The search of the stellar clusters in vicinity of YSOs with high and middle masses

Similar documents
Faber-Jackson relation: Fundamental Plane: Faber-Jackson Relation

Using Photometric Data to Derive an HR Diagram for a Star Cluster

IV. Molecular Clouds. 1. Molecular Cloud Spectra

A Star and Gas Surface Density Correlation within Nearby Molecular Clouds

Star Formation in the Large Magellanic Cloud: Tracing an Evolution of Giant Molecular Clouds

The Solar Journey: Modeling Features of the Local Bubble and Galactic Environment of the Sun

Ellipticals. Elliptical galaxies: Elliptical galaxies: Some ellipticals are not so simple M89 E0

Classroom Exercise ASTR 390 Selected Topics in Astronomy: Astrobiology A Hertzsprung-Russell Potpourri

Debris disks at high resolution. Mark Wyatt Rachel Smith Institute of Astronomy, Cambridge

Indiana University Science with the WIYN One Degree Imager

Class #14/15 14/16 October 2008

Einstein Rings: Nature s Gravitational Lenses

Star Clusters. Star Clusters E NCYCLOPEDIA OF A STRONOMY AND A STROPHYSICS

Initial Highlights from the Gould Belt Survey

TRANSITING EXOPLANETS

Lecture 14. Introduction to the Sun

arxiv: v1 [astro-ph.sr] 14 Apr 2011

The Evolution of GMCs in Global Galaxy Simulations

arxiv: v1 [astro-ph] 12 Oct 2008

Virtual Observatory tools for the detection of T dwarfs. Enrique Solano, LAEFF / SVO Eduardo Martín, J.A. Caballero, IAC

Origins of the Cosmos Summer Pre-course assessment

Optical Standards. John Nichol BSc MSc

The Size & Shape of the Galaxy

Dwarf Elliptical andFP capture the Planets

Nuclear fusion in stars. Collapse of primordial density fluctuations into galaxies and stars, nucleosynthesis in stars

The CGM around Dwarf Galaxies

Lecture 3 Properties and Evolution of Molecular Clouds. Spitzer space telescope image of Snake molecular cloud (IRDC G

Version A Page The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart.

Understanding Solar Variability as Groundwork for Planet Transit Detection

This paper is also taken for the relevant Examination for the Associateship. For Second Year Physics Students Wednesday, 4th June 2008: 14:00 to 16:00

Adaptation of General Purpose CFD Code for Fusion MHD Applications*

Copyright 2011 Casa Software Ltd. Centre of Mass

Software challenges in the implementation of large surveys: the case of J-PAS

Magellanic Cloud planetary nebulae as probes of stellar evolution and populations. Letizia Stanghellini

ASTRONOMY AND ASTROPHYSICS. Deep search for CO emission in the Low Surface Brightness galaxy Malin 1. J. Braine 1, F. Herpin 1,2, and S.J.E.

Data Provided: A formula sheet and table of physical constants is attached to this paper. DARK MATTER AND THE UNIVERSE

CALCULATION OF CLOUD MOTION WIND WITH GMS-5 IMAGES IN CHINA. Satellite Meteorological Center Beijing , China ABSTRACT

Breakthrough Listen Follow-up of a Transient Signal from the RATAN-600 Telescope in the Direction of HD

circular motion & gravitation physics 111N

Resultados Concurso Apex 2014-A

Observing the Universe

Awell-known lecture demonstration1

A Universe of Galaxies

Description of the Dark Energy Survey for Astronomers

arxiv: v1 [astro-ph.sr] 27 Mar 2014

Proceedings of the NATIONAL ACADEMY OF SCIENCES

Rest optical spectroscopy of FeLoBALs and LoBALs at intermediate redshift

Class 2 Solar System Characteristics Formation Exosolar Planets

Testing maser-based evolutionary schemes: a new search for 37.7-GHz methanol masers

Populations and Components of the Milky Way

arxiv:astro-ph/ v1 31 Jan 2001

6 A High Merger Fraction in the Rich Cluster MS at z =0:83: Direct Evidence for Hierarchical Formation of Massive Galaxies y

The IntelliMagic White Paper: Green Storage: Reduce Power not Performance. December 2010

The Star Formation Histories of Disk and E/S0 Galaxies from Resolved Stars

Hubble Diagram S George Djorgovski. Encyclopedia of Astronomy & Astrophysics P. Murdin

Demonstration of the Applicability of 3D Slicer to Astronomical Data Using

The Virtual Observatory: What is it and how can it help me? Enrique Solano LAEFF / INTA Spanish Virtual Observatory

Chapter 15.3 Galaxy Evolution

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid.

The impact of window size on AMV

The Hidden Lives of Galaxies. Jim Lochner, USRA & NASA/GSFC

Light. What is light?

