A Revision of the X-Ray Properties of MWC 297

Total Page:16

File Type:pdf, Size:1020Kb

A Revision of the X-Ray Properties of MWC 297 A&A 447, 1041–1048 (2006) Astronomy DOI: 10.1051/0004-6361:20053630 & c ESO 2006 Astrophysics Chandra X-ray observations of the stellar group near the Herbig Be star MWC 297 A revision of the X-ray properties of MWC 297 F. Damiani, G. Micela, and S. Sciortino INAF - Osservatorio Astronomico di Palermo G.S.Vaiana, Piazza del Parlamento 1, 90134 Palermo, Italy e-mail: [email protected] Received 14 June 2005 / Accepted 11 October 2005 ABSTRACT We present a Chandra ACIS-I X-ray observation of the region near the Herbig early-Be star MWC 297, where we detect a tight group of point X-ray sources. These are probably physically associated to MWC 297, because of their obvious clustering with respect to the more scattered field-source population. These data are compared to earlier ASCA data with much poorer spatial resolution, from which the detection of strong quiescent and flaring emission from MWC 297 itself was claimed. We argue that this star, contributing only 5% to the total X-ray emission of the group, was probably not the dominant contributor to the observed ASCA emission, while the X-ray brightest star in the group is a much better candidate. This is also supported by the spectral analysis of the Chandra data, with reference to the ASCA spectra. We conclude that none of the X-ray data available for MWC 297 justify the earlier claim of strong magnetic activity in this star. The X-ray emission of MWC 297 during the Chandra observation is even weaker than that found in other Herbig stars with the same spectral type, even accounting for its large line-of-sight absorption. Key words. stars: early-type – stars: individual: MWC 297 – stars: emission-line, Be – stars: coronae – stars: pre-main sequence – X-rays: stars 1. Introduction reported the detection of a large flare in an X-ray observation of this object, made with the ASCA satellite, since this type MWC 297 is a Herbig Be star, a more massive analogue of of variability is associated with magnetic-related activity, or- very young, pre-main-sequence (PMS) stars like T Tauri stars. dinarily found in stars later than mid-F, but disappearing for It shows all “classical” features of the class, namely a B-type earlier-type stars, where surface convection is absent, and any spectrum with strong emission lines, and is deeply embedded dynamo-related magnetic activity should cease. Among Herbig in a nebulous region (Herbig 1960). Indeed, it is one of the Ae-Be stars, MWC 297 is the only star where such type of vari- earliest-type stars in its class. Its spectral type was not de- ability has been found in the ASCA survey of Hamaguchi et al. fined in detail until recently, being its spectrum dominated by (2005), with the insignificant exception of TY CrA, which has emission lines: the study of Finkenzeller & Mundt (1985) does a known later-type companion. not assign a spectral type, Hillenbrand et al. (1992) tabulate a type O9, while a dedicated study by Drew et al. (1997) con- Herbig stars like MWC 297 are particularly interesting cluded that this star is of type B1.5, with only half a subclass objects for studies of possible magnetic activity, since they uncertainty. All these studies were made more difficult by the are stars in a fast transition phase, between their formation large visual extinction towards the star, whose estimates by var- and their settling on the main sequence, and some models ious studies seem to converge towards the value AV = 8. This (Siess et al. 2000) predict a transient subphotospheric con- is also the value derived by Drew et al. (1997), who moreover vection zone, which might sustain magnetic activity for some argue that the most likely distance of this star is 250 ± 50 pc, time. This is indeed suggested by observations of optical/UV much nearer than previous estimates of about 500 pc (Cantó lines in some Herbig Ae stars (AB Aur, Praderie et al. 1986; et al. 1984; Bergner et al. 1988). HD 104237, Donati et al. 1997; HD 139614, Hubrig et al. As an early type star, the phenomena which can be ex- 2004). Therefore, a further study of the X-ray emission of pected from MWC 297 should be similar to those encountered MWC 297 is made here, using archive data taken with the in OB stars, and unlike those of late-type stars. It was there- Chandra X-ray Observatory ACIS-I imaging spectrometer. fore surprising that Hamaguchi et al. (2000, henceforth HTBK) This