14 results on '"Besel, M.-A."'
Search Results
2. Dispersoid composition in zirconium containing Al-Zn-Mg-Cu (AA7010) aluminium alloy
- Author
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Cassell, A.M., Robson, J.D., Race, C.P., Eggeman, A., Hashimoto, T., and Besel, M.
- Published
- 2019
- Full Text
- View/download PDF
3. Damage accumulation of graded steel
- Author
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Besel, M., Brueckner-Foit, A., Zeismann, F., Gruening, A., and Mannel, J.
- Published
- 2010
- Full Text
- View/download PDF
4. Residual stress relaxation of deep-rolled austenitic steel
- Author
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Nikitin, I. and Besel, M.
- Published
- 2008
- Full Text
- View/download PDF
5. Correlation between residual stress and plastic strain amplitude during low cycle fatigue of mechanically surface treated austenitic stainless steel AISI 304 and ferritic–pearlitic steel SAE 1045
- Author
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Nikitin, I. and Besel, M.
- Published
- 2008
- Full Text
- View/download PDF
6. Complete infrared spectral energy distributions of mm detected quasars at z>5
- Author
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Leipski, C., Meisenheimer, K., Walter, F., Besel, M. -A., Dannerbauer, H., Fan, X., Haas, M., Klaas, U., Krause, O., and Rix, H. -W.
- Subjects
Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics::Solar and Stellar Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics::Galaxy Astrophysics ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
We present Herschel far-infrared (FIR) photometry of eleven quasars at redshift z>5 that have previously been detected at 1.2mm. We perform full spectral energy distribution (SED) fits over the wavelength range lambda_rest ~0.1-400mu for those objects with good Herschel detections. These fits reveal the need for an additional far-infrared (FIR) component besides the emission from a dusty AGN-powered torus. This additional FIR component has temperatures of T_FIR ~ 40-60K with luminosities of L_(8-1000mu) ~ 10^13 L_sun (accounting for 25-60% of the bolometric FIR luminosity). If the FIR dust emission is due to star formation it would suggest star formation rates in excess of 1000 solar masses per year. We show that at long wavelengths (lambda_rest > 50mu) the contribution of the AGN-powered torus emission is negligible. This explains how previous FIR studies of high-redshift quasars that relied on single component fits to (ground-based) observations at lambda_obs > 350mu reached T_FIR and L_FIR values similar to our complete SED fits. Stacking the Herschel data of four individually undetected sources reveals a significant average signal in the PACS bands but not in SPIRE. The average SED of sources with individual Herschel detections shows a striking surplus in near- and mid-infrared emission when compared to common AGN templates. The comparison between two average SEDs (sources with and without individual Herschel detections) matched in the UV/optical indicates that for these objects the strength of the MIR emission may correlate with the strength of the FIR emission., Comment: 15 pages, 7 figures, accepted for publication in ApJ
- Published
- 2013
7. Effect of low-frequency on fatigue behaviour of austenitic steel AISI 304 at room temperature and 25 °C
- Author
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Nikitin, I. and Besel, M.
- Published
- 2008
- Full Text
- View/download PDF
8. Influence of joint line remnant on crack paths under static and fatigue loadings in friction stir welded Al-Mg-Sc alloy.
- Author
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Besel, Y., Besel, M., Mercado, U. Alfaro, Kakiuchi, T., and Uematsu, Y.
- Subjects
- *
JOINTS (Engineering) , *FRICTION stir welding , *ALUMINUM-magnesium alloys , *SURFACES (Technology) , *CRACK propagation - Abstract
The influence of the joint line remnant (JLR) on tensile and fatigue fracture behaviour has been investigated in a friction stir welded Al-Mg-Sc alloy. JLR is one of the microstructural features formed in friction stir welds depending on welding conditions and alloy systems. It is attributed to initial oxide layer on butting surfaces to be welded. In this study, two different tool travel speeds were used. JLR was formed in both welds but its spatial distribution was different depending on the tool travel speeds. Under the tensile test, the weld with the higher heat input fractured partially along JLR, since strong microstructural inhomogeneity existed in the vicinity of JLR in this weld and JLR had weak bonding. Resultantly, the mechanical properties of this weld were deteriorated compared with the other weld. Fatigue crack initiation was not affected by the existence of JLR in all welds. But the crack propagated preferentially along JLR in the weld of the higher heat input, when it initiated on the retreating side. Consequently, such crack propagation behaviour along JLR could bring about shorter fatigue lives in larger components in which crack growth phase is dominant. [ABSTRACT FROM AUTHOR]
