17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel...

48
17/Nov/2009 1 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA

Transcript of 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel...

Page 1: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 1SUNY Stony Brook Astrochemistry Lecture

Astrochemistry

Adwin BoogertNASA Herschel Science

Center,Caltech, Pasadena, CA

Page 2: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 2SUNY Stony Brook Astrochemistry Lecture

Contents

What is Astrochemistry? Chemical Reactions in Space

Gas Phase neutral and ion reactionsGrain surface chemistry

TunnelingMantle growthIce formation threshold

Ice processingLaboratory simulationsThermal processingEnergetic processing

Observing Interstellar MoleculesGas Phase

IR versus radio observationsDetected Species

Page 3: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 3SUNY Stony Brook Astrochemistry Lecture

Contents

Observing Interstellar MoleculesSolid State

Band profilesPolar versus apolar ices; SublimationAmorphous versus Crystalline ices; Time scalesGrain size/shape effectsColumn densities

Molecular Evolution:Dense CloudsLow and High Mass Young StarsHot Cores+DisksStarsStellar DeathDiffuse Clouds

Astrobiology Future: Herschel, ALMA, JWST

Page 4: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 4SUNY Stony Brook Astrochemistry Lecture

Reading

Material covered in this lecture is described at a similar level in

“Complex Organic Interstellar Molecules”, E. Herbst and E. F. van Dishoeck, ARA&A 2009, 47, 427-480. No need to read sections 2, 3.3, 5.2, 5.3, 6.4-6.6.

For the interested:

More advanced astrochemistry chapters in “The Physics and Chemistry of the Interstellar Medium”, A. G. G. M. Tielens, ISBN 0521826349. Cambridge, UK: Cambridge University Press, 2005.

Astrobiology: “An Introduction to Astrobiology”, eds. I. Gilmour and M. A. Sephton, ISBN 0521546214. Cambridge, UK: Cambridge University Press, 2003, 2004.

Page 5: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 5SUNY Stony Brook Astrochemistry Lecture

What is Astrochemistry?

Astrochemistry studies molecules anywhere in the universe:

•how are they formed?•how are they destroyed?•how complex can they get ?•how does molecular composition vary from place to place?•use them as tracer of physical conditions (temperature, density)? •how are molecules in space related to life as we know it (astrobiology)?

Page 6: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 6SUNY Stony Brook Astrochemistry Lecture

Chemical Reactions in Space

Key factors in interstellar chemistry:

Abundance H factor 1000 larger than any other (reactive) elementsAway from very strong UV fields: H,N,C,O atoms 'locked up' in H2, N2, CO. Left over atoms determine chemical environment:

Reducing environment if H>OOxidizing environment if H<O

CosmicAbundances

H 0.9 H2

He 0.1 inertO 7e-4 COC 3e-4 CON 1e-4 N2

Ne 8e-5 inertSi 3e-5 dustMg 3e-5 dustS 2e-5 Fe 4e-6 dust

Page 7: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 7SUNY Stony Brook Astrochemistry Lecture

Chemical Reactions in Space

More key factors in interstellar chemistry:

Densities atoms and molecules in interstellar medium extremely low: 1-105 particles/cm3. Compare:

earth atmosphere 1019

ultra-high vacuum 108

Therefore chemistry quite unusual compared to earth standards. Rare earth species (discussed in a few slides) are abundant in the ISM:

HCO+ [formyl ion]H3

+ [protonated dihydrogen]

Types of chemistry:

Gas phase chemistryGrain surface chemistry (freeze out <100 K)Energetic processing ices

Page 8: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 8SUNY Stony Brook Astrochemistry Lecture

Gas Phase Chemical Networks

Despite extreme vacuum conditions, long time scales allow for complex gas phase chemistry.

Ion-neutral reactions orders of magnitude faster than neutral-neutral.

