Red Supergiants As Extragalactic Abundance Probes: Establishing the J-Band Technique

Total Page:16

File Type:pdf, Size:1020Kb

Red Supergiants As Extragalactic Abundance Probes: Establishing the J-Band Technique Red Supergiants as Extragalactic Abundance Probes: Establishing the J-Band Technique J. Zachary Gazak Thesis Committee: Rolf Kudritzki (Chair), Josh Barnes, Fabio Bresolin, Ben Davies, Lisa Kewley, John Learned, and John Rayner ABSTRACT We propose to study the metallicity evolution of star forming galaxies and the ex- panding universe by developing, calibrating, and utilizing methods to extract elemental abundances from quantitative spectroscopy of red supergiants (RSGs). The extreme IR luminosities of RSGs allow for spectroscopic observations over extragalactic distances. By observing a population of RSGs in a target galaxy, the current enrichment as a function of spatial position allows insight into the evolution of the galaxy. By bypass- ing current methodologies (which demand spectral resolutions in excess of R=20,000) in favor of newly proposed analysis techniques requiring more modest resolutions of R ∼3000 in the J band (1.15 - 1.23 µm), our observational efficiency will far exceed current standards. With multi-object capable instruments on both Keck and Subaru we can extend what is possible both in terms of objects observed and accessible dis- tances. In recent years, the advent of quantitative spectroscopy of extragalactic blue supergiants has revolutionized how we understand chemical enrichment and extragalac- tic distances while exposing significant drawbacks in the assumptions and calibrations of non-stellar techniques. By extending our knowledge to an additional population we conduct a critical test of the existing techniques, increased confidence and spatial res- olution in metallicity gradients, and expose a rich new source of information on α/Fe abundances. Furthermore, we pose ourselves to fully exploit the capabilities of future telescopes. Current instruments on Keck and Subaru allow for studies up to 10 Mpc while the next generation of extremely large telescopes will extend this range to at least 30 Mpc, at which point the techniques can be unleashed on entire galaxy clusters. Thus the investment of effort and telescope time for this project are justified by immediate significant scientific returns and the promise that those returns will be dwarfed by future applications of the techniques developed. 1. Introduction Measuring the chemical composition of−and distances to−star forming galaxies have become pivotal goals for modern astrophysics due to the insight they provide into the evolution of galaxies and of the expanding universe. Unraveling the chemical enrichment history of the universe dictates first a clear understanding of the stars which drive that enrichment and the galaxies providing for the formation of those stars. While a solid understanding of the formation and evolution of galaxies remains elusive, the relationship between central metallicity and galactic mass appears to be a critical component (Lequeux et al. 1979; Tremonti et al. 2004; Maiolino et al. 2008), and the metallicity gradient provides a wealth of information needed to describe the complex dynamics of galaxy evolution, including clustering, merging, infall, galactic winds, star formation history, and IMF (Prantzos & Boissier 2000; Colavitti et al. 2008; Yin et al. 2009; S´anchez-Bl´azquezet al. 2009; De Lucia et al. 2004; de Rossi et al. 2007; Finlator & Dav´e2008; Brooks et al. 2007; K¨oppen et al. 2007; Wiersma et al. 2009). However, as intriguing as the observations of the mass-metallicity relationship and the metallic- ity gradients of galaxies are, the published results are highly uncertain. They rely on spectroscopy of H ii region emission lines, mostly oxygen, and the \strong line" analysis method, which uses the fluxes of the strongest forbidden lines (most often [OII] and [OIII]) relative to Hβ (Kewley & Ellison 2008). These methods depend strongly on the choice of calibration, and utilizing different commonly accepted calibrations yields varying and sometimes conflicting results from the same data sets (Fig. 1). Such results have undermined the confidence in observations based on these methods (Kewley & Ellison 2008; Kudritzki et al. 2008; Bresolin et al. 2009). Furthermore, the strong line (collisional) metallicities tend to disagree with recombination line metallicities from the same H ii regions, which measure 0.2 to 0.3 dex higher. Finally, above roughly half solar metallicity, spectral line