PTYS/ASTR 206 Section 2 Spring 2007 Homework #2 (Page 1/5) NAME: KEY

Mass limit on Nemesis

arxiv:astro-ph/ v1 30 Jan 1996

PHY114 S11 Term Exam 3

Towards the Detection and Characterization of Smaller Transiting Planets

Sound absorption and acoustic surface impedance

8.1 Radio Emission from Solar System objects

AP PHYSICS C Mechanics - SUMMER ASSIGNMENT FOR

Physics 210 Q ( PHYSICS210BRIDGE ) My Courses Course Settings

Lecture 6: distribution of stars in. elliptical galaxies

Dinamica del Gas nelle Galassie II. Star formation

Dimensional analysis is a method for reducing the number and complexity of experimental variables that affect a given physical phenomena.

3. KINEMATICS IN TWO DIMENSIONS; VECTORS.

DIRECT ORBITAL DYNAMICS: USING INDEPENDENT ORBITAL TERMS TO TREAT BODIES AS ORBITING EACH OTHER DIRECTLY WHILE IN MOTION

Schmidt s Conjecture and Star Formation in Giant Molecular Clouds and Galaxies

Physical Quantities and Units

Pablo Laguna Center for Relativistic Astrophysics School of Physics Georgia Tech, Atlanta, USA

1 Introduction. Name: 1.1 Spectral Classification of Stars. PHYS-1050 Hertzsprung-Russell Diagram Solutions Spring 2013

The Chemical Composition of a Molecular Cloud at the Outer Edge of the Galaxy

Star formation relations across the CO ladder and redshift Thomas R. Greve (University College London)

Atomic and Nuclear Physics Laboratory (Physics 4780)

Resultados Concurso Apex 2007

Observations of DCO + : Tracing the abundance of CO and N 2 in prestellar. cores. Laurent Pagani LERMA, UMR8112 du CNRS, Observatoire de Paris

Galaxy Morphological Classification

Phys222 Winter 2012 Quiz 4 Chapters Name

IRAS in BHR 71 a binary protostellar system?

DETERMINATION OF THE HEAT STORAGE CAPACITY OF PCM AND PCM-OBJECTS AS A FUNCTION OF TEMPERATURE. E. Günther, S. Hiebler, H. Mehling

White Dwarf Properties and the Degenerate Electron Gas

Elliptical Galaxies. Houjun Mo. April 19, Basic properties of elliptical galaxies. Formation of elliptical galaxies

NGUYEN LUONG QUANG. Président du jury: J. Le Bourlot Rapporteurs: H. Beuther, T. Moore Examinateurs: I. Bonnell, F. Boulanger, F. Combes, F.

Chapter 13: Fibonacci Numbers and the Golden Ratio

The Gaia Archive. Center Forum, Heidelberg, June 10-11, Stefan Jordan. The Gaia Archive, COSADIE Astronomical Data

COMPARISON OF GAS AND DUST COOLING RATES IN NEARBY GALAXIES

Blackbody radiation derivation of Planck s radiation low

How To Process Data From A Casu.Com Computer System

Sound. References: L.D. Landau & E.M. Lifshitz: Fluid Mechanics, Chapter VIII F. Shu: The Physics of Astrophysics, Vol. 2, Gas Dynamics, Chapter 8

Schmidt s Conjecture and Star Formation in Giant Molecular Clouds and Galaxies. João Alves, University of Vienna

Transcription:

The search of the stellar clusters in vicinity of YSOs with high and middle masses Naira M. Azatyan, Elena H. Nikoghosyan NAS RA V. Ambartsumian Byurakan Astrophysical Observatory (BAO), Byurakan 0213, Aragatzotn province, Armenia E-mail: nayazatyan@gmail.com Abstract. The results of the searching on the bases of GPS UKIDSS survey's data of dense compact stellar clusters in the vicinity of 20YSOs with high and middle masses are presented. Totally, we have revealed clusters in 13 areas. Around 5 objects (IRAS 18151 1208, IRAS 18316 0602, IRAS 19110+1045, IRAS 19213+1723, IRAS 20056+3350) they are newly detected. The radii and stellar density have significant gradient: from 0.2 to 2.7 pc and from 3 to 1000 stars/pc 2 respectively. Key words: stars: formation stars: clusters stars: luminosity function - infrared: stars. 1. Introduction Nowadays there are a large number of observational data, which indicate that the process of star formation in the stellar clusters of the galactic disk is a multistage process, and therefore, in one cluster can be simultaneously observed the objects at different stages of evolution. Perhaps, the embedded dense compact groups or compact clusters of young stellar objects located around the YSO or a pair of YSOs with high or middle masses can be referred to the youngest objects(lada& Lada 2003).The study of such young formations may be of interest to a number of issues related to the theory of evolution of both the separate stellar objects with different masses and the clusters in general. After the development of observational astronomy in infrared and radio ranges have been published a number of works on the search and study of such centers of star formation (Bica et al. 2003, Kumar et al. 2006-2MASS, Mercer et al. 2005 - Spitzer GLIMPS).However, it should be noted that search of such compact young clusters does not always give a positive result. For example, in (Kumar et al. 2006) the clusters are revealed only in the vicinity of57 out of 217 YSOs with high and middle masses(only 26%). Why they are not detected in other 74% areas? Is it reflecting the real situation or incompleteness of observational data? The aim of this work is also the search of the compact clusters associated with active YSOs with high and middle masses based on the deep NIR survey (K < 18. m 05) GPS UKIDSS. 1