Species with ionization potential <13.6 eV likely photo-ionized (CC+)

Cosmic rays also important ionization sources

Page 9: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 9SUNY Stony Brook Astrochemistry Lecture

Some Key Gas Phase Reactions H3

+: (recently discovered, see http://h3plus.uiuc.edu)

H2 + CR H2+ + e-

H2+ + H2 H3

+ + H

HCO+:

H3+ + CO HCO+ + H2

H2O:

O + H+ O+ + H

O+ + H2 OH+ + H

OH+ + H2 H2O+ + H

H2O+ + H2 H3O

+ + H

H3O+ + e- H2O + H

Collides and excites H2, source of UV in dense clouds

Page 10: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 10SUNY Stony Brook Astrochemistry Lecture

More realistic grain:

Many molecules (H2, H2O) much more

easily formed on grain surfaces. Freeze out

<100 K.

Interstellar ‘ice’ or ‘dirty ice’: any frozen volatile, e.g. H2O, H2O mixtures, pure CO.

Grain Surface Chemistry

Page 11: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 11SUNY Stony Brook Astrochemistry Lecture

Grain Surface Chemistry “Grain surfaces are the watering holes of

astrochemistry where species come to meet and mate.” (Tielens 2005)

Species accreted from gas are chemisorbed or physisorbed on grains, allowing for much longer time to find reaction partner than in gas phase

Species move fast over surface, meeting partners many times, allowing for tunneling through activation barriers. e.g. H atom has 50% probability of tunneling through 3400 K barrier.

At molecular cloud densities (104-105 cm-3) it takes a few days for an atom to stick to a grain and 5*105 yrs for all gas to deplete on grains, much less than cloud lifetime.

Page 12: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 12SUNY Stony Brook Astrochemistry Lecture

Ice Mantle Growth

H2O formed by grain surface reactions, CO formed in gas and inertly condenses on grains.Grain mantle thickness: Mass growth rate: dm/dt=S**a2*n*<v>*<m> Radius growth rate: da/dt=(dm/dt)/(4**a2*) da/dt=S*n*<v>*<m>/(4*)

Mantle thickness independent of grain radius Dense clouds can have mantles as thick as 0.1 um, and in deeply embedded protostars even more. Mantle thicker than most grain cores according to MRN grain size distribution

n(a)~a-3.5, amin=0.005 μm, amax=0.25 μm

Page 13: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 13SUNY Stony Brook Astrochemistry Lecture

Ice Mantle GrowthDue to grain temperature and interstellar radiation field ices form only if visual extinction (AV) large enough: the ice formation thresholdTaurus cloud: H2O ices absent below visual extinction AV~3 and CO ices below AV~7. Difference due to lower Tsub of CO. Variation between clouds due to different temperature/radiation field

Col

umn

Den

sity

COH2O

Extinction (AV)

Page 14: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 14SUNY Stony Brook Astrochemistry Lecture

Chemical processes occurring in

space can be simulated in laboratory

at low T (≥10 K) and low pressure. Thin films of ice condensed on a

surface and absorption or reflection

spectrum taken.Temperature and irradiation by

UV light or energetic particles of ice

sample can be controlled.Astrophysical laboratories:

Leiden, Catania, NASA

Ames/Goddard, Paris

Gerakines et al. A&A 357, 793 (2000)

Simulating Interstellar Ices

Page 15: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 15SUNY Stony Brook Astrochemistry Lecture

Thermal Processing of Ices

New molecules easily produced by heating acid/base mixtures.

Example shown H

2O/NH

3/HNCO=120/10/1 at 15,

52, 122 K NH3+HNCO -->NH4

+ + OCN-

NH4+ and OCN- have spectral

characteristics that fit interstellar 4.62 and 6.85 μm bands.

Relative intensities not in agreement with observations, however, when requiring charge balance; further study needed.

Van Broekhuizen et al., A&A 415, 425 (2004)

Page 16: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 16SUNY Stony Brook Astrochemistry Lecture

Energetic Processing of Ices

Chemical processing of ices by UV photons and cosmic rays can be simulated

Top figure shows H2O/CO/NH

3 ice

mixture after photo-processing with hard UV photons

Bottom figure shows similar spectra compared to a YSO. Heating after irradiation can explain the 6.85 μm band.

Long exposure to photons or particles can form very complex molecules, incl. Amino acids and PAHs.

Relevance to interstellar medium is hard to prove.

