105 research outputs found

    Long Period Variables in Local Group Dwarf Galaxies

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    In this work the results are presented of an extensive search for Long Period Variables stars (LPVs) in a sample of Local Group irregular dwarf galaxies. The methods applied for the detection and the extraction of the variable sources are explained. Extensive completeness simulations were carried out to asses the impact on the resulting catalog caused by the observing pattern and algorithms used. The resulting catalog of LPVs was together with color-magnitude diagrams used to draw conclusions on the star-formation history in these galaxies

    The evolution of the luminosity functions in the FORS Deep Field from low to high redshift. I. The blue bands

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    We use the very deep and homogeneous I-band selected dataset of the FORS Deep Field (FDF) to trace the evolution of the luminosity function over the redshift range 0.5<z<5.00.5 < z < 5.0. We show that the FDF I-band selection down to IAB=26.8I_{AB}=26.8 misses of the order of 10% of the galaxies that would be detected in a K-band selected survey with magnitude limit KAB=26.3K_{AB}=26.3 (like FIRES). Photometric redshifts for 5558 galaxies are estimated based on the photometry in 9 filters (U, B, Gunn g, R, I, SDSS z, J, K and a special filter centered at 834 nm). A comparison with 362 spectroscopic redshifts shows that the achieved accuracy of the photometric redshifts is Δz/(zspec+1)0.03\Delta z / (z_{\rm spec}+1) \le 0.03 with only ~1% outliers. This allows us to derive luminosity functions with a reliability similar to spectroscopic surveys. In addition, the luminosity functions can be traced to objects of lower luminosity which generally are not accessible to spectroscopy. We investigate the evolution of the luminosity functions evaluated in the restframe UV (1500 Å and 2800 Å), u', B, and g' bands. Comparison with results from the literature shows the reliability of the derived luminosity functions. Out to redshifts of z2.5z\sim 2.5 the data are consistent with a slope of the luminosity function approximately constant with redshift, at a value of 1.07±0.04-1.07 \pm 0.04 in the UV (1500 Å, 2800 Å) as well as u', and 1.25±0.03-1.25\, \pm\, 0.03 in the blue (g', B). We do not see evidence for a very steep slope (α1.6\alpha \le -1.6) in the UV at z3.0\langle z \rangle\sim 3.0 and z4.0\langle z \rangle\sim 4.0 favoured by other authors. There may be a tendency for the faint-end slope to become shallower with increasing redshift but the effect is marginal. We find a brightening of MM^\ast and a decrease of ϕ\phi^\ast with redshift for all analyzed wavelengths. The effect is systematic and much stronger than what can be expected to be caused by cosmic variance seen in the FDF. The evolution of MM^\ast and ϕ\phi^\ast from z=0z=0 to z=5z=5 is well described by the simple approximations M(z)=M0+aln(1+z)M^\ast(z)= M^\ast_0 + {a} \ln\,(1+z) and ϕ(z)=ϕ0(1+z)b\phi^\ast(z)= \phi^\ast_0 (1+z)^{b} for MM^\ast and ϕ\phi^\ast. The evolution is very pronounced at shorter wavelengths (a=2.19a=-2.19, and b=1.76b=-1.76 for 1500 Å rest wavelength) and decreases systematically with increasing wavelength, but is also clearly visible at the longest wavelength investigated here (a=1.08a=-1.08, and b=1.29b=-1.29 for g'). Finally we show a comparison with semi-analytical galaxy formation models

    The evolution of the luminosity functions in the FORS deep field from low to high redshift - II. The red bands