instrument has a roughly similar bandpass and effective Article published by EDP Sciences and available at http://www.edpsciences.org/aa or http://dx.doi.org/10.1051/0004-6361:20053630 1042 F. Damiani et al.: X-ray observations of MWC 297 Fig. 1. Chandra ACIS-I image of the MWC 297 region, slightly smoothed to highlight the sources. The (windowed) field of view has a size of 16.9 × 8.7. The out- lined rectangle (of size 2.3 × 2.0) contains MWC 297, and is zoomed in Fig. 2. The group of X-ray sources in this region was not resolved by ASCA. North is up and East to the left. area as the (combined) ASCA SIS and GIS detectors but much region have a large HR1, and are probably highly absorbed. better spatial resolution, of order of 0.5, while that of ASCA A more detailed analysis is made in Sect. 4. was of order of 3. Our X-ray source #12 coincides closely with the position of MWC 297 (from the SIMBAD database), and a zoom of the ACIS image near the star is shown in Fig. 2a. The very good 2. Chandra X-ray observation and source spatial resolution of Chandra is able to resolve the MWC 297 detection X-ray source from a neighboring one, only about 3 arcsec apart. The field shown in Fig. 2a is only 2.3 × 2.0 in size, and there- MWC 297 was observed with the ACIS-I CCD imaging fore comparable to the ASCA PSF. The nine X-ray sources we spectrometer onboard the Chandra X-ray Observatory on detect in this region were merged into one when observed with − September 21 22, 2001. The exposure time was 37 330 s. A ASCA. A proper comparison between these new data and the “windowed” observing mode was used, yielding a field of view older ones from ASCA should involve the entire group of nine . × . (FOV)of169 8 7 (Fig. 1). ACIS sources (henceforth called as “MWC 297 group”), not We have detected X-ray sources in the field using just the MWC 297 source. It turns out that MWC 297 is not the PWDetect, a wavelet-based detection algorithm developed at brightest X-ray source in its group: sources #5 and #6 are much INAF-Osservatorio Astronomico di Palermo, and available as brighter (they are the two sources in the upper-right quadrant 1 a Chandra contributed software ; it inherits basic features of Fig. 2a). Table 2 lists the relative contributions to the to- of its previous ROSAT version, described in Damiani et al. tal X-ray count rate among members of the MWC 297 group. (1997a,b). Using this method, we detected 27 point sources Note that since some of the sources are underexposed (falling (with less than one expected spurious), listed in Table 1. in inter-chip gaps, barely visible in Fig. 1) the actually detected We have applied a Kolmogorov-Smirnov test for source counts do not scale with the same proportion, but the count rate variability, and we have found only one source (#1 in Table 1) accounts properly for this, yielding the “true” intensity of the with significant variability above 99% confidence level. This sources. source is about 8 arcmin West of MWC 297 (the source at far The close spatial association of X-ray sources in the right in Fig. 1), and even with the poorer ASCA spatial resolu- MWC 297 group (1/3 of all sources in the field, in 1/32 of the tion could not have been confused with MWC 297 itself. area) suggests that this group is a physical association, not a We also report in Table 1 two hardness ratios2 chance one. The existence of a small cluster of infrared objects (columns HR1 and HR2), each defined as (H − S )/(H + S ), around MWC 297 was already reported by Testi et al. (1998), where H and S are the source counts in two energy bands, here and by Bica et al. (2003). Therefore, we may safely assume that chosen as [1.3−2.5] and [0.3−1.3] keV for HR1, and [2.5−8.0] all objects in the group have nearly the same age and distance and [1.3−2.5] keV for HR2. HR1 describes roughly the low- as MWC 297, when trying to determine their nature. energy cutoff caused by heavy absorption of soft X-rays, while a large value of HR2 is generally indicative of a high-energy component (high temperatures). Most X-ray sources in this 3. X-ray source identification To obtain some information on the nature of the detected 1 See http://www.astropa.unipa.it/progetti_ricerca/ PWDetect/ sources, none of which (except for MWC 297) can be associ- 2 We selected the energy bands used to compute these hardness ra- ated with objects in the SIMBAD database, we have searched tios in such a way as to maximize the average observed source counts the 2MASS catalog (Cutri et al.