saturation effects prevent accurate abundance measurements (Stasi´nska 2005). As we reach to higher and higher redshifts with galaxy surveys containing incredible numbers of sources, new observations and calibrations are needed on the most nearby galaxies. The ideal targets for such work are the drivers of galaxy evolution and enrichment−the young, high mass stars which convert hydrogen and helium into heaver elements and deliver those nuclear processed materials back into the interstellar medium (ISM). Indeed it is these massive stars which represent the most salient tracers of the metallicity structure of galaxies as their spectra are imprinted with atmospheric chemical compositions and their short lifetimes dictate that this composition mirrors that of their local ISM. Because of this direct link to galaxy evolution, the impact of investigations targeting individual stars in galaxies has become a convincing motivator for investments of time on the largest telescopes in the world. This new focus is due in part to the advent of atmospheric spectral synthesis modeling, through which spectra of individual stars can be quantitatively studied to extract basic stellar parameters (temperatures and gravities) and accurate chemical abundances of many elements. In this way only the physics of radiative transfer and understanding of atomic structure are needed: few or no empirical calibration techniques are required. Another key development has been the multi-object spectrograph (MOS) which provides an efficiency boost by allowing for the simultaneous collection of many spectra. MOS based instruments make extragalactic stellar astronomy possible even when required integration times reach and sometimes exceed a full night per target. 2 (a) (b) Fig. 1.| (a) The mass-metallicity relationship of star forming galaxies in the nearby universe obtained by applying several widely used empirical metallicity calibrations based on different strong line ratios. This figure illustrates that there is an effect not only on the absolute scale, but also on the relative shape of this relationship. Adapted from Kewley & Ellison (2008). (b) H ii region galactocentric oxygen abundance gradients in the spiral galaxy NGC 300 obtained from the same dataset but different strong line calibra- tions: McGaugh 1991 = M91, Tremonti et al. 2004 = T04, Kewley & Dopita 2002 = KD02, and Pettini & Pagel 2004 = PP04, as shown by the labels to the corresponding least squares fits (from Bresolin et al. 2009). These abundances are compared with auroral line-based abundances determined by Bresolin et al. (2009), which are shown by the full and open circle symbols, and the corresponding linear fit is shown by the continuous line. R25 is the isophotal radius (5.33 kpc). See also Fig. 2. To date the majority of extragalactic quantitative stellar spectroscopy has been undertaken using blue supergiants (BSGs) with observations at optical wavelengths (Bresolin et al. 2001, 2002). BSG chemical compositions are extracted using quantitative techniques with low resolution spectra (Urbaneja et al. 2003; Kudritzki et al. 2008). These techniques have been applied to a number of Local Group galaxies (WLM − Bresolin et al. 2006; Urbaneja et al. 2008; NGC 3109 − Evans et al. 2007; IC1613 − Bresolin et al. 2007; M33 − U et al. 2009), with continued efforts by our group both nearby (M33, NGC6822) and at greater distances (M81, NGC2403). The intent of this dissertation is twofold. First, we plan to develop and exploit techniques for a new, independent stellar population capable of providing reliable chemical enrichment information and an additional test on the BSG methods discussed above. Red supergiants (RSGs) are young, extremely luminous stars which emit strongly in the IR and represent a natural choice for this new population. Second, we will utilize the dominance of these stars on the integrated IR light of young super star clusters (SSCs) to trace metallicities of coeval populations at a larger variety of ages and to greater distances. RSGs are evolutionary successors to BSGs and as such evolve from stars of similar initial mass and thus represent with equal fidelity the chemical makeup of the young stellar population. The extreme luminosities of RSGs peak at ∼ 1µm with absolute J-band magnitudes of MJ = -8 to -11. Their spectra in this bandwidth are rich with features providing diagnostics for extraction of accurate abundances of multiple elements. To date the crippling limitation of utilizing RSGs for extragalactic work has been the need for spectral resolution in 3 Fig. 2.| Radial oxygen abundance gradient obtained from H ii regions (circles) and blue supergiants (star symbols: B supergiants; open squares: A supergiants). The regression to the H ii region data is shown by the continuous line. The dashed line represents the regression to the BA supergiant star data. For reference, the oxygen abundances of the Magellanic Clouds (LMC, SMC) and the solar photosphere are marked. From Bresolin, Gieren, Kudritzki et al. (2009). excess of R=20,000. Recent work by collaborators has demonstrated a promising technique to access accurate chemical composition information from quantitative spectroscopy in the J band (1.15