See slides on diffuse medium

415, 425-436 (2004)

Page 17: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 17SUNY Stony Brook Astrochemistry Lecture

Observing Gas Phase Molecules

symmetric stretch v1 bend v2 asymmetric stretch v1

rotation axis A rotation axis Crotation axis B

H2O vibration modes

H2O rotation modes

Molecules detected (mostly) by vibrational and rotational transitions, at infrared and radio wavelengths.

Electronic transitions occur at X-ray/UV wavelengths →extinction-limited

Page 18: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 18SUNY Stony Brook Astrochemistry Lecture

Observing Gas Phase MoleculesRo-vibrational transition rules lead to characteristic P and R branch spectrum, if there is

permanent (e.g. CO) or induced (e.g. CH4)

dipole moment. N2 and O

2 cannot be observed

this way. Example CO fundamental (J=1, v=1):

Pure rotational lines occur mostly in the far-IR/submm for species with permament dipole moments (e.g. CO, but not CH

4)

Note that in solid state, no rotations allowed, leadingto one broad vibrational spectrum

115 GHz

807 GHz

576 GHz

922 GHz

691 GHz

461 GHz

231 GHz 346 GHz

Page 19: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 19SUNY Stony Brook Astrochemistry Lecture

Observing Gas Phase Molecules: Inventory

129 gas phase molecules currently detected in space(123 listed here)

http://www.cv.nrao.edu/~awootten/allmols.html

Page 20: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 20SUNY Stony Brook Astrochemistry Lecture

Observing Solid State Molecules

H2O ice has many broad absorption bands:

● Symmetric stretch● Asymmetric stretch● Bending mode● Libration mode● Combination modes● Lattice mode● etc...

Width, position and shape determined by solid state (dipole) interactions → band profile powerful diagnostic of ice environment and structure

Page 21: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 21SUNY Stony Brook Astrochemistry Lecture

Ice Band ProfilesPolar vs Apolar Ices

Molecular dipole moment determines physical and spectral characteristics. Compare solid H

2O

and CO: Sublimation temperature much

higher for H2O (90 K vs. 18 K in space)

Bands much broader for H2O H2O/CO mixtures: distinct polar

and apolar ices with different H2O/CO ratios that can spectroscopically be distinguished and sublimate at different T.

Highly relevant for icy bodies (e.g. comets) as well, as dipole moment determines outgassing behaviour. 'Pockets' of apolar CO may result in sudden sublimation.

Page 22: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 22SUNY Stony Brook Astrochemistry Lecture

• CO band consists of 3 components, explained by laboratory simulations as originating from CO in 3 distinct mixtures:

– 'polar' H2O:CO

– 'apolar' CO2:CO

– 'apolar' pure CO

(Boogert, Hogerheijde & Blake, ApJ 568,761, 2002)

Ice Band ProfilesPolar vs Apolar Ices

Page 23: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 23SUNY Stony Brook Astrochemistry Lecture

Ice Band ProfilesPolar vs Apolar Ices

Indeed, CO ice profiles vary dramatically in different lines of sight, as apolar component highly volatile. 'Older' YSOs have less apolar CO

Page 24: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 24SUNY Stony Brook Astrochemistry Lecture

Ice Band ProfilesAmorphous vs. Crystalline

Interstellar H2O ices formed in amorphous phase, as evidencedby prominent 'blue' wing. Crystallization by protostellar heat.[long wavelength wingoriginates from scattering on large

grains and NH3:H2O complexes]

Crystallization temperature ~120 Kin laboratory, but ~70 K in spacedue to longer time scales.

[Time scale ~exp(Ebarrier/T) (~1 hour in lab, 105 yr in space). For same reason sublimation temperature in lab (~180 K)higher than in space (~90 K)].

Page 25: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 25SUNY Stony Brook Astrochemistry Lecture

Ice Band ProfilesGrain Shape and Size Effects

Laboratory and interstellar absorption spectra cannot always be directly compared: Scattering on large (micron sized) grains leads to 3 μm red wing (often observed)Surface modes in small grains may lead to large absorption profile variations:

For ice refractive index m=n+ik, absorption cross section ellipsoidal grain proportional to (Mie theory) (2nk/L2)/[(1/L-1+n2-k2)2+(2nk)2]

Resonance for sphere (L=1/3) occurs at k2-n2=2, so at large k (=strong transitions)Important for pure CO, but not for CO diluted in H2O and also not for 13CO.

