N. Honingh
University of Cologne
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by N. Honingh.
Astronomy and Astrophysics | 2010
M. Gerin; M. De Luca; J. R. Goicoechea; E. Herbst; E. Falgarone; B. Godard; T. A. Bell; A. Coutens; M. Kaźmierczak; Paule Sonnentrucker; J. H. Black; David A. Neufeld; T. G. Phillips; J. C. Pearson; Paul B. Rimmer; G. Hassel; Dariusz C. Lis; C. Vastel; F. Boulanger; J. Cernicharo; E. Dartois; P. Encrenaz; Thomas F. Giesen; Paul F. Goldsmith; Harshal Gupta; C. Gry; P. Hennebelle; P. Hily-Blant; C. Joblin; R. Kołos
We report the detection of the ground state N, J = 1, 3/2 → 1, 1/2 doublet of the methylidyne radical CH at ∼532 GHz and ∼536 GHz with the Herschel/HIFI instrument along the sight-line to the massive star-forming regions G10.6–0.4 (W31C), W49N, and W51. While the molecular cores associated with these massive star-forming regions show emission lines, clouds in the diffuse interstellar medium are detected in absorption against the strong submillimeter background. The combination of hyperfine structure with emission and absorption results in complex profiles, with overlap of the different hyperfine components. The opacities of most of the CH absorption features are linearly correlated with those of CCH, CN, and HCO + in the same velocity intervals. In specific narrow velocity intervals, the opacities of CN and HCO + deviate from the mean trends, giving rise to more opaque absorption features. We propose that CCH can be used as another tracer of the molecular gas in the absence of better tracers, with [CCH]/[H2] ∼3.2 ± 1.1 × 10 −8 . The observed [CN]/[CH], [CCH]/[CH] abundance ratios suggest that the bulk of the diffuse matter along the lines of sight has gas densities nH = n(H) + 2n(H2) ranging between 100 and 1000 cm −3 .
Astronomy and Astrophysics | 2008
C. Kramer; M. Cubick; M. Röllig; K. Sun; Yoshinori Yonekura; M. Aravena; Frank Bensch; Frank Bertoldi; L. Bronfman; M. Fujishita; Yasuo Fukui; U. U. Graf; M. Hitschfeld; N. Honingh; S. Ito; H. Jakob; K. Jacobs; U. Klein; Bon-Chul Koo; J. May; M. Miller; Yosuke Miyamoto; Norikazu Mizuno; Toshikazu Onishi; Y.-S. Park; Jorge L. Pineda; David Rabanus; H. Sasago; R. Schieder; R. Simon
Context. The Carina region is an excellent astrophysical laboratory for studying the feedback mechanisms of newly born, very massive stars within their natal giant molecular clouds (GMCs) at only 2.35 kpc distance. Aims. We use a clumpy PDR model to analyse the observed intensities of atomic carbon and CO and to derive the excitation conditions of the gas. Methods. The NANTEN2-4 m submillimeter telescope was used to map the [C i] 3 P1− 3 P0, 3 P2− 3 P1 and CO 4–3, 7–6 lines in two 4 � × 4 � regions of Carina where molecular material interfaces with radiation from the massive star clusters. One region is the northern molecular cloud near the compact OB cluster Tr 14, and the second region is in the molecular cloud south of η Car and Tr 16. These data were combined with 13 CO SEST spectra, HIRES/IRAS 60 µm and 100 µm maps of the FIR continuum, and maps of 8 µm IRAC/Spitzer and MSX emission. Results. We used the HIRES far-infrared dust data to create a map of the FUV field heating the gas. The northern region shows an FUV fi eld of af ew 10 3 in Draine units while the field of the southern region is about a factor 10 weaker. While the IRAC 8 µm emission lights up at the edges of the molecular clouds, CO and also [C i] appear to trace the H2 gas column density. The northern region shows a complex velocity and spatial structure, while the southern region shows an edge-on PDR with a single Gaussian velocity component. We constructed models consisting of an ensemble of small spherically symmetric PDR clumps within the 38 �� beam (0.43 pc), which follow canonical power-law mass and mass-size distributions. We find that an average local clump density of 2 × 10 5 cm −3 is needed to reproduce the observed line emission at two selected interface positions. Conclusions. Stationary, clumpy PDR models reproduce the observed cooling lines of atomic carbon and CO at two positions in the Carina Nebula.