Recommended publications
  • RTT TECHNOLOGY TOPIC January 2015 Defence Spectrum – the New Battleground?
    RTT TECHNOLOGY TOPIC January 2015 Defence Spectrum – the new battleground? In this month’s technology topic we look at contemporary military radio developments, the integration of LTE user devices into defence communication systems, the relevance of military research to 5 G deployment efficiency and related spectral utilisation and regulatory issues. Defence communication systems are deployed across the whole radio spectrum from long wave to light. This includes mobile communication systems at VHF and UHF and L Band and S band, LEO, MEO and GSO satellite systems (VHF to E band) and mobile and fixed radar (VHF to E band). Legacy defence systems are being upgraded to provide additional functionality. This requires more rather than less spectrum. Increased radar resolution requires wider channel bandwidths; longer range requires more power and improved sensitivity. Improved sensitivity increases the risk of inter system interference. Emerging application requirements including unmanned aerial vehicles require a mix of additional terrestrial, satellite and radar bandwidth. These requirements are geographically and spectrally diverse rather than battlefield and spectrally specific. The assumption in many markets is that the defence industry will be willing and able to surrender spectrum for mobile broadband consumer and civilian use. The AWS 3 auction in the US is a contemporary example with a $5 billion transition budget to cover legacy military system decommissioning in the DOD coordination zone between 1755 and 1780 MHz This transition strategy assumes an increased use of LTE network hardware and user hardware in battlefield systems. While this might imply an opportunity for closer coordination and cooperation between the mobile broadband and defence community it seems likely that an increase in the amount of defence bandwidth needed to support a broadening range of RF dependent systems could be a problematic component in the global spectral allocation and auction process.
    [Show full text]
  • Ncar S-Pol Second Frequency (K -Band) Radar
    P12R.6 NCAR S-POL SECOND FREQUENCY (KA-BAND) RADAR Gordon Farquharson,∗ Frank Pratte, Milan Pipersky, Don Ferraro, Alan Phinney, Eric Loew, Robert Rilling, Scott Ellis, and Jothiram Vivekanandan National Center for Atmospheric Research, Boulder, Colorado 1. INTRODUCTION The National Center for Atmospheric Research (NCAR) has recently extended the observational capability of the S-band dual-polarimetric weather radar system (S-Pol, Keeler et al. (2000)) by adding a Ka-band (35 GHz) po- larimetric Doppler radar (Vivekanandan et al., 2004). The Transmitter Ka-band radar employs a dual channel receiver and can be configured for either HH and HV, or HH and VV polari- metric measurements. The Ka-band and S-band antenna beams are matched and aligned, and timing signals for both systems are generated from the Global Position Sys- tem (GPS) ensuring that a common resolution volume is sampled by both systems. This dual-wavelength capabil- ity provides the potential for retrieving water vapor profiles Radar Processor (Ellis et al., 2005) and liquid water content in Rayleigh scattering conditions (Vivekanandan et al., 1999), im- proving remote sensing of various precipitation types, and studies on cloud microphysics. 2. RADAR DESCRIPTION Receiver The K -band radar is housed in three enclosures which a Figure 1: K -band radar attached to the S-band dish. The are mounted to the S-Pol S-band dish and pedestal struc- a transmitter, receiver, and processor enclosures are vis- ture (Figure 1); these include the transmitter enclosure, ible. The K -band antenna is mounted to the receiver the receiver enclosure, and the radar processor enclo- a enclosure and is facing away from the viewer in the pho- sure.