Page 26: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 26SUNY Stony Brook Astrochemistry Lecture

Ice Column Densities and Abundances

Ice column densities:N=peak*FWHM/Alab

Alab integrated band strength measured in laboratory

A[H2O 3 m]=6.2x10-16cm/mol. Order of magnitude in quiescent dense clouds:

N(H2O-ice)=1018 cm-2 For reference: this is ice layer of 0.3 m at 1 g/cm3 in laboratory, but....

Ice abundance: X(H2O-ice)=N(H2O-ice)/NH~10-4

This is comparable to X(CO-gas)

Page 27: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 27SUNY Stony Brook Astrochemistry Lecture

'Typical' abundances w.r.t. H2O ice

Ice Inventory

CO few-50%

CO215-35%

CH42-4%

CH3OH <8, 30%

HCOOH 3-8%

[NH3]<10, 40% (?)

H2CO <2, 7%

[HCOO-] 0.3%OCS <0.05, 0.2%

[SO2]<=3%

[NH4+] 3-12%

[OCN-] <0.2, 7%

Note far fewer ices detected than gas phase species. This is because ices can only be detected by absorption spectroscopy.

Page 28: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 28SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution

Next slides molecular evolution:

–Dense Clouds–Young Stars–Hot Cores/Disks–Stars–Stellar Death–Diffuse Clouds–Astrobiology

Not independent environments. Cycling of matter is key.

Page 29: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 29SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Diffuse vs.

Dense MediumHubble telescope image of M51

shows •massive young stars (red)•'normal' stars (white)•molecular clouds (black)•diffuse clouds in between•clouds 'processed' by UV photons

massive stars•very similar to our own Galaxy•Cycling between environments as

spiral density wave passes

Page 30: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 30SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Diffuse vs.

Dense MediumCO J=1-0 image M51 highlighting

giant molecular clouds.

[Obtained with CARMA array in

Owens Valley by Jin Koda]

Page 31: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 31SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Dense Core

•Molecules in core freeze out

at sublimation temperature

of molecule.•H2O T=90 K

•CO T=16 K

Background star

H2O

H2ONH4

+

silicates

extin

ctio

n

Wavelength

Page 32: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 32SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Dense Core•CO sublimation temperature ~16 K•In densest part of core, most CO

freezes out•N2 and H2 lower sublimation

temperature (<13 K)•cosmic rays penetrate deep in core, ionizing H2, forming N2H

+

•H2 + CR H2+ + e-

H2+ + H2 H3

+ + H

H3+ + N2 N2H

+ + H2

•N2H+ observable at sub-mm

frequencies (e.g. Herschel)•better dense cloud tracer than CO

Page 33: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 33SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Young Stars

•Deep ice bands observed toward young

stars. •As star ages, ices heated: crystallization

and sublimation (most volatile species, e.g.

CO) first.

Page 34: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 34SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Young Stars

Observational evidence for thermal processing of ices near YSOs:

Solid 13CO2 band profile varies toward different protostars…

Page 35: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 35SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Young Stars

Observational evidence for thermal processing of ices near YSOs:

Solid 13CO2 band profile varies toward different protostars…

…and laboratory simulated spectra show this is due to CO2:H2O mixture progressively heated by young star (Boogert et al. 2000; Gerakines et al. 1999)

Page 36: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 36SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Young Stars Observational evidence for thermal

processing of ices near YSOs:

Solid 13CO2 band profile varies toward different protostars…

…and laboratory simulated spectra show this is due to CO2:H2O mixture progressively heated by young star (Boogert et al. 2000; Gerakines et al. 1999)

H2O crystallization (Smith et al.

1989) gas/solid ratio increases (van

Dishoeck et al. 1997) Detailed modelling gas phase mm-

wave observations (van der Tak et al. 2000)

Little evidence for energetic processing of ices, however......

Page 37: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 37SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Hot Cores•......., but in immediate vicinity of YSO ices evaporate, and warm gas directly

observable at submm/radio wavelengths in rotational transitions.•(sub)millimeter-wave gas phase measurements orders of magnitude more sensitive to abundances than IR ice observations•Regions called hot cores for massive young stars and corinos for low mass stars.