Astronomy and Astrophysics | 2010
T. G. Phillips; Edwin A. Bergin; Dariusz C. Lis; David A. Neufeld; T. A. Bell; S. Wang; Nathan R. Crockett; M. Emprechtinger; Geoffrey A. Blake; E. Caux; C. Ceccarelli; J. Cernicharo; C. Comito; F. Daniel; M.-L. Dubernet; P. Encrenaz; M. Gerin; Thomas F. Giesen; J. R. Goicoechea; Paul F. Goldsmith; E. Herbst; C. Joblin; Doug Johnstone; William D. Langer; W. D. Latter; S. Lord; S. Maret; P. G. Martin; Gary J. Melnick; K. M. Menten
We report a detection of the fundamental rotational transition of hydrogen fluoride in absorption towards Orion KL using Herschel/HIFI. After the removal of contaminating features associated with common molecules (“weeds”), the HF spectrum shows a P-Cygni profile, with weak redshifted emission and strong blue-shifted absorption, associated with the low-velocity molecular outflow. We derive an estimate of 2.9 × 10^(13) cm^(-2) for the HF column density responsible for the broad absorption component. Using our best estimate of the H_2 column density within the low-velocity molecular outflow, we obtain a lower limit of ~1.6 × 10^(-10) for the HF abundance relative to hydrogen nuclei, corresponding to ~0.6% of the solar abundance of fluorine. This value is close to that inferred from previous ISO observations of HF J = 2–1 absorption towards Sgr B2, but is in sharp contrast to the lower limit of 6 × 10^(-9) derived by Neufeld et al. for cold, foreground clouds on the line of sight towards G10.6-0.4.
Astronomy and Astrophysics | 2010
S. Bruderer; Arnold O. Benz; E. F. van Dishoeck; M. Melchior; S. D. Doty; F. F. S. van der Tak; P. Stäuber; S. F. Wampfler; C. Dedes; U. A. Yıldız; L. Pagani; T. Giannini; Th. de Graauw; N. Whyborn; D. Teyssier; Willem Jellema; R. Shipman; R. Schieder; N. Honingh; E. Caux; W. Bächtold; A. Csillaghy; C. Monstein; R. Bachiller; Alain Baudry; M. Benedettini; Edwin A. Bergin; P. Bjerkeli; Geoffrey A. Blake; Sylvain Bontemps
The Heterodyne Instrument for the Far Infrared (HIFI) onboard the Herschel Space Observatory allows the first observations of light diatomic molecules at high spectral resolution and in multiple transitions. Here, we report deep integrations using HIFI in different lines of hydrides towards the high-mass star forming region AFGL 2591. Detected are CH, CH + , NH, OH + ,H 2O + , while NH + and SH + have not been detected. All molecules except for CH and CH + are seen in absorption with low excitation temperatures and at velocities different from the systemic velocity of the protostellar envelope. Surprisingly, the CH(JF,P = 3/22,− − 1/21,+ )a nd CH + (J = 1−0, J = 2−1) lines are detected in emission at the systemic velocity. We can assign the absorption features to a foreground cloud and an outflow lobe, while the CH and CH + emission stems from the envelope. The observed abundance and excitation of CH and CH + can be explained in the scenario of FUV irradiated outflow walls, where a cavity etched out by the outflow allows protostellar FUV photons to irradiate and heat the envelope at larger distances driving the chemical reactions that produce these molecules.