    [Show full text]
  • Spectrum and the Technological Transformation of the Satellite Industry Prepared by Strand Consulting on Behalf of the Satellite Industry Association1
    Spectrum & the Technological Transformation of the Satellite Industry Spectrum and the Technological Transformation of the Satellite Industry Prepared by Strand Consulting on behalf of the Satellite Industry Association1 1 AT&T, a member of SIA, does not necessarily endorse all conclusions of this study. Page 1 of 75 Spectrum & the Technological Transformation of the Satellite Industry 1. Table of Contents 1. Table of Contents ................................................................................................ 1 2. Executive Summary ............................................................................................. 4 2.1. What the satellite industry does for the U.S. today ............................................... 4 2.2. What the satellite industry offers going forward ................................................... 4 2.3. Innovation in the satellite industry ........................................................................ 5 3. Introduction ......................................................................................................... 7 3.1. Overview .................................................................................................................. 7 3.2. Spectrum Basics ...................................................................................................... 8 3.3. Satellite Industry Segments .................................................................................... 9 3.3.1. Satellite Communications ..............................................................................
    [Show full text]
  • And H-Band Spectra of Globular Clusters in The
    A&A 543, A75 (2012) Astronomy DOI: 10.1051/0004-6361/201218847 & c ESO 2012 ! Astrophysics Integrated J-andH-band spectra of globular clusters in the LMC: implications for stellar population models and galaxy age dating!,!!,!!! M. Lyubenova1,H.Kuntschner2,M.Rejkuba2,D.R.Silva3,M.Kissler-Patig2,andL.E.Tacconi-Garman2 1 Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany e-mail: [email protected] 2 European Southern Observatory, Karl-Schwarzschild-Str. 2, 85748 Garching bei München, Germany 3 National Optical Astronomy Observatory, 950 North Cherry Ave., Tucson, AZ, 85719 USA Received 19 January 2012 / Accepted 1 May 2012 ABSTRACT Context. The rest-frame near-IR spectra of intermediate age (1–2 Gyr) stellar populations aredominatedbycarbonbasedabsorption features offering a wealth of information. Yet, spectral libraries that include the near-IR wavelength range do not sample a sufficiently broad range of ages and metallicities to allowforaccuratecalibrationofstellar population models and thus the interpretation of the observations. Aims. In this paper we investigate the integrated J-andH-band spectra of six intermediate age and old globular clusters in the Large Magellanic Cloud (LMC). Methods. The observations for six clusters were obtained with the SINFONI integral field spectrograph at the ESO VLT Yepun tele- scope, covering the J (1.09–1.41 µm) and H-band (1.43–1.86 µm) spectral range. The spectral resolution is 6.7 Å in J and 6.6 Å in H-band (FWHM). The observations were made in natural seeing, covering the central 24"" 24"" of each cluster and in addition sam- pling the brightest eight red giant branch and asymptotic giant branch (AGB) star candidates× within the clusters’ tidal radii.
    [Show full text]
  • X-Band Tt&C and K-Band Downlink Antennas For
    X-BAND TT&C AND K-BAND DOWNLINK ANTENNAS FOR FUTURE LEO MISSIONS Martin Wenåker [email protected] RUAG Space AB Jan Zackrisson [email protected] Hans Ekström [email protected] Gothenburg, Sweden Johan Petersson [email protected] Patrik Dimming [email protected] P-1342182-RSE Presentation Outline . Introduction . Design Background and Heritage . X-Band TT&C Antenna . K-/Ka-Band Beacon/DDL Antenna . Conclusion 2/17 | X-BAND TT&C AND K-BAND DOWNLINK ANTENNAS FOR FUTURE LEO MISSIONS | RUAG Space | January 22, 2020 Introduction . X-Band TT&C antenna . K-/Ka-Band Beacon/DDL Antenna − Designed and manufactured as an EM − Pre-development running in parallel activity in an add-on to the original with the X-Band continuing study study − Novel dual band design 3/17 | X-BAND TT&C AND K-BAND DOWNLINK ANTENNAS FOR FUTURE LEO MISSIONS | RUAG Space | January 22, 2020 Design Background and Heritage – Ruag Space . Ruag space antenna activities started in the mid 70’s within wide coverage antennas > 300 helix antennas delivered . Other types of antennas are also designed and developed − Reflector antennas (JWST, SIRAL/Cryosat) − Array antennas (Array elements for telecom) − Slot antennas (ERS1/ERS2 , MetOp SG Scatterometer) 4/17 | X-BAND TT&C AND K-BAND DOWNLINK ANTENNAS FOR FUTURE LEO MISSIONS | RUAG Space | January 22, 2020 Design Background and Heritage – Ruag Space . Several variants are used for our helix antennas . Three main variants − Wires - shaped to a helix radiator − Etched metallic strips on substrates - shaped to a helix radiator − Machined in one piece of metal - shaped to a helix radiator 5/17 | X-BAND TT&C AND K-BAND DOWNLINK ANTENNAS FOR FUTURE LEO MISSIONS | RUAG Space | January 22, 2020 X-Band TT&C Antenna .
