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A Comparison of A Comparison of

Protostellar Luminosity Protostellar Luminosity Functions Across Diverse Functions Across Diverse Star Forming Environments Star Forming Environments

E. Kryukova E. Kryukova (U. of Toledo) (U. of Toledo) S. T.

S. T. Megeath Megeath (U. of Toledo) (U. of Toledo) Collaborators:

Collaborators:

R. R. Gutermuth Gutermuth (U. of (U. of Massachussets Massachussets ); J. ); J. Pipher Pipher (U. of Rochester); (U. of Rochester);

T. Allen (U. of Toledo); L. E. Allen (NOAO); P. C. Myers

T. Allen (U. of Toledo); L. E. Allen (NOAO); P. C. Myers (SAO); (SAO);

J. Muzerolle J. Muzerolle (STScI ( STScI); Cygnus ); Cygnus -X Legacy Team - X Legacy Team

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Fundamental Question:

Fundamental Question:

How does environment affect star How does environment affect star formation and the properties of formation and the properties of

nascent stars?

nascent stars?

Protostars

Protostars are still located in their natal environment, are still located in their natal environment, allowing us to connect the star formation process to allowing us to connect the star formation process to

its environment.

its environment.

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Core mass function Core mass function

Protostellar

Protostellar luminosity luminosity function

function

Da Rio et al. 2010

Initial mass function Initial mass function

Sadavoy et al. 2010

Protostellar luminosity:

r M GM acc

L

L L

L =

*

+ =

*

+

&

Protostellar luminosity is in part a measure of mass accretion rate.

“Luminosity Problem”:

Protostars have luminosities less than would be expected for the accretion rate determined from the anticipated IMF and observed star formation rate (Kenyon &

Hartmann 1990, Dunham et al.

2010).

(4)

Spitzer surveys have provided an Spitzer surveys have provided an unprecedented sample of

unprecedented sample of protostars protostars in clouds in clouds at distances < 1

at distances < 1 kpc kpc with diverse properties: with diverse properties:

Clouds with distributed, low

Clouds with distributed, low- -mass star formation (SF): mass star formation (SF):

Taurus, Lupus,

Taurus, Lupus, Chamaeleon Chamaeleon (34 protostar (34 protostar candidates) candidates) Clouds with clustered, low

Clouds with clustered, low- - mass SF: mass SF:

Serpens

Serpens (40), (40), Perseus Perseus (58), (58), Ophiuchus Ophiuchus (24) (24) Clouds with high

Clouds with high- - and low- and low - mass SF: mass SF:

Orion (274),

Orion (274), Cep Cep OB3 (97), Mon R2 (89) OB3 (97), Mon R2 (89)

To compare star formation in these clouds spanning a range of To compare star formation in these clouds spanning a range of diverse environments, we have constructed

diverse environments, we have constructed protostellar protostellar luminosity luminosity functions for each of these kinds of clouds.

functions for each of these kinds of clouds.

Orion Perseus

Serpens

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Select

Select protostarsprotostars by their mid-by their mid-IR colors (IR colors (MegeathMegeath et al. 2009).

et al. 2009).

The protostarThe protostar sample includes sources with both sample includes sources with both flat and rising

flat and rising SEDs. SEDs.

Our sample will not contain very deeply Our sample will not contain very deeply

embedded Class 0 sources with faint [24]

embedded Class 0 sources with faint [24]

emission.

emission.

Cutoff magnitude

Minimize contamination due to galaxies by Minimize contamination due to galaxies by comparing [24] with a set of galaxies from the comparing [24] with a set of galaxies from the SWIRE sample and setting the [24] cutoff

SWIRE sample and setting the [24] cutoff magnitude.

magnitude.

We require

We require protostarsprotostars to have [24] detections and to have [24] detections and Av > 3.

Av > 3.

Infrared

Infrared Protostar Protostar Candidate Selection Candidate Selection

Rising Spectrum Protostars

Flat Spectrum Protostars

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1. Calculate 3-24 micron SED slope from IRAC and MIPS data.

2. Integrate over 1-24 micron bands to calculate mid-IR luminosity.

3. Convert mid-IR to bolometric luminosities using an empirically derived relationship.

c2d protostars with known bolometric luminosities

IRAC 2MASS

MIPS

Luminosity

Luminosity - - Slope Relationship Slope Relationship

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Contamination Removal Contamination Removal

Possible sources of contamination:

Possible sources of contamination:

1. Reddened Class II Estimated with a Monte Carlo simulation that uses a representative

sample of Orion Class II sources and extinction maps for each cloud to predict the number of reddened disks misidentified as protostars.

2. Edge-on Disk

Estimated using technique from Gutermuth et al. 2009 and a low- Av sample of YSOs from Cep OB3b.