Recommended publications
  • A Plea for a High-Multiplex J-Band Spectrograph @ VLT Alvio Renzini, MOS Workshop, ESO March 910, 2009
    A Plea for a high-multiplex J-Band spectrograph @ VLT Alvio Renzini, MOS Workshop, ESO March 910, 2009 Beyond redshift 1.4 life gets hard for spectroscopists starforming weakly SF passive Getting redshifts of red galaxies by looking in the ultraviolet (!) Cimatti et al. 2008 13 GMASS Passive galaxies at <z>=1.6 30 to 60 hours per galaxy Total integration time for this stacked FORS2 spectrum: 480h (!) Getting redshifts of emission-line galaxies using absorption lines An example from zCOSMOS: The VIMOS spectrum of a typical SF galaxy @ z~2 Our Preferred playgroud: BzK-selected galaxies COSMOS Field, sBzK's 1.4<z<2.5 McCracken et al. 2009 pBzK's Today, some z>1.4 Pilot Experiments over the GOODS-South field, using the database from Daddi et al. 2007 stars SFR vs Mass for ~1000 BzK Galaxies SFR from rest- frame UV + extinction correction All mass & SFR data from Daddi et al. 2007! BzK-selected 1.4<z<2.5 galaxies in GOODS-S to KVega < 22 Data from Daddi et al 2007 16% 84% To B=25, the current limit of VIMOS w/ 5h integration, one picks only <~16% of the total SFR at 1.4<z<2.5. The most actively SF galaxies are fainter than B=25 The problem is that more actively SF galaxies are more extincted and with VIMOS we are forced to look at them in the rest-frame UV When Extinction is important, it helps going to the infrared One needs an high- multiplex Near-IR multiobject spectrograph! Getting just to the J band allows to do emission line ([OII]) redshifts Most actively SF galaxies are the brightest in the J band an d passive ones kick in Of course, more massive SF galaxies are more extincted And, again, with VIMOS we are forced to look at them in the most extincted rest-frame UV (!!!) And therefore we lose most of the stellar mass @z~2 in a B-magnitude limited sample, to which we are forced w/ VIMOS Again, going to Just the J band would help enormously! But where, how, and when? The same using 25,707 galaxies at 1.4<z<2.5 in the COSMOS field Star Formation Rate J mag B mag ..
    [Show full text]
  • Radio Emission in Ultracool Dwarfs: the Nearby Substellar Triple System VHS 1256–1257 J
    A&A 610, A23 (2018) https://doi.org/10.1051/0004-6361/201732130 Astronomy & © ESO 2018 Astrophysics Radio emission in ultracool dwarfs: The nearby substellar triple system VHS 1256–1257 J. C. Guirado1,2, R. Azulay1,3, B. Gauza4,5,6, M. A. Pérez-Torres7,8, R. Rebolo4,5,9, J. B. Climent1, and M. R. Zapatero Osorio10 1 Departament d’Astronomia i Astrofísica, Universitat de València, C. Dr. Moliner 50, 46100 Burjassot, València, Spain e-mail: [email protected] 2 Observatori Astronòmic, Universitat de València, Parc Científic, C. Catedrático José Beltrán 2, 46980 Paterna, València, Spain 3 Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany 4 Instituto de Astrofísica de Canarias, 38200 La Laguna, Tenerife, Spain 5 Departamento de Astrofísica, Universidad de La Laguna, 38206 La Laguna, Tenerife, Spain 6 Departamento de Astronomía, Universidad de Chile, Camino el Observatorio 1515, Casilla 36-D, Las Condes, Santiago, Chile 7 Instituto de Astrofísica de Andalucía (IAA, CSIC), Glorieta de la Astronomía, s/n, 18008 Granada, Spain 8 Departamento de Física Teórica, Facultad de Ciencias, Universidad de Zaragoza, 50009 Zaragoza, Spain 9 Consejo Superior de Investigaciones Científicas, 28006 Madrid, Spain 10 Centro de Astrobiología (CSIC-INTA), Crta. Ajalvir km 4, 28850 Torrejón de Ardoz, Madrid, Spain Received 19 October 2017 / Accepted 1 December 2017 ABSTRACT Aims. With the purpose of investigating the radio emission of new ultracool objects, we carried out a targeted search in the recently discovered system VHS J125601.92–125723.9 (hereafter VHS 1256–1257); this system is composed by an equal-mass M7.5 binary and a L7 low-mass substellar object located at only 15.8 pc.
