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CH+ and DIBs toward Herschel 36
Takeshi Oka Department of Astronomy and Astrophysics and Department of Chemistry The Enrico Fermi Institute, University of Chicago DIBs group Jamuary 17, 2012
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Two discoveries HD 204827 Treasure house of C3, C2 C2 DIBs HD 183143
Herschel J = 1 CH+, Radiative pumping DIBs and dust emission
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CH+ in the J = 1 excited rotational level
and radiative temperature of dust emission 2 1 R(0) R(1) Q(1) Ted Dunham 1937 2 spontaneous emission J + 1 → J Te ~ Tr ~ 17.5 K Einstein’s coefficient A = s-1 ncrit = 3 × 106 cm-3 1 Dirac 1927 ν = GHz ~ K μ = 1.7 Debye
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AV ~ 60 AV ~ 40 Goto, Stecklum, Linz, Feldt, Henning, Pascucci, Usuda, 2006, ApJ, 649, 299
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Two preliminaries Rotation of linear molecules Three temperatures
2 1 Rotational constant CH ,137 MHz cm K HC5N 1,331 MHz cm K Moment of inertia HC11N MHz cm K R(J) J + 1 ← J ν = ν0 + B’(J + 1)(J +2) – BJ(J + 1) = ν0 + 2B’(J + 1) + (B’ – B)J(J + 1) R(1) R(0) Q(J) J ← J ν = ν0 + B’J(J +1) – BJ(J + 1) = ν (B’ – B)J(J + 1) Q(1) P(J) J ˗ 1 ← J ν = ν0 + B’(J + 1)(J +2) – BJ(J + 1) = ν0 – 2B’J (B’ – B)J(J + 1) Three temperatures Kinetic temperature Tk Collision Maxwell 1857 n(v) ~ v2exp(-mv2/kTk) 2 Excitation temperature Te Observed Boltzmann 1860 n(J) ~ gJexp(-EJ/kTe) 1 Radiative temperature Tr Radiation Planck 1900
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Effect of dust emission on DIBs toward Her 36
λ λ λ λ
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Simulation of DIB velocity profiles
with 17.5 K dust emissiom and the 2.7 K background radiation Collision only Radiation and collision , Einstein 1916 Goldreich and Kwan 1974
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Rotational distribution n(J)
B = K μ = 5 Debye C = 3 × s-1 B = 0.07 K μ = 4 Debye C = 10-7 s-1
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Calculated spectra C12
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Calculated spectra C6 B’ – B = 0.04B Δν
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