2. The objects selection and investigation methods 2.1. Objects selection. For the search the compact clusters have been chosen the IRAS sources from the list of objects in Varricatt et al.(2010). This list includes 50 YSOs with high and middle masses, in which the various manifestation of activity (H2and CO outflows, NH3, H2O and CH3OH emission and etc.) are observed. All objects are associated with UC HII regions. From this list have been chosen the objects covered by GPS UKIDSS. In total 20 areas were chosen and one of them, namely, IRAS 05137+3919 was already detail examined in Nikoghosyan&Azatyan (2014), where in cluster with radius 1.5 the 80 PMS were revealed. 2.2. The used data. In this work, we used the images, astrometric and photometric data obtained from GPS UKIDSS survey (Lucas et al. 2008). The astrometric accuracy and resolution of images are 0.1arcsec/pix. For the purity of the sample with respect to the photometric parameters, we have selected objects with K<18. m 05.Furthermore, we excluded those objects for which the probability that they are the result of various kinds of noise or defects of image is more than 90% and objects, which coordinates coincide with the Н 2 knots of outflows (Varricatt et al. 2010). 2.3. The clusters identification. To identify the cluster we have constructed the spatial distribution around each IRAS source in the 4 x 4 area. The density was determined simply by dividing the number of stars by the square of box with b х b dimension and step a. For each cluster, sizes of box and step determined empirically to improve the statistical significance of local peaks stellar density in order to maximize the ability to detect the clusters. The cluster was considered really exist, if the surface density around IRAS sources exceed the average density of background more than 2.The isochrones of areas, where revealed the clusters are presented in Fig. 3(the lowest level of isochrones is higher of average field density on 2 ). To confirm the existence of the clusters, as well as to refine their size, we have built also a radial distribution of surface density with respect to the geometric center of the cluster, whose position is marked by cross in Fig. 3. As the radius of the cluster, we have taken the distance from the cluster center, from which, according to the Poisson distribution, the fluctuation of the stellar density in the rings, with a probability of more than 1%, has been random character. One example of the radial density distribution in the cluster is presented in Fig. 1. The density distribution clearly shows that cluster radius is 1.5' and the objects in the cluster distribute not uniform forming subgroups, which also reflect isochrones in Fig. 3. 2

2.4. Photometric analyzes. For the study of nature of the stellar objects of the clusters, we have built JH/HK two-color diagram. One example of the JH/HK two-color diagram is presented in Fig. 2. The J, H, K magnitudes were corrected for absorption, borrowed from http://astro.kent.ac.uk/~df/query_input.html web page. As we can see on the diagram, the significant number of objects are located to the right from the reddening vectors, fall in the area of the Herbig Ae/Be, TTau stars and Class I YSOs, i.e. have a significant infrared excess and are likely PMS stars candidates. We have estimated the probable number of PMS objects in each cluster(n (PMS), see Table 1). Fig.1. The radial distribution of stellar density. Fig. 2. JH/HK two-color diagram. MS and giant branch are adopted from (Bessell& Brett, 1988), TTau locus and reddening vector from (Meyer & Calvet, 1997), H Ae/Be curve and location of Class I YSOs from (Lada & Adams, 1992). To convert JHK magnitudes from UKIRT to CIT photometric system were used the ratios from (Carpenter, 2001). To conform presence of clusters by KLF we applied Kolmogorov-Smirnov test and compared distributions of magnitudes in the cluster region and surrounding field. Last column in Table 1 represent the results of Kolmogorov-Smirnov test (P KS ). 3. Results. Using the above methods, we were able to detect the presence of the stellar cluster around 13 out of 19 IRAS sources. The main parameters for 10 of them are presented in Table 1, where are: (1) - IRAS source; (2) and (3) - the coordinates of the geometric center (4) - the distances to the IRAS sources, barrowed from (Varricatt et al. 2010 and ref. therein); (5) - radiuses of cluster; 3