    [Show full text]
  • Modeling the Near-Infrared Lines of O-Type Stars
    A&A 422, 275–288 (2004) Astronomy DOI: 10.1051/0004-6361:20047174 & c ESO 2004 Astrophysics Modeling the near-infrared lines of O-type stars A. Lenorzer1,M.R.Mokiem1,A.deKoter1,andJ.Puls2 1 Astronomical Institute “Anton Pannekoek”, Kruislaan 403, 1098 SJ Amsterdam, The Netherlands 2 Institut f¨ur Astronomie und Astrophysik, Universit¨atssternwarte, Scheinerstr. 1, 81679 M¨unchen, Germany Received 30 January 2004 / Accepted 30 March 2004 Abstract. We use a grid of 30 line-blanketed unified stellar photosphere and wind models for O-type stars; computed with the code in order to evaluate its potential in the near-infrared spectral domain. The grid includes dwarfs, giants and supergiants. We analyse the equivalent width behaviour of the 20 strongest lines of hydrogen and helium in spectral windows that can be observed using ground-based instrumentation and compare the results with observations. Our main findings are that: i) He /He line ratios in the J, H and K bands correlate well with the optical ratio employed in spectral classification, and can therefore be used to determine the spectral type; ii) in supergiant stars the transition from the stellar photosphere to the wind follows a shallower density gradient than the standard approach followed in our models, which can be mimicked by adopting a lower gravity in our prescription of the density stratification; iii) the Brγ line poses a number of peculiar problems which might partly be related to wind clumping; and iv) the Brα line is an excellent mass-loss indicator. For the first and last item we provide quantitative calibrations.
    [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]
  • Effect of Ammonium Sulphate on Dielectric Properties of Soil at X & J-Band Microwave Frequency
    International Journal of Recent Technology and Engineering (IJRTE) ISSN: 2277-3878, Volume-8 Issue-4, November 2019 Effect of Ammonium Sulphate on Dielectric Properties of Soil AT X & J-Band Microwave Frequency Syeda Ruhi Nishat, Gulam Rabbani, H.C. Chaudhari, Y.H.Shaikh Abstract: Microwave play important role in the moisture detec- have measured the complex dielectric constant of soils as a tion of soil plant and other agricultural product. In present paper function of water content and temperature over the fre- the study of effect of ammonium sulphate on microwave dielec- quency range from 0.1 to 26 GHz .Peplinski N. R. et al. [4] tric properties of soil is presented. For this three soil samples also studied the dielectric constant ε' and dielectric loss ε" of were collected from different geographical region of Maharash- tra. The infinite sample method was employed for the determina- four soil types having various moisture contents in the fre- tion of storage factor (ε’) and loss factor (ε”) of the soils. In this quency range between 0.3GHz and 1.3 GHz In a detailed paper the effect of ammonium sulphate on dielectric properties of study, Sengwa R. J. and Soni A. [5] have reported the varia- soil when X and J-band microwave frequencies incident on it is tion of dielectric constant with density of dry minerals of discussed. The variation in values of dielectric properties of these soil at 10.1 GHz. Chaudhari H. C. and Shinde V. J. [14] soil samples mixed with different chemical contents are then have reported that the dielectric properties of dry soil at measured at frequency 6 GHz and 9.86 GHz.