Proceedings of SPIE | 2008
Thijs de Graauw; Nick Whyborn; Frank Helmich; P. Dieleman; Peter Roelfsema; E. Caux; T. G. Phillips; Jurgen Stutzki; D. A. Beintema; Arnold O. Benz; Nicolas Biver; A. C. A. Boogert; F. Boulanger; Sergey Cherednichenko; Odile Coeur-Joly; C. Comito; E. Dartois; Albrecht de Jonge; Gert de Lange; Ian Delorme; Anna DiGiorgio; Luc Dubbeldam; Kevin Edwards; Michael Fich; Rolf Güsten; Fabrice Herpin; N. Honingh; Robert Huisman; Herman Jacobs; Willem Jellema
This paper describes the Heterodyne Instrument for the Far-Infrared (HIFI), to be launched onboard of ESAs Herschel Space Observatory, by 2008. It includes the first results from the instrument level tests. The instrument is designed to be electronically tuneable over a wide and continuous frequency range in the Far Infrared, with velocity resolutions better than 0.1 km/s with a high sensitivity. This will enable detailed investigations of a wide variety of astronomical sources, ranging from solar system objects, star formation regions to nuclei of galaxies. The instrument comprises 5 frequency bands covering 480-1150 GHz with SIS mixers and a sixth dual frequency band, for the 1410-1910 GHz range, with Hot Electron Bolometer Mixers (HEB). The Local Oscillator (LO) subsystem consists of a dedicated Ka-band synthesizer followed by 7 times 2 chains of frequency multipliers, 2 chains for each frequency band. A pair of Auto-Correlators and a pair of Acousto-Optic spectrometers process the two IF signals from the dual-polarization front-ends to provide instantaneous frequency coverage of 4 GHz, with a set of resolutions (140 kHz to 1 MHz), better than < 0.1 km/s. After a successful qualification program, the flight instrument was delivered and entered the testing phase at satellite level. We will also report on the pre-flight test and calibration results together with the expected in-flight performance.
Astronomy and Astrophysics | 2010
Nathan R. Crockett; Edwin A. Bergin; S. Wang; Dariusz C. Lis; T. A. Bell; Geoffrey A. Blake; Abraham Cornelis Adwin Boogert; B. Bumble; S. Cabrit; E. Caux; C. Ceccarelli; J. Cernicharo; C. Comito; F. Daniel; M.-L. Dubernet; M. Emprechtinger; P. Encrenaz; E. Falgarone; M. Gerin; Thomas F. Giesen; J. R. Goicoechea; Paul F. Goldsmith; H. Gupta; R. Güsten; Paul Hartogh; Frank Helmich; Eric Herbst; N. Honingh; C. Joblin; Doug Johnstone
We present the first high spectral resolution observations of Orion KL in the frequency ranges 1573.4–1702.8 GHz (band 6b) and 1788.4–1906.8 GHz (band 7b) obtained using the HIFI instrument on board the Herschel Space Observatory. We characterize the main emission lines found in the spectrum, which primarily arise from a range of components associated with Orion KL including the hot core, but also see widespread emission from components associated with molecular outflows traced by H_2O, SO_2, and OH. We find that the density of observed emission lines is significantly diminished in these bands compared to lower frequency Herschel/HIFI bands.
Astronomy and Astrophysics | 2010
D. Johnstone; Michel Fich; C. McCoey; T. A. van Kempen; A. Fuente; L. E. Kristensen; J. Cernicharo; P. Caselli; R. Visser; R. Plume; Gregory J. Herczeg; E. F. van Dishoeck; S. F. Wampfler; R. Bachiller; Alain Baudry; M. Benedettini; Edwin A. Bergin; Arnold O. Benz; P. Bjerkeli; Geoffrey A. Blake; Sylvain Bontemps; J. Braine; S. Bruderer; C. Codella; F. Daniel; A. M. di Giorgio; C. Dominik; S. D. Doty; P. Encrenaz; T. Giannini
Aims. We present preliminary results of the first Herschel spectroscopic observations of NGC 7129 FIRS2, an intermediate mass star-forming region. We attempt to interpret the observations in the framework of an in-falling spherical envelope. Methods. The PACS instrument was used in line spectroscopy mode ( R = 1000-5000) with 15 spectral bands between 63 and 185 mu m. This provided good detections of 26 spectral lines seen in emission, including lines of H2O, CO, OH, O I, and C II. Results. Most of the detected lines, particularly those of H2O and CO, are substantially stronger than predicted by the spherical envelope models, typically by several orders of magnitude. In this paper we focus on what can be learned from the detected CO emission lines. Conclusions. It is unlikely that the much stronger than expected line emission arises in the (spherical) envelope of the YSO. The region hot enough to produce such high excitation lines within such an envelope is too small to produce the amount of emission observed. Virtually all of this high excitation emission must arise in structures such as as along the walls of the outflow cavity with the emission produced by a combination of UV photon heating and/or non-dissociative shocks.
