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A Panoramic View of Star Formation in Milky Way: Recent Results from Galactic Plane FIR/Sub-mm Surveys

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2017

Publication Year

2020-08-26T11:08:05Z

Acceptance in OA@INAF

A Panoramic View of Star Formation in Milky Way: Recent Results from Galactic Plane FIR/Sub-mm Surveys

Title

ELIA, Davide Quintino

Authors

10.5281/zenodo.1153787

DOI

http://hdl.handle.net/20.500.12386/26835

(2)

A PANORAMIC VIEW OF STAR

FORMATION IN MILKY WAY:

RECENT RESULTS FROM GALACTIC

PLANE FIR/SUB-MM SURVEYS

(3)

Mo lin ari + 20 14 , PP VI

Large surveys forever

Importance of large panoramic surveys not only to obtain statistically significant samples of sources and structures, but also to investigate large-scale phenomena

(4)

Herschel-­‐SPIRE  250  micron  maps  of  the   por:on  of  the  Galac:c  Plane  observed  in   the  FQS  project.  

12CO  (1-­‐0)  map  integrated  over  the  

velocity  range  8  -­‐24  km  s-­‐1.  

The Forgotten Quadrant Survey

600 hr ESO project at ARO 12-m (IAPS-OAA-IRA)

A

12

CO and

13

CO (1-0) survey of a strip (220° < l < 240°

(5)

Hi-GAL

The Herschel infrared Galactic Plane Survey

Galaxy-wide Census, Luminosity,

Mass and SED of dust structures at

all scales from massive YSOs to

Spiral Arms

Simultaneous 5-bands

(

70-160-250-350-500µm

) continuum

mapping of 720 sq. deg. of the Galactic

Plane (|

b

|≤1°)

With almost 900 hours observing time is the

largest OPEN TIME Herschel KP

(6)

Four scientific work packages (WP1-4):

WP1 – diffuse structure (filaments, bubbles) analysis

WP2 – compact structure (clump) analysis

WP3 – distance estimation

WP4 – combination of WP1-3 into a global scenario of the Galaxy

as a star formation engine

one technical work packages

WP5

Tools and Infrastructures:

Database and Virtual Observatory Infrastructure

Data Mining Systems

3D Visual Analytics systems

Science Gateway

…other packages dedicated to dissemination, management and

coordination activities.

(7)

VIALACTEA is statistics

Estimating completeness limits is not for the faint-hearted !

Molinari+ 2016, Merello+ 2017

(8)

The Hi-GAL Compact Source

“Physical Catalog”

The underlying idea behind this catalog is to extract

physical information from the SEDs of the sources,

collected from 21 to 1100 µm.

Cross-correlation with other tracers represents

a further development of this work.

SED selection is performed in the 160-500 µm

range: only SED eligible for greybody fit are taken

into account.

(9)

Source statistics

-71° < l < 68° 0° < l < 360° 70 µm 122971 141994 160 µm 292051 322827 250 µm 280258 355924 350 µm 161855 215134 500 µm 85880 110991

Hi-GAL is statistics

First-generation Hi-GAL Photometric Catalogues created using CuTEx

package (Molinari+11).

Molinari+2016, Merello+2017

(10)

HI-GAL 5-BAND CATALOG (~9.4 X105 ENTRIES)

HI-GAL 5-BAND FILTERED CATALOG (~1.5 X105ENTRIES)

+

ANCILLARY PHOTOMETRY (MIR, SUB-MM), KINEMATIC DISTANCES

PHYSICAL PROPERTY CATALOG (~1.5 X105 ENTRIES)

INNER GALAXY (~105 ENTRIES) OUTER GALAXY (~5 X104ENTRIES) Elia+ 2017, MNRAS Merello+ 2017, in prep. SED SELECTION   GREY-BODY FIT  

SEDS ARE FURTHER SPLIT IN A “LOW-”

(11)
(12)

Clump demographics

PROTO-STELLAR, 24584 PRE-STELLAR, 34023 UNBOUND, 3831 PRE-STELLAR, 25648 UNBOUND, 12836 PROTO-STELLAR, 15834 PRE-STELLAR, 19195 UNBOUND, 1615 PRE-STELLAR, 14355 UNBOUND, 6066

“High-reliability” catalog “Low-reliability” catalog

whole catalog

with distance

(13)

Source disposition in the inner Galaxy

Ranges corresponding to the tips of the Galactic bar (-30° < l < -20°,

19° < l < 33°) also studied in Veneziani+2017

u  Proto-stellar

u Pre-stellar

(let’s use this color convention throughout this presentation!)

Arm prescription

(14)

Size distributions

•  The angular size is calculated starting from the one estimated by CuTEx at

250 μm.

•  Most sources fulfill the definition of “clump” (e.g., Bergin & Tafalla, 2007).

