Transcript

What Sculpts What Sculpts the Interstellar the Interstellar

Medium?Medium?

Alyssa A. Goodman

Harvard University

Galaxies & Museums

Galaxies Galaxies && MuseumsMuseums

• Galactic Rotation + Gravity– GMCs (105=106 MD)

• SNe, GRBs, OB winds– Cloud complex (sub-GMC)

• MHD waves, MHD turbulence, shocks– More "internal structure," – sometimes resulting in "cores"

• Star-Formation, Evaporation– Eventual disappearance of gas

• Geology– Deposit of Marble

• Saws & Dynamite– Block with specific aspect ratio

• Series of chisels– Head, Arms, Legs, then

Fingers, Toes, Eyes, Mouth– sometimes human form

• Wars, Wind– Eventual disappearance of art

Outflows

MHD Waves

Thermal Motions

MHD Turbulence

Infall

SNe/GRBH II Regions

B, G, T or 's alone

many different varieties

Tools for finding the toolsTools for finding the tools

Key Method:Key Method: Use the velocity field– third (really fourth) dimension– valuable information on energetics

ToolsTools for finding the tools for finding the tools

-Introduction to measuring velocity structureIntroduction to measuring velocity structure

-Blasting-Blasting UMaj Example: Specialized Velocity Analysis

-Chiseling-Chiseling Generic chiseling: Line width-Size relations "In our own image": Coherent Dense Cores Quality Control: The Spectral Correlation Function

-"Weathering"-"Weathering" Sandblasting? Extinction Studies

Velocity as a "Fourth" DimensionSpectral Line Observations

Mountain RangeNo loss of

information

Loss of1 dimension

W3

-49 to -41 km/sec-39to-31km/sec

Kannappan & Goodman 1999 & Dowell 1998

o4% polarizati n

13CO Channel Maps13CO Integrated Intensity

Dust Thermal Emission

BlastingBlasting

Pound & Goodman 1997

Ursa Major HLC

Complex

• “High-latitude”= very nearbyvery nearby (DUMAJ~100 pc)

• ~No star formation~No star formation1

• Energy distribution very differentEnergy distribution very different than star-forming regions

High Latitude CloudHigh Latitude Cloud2

Gravitational << Magnetic ≈ Kinetic

Star-Forming CloudStar-Forming Cloud3

Gravitational ≈ Magnetic ≈ Kinetic

(1) Magnani et al. 1996; (2) Myers, Goodman, Güsten & Heiles 1995; (3) Myers & Goodman 1988

High-latitude CloudsHigh-latitude Clouds

The Velocity Field in The Velocity Field in Ursa MajorUrsa Major

H I CO

Pound & Goodman 1997

vv and and vvLSRLSR GradientsGradients

35.00

36.25

37.50

38.75

142.50 141.00

3

6

9

12

15

0 2 4 6 8

v

vLSR

Lat

itud

e [d

eg]

Longitude [deg]

Hat Creek H I Data

vz,obs

vz,obs

y

z

Line widthprimarily

tangential

Line widthprimarily

radial

z

-y

vradvtan

Line widthprimarily

radial

Line widthprimarily

tangential

vtanvrad

vtanvrad

In General... ...in Ursa Major

implication:

implication:

Confirmation: Position Velocity Confirmation: Position Velocity Diagrams for H I and CODiagrams for H I and CO

CO

H I

Position Along Filament 1

Position Along Filament 2

CO Blueshifted w.r.t. H I in both filaments, in arc-like patternCO Blueshifted w.r.t. H I in both filaments, in arc-like pattern

vz,obsRed

Blue

Observed in Ursa Major

CO blueshifted

w.r.t H I Shell

y

2 1

43

vz,rot

vz,exp

vz,rot

vz,expz

Implications of Ursa Major StudyImplications of Ursa Major Study

• Many HLC’s may be related to “supershell” structures; some shells harder to identify than NCP Loop.

• (Commonly observed) velocity offsets between atomic and molecular gas may be due to impacts, followed by conservation of momentum. Use this as a clue in other cases.