Cazaux et al. 2004

Page 38: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 38SUNY Stony Brook Astrochemistry Lecture

A. Wootten, “Science with ALMA” Madrid 2006.SGR B2(N), ALMA Band 6 mixer at SMT

Have to be able to separate flowers from the weeds

Molecular Evolution: Hot Cores

Formic acid

Methyl

formate

Formic acid

Dimethyl ether

Page 39: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 39SUNY Stony Brook Astrochemistry Lecture

Herschel/HIFI: 480-1916 GHz (625-157 μm). Resolving Power up to 10 million, or <0.1 km/s

Molecular Evolution: Hot Cores

CH3OH gas cell measurement using HIFI

(Teyssier et al. 2005)

Page 40: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 40SUNY Stony Brook Astrochemistry Lecture

Molecules are (Nearly) Everywhere…even on the Sun•T>5000 K, most molecules dissociate•Lower T, molecules quite easily formed, as demonstrated by H2O detection in sun spots (T~3000 K)

~13 um

Page 41: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 41SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Stellar Death

Cas A, SpitzerSN 1987A, HST

Stars at end burning phase expel massive shells of matter, enriching ISM with new elements and dust

Effect on chemistry strongly depends on stellar mass, and episode of explosion.

Some form oxygen-rich dust (silicates), othersgraphitic dust (and PAHs).

Supernovae vaporize environment, destroying or modifying dust (graphite →diamond).

Molecules (CO and SiO) formed in ejecta

Produce cosmic rays

Page 42: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 42SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Diffuse Medium, Mystery 1

•Diffuse Interstellar Bands discovered in 1922

in optical spectra of diffuse medium. •Over 200 bands detected.•Probably a large gas phase species•Polycyclic Aromatic Hydrocarbons possible•spherical C60, “Buckminster Fullerenes”,

“Buckyballs”•problem not solved...: 1 DIB, 1 carrier?

PAHs

Buckyball

Page 43: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 43SUNY Stony Brook Astrochemistry Lecture

Another enigmatic diffuse medium feature.... the 3.4 um absorption band toward the Galactic Center).

Triple peaks due to hydrocarbons (-CH, -CH2, -

CH3), but what kind of

hydrocarbon?

Pendleton et al. 1994, Adamson et al. 1998, Chiar et al. 1998, Chiar et al. 2000

Molecular Evolution: Diffuse Medium, Mystery 2

-CH-

-CH2--CH3-

Page 44: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 44SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Diffuse Medium, Mystery 2

Bacteria? Apples?

Page 45: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 45SUNY Stony Brook Astrochemistry Lecture

Greenberg et al. ApJ 455, L177 (1995): launched processed ice sample in earth orbit exposing directly to solar radiation (EUREKA experiment). Yellow stuff turned brown: highly carbonaceous residue, also including PAH.

Molecular Evolution: Diffuse Medium, Mystery 2

Page 46: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 46SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: Diffuse Medium, Mystery 2

Little evidence production by UV/CR bombardment of ices: band not polarized as opposed to silicates/ices: not in processed mantle but

separate grains 3.4 um band observed in dense clouds, but not triple peaked. Likely NH3.H2O

hydrate. Due to Low infrared sensitivity? Better observe sublimated species (more sensitive)

formed in evolved star envelopes, and injected in ISM?

Page 47: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 47SUNY Stony Brook Astrochemistry Lecture

Molecular Evolution: AstrobiologyDo molecules formed in interstellar medium have anything to do with formation of life?This is topic of astrobiology.Amino acids building blocks of most complex molecules in living organisms...protein.It has been produced in laboratory by heavy processing interstellar ice analog. Also, chirality of amino acids in protein is left-handed. May have been caused by nearby massive star producing circularly polarized light

Page 48: 17/Nov/20091 SUNY Stony Brook Astrochemistry Lecture Astrochemistry Adwin Boogert NASA Herschel Science Center, Caltech, Pasadena, CA.

17/Nov/2009 48SUNY Stony Brook Astrochemistry Lecture

Future of Astrochemistry is Bright....

Herschel Space Observatory

Atacama Large MM Array

James Webb Space Telescope

….plus a lot more……