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Delve into the vast world of interstellar medium, where gases, dust particles, and molecules reside between stars. Learn about molecular cloud formation, spectral-line radiation, and the discovery of unique interstellar molecules. Discover the significance of H3+ ions and cosmic ray ionization rates in diffuse molecular clouds. Unravel the mysteries of maser emission, Milky Way rotation, and the missing mass conundrum. Dive into the realm of prebiotic molecules and the cutting-edge research conducted with radio telescopes like the GBT and ALMA.
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The Interstellar Medium and Interstellar Molecules Ronald Maddalena National Radio Astronomy Observatory
Interstellar 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
Non-Thermal Continuum RadiationFree-Free Emission • Ionized regions (HII regions and planetary nebulae) • Free electrons accelerated by encounters with free protons
Spectral-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., N=177 to M = 176)
Spectral-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.
Interstellar 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 (< 100 K) • Some molecules (e.g., H2) form on dust grains • Most form via ion-molecular gas-phase reactions • Exothermic • Charge transfer
Interstellar 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
Molecular 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 Galaxy’s volume. • Concentrated in spiral arms • Dust Clouds = Molecular Clouds
Ion-molecular gas-phase reactionsExamples of types of reactions C+ + H2→ CH2+ + hν (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 + hν (Radiative) Fe+ + grain → Fe + hν (Grain)
Importance 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 can’t penetrate dark clouds
Spectral-Line RadiationMilky Way Rotation and Mass? • For any cloud • Observed velocity = difference between projected Sun’s motion and projected cloud motion. • For cloud B • The highest observed velocity along the line of site • VRotation = Vobserved + Vsun*sin(L) • R = RSun * sin(L) • Repeat for a different angle L and cloud B • Determine VRotation(R) • From Newton’s law, derive M(R) from V(R)