ChiselingChiseling

Generic ChiselingGeneric Chiseling ( (((B, G, T, B, G, T, 's 's )) ))Self-similar structure

Line width-Size RelationsLine width-Size Relations ((v~Rv~Raa))

"In our own image""In our own image"Putting down the chisel:Putting down the chisel: Coherent Dense Cores Coherent Dense Cores

Quality ControlQuality ControlThe Spectral Correlation Function The Spectral Correlation Function [which [which ((B, G, T, B, G, T, 's 's )?] )?]

Self-similar StructureSelf-similar Structure on scales from 100 pc to 0.1 pc...in Orion

65 pc

Maddalena et al. 1986CO Map, 8.7 arcmin resolution

Columbia-Harvard “Mini”

Dutrey et al. 1991C18O Map, 1.7 arcmin resolution

AT&T Bell-Labs 7-m

3.5 pc0.6 pc0.6 pc

Wiseman 1995Wiseman 1995NHNH33 Map, 8 arcsec resolution Map, 8 arcsec resolution

VLAVLA

3.5 pc0.6 pc0.6 pc

Types of Line width-Size RelationsTypes of Line width-Size Relations

Tracer 5

Tracer 1Tracer 2Tracer 3Tracer 4

Ensemble of CloudsEnsemble of Clouds

FWHM of Various Tracers ShownObserved Size

Non

-th

erm

al

Lin

e W

idth

Type 1: “Larson’s Law”Type 1: “Larson’s Law”

Gives overall state of ISM~magnetic virial equilibrium.See Larson 1981; Myers & Goodman 1988 for examples.

v~R0.5

““Larson’s LawLarson’s Law” ” Scaling RelationsScaling Relations (1981)(1981)

(line width)~(size)1/2 (density)~(size)-1

Curves assume M=K=G (Myers & Goodman 1988)

Galaxy

"Velocity Coherent" Dense Core

Young Stellar Object +Outflow

Stars

time

Self-Similar, Turbulent,"Larson's Law" Clouds

What What chiseling can chiseling can

produce...produce...

(a.k.a. GMC or Cloud Complex)

Coherent Cores: “Islands of Calm Coherent Cores: “Islands of Calm in a Turbulent Sea”in a Turbulent Sea”

"Rolling Waves" by KanO Tsunenobu © The Idemitsu Museum of Arts.

Hint #1: Independent Core RotationHint #1: Independent Core Rotation

Goodman, Benson, Fuller & Myers 1993

Hint #2: Constant Line Width in Cores?Hint #2: Constant Line Width in Cores?

Example of the (Original) Evidence for CoherenceExample of the (Original) Evidence for Coherence

2

3

4

5

6

7

8

9

1

vN

T[km

s-1

]

6 7 8 90.1

2 3 4 5 6 7 8 91

TA [K]

34567890.1

23

"Radius" from Peak [parsecs]

TMC-1C, NH3 (1, 1)

vNT=(0.20±0.02)T A-0.11±0.07

2

3

4

5

6

7

8

9

1

vN

T [k

m s

-1]

3 4 5 6 7 8 91

2

TA [K]

3456780.1

23456781

2345

"Radius" from Peak [parsecs]

vNT=(0.64±0.05)T A-0.7±0.2

TMC-1C, OH 1667 MHz

vNT(1.00.2)R0.270.08 vNT

(0.300.09)R0.120.08

Type 4 Line width-“Size” RelationsType 4 Line width-“Size” Relations

Goodman, Barranco, Heyer & Wilner 1998

Types of Line width-Size RelationsTypes of Line width-Size Relations““Type 4:” Single Cloud Observed in a Type 4:” Single Cloud Observed in a SingleSingle Tracer Tracer

Gives information on power spectrum of velocity fluctuations.See Barranco & Goodman 1998; Goodman, Barranco, Heyer & Wilner 1998.

Observed Size

Type 4

Type 4

Non

-th

erm

al

Lin

e W

idth

Types of Line width-Size RelationsTypes of Line width-Size Relations

Observed Size

““Type 3:” Single Cloud Observed in Multiple TracersType 3:” Single Cloud Observed in Multiple Tracers

Non

-th

erm

al

Lin

e W

idth

Density

Types of Line width-Size RelationsTypes of Line width-Size Relations

Observed Size

““Type 3:” Single Cloud Observed in Multiple TracersType 3:” Single Cloud Observed in Multiple Tracers

Non

-th

erm

al

Lin

e W

idth

Gives pressure structure of an individual cloud. See Fuller & Myers 1992.