IEEE Microwave and Wireless Components Letters | 2006
Pedro Pablo Munoz; Sven Holger Bedorf; Michael W. Brandt; Thomas Tils; N. Honingh; Karl Jacobs
We describe the design and performance of waveguide mixers at 1.4 THz and 1.9 THz based on NbTiN phonon-cooled hot electron bolometers (HEBs) fabricated on a 2-mum thick Si3N4 membrane. The membrane is bonded to a silicon frame in the mixer block using a flip chip process. Simulated RF coupling is compared with experimental results, showing good agreement. Receiver noise temperature measurements show uncorrected values of 1600 K at 1.4 THz and 2100 K at 1.9 THz, both at 1.5GHz intermediate frequency. Device cooling on the membrane seems not to be problematic. The mixers are used in receivers for the Stratospheric Observatory for Infrared Astronomy (SOFIA) [German REceiver At THz frequencies (GREAT)] and the Atacama path finder experiment (APEX) [CO, N+, deuterium observations receiver (CONDOR)]
Astronomy and Astrophysics | 2008
M. Hitschfeld; M. Aravena; C. Kramer; Frank Bertoldi; J. Stutzki; Frank Bensch; L. Bronfman; M. Cubick; M. Fujishita; Yasuo Fukui; U. U. Graf; N. Honingh; S. Ito; H. Jakob; K. Jacobs; U. Klein; Bon-Chul Koo; J. May; M. Miller; Yosuke Miyamoto; Norikazu Mizuno; Toshikazu Onishi; Y.-S. Park; Jorge L. Pineda; David Rabanus; M. Röllig; H. Sasago; R. Schieder; R. Simon; K. Sun
Studying molecular gas in the central regions of the star burst galaxies NGC4945 and Circinus enables us to characterize the physical conditions and compare them to previous local and high-z studies. We estimate temperature, molecular density and column densities of CO and atomic carbon. Using model predictions we give a range of estimated CO/C abundance ratios. Using the new NANTEN2 4m sub-millimeter telescope in Pampa La Bola, Chile, we observed for the first time CO 4-3 and [CI] 3P1-3 P0 at the centers of both galaxies at linear scale of 682 pc and 732 pc respectively. We compute the cooling curves of 12CO and 13CO using radiative transfer models and estimate the physical conditions of CO and [CI]. The centers of NGC4945 and Circinus are very [CI] bright objects, exhibiting [CI] 3P1 - 3 P0 luminosities of 91 and 67Kkms-1kpc2, respectively. The [CI] 3P1-3 P0/CO 4-3 ratio of integrated intensities are large at 1.2 in NGC4945 and 2.8 in Circinus. Combining previous CO J= 1-0, 2-1 and 3-2 and 13CO J= 1-0, 2-1 studies with our new observations, the radiative transfer calculations give a range of densities, n(H2) = 10^3-3*104^cm-3, and a wide range of kinetic temperatures, Tkin = 20 - 100K, depending on the density. Future CO J= 7-6 and [CI] 2-1 observations will be important to resolve the ambiguity in the physical conditions and confirm the model predictions.
Astronomy and Astrophysics | 2015
L. Rezac; Paul Hartogh; R. Güsten; Helmut Wiesemeyer; Heinz-Wilhelm Hübers; C. Jarchow; Heiko Richter; B. Klein; N. Honingh
Context. The Stratospheric Observatory for Infrared Astronomy (SOFIA) with its 2.5 m telescope provides new science opportunities for spectroscopic observations of planetary atmospheres in the far-infrared wavelength range. Aims. This paper presents first results from the 14 May, 2014 observing campaign of the Martian atmosphere at 4.7 THz using the German REceiver for Astronomy at Terahertz frequencies (GREAT) instrument. Methods. The atomic oxygen 63 m transition, OI, was detected in absorption against the Mars continuum, with a high signal-to-noise ratio ( 35). A beam-averaged atomic oxygen from a global circulation model was used as input to the radiative transfer simulations of the observed line area and to obtain a new estimate on the column density using a grid-search method. Results. Minimizing di erences between the calculated and observed line intensities in the least-square sense yields an atomic oxygen column density of (1:1 0:2) 10 17 cm 2 . This value is about twice as low as predicted by a modern photochemical model of Mars. The radiative transfer simulations indicate that the line forms in the upper atmospheric region over a rather extended altitude region of 70‐120 km. Conclusions. For the first time, a far-infrared transition of the atomic oxygen line was detected in the atmosphere of Mars. The absorption depth provides an estimate on the column density, and this measurement provides additional means to constrain the photochemical models in global circulation models and airglow studies. The lack of other means for monitoring the atomic oxygen in the Martian upper atmosphere makes future observations with the SOFIA observatory highly desirable.