abundance and PRV. The respective resolving powers of these modes are R~ 25,000, 40,000 and 120,000. We also anticipate having an R~40,000 Multi-object Spectroscopy mode with a multiplex of ~40 fibers. In PRV mode, each of the seven 8.4m GMT primary mirror sub-apertures feeds an individual fiber, which is scrambled after pupil-slicing. The goal radial velocity precision of G-CLEF is ∂V <10 cm/sec radial. In this paper, we provide a flowdown from fiducial science programs to design parameters. We discuss the optomechanical, electrical, structural and thermal design and present a roadmap to first light at the GMT.


Proceedings of SPIE | 2012

A prototype phasing camera for the Giant Magellan Telescope

Srikrishna Kanneganti; Brian A. McLeod; Mark Ordway; John B. Roll; Stephen A. Shectman; Antonin H. Bouchez; Johanan L. Codona; Roger Eng; Thomas Gauron; Felix Handte; Timothy Norton; Phil Streechon; David R. Weaver

Achieving the diffraction limit with the adaptive optics system of the 25m Giant Magellan Telescope will require that the 7 pairs of mirror segments be in phase. Phasing the GMT is made difficult because of the 30-40cm gaps between the primary mirror segments. These large gaps result in atmospheric induced phase errors making optical phasing difficult at visible wavelengths. The large gaps between the borosilicate mirror segments also make an edge sensing system prone to thermally induced instability. We describe an optical method that uses twelve 1.5-m square subapertures that span the segment boundaries. The light from each subaperture is mapped onto a MEMS mirror segment and then a lenslet array which are used to stabilize the atmospherically induced image motion. Centroids for stabilization are measured at 700nm. The piston error is measured from the fringes visible in each of the 12 stabilized images at 2.2 microns. By dispersing the fringes we can resolve 2π phase ambiguities. We are constructing a prototype camera to be deployed at the 6.5m Magellan Clay telescope.


Proceedings of SPIE | 2014

A preliminary design for the GMT-Consortium Large Earth Finder (G-CLEF)

Andrew Szentgyorgyi; Stuart I. Barnes; Jacob L. Bean; Bruce C. Bigelow; Antonin H. Bouchez; Moo-Young Chun; Jeffrey D. Crane; Harland W. Epps; Ian Evans; Janet Evans; Anna Frebel; Gabor Furesz; Alex Glenday; Dani Guzman; Tyson Hare; Bi-Ho Jang; Jeong-Gyun Jang; Ueejong Jeong; Andres Jordan; Kang-Min Kim; Jihun Kim; Chih-Hao Li; Mercedes Lopez-Morales; Kenneth McCracken; Brian A. McLeod; Mark Mueller; Ja-Kyung Nah; Timothy Norton; Heeyoung Oh; Jae Sok Oh

The GMT-Consortium Large Earth Finder (G-CLEF) is an optical-band echelle spectrograph that has been selected as the first light instrument for the Giant Magellan Telescope (GMT). G-CLEF is a general-purpose, high dispersion spectrograph that is fiber fed and capable of extremely precise radial velocity measurements. The G-CLEF Concept Design (CoD) was selected in Spring 2013. Since then, G-CLEF has undergone science requirements and instrument requirements reviews and will be the subject of a preliminary design review (PDR) in March 2015. Since CoD review (CoDR), the overall G-CLEF design has evolved significantly as we have optimized the constituent designs of the major subsystems, i.e. the fiber system, the telescope interface, the calibration system and the spectrograph itself. These modifications have been made to enhance G-CLEF’s capability to address frontier science problems, as well as to respond to the evolution of the GMT itself and developments in the technical landscape. G-CLEF has been designed by applying rigorous systems engineering methodology to flow Level 1 Scientific Objectives to Level 2 Observational Requirements and thence to Level 3 and Level 4. The rigorous systems approach applied to G-CLEF establishes a well defined science requirements framework for the engineering design. By adopting this formalism, we may flexibly update and analyze the capability of G-CLEF to respond to new scientific discoveries as we move toward first light. G-CLEF will exploit numerous technological advances and features of the GMT itself to deliver an efficient, high performance instrument, e.g. exploiting the adaptive optics secondary system to increase both throughput and radial velocity measurement precision.