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    We present the redshift evolution of the restframe galaxy luminosity function (LF) in the red r', i', and z' bands, as derived from the FORS Deep Field (FDF), thus extending our earlier results to longer wavelengths. Using the deep and homogeneous I-band selected dataset of the FDF, we were able to follow the red LFs over the redshift range 0.5<z<3.50.5 < z < 3.5. The results are based on photometric redshifts for 5558 galaxies derived from the photometry in 9 filters and achieving an accuracy of Δz/(zspec+1)0.03\Delta z / (z_{\rm spec}+1) \le 0.03 with only ~1 1% outliers. A comparison with results from the literature shows the reliability of the derived LFs. Because of the depth of the FDF, we can give relatively tight constraints on the faint-end slope α of the LF; the faint-end of the red LFs does not show a large redshift evolution and is compatible within 1σ1\sigma to 2σ2\sigma with a constant slope over the redshift range 0.5 \la z \la 2.0. Moreover, the slopes in r', i', and z' are very similar to a best-fitting value of α=1.33±0.03\alpha=-1.33 \pm 0.03 for the combined bands. There is a clear trend of α to steepen with increasing wavelength: αUV&u=1.07±0.04\alpha_{{\rm UV} \& u'}=-1.07 \pm 0.04 \rightarrow αg&B=1.25±0.03\alpha_{g' \& B}=-1.25 \pm 0.03 \rightarrow αr&i&z=1.33±0.03\alpha_{r' \& i' \& z'}=-1.33 \pm 0.03. We subdivided our galaxy sample into four SED types and determined the contribution of a typical SED type to the overall LF. We show that the wavelength dependence of the LF slope can be explained by the relative contribution of different SED-type LFs to the overall LF, as different SED types dominate the LF in the blue and red bands. Furthermore we also derived and analyzed the luminosity density evolution of the different SED types up to z2z \sim 2. We investigated the evolution of MM^\ast and ϕ\phi^\ast by means of the redshift parametrization M(z)=M0+aln(1+z)M^\ast(z)= M^\ast_0 + {a} \ln\,(1+z) and ϕ(z)=ϕ0(1+z)b\phi^\ast(z)= \phi^\ast_0 (1+z)^{b}. Based on the FDF data, we found only a mild brightening of MM^\ast (ar0.8a_{r'} \sim -0.8, and ai,z0.4a_{i',z'} \sim -0.4) and a decreasing ϕ\phi^\ast (br,i,z0.6 b_{r',i',z'} \sim -0.6) with increasing redshift. Therefore, from z0.5\langle z \rangle\sim 0.5 to z3\langle z \rangle\sim 3 the characteristic luminosity increases by ~0.8, ~0.4, and ~0.4 mag in the r', i', and z' bands, respectively. Simultaneously the characteristic density decreases by about 40% in all analyzed wavebands. A comparison of the LFs with semi-analytical galaxy formation models by Kauffmann et al. (1999) shows a similar result to the blue bands: the semi-analytical models predict LFs that describe the data at low redshift very well, but show growing disagreement with increasing redshifts.

    The FORS Deep Field: Field selection, photometric observations and photometric catalog

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    The FORS Deep Field project is a multi-colour, multi-object spectroscopic investigation of a ~ 7arcmin x 7arcmin region near the south galactic pole based mostly on observations carried out with the FORS instruments attached to the VLT telescopes. It includes the QSO Q 0103-260 (z = 3.36). The goal of this study is to improve our understanding of the formation and evolution of galaxies in the young Universe. In this paper the field selection, the photometric observations, and the data reduction are described. The source detection and photometry of objects in the FORS Deep Field is discussed in detail. A combined B and I selected UBgRIJKs photometric catalog of 8753 objects in the FDF is presented and its properties are briefly discussed. The formal 50% completeness limits for point sources, derived from the co-added images, are 25.64, 27.69, 26.86, 26.68, 26.37, 23.60 and 21.57 in U, B, g, R, I, J and Ks (Vega-system), respectively. A comparison of the number counts in the FORS Deep Field to those derived in other deep field surveys shows very good agreement

    Wendelstein observatory operations software

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    Wendelstein observatory control software

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    LMU München operates an astrophysical observatory on Mt. Wendelstein (Hopp et al. 2008). The 2m Fraunhofer telescope (Thiele et al. 2012; Hopp et al. 2012) is equipped with a 0.5 × 0.5 square degree field-of-view wide field camera (Gössl et al. 2012) and a 3 channel optical/NIR camera (Lang-Bardl et al. 2010, 2016). Two fiber coupled spectrographs (Fabricius et al. 2012; Pfeiffer et al. 1998; Brucalassi et al. 2012) and a wavefront sensor will be added in the near future. The observatory hosts a multitude of supporting hardware, i.e. allsky cameras, webcams, meteostation, air conditioning etc. All scientific hardware can be controlled through a single, central “Master Control Program” (MCP). At the ADASS conference in 2014 we presented the overall Wendelstein Observatory software concept (Gössl et al. 2014). Here we explain concept and implementation of the MCP as a multi-threaded Python daemon in the area of conflict between debuggability and Don't Repeat Yourself (DRY)
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