- Published
- 2016
- Full Text
- View/download PDF
9. COMPLETE INFRARED SPECTRAL ENERGY DISTRIBUTIONS OF MILLIMETER DETECTED QUASARS AT z > 5.
- Author
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LEIPSKI, C., MEISENHEIMER, K., WALTER, F., BESEL, M.-A., DANNERBAUER, H., FAN, X., HAAS, M., KLAAS, U., KRAUSE, O., and RIX, H.-W.
- Subjects
SPECTRAL energy distribution ,INFRARED radiation ,QUASARS ,ASTRONOMICAL photometry ,ACTIVE galaxies - Abstract
We present Herschel far-infrared (FIR) photometry of 11 quasars at redshiftz > 5 that have previously been detected at 1.2 mm. We perform full spectral energy distribution (SED) fits over the wavelength range λ
rest ~ 0.1-400 μm for those objects with good Herschel detections. These fits reveal the need for an additional FIR component besides the emission from a dusty active galactic nucleus (AGN)-powered torus. This additional FIR component has temperatures of TFIR ~ 40-60 K with luminosities of L8-1000 μm ~ 1013 L⊙ (accounting for 25%-60% of the bolometric FIR luminosity). If the FIR dust emission is due to star formation it would suggest star formation rates in excess of 1000 solar masses per year. We show that at long wavelengths (λrest ≳ 50 μm) the contribution of the AGN-powered torus emission is negligible. This explains how previous FIR studies of high-redshift quasars that relied on single-component fits to (ground-based) observations at λobs ≳ 350 μm reached TFIR and LFIR values similar to our complete SED fits. Stacking the Herschel data of four individually undetected sources reveals a significant average signal in the PACS bands but not in SPIRE. The average SED of sources with individual Herschel detections shows a striking surplus in near- and mid-infrared (MIR) emission when compared to common AGN templates. The comparison between two average SEDs (sources with and without individual Herschel detections) matched in the UV/optical indicates that for these objects the strength of the MIR emission may correlate with the strength of the FIR emission. [ABSTRACT FROM AUTHOR]- Published
- 2013
- Full Text
- View/download PDF
10. Observations of infrared echoes around Cassiopeia A with WISE.
- Author
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Besel, M.-A. and Krause, O.
- Subjects
- *
INTERSTELLAR medium , *ASTROPHYSICS , *MATTER , *SPACE environment , *SUPERNOVAE , *CASSIOPEIA (Constellation) - Abstract
Context. Light echoes of supernovae have proven to be a viable tool for characterizing both the supernova explosion mechanism and the surrounding circumstellar and interstellar medium. Aims. We explore new possibilities for identifying infrared echoes with WISE data and extend the area of known echoes around the supernova remnant Cassiopeia A in different illumination conditions. Methods. Preliminary release WISE data around Cassiopeia A is analyzed and compared to Spitzer-MIPS data. While Spitzer-WISE difference images directly show evidence of infrared light echoes, they can also be identified according to their 22/12 μm flux ratio. Results. We find that WISE allows the detection of previously unknown infrared echoes in various illumination conditions. For the first time, infrared echoes at distances greater than 800 pc from a supernova remnant have been found. The 22/12 μm flux ratio criterion can be used as a conceptual factor for identifying infrared echoes around other supernovae as well as providing insights into the dust processing conditions of the interstellar medium. [ABSTRACT FROM AUTHOR]
- Published
- 2012
- Full Text
- View/download PDF
11. Dust in historical Galactic Type Ia supernova remnants with Herschel★.
- Author
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Gomez, H. L., Clark, C. J. R., Nozawa, T., Krause, O., Gomez, E. L., Matsuura, M., Barlow, M. J., Besel, M.-A., Dunne, L., Gear, W. K., Hargrave, P., Henning, Th., Ivison, R. J., Sibthorpe, B., Swinyard, B. M., and Wesson, R.