    [Show full text]
  • A Narrow J-Band Search for Z∼ 9 Lyα Emitting Galaxies Directed Towards
    Mon. Not. R. Astron. Soc. 384, 1039–1044 (2008) doi:10.1111/j.1365-2966.2007.12404.x ZEN2: a narrow J-band search for z ∼ 9Lyα emitting galaxies directed towards three lensing clusters J. P. Willis,1 F. Courbin,2 J.-P. Kneib3 and D. Minniti4 1Department of Physics and Astronomy, University of Victoria, Elliot Building, 3800 Finnerty Road, Victoria, BC, V8P 1A1, Canada 2Laboratoire d’Astrophysique, Ecole Polytechnique Fed´ erale´ de Lausanne (EPFL), 1290 Sauverny, Switzerland 3Laboratoire d’Astrophysique de Marseille, Traverse du Siphon BP8, 13376 Marseille Cedex 12, France 4Department of Astronomy, P. Universidad Catolica,´ Av. Vicuna˜ Mackenna 4860, Casilla 306, Santiago 22, Chile Accepted 2007 September 3. Received 2007 August 24; in original form 2007 July 30 ABSTRACT We present the results of a continuing survey to detect Lyα emitting galaxies at redshifts z ∼ 9: the ‘z equals nine’ (ZEN) survey. We have obtained deep VLT Infrared Spectrometer and Array Camera observations in the narrow J-band filter NB119 directed towards three massive lensing clusters: Abell clusters 1689, 1835 and 114. The foreground clusters provide a magnified view of the distant Universe and permit a sensitive test for the presence of very high redshift galaxies. We search for z ∼ 9Lyα emitting galaxies displaying a significant narrow-band excess relative to accompanying J-band observations that remain undetected in Hubble Space Telescope (HST)/Advanced Camera for Surveys (ACS) optical images of each field. No sources consistent with this criterion are detected above the unlensed 90 per cent −18 −1 −2 point-source flux limit of the narrow-band image, FNB = 3.7 × 10 erg s cm .
    [Show full text]
  • H-Band Spectroscopic Classification of OB Stars
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server H−Band Spectroscopic Classification of OB Stars R. D. Blum1,T.M.Ramond,P.S.Conti JILA, University of Colorado Campus Box 440, Boulder, CO, 80309 [email protected] [email protected] [email protected] D. F. Figer Division of Astronomy, Department of Physics & Astronomy, University of California, Los Angeles, CA, 90095 fi[email protected] K. Sellgren Department of Astronomy, The Ohio State University 174 W. 18th Ave., Columbus, OH, 43210 [email protected] accepted for publication in the AJ ABSTRACT We present a new spectroscopic classification for OB stars based on H−band (1.5 µmto1.8µm) observations of a sample of stars with optical spectral types. Our initial sample of nine stars demonstrates that the combination of He I 1.7002 µm and H Brackett series absorption can be used to determine spectral types for stars between ∼ O4 and B7 (to within ∼±2 sub–types). We find that the Brackett series exhibits luminosity effects similar to the Balmer series for the B stars. This classification scheme will be useful in studies of optically obscured high mass star forming regions. In addition, we present spectra for the OB stars near 1.1 µmand1.3µm which may be of use in analyzing their atmospheres and winds. Subject headings: infrared: stars — stars: early–type — stars: fundamental parameters 1Hubble Fellow –2– 1. INTRODUCTION OB stars are massive and thus short lived. Because they have short lives, they will be confined to regions relatively close to their birthplaces and will be found close to the Galactic plane.