    [Show full text]
  • The UKIRT Infrared Deep Sky Survey ZY JHK Photometric System: Passbands and Synthetic Colours
    Mon. Not. R. Astron. Soc. 367, 454–468 (2006) doi:10.1111/j.1365-2966.2005.09969.x The UKIRT Infrared Deep Sky Survey ZY JHK photometric system: passbands and synthetic colours P. C. Hewett,1⋆ S. J. Warren,2 S. K. Leggett3 and S. T. Hodgkin1 1Institute of Astronomy, Madingley Road, Cambridge CB3 0HA 2Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2AZ 3United Kingdom Infrared Telescope, Joint Astronomy Centre, 660 North A‘ohoku Place, Hilo, HI 96720, USA Accepted 2005 December 7. Received 2005 November 28; in original form 2005 September 16 ABSTRACT The United Kingdom Infrared Telescope (UKIRT) Infrared Deep Sky Survey is a set of five surveys of complementary combinations of area, depth and Galactic latitude, which began in 2005 May. The surveys use the UKIRT Wide Field Camera (WFCAM), which has a solid angle of 0.21 deg2. Here, we introduce and characterize the ZY JHK photometric system of the camera, which covers the wavelength range 0.83–2.37 µm. We synthesize response functions for the five passbands, and compute colours in the WFCAM, Sloan Digital Sky Survey (SDSS) and two-Micron All Sky Survey (2MASS) bands, for brown dwarfs, stars, galaxies and quasars of different types. We provide a recipe for others to compute colours from their own spectra. Calculations are presented in the Vega system, and the computed offsets to the AB system are provided, as well as colour equations between WFCAM filters and the SDSS and 2MASS passbands. We highlight the opportunities presented by the new Y filter at 0.97–1.07 µm for surveys for hypothetical Y dwarfs (brown dwarfs cooler than T), and for quasars of very high redshift, z > 6.4.
    [Show full text]
  • Are the Hosts of Gamma-Ray Bursts Sub-Luminous and Blue Galaxies ? ?, ??
    (y) View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Are the hosts of Gamma-Ray Bursts sub-luminous and blue galaxies ? ?; ?? E. Le Floc’h1, P.-A. Duc1;2,I.F.Mirabel1;3, D.B. Sanders4;5,G.Bosch6, R.J. Diaz7, C.J. Donzelli8, I. Rodrigues1, T.J.-L. Courvoisier9;10,J.Greiner5, S. Mereghetti11, J. Melnick12,J.Maza13,and D. Minniti14 1 CEA/DSM/DAPNIA Service d’Astrophysique, F-91191 Gif-sur-Yvette, France 2 CNRS URA 2052, France 3 Instituto de Astronom´ıa y F´ısica del Espacio, cc 67, suc 28. 1428 Buenos Aires, Argentina 4 Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, United States 5 Max-Planck-Institut f¨ur Extraterrestrische Physik, D-85740, Garching, Germany 6 Facultad de Cs. Astronomicas y Geof´ısica, Paseo del Bosque s/n, La Plata, Argentina 7 Observatorio Astron´omico de C´ordoba & SeCyT, UNC, Laprida 854, Cordoba [5000], Argentina 8 IATE, Observatorio Astron´omico & CONICET, Laprida 854, Cordoba [5000], Argentina 9 INTEGRAL Science Data Center, Ch. d’Ecogia 16, CH-1290 Versoix, Switzerland 10 Geneva Observatory, Ch. des Maillettes 11, 1290 Sauverny, Switzerland 11 Istituto di Astrofisica Spaziale e Fisica Cosmica, Sezione di Milano “G. Occhialini”, via Bassini 15, I-20133 Milan, Italy 12 European Southern Observatory, Alonso de Cordova 3107, Santiago, Chile 13 Departamento de Astronom´ıa, Universidad de Chile, Casilla 36-D, Santiago, Chile 14 Department of Astronomy, Pontifica Universidad Cat´olica, Av. Vicu˜na Mackenna 4860, Santiago, Chile Received December 6, 2002 / Accepted December 23, 2002 Abstract.