Proceedings of SPIE | 2016

The GMT-Consortium Large Earth Finder (G-CLEF): an optical Echelle spectrograph for the Giant Magellan Telescope (GMT)

Andrew Szentgyorgyi; Daniel Baldwin; Stuart Barnes; Jacob L. Bean; Sagi Ben-Ami; Patricia Brennan; Jamie Budynkiewicz; Moo Young Chun; Charlie Conroy; Jeffrey D. Crane; Harland W. Epps; Ian Evans; Janet Evans; Jeff Foster; Anna Frebel; Thomas Gauron; Dani Guzman; Tyson Hare; Bi Ho Jang; Jeong Gyun Jang; Andrés Jordán; Jihun Kim; Kang Miin Kim; Claudia Mendes Oliveira; Mercedes Lopez-Morales; Kenneth McCracken; Stuart McMuldroch; Joseph Miller; Mark Mueller; Jae Sok Oh

The GMT-Consortium Large Earth Finder (G-CLEF) will be a cross-dispersed, optical band echelle spectrograph to be delivered as the first light scientific instrument for the Giant Magellan Telescope (GMT) in 2022. G-CLEF is vacuum enclosed and fiber-fed to enable precision radial velocity (PRV) measurements, especially for the detection and characterization of low-mass exoplanets orbiting solar-type stars. The passband of G-CLEF is broad, extending from 3500Å to 9500Å. This passband provides good sensitivity at blue wavelengths for stellar abundance studies and deep red response for observations of high-redshift phenomena. The design of G-CLEF incorporates several novel technical innovations. We give an overview of the innovative features of the current design. G-CLEF will be the first PRV spectrograph to have a composite optical bench so as to exploit that material’s extremely low coefficient of thermal expansion, high in-plane thermal conductivity and high stiffness-to-mass ratio. The spectrograph camera subsystem is divided into a red and a blue channel, split by a dichroic, so there are two independent refractive spectrograph cameras. The control system software is being developed in model-driven software context that has been adopted globally by the GMT. G-CLEF has been conceived and designed within a strict systems engineering framework. As a part of this process, we have developed a analytical toolset to assess the predicted performance of G-CLEF as it has evolved through design phases.


Proceedings of SPIE | 2014

The Giant Magellan Telescope active optics system

Brian A. McLeod; Antonin H. Bouchez; Brady Espeland; José M. Filgueira; Matt Johns; Timothy Norton; Mark Ordway; William A. Podgorski; John B. Roll; Carey Smith

The Giant Magellan Telescope active optics system is required to maintain image quality across a 20 arcminute diameter field of view. To do so, it must control the positions of the primary mirror and secondary mirror segments, and the figures of the primary mirror segments. When operating with its adaptive secondary mirror, the figure of the secondary is also controlled. Wavefront and fast-guiding measurements are made using a set of four probes deployed around the field of view. Through a set of simulations we have determined a set of modes that will be used to control fielddependent aberrations without degeneracies.


Proceedings of SPIE | 2012

The F/5 instrumentation suite for the Clay Telescope

Andrew Szentgyorgyi; Brian A. McLeod; Daniel G. Fabricant; Robert G. Fata; Timothy Norton; Mark Ordway; John B. Roll; Henry Bergner; Maureen A. Conroy; D. Curley; Harland W. Epps; T. Gauron; John C. Geary; Mark Mueller; Alan Uomoto; Stephen M. Amato; J. Barberis; Roger Eng; Gabor Furesz; Edward Hertz; C. Hull; Kenneth McCracken; George U. Nystrom; David J. Osip; P. Palunas; F. Perez; F. Sanchez; V. Suc; David R. Weaver; Deborah F. Woods

The f/5 instrumentation suite for the Clay telescope was developed to provide the Magellan Consortium observer community with wide field optical imaging and multislit NIR spectroscopy capability. The instrument suite consists of several major subsystems including two focal plane instruments. These instruments are Megacam and MMIRS. Megacam is a panoramic, square format CCD mosaic imager, 0.4° on a side. It is instrumented with a full set of Sloan filters. MMIRS is a multislit NIR spectrograph that operates in Y through K band and has long slit and imaging capability as well. These two instruments can operate both at Magellan and the MMT. Megacam requires a wide field refractive corrector and a Topbox to support shutter and filter selection functions, as well as to perform wavefront sensing for primary mirror figure correction. Both the corrector and Topbox designs were modeled on previous designs for MMT, however features of the Magellan telescope required considerable revision of these designs. In this paper we discuss the optomechanical, electrical, software and structural design of these subsystems, as well as operational considerations that attended delivery of the instrument suite to first light.