    [Show full text]
  • Near–Infrared Classification Spectroscopy: J–Band Spectra Of
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Near{Infrared Classification Spectroscopy: J{Band Spectra of Fundamental MK Standards Lloyd Wallace Kitt Peak National Observatory, NOAO1, Tucson, AZ 85726 Michael R. Meyer2 Steward Observatory, The University of Arizona, Tucson, AZ 85721–0065 [email protected] Kenneth Hinkle Kitt Peak National Observatory, NOAO1, Tucson, AZ 85726 [email protected] and Suzan Edwards Astronomy Department, Smith College, Northampton, Massachusetts 01063 ABSTRACT We present a catalog of J–band spectra for 88 fundamental MK standard stars observed at a resolving power of R ∼ 3000. This contribution serves as a companion atlas to the K–band spectra published by Wallace and Hinkle (1997) and the H–band atlas of Meyer et al. (1998). We report data from 7400–9550 cm−1 (1.05–1.34 µm) for stars of spectral types O7–M6 and luminosity classes I–V as defined in the MK system. In reducing these data, special care has been taken to remove time–variable telluric features of water vapor. We identify atomic and molecular indices which are both temperature and luminosity sensitive that aid in the classification of stellar spectra in the J–band. In addition to being useful in the classification of late–type stars, the J–band contains several features of interest in the study of early–type stellar photospheres. These data are available electronically for anonymous FTP in addition to being served on the World Wide Web. Subject headings: infrared: stars – line: identification – stars: fundamental parameters 1Operated by the Association of Universities for Research in Astronomy, Inc.
    [Show full text]
  • Terahertz Emitter Using Resonant-Tunneling Diode and Applications
    sensors Review Terahertz Emitter Using Resonant-Tunneling Diode and Applications Masahiro Asada 1,* and Safumi Suzuki 2 1 Institute of Innovative Research, Tokyo Institute of Technology, Tokyo 152-8552, Japan 2 Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Tokyo 152-8552, Japan; [email protected] * Correspondence: [email protected] Abstract: A compact source is important for various applications utilizing terahertz (THz) waves. In this paper, the recent progress in resonant-tunneling diode (RTD) THz oscillators, which are compact semiconductor THz sources, is reviewed, including principles and characteristics of oscillation, studies addressing high-frequency and high output power, a structure which can easily be fabricated, frequency tuning, spectral narrowing, different polarizations, and select applications. At present, fundamental oscillation up to 1.98 THz and output power of 0.7 mW at 1 THz by a large-scale array have been reported. For high-frequency and high output power, structures integrated with cylindrical and rectangular cavities have been proposed. Using oscillators integrated with varactor diodes and their arrays, wide electrical tuning of 400–900 GHz has been demonstrated. For spectral narrowing, a line width as narrow as 1 Hz has been obtained, through use of a phase-locked loop system with a frequency-tunable oscillator. Basic research for various applications—including imaging, spectroscopy, high-capacity wireless communication, and radar systems—of RTD oscillators has been carried out. Some recent results relating to these applications are discussed. Citation: Asada, M.; Suzuki, S. Keywords: terahertz oscillator; resonant-tunneling diode; frequency tuning; spectral narrowing; Terahertz Emitter Using polarizations; spectroscopy; wireless communication; radar Resonant-Tunneling Diode and Applications.
    [Show full text]
  • Terahertz Wave Generation Using a Soliton Microcomb
    Terahertz wave generation using a soliton microcomb SHUANGYOU ZHANG,1 JONATHAN M. SILVER,1,2 XIAOBANG SHANG,1 LEONARDO DEL BINO,1,3 NICK M. RIDLER,1 AND PASCAL DEL’HAYE1, * 1National Physical Laboratory (NPL), Teddington, TW11 0LW, United Kingdom 2City, University of London, London, EC1V 0HB, United Kingdom 3Heriot-Watt University, Edinburgh, EH14 4AS, Scotland *[email protected] Abstract: The Terahertz or millimeter wave frequency band (300 GHz - 3 THz) is spectrally located between microwaves and infrared light and has attracted significant interest for applications in broadband wireless communications, space-borne radiometers for Earth remote sensing, astrophysics, and imaging. In particular optically generated THz waves are of high interest for low-noise signal generation. Here, we propose and demonstrate stabilized terahertz wave generation using a microresonator-based frequency comb (microcomb). A unitravelling- carrier photodiode (UTC-PD) converts low-noise optical soliton pulses from the microcomb to a terahertz wave at the soliton’s repetition rate (331 GHz). With a free-running microcomb, the Allan deviation of the Terahertz signal is 4.5×10-9 at 1 s measurement time with a phase noise of -72 dBc/Hz (-118 dBc/Hz) at 10 kHz (10 MHz) offset frequency. By locking the repetition rate to an in-house hydrogen maser, in-loop fractional frequency stabilities of 9.6×10-15 and 1.9×10-17 are obtained at averaging times of 1 s and 2000 s respectively, limited by the maser reference signal. Moreover, the terahertz signal is successfully used to perform a proof-of- principle demonstration of terahertz imaging of peanuts.
