Title: The Interstellar Medium and Interstellar Molecules
1The Interstellar Medium and Interstellar
Molecules
- Ronald Maddalena
- National Radio Astronomy Observatory
2Interstellar Medium The Material Between the
Stars
- Constituents
- Gases
- Hydrogen (92 by number)
- Helium (8)
- Oxygen, Carbon, etc. (0.1)
- Dust Particles
- 1 of the mass of the ISM
- Average Density 1 H atom / cm3
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5Interstellar Medium Properties
State of H C Temperature Densities (H/cm3) Percent Volume
HII Regions Planetary Nebulae H, C Ionized 5000 K 0.5 lt 1
Diffuse ISM H, C Ionized 1,000,000 K 0.01 50
Diffuse Atomic H2 lt 0.1 C Ionized 30-100 K 10-100 30
Diffuse Molecular 0.1 lt H2 lt 50 C gt 50 30-100 K 100-500 10
Translucent Molecular H2 1 C lt 0.5, CO lt 0.9 15-50 K 500-5000? Small
Dense Molecular H2 1 CO gt 0.9 10-50 K gt 104 10
6Interstellar Medium Properties
7Interstellar Medium Life Cycle
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9HII Regions Planetary Nebulae
- Isolated regions where H is ionized.
- UV from hot (20,000 50,000 K), blue stars
produces ionization. - HII Regions
- Young, massive, short-lived (lt few x 106 years)
stars. - HII Regions have short lives.
- Near regions where they formed.
- Planetary nebulae
- Evolved (white dwarf) stars
10Planetary Nebula and HII Regions
11Non-Thermal Continuum RadiationFree-Free Emission
- Ionized regions (HII regions and planetary
nebulae) - Free electrons accelerated by encounters with
free protons
12Thermal Continuum Radiation
- Characteristics
- Opaque Black Body
- Isothermal
- In Equilibrium
- Plancks Law
- I Intrinsic Intensity (ergs/cm2/sec/Hz).
- h Plancks Constant
- k Boltzmans Constant
- T in K
- ? in Hz
- Radio Approximation
13Non-Thermal Continuum Radiation
- Synchrotron Radiation
- Free Electrons
- Magnetic Fields
- Discrete Sources
- Supernovae Remnants
- General Interstellar Medium
- I ? ?? with ? between -0.2 and 1.2
14Spectral-Line RadiationRecombination Lines
- Discovered in 1965 by Hogburn and Mezger
- Ionized regions (HII regions and planetary
nebulae) - Free electrons temporarily recaptured by a proton
- Atomic transitions between outer orbital (e.g.,
N177 to M 176)
15Spectral-Line RadiationHyperfine transition of
Hydrogen
- Discovered by Ewen and Purcell in 1951.
- Found in regions where H is atomic.
- Spin-flip (hyperfine) transition
- Electron protons have spin
- In a H atoms, spins of proton and electron may be
aligned or anti-aligned. - Aligned state has more energy.
- Difference in Energy h v
- v 1420 MHz
- An aligned H atom will take 11 million years to
flip the spin of the electron. - But, 1067 atoms in Milky Way
- 1052 H atoms per second emit at 1420 MHz.
16Atomic Hydrogen
17Spectral-Line RadiationWhat do they tell us?
- Number of emitting regions in that direction.
- Frequency of center of line ? Objects velocity
- Doppler Effect
- Frequency Observed Frequency Emitted / (1
V/c) - Width of line ? Motion of gas within the region
- Height of the line ? Maybe temperature of the gas
- Area under the line ? Maybe number of atoms in
that direction.
18Interstellar Molecules
- Hydroxyl (OH) first molecule found with radio
telescopes (1964). - Molecule Formation
- Need high densities
- Lots of dust needed to protect molecules for
stellar UV - But, optically obscured need radio telescopes
- Low temperatures (lt 100 K)
- Some molecules (e.g., H2) form on dust grains
- Most form via ion-molecular gas-phase reactions
- Exothermic
- Charge transfer
19Interstellar Molecules
- About 90 of the over 130 interstellar molecules
discovered with radio telescopes. - Rotational (electric dipole) Transitions
- Up to thirteen atoms
- Many carbon-based (organic)
- Many cannot exist in normal laboratories (e.g.,
OH) - H2 most common molecule
- No dipole moment so no radio transition.
- Only observable in UV (rotational)
- Astronomers use CO as a tracer for H2
20Molecular Clouds
- Discovered 1970 by Penzias, Jefferts, Wilson
and others. - Coldest (5-30 K), densest (100 106 H atoms/cm3)
parts of the ISM. - Where stars are formed
- 25-50 of the ISM mass
- A few percent of the Galaxys volume.
- Concentrated in spiral arms
- Dust Clouds Molecular Clouds
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23Discovery of Ethanol
24Molecules Discovered by the GBT
25Grain Chemistry
26Ion-molecular gas-phase reactions
27Ion-molecular gas-phase reactionsExamples of
types of reactions
C H2 ? CH2 h?
(Radiative Association) H2 H2 ? H3
H (Dissociative Charge
Transfer) H3 CO ? HCO H2
(Proton Transfer) H3 Mg ?
Mg H2 H (Charge
Transfer) He CO ? He C O
(Dissociative Charge Transfer) HCO e ? CO
H
(Dissociative) C e ? C h?
(Radiative) Fe grain ? Fe h?
(Grain)
28Importance of H3
29Importance of H3 -- Recent results
- First detected in 1994 in the infrared
- Creation
- H2 cr ? H2 e
- H2 H2 ? H3 H
- Destruction
- H3 e ? H H2 or 3H
- New laboratory measurements for reaction rates
- Dense Molecular clouds expected and measured
H3 agree - Diffuse Molecular clouds measured H3 is 100x
higher than expected - Cosmic ray ionization rate has to be higher in
diffuse clouds than in dark clouds. Why? - Confinement of cr in the diffuse molecular clouds
- Higher number of low energy cr than in current
theory and which cant penetrate dark clouds
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31Maser Emission
32Spectral-Line RadiationMilky Way Rotation and
Mass?
- For any cloud
- Observed velocity difference between projected
Suns motion and projected cloud motion. - For cloud B
- The highest observed velocity along the line of
site - VRotation Vobserved Vsunsin(L)
- R RSun sin(L)
- Repeat for a different angle L and cloud B
- Determine VRotation(R)
- From Newtons law, derive M(R) from V(R)
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34Massive Supernovae
35Missing Mass
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38Prebiotic Molecules
39The GBT and ALMA
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44Where to Get More Information
- Harwitt Astrophysical Concepts
- Verschuur and Kellerman Galactic and
Extra-Galactic Radio Astronomy - Verschuur Invisible Universe Revealed
- Kraus Radio Astronomy
- Burke and Graham Smith Radio Astronomy