    [Show full text]
  • Geometric Distances of Quasars Measured by Spectroastrometry and Reverberation Mapping: Monte Carlo Simulations
    DRAFT VERSION MARCH 2, 2021 Typeset using LATEX default style in AASTeX62 Geometric Distances of Quasars Measured by Spectroastrometry and Reverberation Mapping: Monte Carlo Simulations YU-YANG SONGSHENG,1, 2 YAN-RONG LI,1 PU DU,1 AND JIAN-MIN WANG1, 2, 3 1Key Laboratory for Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, 19B Yuquan Road, Beijing 100049, China 2University of Chinese Academy of Sciences, 19A Yuquan Road, Beijing 100049, China 3National Astronomical Observatories of China, Chinese Academy of Sciences, 20A Datun Road, Beijing 100020, China (Received ***; Revised ***; Accepted ***) ABSTRACT Recently, GRAVITY onboard the Very Large Telescope Interferometer (VLTI) first spatially resolved the structure of the quasar 3C 273 with an unprecedented resolution of 10µas. A new method of measuring ∼ parallax distances has been successfully applied to the quasar through joint analysis of spectroastrometry (SA) and reverberation mapping (RM) observation of its broad line region (BLR). The uncertainty of this SA and RM (SARM) measurement is about 16% from real data, showing its great potential as a powerful tool for precision cosmology. In this paper, we carry out detailed analyses of mock data to study impacts of data qualities of SA observations on distance measurements and establish a quantitative relationship between statistical uncertainties of distances and relative errors of differential phases. We employ a circular disk model of BLR for the SARM analysis. We show that SARM analyses of observations generally generate reliable quasar distances, even for relatively poor SA measurements with error bars of 40% at peaks of phases. Inclinations and opening angles of ◦ BLRs are the major parameters governing distance uncertainties.
    [Show full text]
  • Uva-DARE (Digital Academic Repository)
    UvA-DARE (Digital Academic Repository) Terahertz-assisted excitation of the 1.5mm photoluminescence of Er in crystalline Si Moskalenko, A.S.; Yassievich, I.N.; Forcales Fernandez, M.; Klik, M.A.J.; Gregorkiewicz, T. Publication date 2004 Document Version Final published version Published in Physical Review B Link to publication Citation for published version (APA): Moskalenko, A. S., Yassievich, I. N., Forcales Fernandez, M., Klik, M. A. J., & Gregorkiewicz, T. (2004). Terahertz-assisted excitation of the 1.5mm photoluminescence of Er in crystalline Si. Physical Review B, 70, 155201. General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:29 Sep 2021 PHYSICAL REVIEW B 70, 155201 (2004) Terahertz-assisted excitation of the 1.5-␮m photoluminescence of Er in crystalline Si A.