3. Background Galaxy Estimated using the SWIRE sample.

IR protostar candidates

Reddened Class II

Galaxies

Edge-on

Disks

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Luminosity functions peak near 1 Lsun for clouds which form high mass stars, and at 0.1 Lsun for Perseus and

Ophiuchus.

Orion, Cep OB3, and Mon R2 show tails extending to luminosities > 100 Lsun.

Combined luminosity functions differ between high mass SF clouds and low mass SF clouds, with a KS test

probability P = 0.02.

Luminosities less than expected for continuous accretion over 5 x 105years (Lacc ~ 5 Lsun), particularly for low mass regions Æ luminosity problem not solved.

140 35 46

20 37 12

16 221 65

Sensitivity limit based on [24] cutoff

Luminosity Functions for Contamination Luminosity Functions for Contamination

Subtracted

Subtracted Protostars Protostars

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P = 0.91

5th

Clustering cutoff length to 5

Clustering cutoff length to 5ththnearest neighbor YSO selected so that there are equal numbers onearest neighbor YSO selected so that there are equal numbers of f clustered and distributed

clustered and distributed protostarsprotostars.. Orion clustered

Orion clustered protostarsprotostarsextend to higher luminosities, difference in clustered and distributed extend to higher luminosities, difference in clustered and distributed luminosity functions are statistically different.

luminosity functions are statistically different.

More crowded regions will be more incomplete to faint

More crowded regions will be more incomplete to faint protostarsprotostars; however, drop off at faint ; however, drop off at faint luminosities appears to be determined primarily by subtraction o

luminosities appears to be determined primarily by subtraction of reddened stars with disks.f reddened stars with disks.

5th

Clustered

Distributed

Clustered Distributed

P < 0.01

Luminosity vs. Clustering: Nearest Neighbor Luminosity vs. Clustering: Nearest Neighbor

( ( nn nn = 5) Distances = 5) Distances

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Protostars

Protostars link the CMF and the IMF.link the CMF and the IMF.

We construct

We construct protostellarprotostellar luminosity functions from Spitzer mid-luminosity functions from Spitzer mid-IR data.IR data.

Contamination due to edge

Contamination due to edge--on or reddened Class II on or reddened Class II YSOsYSOs eliminates a nearly half eliminates a nearly half of all IR

of all IR protostarprotostar candidates, but does not solve the “candidates, but does not solve the “luminosity problemluminosity problem””.. Luminosity functions peak near 1

Luminosity functions peak near 1 LLsunsun for clouds which form high mass stars, and for clouds which form high mass stars, and peak at 0.1

peak at 0.1 LLsunsun for Perseusfor Perseus and Ophiuchusand Ophiuchus..

The luminosity function for clouds which form high mass stars ar

The luminosity function for clouds which form high mass stars are statistically e statistically different from those of clouds which do not.

different from those of clouds which do not.

Orion clustered

Orion clustered protostarsprotostarsextend to higher luminosities than do Orion distributed extend to higher luminosities than do Orion distributed protostars

protostars, and there is a significant difference between luminosity funct, and there is a significant difference between luminosity functions of ions of clustered and distributed populations.

clustered and distributed populations.

Protostellar

Protostellar luminosity functions appear to change with environment (betweenluminosity functions appear to change with environment (between clouds with and without high mass star formation, and between cl

clouds with and without high mass star formation, and between clustered and ustered and distributed regions).

distributed regions).

Given correlation between stellar density and gas density (

Given correlation between stellar density and gas density (GutermuthGutermuth et al. in et al. in prep), is this due to higher gas column

prep), is this due to higher gas column densititesdensitites in regions with clusters and in regions with clusters and nascent high mass stars?

nascent high mass stars?

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Next Step: Cygnus

Next Step: Cygnus - - X (1.7 X (1.7 kpc kpc ) )

Cygnus-X legacy survey: Hora et al. in prep.

3.6 μm blue 4.5 μm green 24 μm red

RA

Dec

Caution: Work in Progress!

Caution: Work in Progress!

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Protostars in DR21 and surroundings

Brightest sources may be affected by saturation/confusion.

Class II not shown

Yellow circles protostars

3.6 μm blue 4.5 μm green 24 μm red

RA

Dec

Beerer et al. 2010

Outflow

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Cygnus

Cygnus - - X Luminosity Function X Luminosity Function

Sensitivity limit based on [24] cutoff Many more protostars in Cygnus-X (770) than Orion (140)

Need to better establish the completeness at both faint and bright luminosities

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Cygnus

Cygnus - - X Luminosity vs. NN Distance ( X Luminosity vs. NN Distance ( nn nn = 5) = 5)

P < 0.01 Clustering cutoff length at

0.52 pc (Orion at 0.19 pc)

Preliminary results indicate that there is a similar

dependence of protostellar luminosity on stellar

density in Cygnus-X as in

Orion.

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