- Subjects
ACTIVE galaxies ,SUPERNOVA remnants ,X-ray spectroscopy ,ASTRONOMICAL photometry ,COSMIC grains ,CIRCUMSTELLAR matter - Abstract
ABSTRACT The origin of interstellar dust in galaxies is poorly understood, particularly the relative contributions from supernovae and the cool stellar winds of low-intermediate-mass stars. Recently, large masses of newly formed dust have been discovered in the ejecta of core-collapse supernovae. Here, we present Herschel Photodetector Array Camera and Spectrometer (PACS) and Spectral and Photometric Imaging Receiver (SPIRE) photometry at 70-500 m of the historical, young supernova remnants: Kepler and Tycho, both thought to be the remnants of Type Ia explosion events. We detect a warm dust component in Kepler's remnant with and mass ; this is spatially coincident with thermal X-ray emission and optical knots and filaments, consistent with the warm dust originating in the circumstellar material swept up by the primary blast wave of the remnant. Similarly for Tycho's remnant, we detect warm dust at with mass . Comparing the spatial distribution of the warm dust with X-rays from the ejecta and swept-up medium, and Hα emission arising from the post-shock edge, we show that the warm dust is swept up interstellar material. We find no evidence of a cool (25-50 K) component of dust with mass ≥0.07 M
⊙ as observed in core-collapse remnants of massive stars. Neither the warm or cold dust components detected here are spatially coincident with supernova ejecta material. We compare the lack of observed supernova dust with a theoretical model of dust formation in Type Ia remnants which predicts dust masses of 88(17) × 10−3 M⊙ for ejecta expanding into ambient surrounding densities of 1(5) cm−3 . The model predicts that silicon- and carbon-rich dust grains will encounter, at most, the interior edge of the observed dust emission at ∼400 years, confirming that the majority of the warm dust originates from swept-up circumstellar or interstellar grains (for Kepler and Tycho, respectively). The lack of cold dust grains in the ejecta suggests that Type Ia remnants do not produce substantial quantities of iron-rich dust grains and has important consequences for the 'missing' iron mass observed in ejecta. Finally, although, we cannot completely rule out a small mass of freshly formed supernova dust, the Herschel observations confirm that significantly less dust forms in the ejecta of Type Ia supernovae than in the remnants of core-collapse explosions. [ABSTRACT FROM AUTHOR]- Published
- 2012
- Full Text
- View/download PDF
12. Surface damage evolution of engineering steel.
- Author
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BESEL, M. and BRUECKNER-FOIT, A.
- Subjects
- *
CARBON steel , *MATERIAL fatigue , *LOADING & unloading , *FERRITES , *FRACTURE mechanics - Abstract
The surface damage evolution of ordinary low carbon steel under mechanical fatigue loading was observed using a long-distance microscope. Fatigue cracks initiated at pits, sulfide inclusions and in the soft ferrite phase. Damage evolution was not only pronounced by the initiation of well-defined cracks. Areas of high plastic activity interspersed with microcracks exist. Coalescence of propagating well-defined cracks with these areas of high plastic activity shows clearly the contribution of such plastified areas to the damage accumulation. Therefore, well-known damage parameters such as line counts (i.e. maximum crack length) are unsuitable to describe the damage evolution. In this paper, a new damage parameter is defined based on the observation that cracks and plastified areas appear as dark regions. It is shown that this parameter satisfies the basic conditions for a damage parameter. It is used to evaluate the damage accumulation quantitatively based on surface observations even for complex damage patterns. [ABSTRACT FROM AUTHOR]
- Published
- 2008
- Full Text
- View/download PDF
13. A COOL DUST FACTORY IN THE CRAB NEBULA: A HERSCHEL STUDY OF THE FILAMENTS.
- Author
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Gomez, H. L., Krause, O., Barlow, M. J., Swinyard, B. M., Owen, P. J., Clark, C. J. R., Matsuura, M., Gomez, E. L., Rho, J., Besel, M. -A, Bouwman, J., Gear, W. K., Henning, Th., Ivison, R. J., Polehampton, E. T., and Sibthorpe, B.