    [Show full text]
  • Tactical Solutions Download This PDF to Explore How Our Antennas
    Left: GDPAA, SOTM on LAV, Abrams Tank TACTICAL SOLUTIONS LAND APPLICATIONS SATCOM-ON-THE-MOVE (SOTM) GEODESIC DOME PHASED ARRAY SILHOUETTE™ Ball provides UHF SOTM systems to U.S. ANTENNA (GDPAA) The Silhouette™ Low Profile UHF SATCOM/ military forces for installation on High Ball and its industry partners designed LOS/MUOS On-The-Move Antenna is Mobility Multipurpose Wheeled Vehicles, the GDPAA Advanced Technology designed for integration on tactical vehicles Light Armored Vehicles and a variety of Demonstration in support of the U.S. Air to provide a ruggedized, affordable, net- naval platforms, Light Armored Vehicles, Force Satellite Control Network’s vision of an centric capability. Silhouette™ antennas and a variety of naval platforms. The Ball integrated satellite control network. Ball was feature an ultra-low profile to minimize the SOTM antenna system is designed to provide tasked to develop, integrate and demonstrate visual signature of a vehicle, clear the line military ground vehicles with worldwide technologies required to validate the GDPAA of fire for remote controlled weapons and mobile satellite communication capability concept. enable the vehicle to be easily transported by while moving at speeds of 50 miles per hour air, land or sea. Silhouette is configurable for or greater. ground and maritime platforms. left: RBD, HALE, TFSM. (AIR, LAND, SEA, SPACE) ADVANCED TECHNOLOGIES RISLEY PRISM BEAM DIRECTOR (RBD) TACTICAL CRYOGENICS no replenishment of cryogens is required, ScanEagle® is a product of Insitu Inc. these cryocoolers allow extended mission The Ball tactical optical RBD provides a Ball cryogenics technologies are being times at temperatures below 25 Kelvin. wide field of regard, conformal and compact applied to tactical military intelligence, optical duplex aperture for aircraft laser surveillance and reconnaissance missions to TACTICAL FAST STEERING MIRRORS communications and laser remote sensing enhance platform and payload capabilities.
    [Show full text]
  • LONG RANGE Radar/Laser Detector User's Manual R1
    R1 LONG RANGE Radar/Laser Detector User’s Manual © 2019 Uniden America Corporation Issue 5, January 2019 Irving, Texas Printed in Korea CUSTOMER CARE At Uniden®, we care about you! If you need assistance, please do NOT return this product to your place of purchase. Save your receipt/proof of purchase for warranty. Quickly find answers to your questions by: 1. Reading your owner’s manual. 2. Visiting our customer support website at www.uniden.com. Images in this manual may differ slightly from your actual product. DISCLAIMER: Radar detectors are illegal in some states. Some states prohibit mounting any object on your windshield. Check applicable law in your state and any state in which you use the product to verify that using and mounting a radar detector is legal. Uniden radar detectors are not manufactured and/or sold with the intent to be used for illegal purposes. Drive safely and exercise caution while using this product. Do not change settings of the product while driving. Uniden expects consumer’s use of these products to be in compliance with all local, state, and federal law. Uniden expressly disclaims any liability arising out of or related to your use of this product. CONTENTS CUSTOMER CARE .......................................................................................................... 2 FEATURES....................................................................................................5 WHAT’S IN THE BOX ...................................................................................6 PARTS OF THE R1 ........................................................................................6
    [Show full text]
  • Surfing the Electromagnetic Spectrum
    NDE: SURFING THE ELECTROMAGNETIC SPECTRUM Harry I. Ringermacher General Electric Global Research Center, Niskayuna, NY 12309 Abstract. Advances in Nondestructive Evaluation demand an arsenal of techniques. This was as true twenty years ago as it is today. As materials and their associated technologies progress, so must the strategy for evaluating the quality of the product. Nondestructive Evaluation is a constant struggle to extract, from classical and quantum physics, the quintessential elements that will optimally address an inspection requirement, apart from purely academic interest. It must work to be useful and thereby advance the field. The electromagnetic spectrum, from Roentgen to Maxwell/Hertz, lies at the foundation of both classical and quantum physics. Not only has NDE plucked pearls form every nook of the spectrum ranging from X-rays to T-rays but also has managed to utilize virtually every known coupling of the spectrum to the classical mechanics of heat and sound. I will “surf” the spectrum to provide a sampling of what NDE has extracted past and present as well as try to couple to its future. Keywords: Electromagnetic, NDE, Eddy Current, Microwave, Terahertz, Digital Radiography, Laser Ultrasound, Thermal Imaging PACS: 41.20.-q , 41.50.+h , 42.55.-f , 44.10.+1 , 87.63.Hg , 87.59.bf INTRODUCTION In this overview of electromagnetic (EM) NDE we will be “surfing the spectrum” from the low frequency end , namely radio waves - with application to eddy current - to the high frequency end of the spectrum, x-rays and gamma-rays. We will sample the best NDE technologies in these areas seen through my own eyes – so, apologies in advance for anyone not mentioned since a complete review is out of the scope of this presentation.
    [Show full text]