(6) - cluster richness (the excessive number of stellar objects relative to field average surface density); (7) - the number of probable candidates for PMS stars; (8) - the maximum difference between distributions of magnitudes in cluster and field obtained by KS test. N PMS Table 1 PKS IRAS (1) 05168+3634 05358+3543 18151 1208 18316 0602 18507+0121 19110+1045 19213+1723 20056+3350 20188+3928 20198+3716 THE PARAMETERS OF THE YOUNG STELLAR CLUSTERS RA [2000] (2) [h;m;s] 05209.2 05 39 11.8 18 17 58.2 18 34 21.3 18 53 17.4 19 13 23.2 19 23 37.3 20 07 31.5 20 20 39.3 20 21 41.1 Dec [2000] (3) [ ;';''] +363710 +35 45 46-12 07 30-05 59 44 +01 2503 +10 50 58 +17 29 01 +33 59 39 +39 3808 +37 25 54 d [kpc] (4) R (pc) (5) 1.5 (2.7) 1.1 (0.6) 0.2 (0.2) 0.5 (0.5) 0.4 (0.5) 0.3 (0.5, 0.7) 0.2 (0.25) 0.6 (0.3) 0.5 (0.6) 1.3 (0.3,2.1) (1) - IRAS source, (2) и (3) - coordinates of the geometric center, (4) - distance, (5) - cluster radius, (6) - richness, (7) - number of probable PMS stars, (8) - probability of KS test. 6.1 1.8 3.0 3.2 3.9 6, 8.3 4.3 1.7 3.9 0.9, 5.5 N (6) 93 154 7 53 45 52 22 93 13 385 (7) 80 73 11 38 13 53 22 53-298 0,003 0.007 0.027 0.001 0.010 0.469 0.031 0.041 0.000 0.010 4

Fig. 3.The maps of the surface densityof clusters.by asterisks marked the location ofirassources, by crosses - the geometric centers, by triangles - MSX sources (Egan et al. 2003), by squares - SCUBA sources (Di Francesco et al. 2008, McCutcheon et al. 1995). 5

In addition to above mentioned 10 IRAS sources, clusters was found in the vicinity of IRAS19374+2352 and IRAS19388+2357 too. Because for these compact stellar groups(r < 0.5 ), by using the same methods, similar results have been already obtained in Faustini et al.(2009) we don't include them in Table 1. In addition, we estimated the number of probable PMS stars (N PMS ), which is 55 and 32 respectively. Around of 7 IRAS sources, namely IRAS 18174-1612, IRAS18360-0537, IRAS18385-0512, IRAS18517+0437, IRAS19092+0841, IRAS19410+2336, IRAS20126+4104 were not revealed the stellar clusters in NIR range. 4. Conclusion. Thus, on the bases of GPS UKIDSS survey data from 20 IRAS sources, including IRAS 05137+3919, in the vicinity of 13 of them the compact young stellar clusters were revealed. This amounts 60% of the total study areas, which is much higher than the results obtained according to the 2MASS survey. The radii of clusters and stellar density have significant gradient and are in the range from 0.2 to 2.7 pc and from 3 to 1000 stars/arcmin 2 respectively. References BessellM. S., BrettJ. M., PASP, 100, 261, 1988 BicaE., DutraC. M., BarbuyB., A&A, 397, 177, 2003; CarpenterJ.M., AJ., 121, 2851, 2001 FrancescoJ. Di, JohnstoneD., KirkH., MacKenzieT., LedwosinskaE., ApJS, 175, 295, 2008; EganM. P., PriceS. D., KraemerK. E., AAS, 203, 5708, 2003; FaustiniF., MolinariS., TestiL., BrandJ., A&A, 503, 801, 2009; KumarM. S. N., KetoE., ClerkinE., A&A, 449, 1033, 2006 LadaC. J., AdamsF. C., AJ., 393, 278, 1992; LadaC. J., LadaE. A., ARA&A, 41, 57, 2003; LucasP. W.,HoareM. G., LongmoreA., SchröderA. C., DavisC. J., et al, MNRAS, 391, 136, 2008; McCutcheonW. H., SatoT., PurtonC. R., MatthewsH. E., DewdneyP. E., AJ, 110, 1762, 1995; MercerE. P., ClemensD. P., MeadeM. R., et al., AJ, 635, 560, 2005; MeyerM. R., CalvetN., AJ., 144, 288, 1997 NikoghosyanE., AzatyanN., Ap, 57, 330, 2014; VarricattW.P., DavisC.J., RamsayS., ToddS.P., MNRAS, 404, 661, 2010; McCutcheonW. H., SatoT., PurtonC. R., MatthewsH. E., DewdneyP. E., AJ, 110, 1762, 1995; 6