0

The (Newer) Evidence for CoherenceThe (Newer) Evidence for Coherence

2

3

4

5

6

7

8

9

1

0.1 2 10x-1 3 4

TA [ ]K

FCRAO C34

(2-1)S

2

3

4

5

6

7

8

9

1

2 3 4 5 6 7 8 91

TA [ ]K

30- IRAM m C34

(2-1)S

2

3

4

5

6

7

8

9

1

2 3 4 5 6 7 8 91

TA [ ]K

30- IRAM m C17

(1-0)O

2

3

4

5

6

7

8

9

1

4 10x0 5 6

TA [ ]K

30- IRAM m C18

(2-1)O

2

3

4

5

6

7

8

9

1

2 10x-1 3 4 5 6

TA [ ]K

FCRAO C17

(1-0)O

2

3

4

5

6

7

8

9

1

2 3 4 5 6 7 8 91

2 3

TA [ ]K

0.010.1110" " [ ]Radius from Peak pc

vNT=(0.64±0.05)T A-0.7±0.2

TMC-1C, OH 1667 MHz

2

3

4

5

6

7

8

9

1

6 7 8 90.1

2 3 4 5 6 7 8 91

TA [K]

34567890.1

23

"Radius" from Peak [pc]

TMC-1C, NH3 (1, 1)

ΔvNT=(0.20±0.02)T A-0.11±0.07

2

3

4

5

6

7

8

9

1

6 7 8 90.1

2 3 4 5 6 7 8 91

2

TA [K]

FCRAO C18

O (1-0)

"Radius" from Peak [pc]

TA [K]

Type 4 slope Type 4 slope appears toappears to

decrease with decrease with density, as predicted.density, as predicted.

FCRAO C17O (1-0) FCRAO C34S (2-1)

The Newest Evidence for CoherenceThe Newest Evidence for Coherence

0.7

0.6

0.5

0.4

0.3

0.2

0.1

[ v km s

-1 ]

0.70.60.50.40.30.20.1

TA [ ]K

N2H+ Thermal Width

N2H+ FCRAO Observations

( , 0.05 )Gaussian Fits deg bins200

100

0

-100

-300-200-1000100

0.5

0.5

0.5

0.45

0.45

0.4

0.4

0.4

0.35

0.35

0.35

0.3

0.3

N2H+: Coherence in the Ionized Gas

Goodman, Arce, Caselli, Heyer, Williams & Wilner 1999

TMC-1C

Coherent Dense CoreCoherent Dense Core

"Velocity Coherent"Core

"Chaff"...

~0.1 pc(in Taurus)

N~R0.1N~R0.9

““Coherence” in Spatial Distribution of Coherence” in Spatial Distribution of StarsStars

Surface Density of Stellar Companions (Taurus)

Parameterized Line Width-Size Relation

Coherent T

urbulent

8

6

4

2

log

c()

[st

ars/

sq. d

eg]

-5 -4 -3 -2 -1 0

log [deg]

10-4

10-3

10-2

10-1

100

Size [pc]Ro

0.1

2

3

4

5

6

7

8

9

1

N

T [km s

-1]

Larson 1995; see also Gomez et al. 1993; Simon 1997Goodman et al. 1998

The Cause of Coherence?The Cause of Coherence?

No ambipolardiffusion yet...

3D MHD simulation of Ostriker, Gammie & Stone (1998)

Most likely suspect:Most likely suspect:• Loss of magnetic

support due to reduced ionization fraction in core. (Scale gives clues.)

Interesting question raised:Interesting question raised:• What causes residual

non-thermal line width?