- Subjects
CRAB Nebula ,NEBULAE ,SUPERNOVA 1054 ,GALAXIES - Abstract
Whether supernovae are major sources of dust in galaxies is a long-standing debate. We present infrared and submillimeter photometry and spectroscopy from the Herschel Space Observatory of the Crab Nebula between 51 and 670 μm as part of the Mass Loss from Evolved StarS program. We compare the emission detected with Herschel with multiwavelength data including millimeter, radio, mid-infrared, and archive optical images. We carefully remove the synchrotron component using the Herschel and Planck fluxes measured in the same epoch. The contribution from line emission is removed using Herschel spectroscopy combined with Infrared Space Observatory archive data. Several forbidden lines of carbon, oxygen, and nitrogen are detected where multiple velocity components are resolved, deduced to be from the nitrogen-depleted, carbon-rich ejecta. No spectral lines are detected in the SPIRE wavebands; in the PACS bands, the line contribution is 5% and 10% at 70 and 100 μm and negligible at 160 μm. After subtracting the synchrotron and line emission, the remaining far-infrared continuum can be fit with two dust components. Assuming standard interstellar silicates, the mass of the cooler component is 0.24
+0.32 – 0.08 M☼ for T = 28.1+5.5 – 3.2 K. Amorphous carbon grains require 0.11 ± 0.01 M☼ of dust with T = 33.8+2.3 – 1.8 K. A single temperature modified blackbody with 0.14 M☼ and 0.08 M☼ for silicate and carbon dust, respectively, provides an adequate fit to the far-infrared region of the spectral energy distribution but is a poor fit at 24-500 μm. The Crab Nebula has condensed most of the relevant refractory elements into dust, suggesting the formation of dust in core-collapse supernova ejecta is efficient. [ABSTRACT FROM AUTHOR]- Published
- 2012
- Full Text
- View/download PDF
14. Dust in historical Galactic Type Ia supernova remnants with Herschel★.
- Author
-
Gomez, H. L., Clark, C. J. R., Nozawa, T., Krause, O., Gomez, E. L., Matsuura, M., Barlow, M. J., Besel, M.-A., Dunne, L., Gear, W. K., Hargrave, P., Henning, Th., Ivison, R. J., Sibthorpe, B., Swinyard, B. M., and Wesson, R.
- Subjects
- *
ACTIVE galaxies , *SUPERNOVA remnants , *X-ray spectroscopy , *ASTRONOMICAL photometry , *COSMIC grains , *CIRCUMSTELLAR matter - Abstract
ABSTRACT The origin of interstellar dust in galaxies is poorly understood, particularly the relative contributions from supernovae and the cool stellar winds of low-intermediate-mass stars. Recently, large masses of newly formed dust have been discovered in the ejecta of core-collapse supernovae. Here, we present Herschel Photodetector Array Camera and Spectrometer (PACS) and Spectral and Photometric Imaging Receiver (SPIRE) photometry at 70-500 m of the historical, young supernova remnants: Kepler and Tycho, both thought to be the remnants of Type Ia explosion events. We detect a warm dust component in Kepler's remnant with and mass ; this is spatially coincident with thermal X-ray emission and optical knots and filaments, consistent with the warm dust originating in the circumstellar material swept up by the primary blast wave of the remnant. Similarly for Tycho's remnant, we detect warm dust at with mass . Comparing the spatial distribution of the warm dust with X-rays from the ejecta and swept-up medium, and Hα emission arising from the post-shock edge, we show that the warm dust is swept up interstellar material. We find no evidence of a cool (25-50 K) component of dust with mass ≥0.07 M⊙ as observed in core-collapse remnants of massive stars. Neither the warm or cold dust components detected here are spatially coincident with supernova ejecta material. We compare the lack of observed supernova dust with a theoretical model of dust formation in Type Ia remnants which predicts dust masses of 88(17) × 10−3 M⊙ for ejecta expanding into ambient surrounding densities of 1(5) cm−3. The model predicts that silicon- and carbon-rich dust grains will encounter, at most, the interior edge of the observed dust emission at ∼400 years, confirming that the majority of the warm dust originates from swept-up circumstellar or interstellar grains (for Kepler and Tycho, respectively). The lack of cold dust grains in the ejecta suggests that Type Ia remnants do not produce substantial quantities of iron-rich dust grains and has important consequences for the 'missing' iron mass observed in ejecta. Finally, although, we cannot completely rule out a small mass of freshly formed supernova dust, the Herschel observations confirm that significantly less dust forms in the ejecta of Type Ia supernovae than in the remnants of core-collapse explosions. [ABSTRACT FROM AUTHOR]
- Published
- 2012
- Full Text
- View/download PDF
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