•  Given a distance, proto-stellar ones are, on average, more compact than

(15)

Temperature distributions

<T

pre

> = 12.0 K

<T

proto

> = 16.0 K

0 10 20 30 40 T[K] 0 2000 4000 6000 Nsources 0 20 40 60 80 100 N(<T)/N tot (%)

(16)

K a uf fm a nn & Pilla i (2 0 1 0 ) K rum holz & Mc K e e (2 0 0 8 ) -2 -1 0 1 Log(Σ/[g cm-2]) 0 500 1000 1500 2000 2500 3000 N -2 -1 0 1 Log(Σ/[g cm-2]) 0 500 1000 1500 2000 2500 3000 N 0 20 40 60 80 100 % On average, proto-stellar sources are denser than pre-stellar ones. 3rd  Larson’s     rela:on  

Mass-Radius relation

pre> = 0.26 g cm-2 proto> = 0.51 g cm-2

(17)

Clump Mass Function Slope

(18)

L

bol

vs M

env

diagram

1 10 100 1000 10000 M (MO •) 100 101 102 103 104 105 Lbol (L O • ) 90% 90%

(19)

-2 -1 0 1 2 3 Log(L/M) 0 500 1000 1500 2000 2500 3000 Nsources -2 -1 0 1 2 3 Log(L/M) 0 500 1000 1500 2000 2500 3000 Nsources 0 20 40 60 80 100 N(<L/M)/N tot (%)

L

bol

/M

env

ratio

Cesaroni+(2015), Hi-GAL

sources detected in CORNISH

Reliable H

II

region candidates

can be searched among

sources above the

L/M > 22.4 L

¤

/M

¤

threshold.

1 10 100 1000 10000 M (MO •) 100 101 102 103 104 105 Lbol (L O • ) 90% 90%

(20)

High-

L

/

M

sources

Compatible with typical

L

/

M

of H

II

regions

MIR-dark sources

Average temperature in the middle

between pre- and proto-stellar

0 10 20 30 40 T[K] 0 2000 4000 6000 Nsources 0 20 40 60 80 100 N(<T)/N tot (%)

u  candidate HII regions

u  MIR-dark

u  all proto-stellar

P a la dini+2 0 1 2

Two possible sub-classes

of proto-stellar sources

(21)

High-

L

/

M

sources

Compatible with typical

L

/

M

of H

II

regions

MIR-dark sources

Average temperature in the middle

between pre- and proto-stellar…

…but these sources

do not constitute the

left tail of the L/M

distribution, and are

highly scattered in

the col-col diagram.

u  candidate HII regions

u  MIR-dark

u  all proto-stellar

-2 -1 0 1 2 3 Log(L/M) 0 500 1000 1500 2000 2500 3000 Nsources -2 -1 0 1 2 3 Log(L/M) 0 500 1000 1500 2000 2500 3000 Nsources 0 20 40 60 80 100 N(<L/M)/N tot (%)

Two possible sub-classes

of proto-stellar sources

(22)

L bol /L subm m = 1 0 0 (Ma ury+, 2 0 1 1 )

L

bol

/L

submm

ratio

0.0 0.5 1.0 1.5 2.0 2.5 3.0 Log(Lbol/Lsmm) 0 500 1000 1500 2000 2500 3000 N sources Equivalent of “Class 0”

Lsubmm calculated for λ > 350 µm

Bolometric Temperature

Tbol = 1.25 ×10−11 −∞νFν dν ∞

Fν dν −∞ ∞

Segregation between pre- and proto-stellar sources appears more evident. The sub-sample of MIR-dark

proto-stellar sources constitutes the left tail of the proto-stellar distribution.

(23)

Dust temperature vs evolutionary descriptors

•  Te m p e rat u re i t s e l f i s a va l i d

evolutionary indicator.

•  Pre-stellar sources follow relations

expected for the greybody (Elia & Pezzuto 2016), while for the same temperature proto-stellar sources generally appear more evolved.

20 25 30 35 T[K] 0.0 0.2 0.4 0.6 0.8 1.0 N HII /N proto [%] C lum ps hosting U C H II re gions (H ofne r+2 0 0 0 ) Lbol Lsubmm ∝ e−n hc 350kT n=1 ∞ ∑ Γ(5 +nβ + i)i i=0 ∞ ∑ &'(350kThc ) * + 4+β+i & ' (( ) * ++ −1 Lbol M ∝ T 4+β T bol∝ 4 +β 4 T

(24)

“Moving away” SF regions

(Baldeschi et al. 2017, I)

(25)

0.75        1        1.5        2        3        5        7  kpc         M > 1282 r pc ! " # $ % & 1.42 Msun

M > 1282

r

pc

!

"

#

$

%

&

1.42

M

sun

Distance bias on M - r relation

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