Length Scales Relevant to CoherenceLength Scales Relevant to Coherence

0.1

2

3

4

5

6

789

1

2

3

4

5

6

78

Velocity [km/s]

0.01 0.1 1 10 100

Size Scale [pc]

100 Myr 10 Myr

1 Myr 100,000 yr 10,000 yr

TimescalesTimescales

Cro

ssin

g Ti

me

Gener

ic lin

e wid

th-s

ize re

latio

n

Cores

Quality ControlQuality ControlLearning More from “Too Much” DataLearning More from “Too Much” Data

2000

2000

1990

1990

1980

1980

1970

1970

1960

1960

1950

1950

Year

100

101

102

103

104

Nch

an

nels, S

/N in

1 h

our, N

pix

els

102

103

104

105

106

107

108

(S/N

)*N

pix

els

*Nch

an

nels

Npixels

S/N

Product

Nchannels

The Spectral Correlation FunctionThe Spectral Correlation Function

Figure from Falgarone et al. 1994 Simulation

Goals of “SCF” ProjectGoals of “SCF” Project• Develop a “sharp tool” for statistical analysis of ISM,

using as much data of a data cube as possible• Compare information from this tool with other tools

(e.g CLUMPFIND, GAUSSCLUMPS, ACF, Wavelets), applied to same cubes

• Use best suite of tools to compare “real” & “simulated” ISM

• Adjust simulations to match, understanding physical inputs

How the SCF WorksHow the SCF Works

• Measures similarity of neighboring spectra within a specified “beam” size– lag & scaling

adjustable– signal-to-noise

equalized See: Rosolowsky, Goodman, Wilner & Williams 1999.

A “Real” Molecular CloudA “Real” Molecular Cloud

IRAM Key Project Data

Initial Comparisons using the SCFInitial Comparisons using the SCF

Falgarone et al. 1994

L1512 (Real Cloud) “Matching?” Turbulence Simulation

IRAM Key Project Data

Initial Comparisons using the SCFInitial Comparisons using the SCF

Gammie, Ostriker & Stone 1998

L1512 (Real Cloud)

IRAM Key Project Data

Better? MHD Simulation

Strong vs. Weak Field

Stone, Gammie & Ostriker 1999•Driven Turbulence; M K; no gravity•Colors: log density•Computational volume: 2563

•Dark blue lines: B-field•Red : isosurface of passive contaminant after saturation

=0.01 =1

T / 10 K

nH 2 / 100 cm-3 B / 1.4 G 2

Goals of “SCF” ProjectGoals of “SCF” Project• Develop a “sharp tool” for statistical analysis of ISM,

using as much data of a data cube as possible• Compare information from this tool with other tools

(e.g CLUMPFIND, GAUSSCLUMPS, ACF, Wavelets), applied to same cubes

• Use best suite of tools to compare “real” & “simulated” ISM

• Adjust simulations to match, understanding physical inputs

Results from SCF Project, 3/99Results from SCF Project, 3/99• Some simulations do match quantitatively better than

others (Goodman & Padoan 1999)

– compared so far: Padoan et al.; Ostriker, Gammie & Stone; Vazquez, Porter, Pouquet et al; MacLow et al.

• Comparison with moment analysis shows SCF more discriminating (Rosolowsky et al. 1999)

• Noise analysis is critical for ALL methods– S/N cutoffs, corrections

– Window size

• SCF used on Galactic H I can identify shells automatically (see Ballesteros, Vazquez & Goodman 1999)

What Sculpts the ISM?What Sculpts the ISM?BlastingBlasting

Origin of High-Latitude CloudsOrigin of High-Latitude Clouds

Generic ChiselingGeneric Chiseling

Line width-Size RelationsLine width-Size Relations ((v~Rv~Raa))

"In our own image""In our own image"Coherent Dense CoresCoherent Dense Cores

Quality ControlQuality ControlThe Spectral Correlation FunctionThe Spectral Correlation Function

Which Which ((B, G, T, B, G, T, 's 's ))??

To be discussed:To be discussed:The Role of ClayThe Role of Clay

Agglomeration, Tidal Stripping, the IMFAgglomeration, Tidal Stripping, the IMF

WeatheringWeathering Museum Destroyed on 100,000 yr time scaleMuseum Destroyed on 100,000 yr time scale

Longest lifetime of Galactic ISM Structures?Longest lifetime of Galactic ISM Structures?

The Role of ChemistryHow much structure is density, how much chemistry?How much structure is density, how much chemistry?

Very Small-Scale StructureInterferometric ObservationsInterferometric Observations

Extinction surveys & Pencil-beam ObservationsExtinction surveys & Pencil-beam Observations

Optical View of W3 RegionOptical View of W3 Region

The Velocity Field in The Velocity Field in Ursa MajorUrsa Major

Pound & Goodman 1997


Top Related