    [Show full text]
  • Quency EPR Spectroscopy
    Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is © the Owner Societies 2018 SUPPORTING INFORMATION Conformation of Bis-nitroxide Polarizing Agents by Multi-fre- quency EPR Spectroscopy Janne Soetbeer, a† Peter Gast, b Joseph J. Walish, c Yanchuan Zhao, c Christy George, a Chen Yang, a Timothy M. Swager, c Robert G. Griffin, a and Guinevere Mathies a*§ a. Francis Bitter Magnet Laboratory and Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. b. Department of Physics, Huygens-Kamerlingh Onnes Laboratory, Leiden University, PO Box 9504, 2300 RA Lei- den, The Netherlands. c. Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. * To whom correspondence should be addressed. † Current address: Laboratory of Physical Chemistry, Department of Chemistry and Applied Biosciences, ETH Zurich, Vladimir-Prelog-Weg 2, 8093 Zürich, Switzerland § Current address: Department of Chemistry, University of Konstanz, 78464 Konstanz, Germany Contents Alignment of J- and D-band spectra S2 Subtracting the mono-nitroxide contributions for BTamide and BTamide-py S3 Fitting error plots S4 Simulation of bis-nitroxide X S6 S1 Alignment of J- and D-band spectra Figure SI-1: EPR spectra of AMUPol in glycerol/water (a,b) and BTurea in DMSO/water (c,d) at X, D, and J band plotted to- gether with spectra of their corresponding mono-nitroxides. On the D-band spectrometer, the field positions are cross- checked during the field sweep with the 1H NMR resonance from a water sample located near the actual sample, which allows accurate determination of the g-values. In (b) and (d), D- and J-band spectra are plotted with the g-values on the x- axis.
    [Show full text]
  • Reappraisal and New Constraints on Europa's Surface Composition with the Near-Infrared Imaging Spectrometer Sinfoni of The
    51st Lunar and Planetary Science Conference (2020) 1964.pdf REAPPRAISAL AND NEW CONSTRAINTS ON EUROPA’S SURFACE COMPOSITION WITH THE NEAR-INFRARED IMAGING SPECTROMETER SINFONI OF THE VLT. N. Ligier1, J. Carter2, F. Poulet2, L. Fletcher3, O. King3, R. Brunetto2, M. Massé4, C. Snodgrass5 1School of Physical Sciences, Open University, Milton Keynes MK7 6AA, UK. 2Université Paris-Saclay, CNRS, Institut d’Astrophysique Spatiale, 91405 Orsay, France. 3Department of Physics and Astronomy, University of Leicester, Leices- ter LE1 7RH, UK. 4Université de Nantes, CNRS, Laboratoire de Planétologie et Géodynamique, 44322 Nantes, France. 5School of Physics and Astronomy, University of Edinburgh, Edinburgh EH8 9YL, UK. First author contact: [email protected] Context: Europa possesses an important geological Acquisition date Distance to Earth Strehl ratio SSP lat./long. activity expressing itself through plate tectonics [1] and 2017/04/21 4.47 A.U. 29.2 ± 3.5 [232ºW, -3ºN] plumes [2]. This activity is allowed thanks to a tens or 2017/04/22 4.48 A.U. 45.0 ± 0.4 [321ºW, -3ºN] hundreds km-thick subglacial liquid ocean very likely in contact with a silicate mantle [3]. By interacting with that 2017/04/26 4.50 A.U. 36.9 ± 0.6 [18ºW, -3ºN] silicate mantle, the subglacial ocean should contain an im- Table 1. Main observational and geographical parameters of portant variety of chemical species, gathering most of the each observation in the J band. These observations mostly cover requirements needed for the apparition and development the trailing hemisphere, where the chlorinated salts were mostly of exobiological activities [4].
    [Show full text]