Proceedings of SPIE | 2014

The G-CLEF spectrograph optical design

Gábor Fűrész; Harland Epps; Stuart I. Barnes; William A. Podgorski; Andrew Szentgyorgyi; Mark Mueller; Daniel Baldwin; Jacob L. Bean; Henry Bergner; Moo-Young Chun; Jeffrey D. Crane; Janet Evans; Ian Evans; Jeff Foster; Thomas Gauron; Dani Guzman; Edward Hertz; Andrés Jordán; Kang-Min Kim; Kenneth McCracken; Timothy Norton; Mark Ordway; Chan Park; Sang Park; Dave Plummer; Alan Uomoto; In-Soo Yuk

The GMT-Consortium Large Earth Finder (G-CLEF) is a fiber fed, optical echelle spectrograph, which has been selected as a first light instrument for the Giant Magellan Telescope (GMT) currently under construction at the Las Campanas Observatory. We designed G-CLEF as a general-purpose echelle spectrograph with a precision radial velocity (PRV) capability goal of 0.1 m/s, which will enable it to detect/measure the mass of an Earth-sized planet orbiting a Solar-type star in its habitable zone. This goal imposes challenging requirements on all aspects of the instrument and some of those are best incorporated directly into the optical design process. In this paper we describe the preliminary optical design of the G-CLEF instrument and briefly describe some novel solutions we have introduced into the asymmetric white pupil echelle configuration.


Proceedings of SPIE | 2014

The opto-mechanical design of the GMT-consortium large earth finder (G-CLEF)

Mark Mueller; Daniel Baldwin; Jacob L. Bean; Henry Bergner; Bruce C. Bigelow; Moo-Young Chun; Jeffrey D. Crane; Jeff Foster; Gábor Fűrész; Thomas Gauron; Dani Guzman; Edward Hertz; Andrés Jordán; Kang-Min Kim; Kenneth McCracken; Timothy Norton; Mark Ordway; Chan Park; Sang Park; William A. Podgorski; Andrew Szentgyorgyi; Alan Uomoto; In-Soo Yuk

The GMT-Consortium Large Earth Finder (G-CLEF) is a fiber fed, optical echelle spectrograph that has been selected as a first light instrument for the Giant Magellan Telescope (GMT) currently under construction at the Las Campanas Observatory in Chile’s Atacama desert region. We designed G-CLEF as a general-purpose echelle spectrograph with precision radial velocity (PRV) capability used for exoplanet detection. The radial velocity (RV) precision goal of GCLEF is 10 cm/sec, necessary for detection of Earth-sized planets orbiting stars like our Sun in the habitable zone. This goal imposes challenging stability requirements on the optical mounts and the overall spectrograph support structures. Stability in instruments of this type is typically affected by changes in temperature, orientation, and air pressure as well as vibrations caused by telescope tracking. For these reasons, we have chosen to enclose G-CLEF’s spectrograph in a thermally insulated, vibration isolated vacuum chamber and place it at a gravity invariant location on GMT’s azimuth platform. Additional design constraints posed by the GMT telescope include: a limited space envelope, a thermal emission ceiling, and a maximum weight allowance. Other factors, such as manufacturability, serviceability, available technology and budget are also significant design drivers. All of the previously listed considerations must be managed while ensuring that performance requirements are achieved. In this paper, we discuss the design of G-CLEF’s optical mounts and support structures including technical choices made to minimize the system’s sensitivity to thermal gradients. A more general treatment of the properties of G-CLEF can be found elsewhere in these proceedings1. We discuss the design of the vacuum chamber which houses the irregularly shaped optical bench and optics while conforming to a challenging space envelope on GMT’s azimuth platform. We also discuss the design of G-CLEF’s insulated enclosure and thermal control systems which maintain the spectrograph at milli-Kelvin level stability while simultaneously limiting the maximum thermal emission into the telescope dome environment. Finally, we discuss G-CLEF’s front-end assembly and fiber-feed system as well as other interface challenges presented by the telescope, enclosure and neighboring instrumentation.

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