天の川銀河研究会 2012/9/6@鹿児島大学 天の川銀河の分子ガスの密度頻度 半田利弘(鹿児島大学) 星間ガスと物質循環 ▶ 星間物質 ■ 星間ガス 電離ガス、中性原子ガス、分子ガス ■ 星間塵 ▶ 星形成の母胎 ■ ■ 宇宙での物質循環 「希薄な星間ガス」から「星」へ ▶ 天の川銀河内での様子を調べる ■ ■ 分布 物理的性質(温度、密度) Gas density: 2 concepts ▶ ISM has a fine structure. ■ sub-cloud scale structure ▶ “gas density” with a limited resolution 1. thermo-dynamical density n → excitation 2. averaged gas density <r> → mass in a volume Gas density structure ▶ Geometrical approach ■ High resolution mapping ▶ Statistical approach ■ ■ Gas density histogram “Probability Density Function” steady state uniform condition Previous works ▶ Column density ■ ■ star forming regions a whole galaxy: LMC in HI ▶ Volume density ■ HI & HII in MWG Wada et al. 2000 Berkhuijsen & Fletcher 2008 AMANOGAWA-2SB survey ▶ 12CO (2-1) & 13CO (2-1) survey ▶ with AMANOGAWA telescope ■ ■ Dish: 60 cm, Beamsize: 9 arcmin RX: 2SB = waveguide sideband-separating SIS simultaneous observations in both lines Tsys=120 K @ zenith ■ Spectrometer: AOS Nakajima et al. (2007) Survey specifications ▶ The Galactic plane ■ Grid spacing: 7.5’ Velocity resolution: 1.3 km s-1 Noise level: ~0.05 K ■ grid and velocity resolution = Colombia survey ■ ■ Dame et al. 2001 180 Integrated intensity maps ▶ Distribution on the sky 12CO(2-1) 150 120 90 60 13CO(2-1) 30 l-v diagrams CO(2-1) ▶ 12Longitude-velocity diagrams +100km/s 13CO(2-1) +100km/s 180 150 120 90 60 30 60 30 Galactic Longitude [deg] 180 150 120 90 Galactic Longitude [deg] 180 samples ▶ In this talk, data for 5o<l<90o, |b|<5o ■ to reduce bias by the local clouds 12CO(2-1) 150 120 90 Galactic Longitude [deg] 60 30 CO intensity correlations ▶ 12CO(2-1) ■ ▶ Ratio<1.0 → subthermally excited 12CO(2-1) ■ vs 12CO(1-0) vs 13CO(2-1) Optical depth effect 12CO(2-1) R12/1-0=0.64±0.058 12CO(1-0) 13CO(2-1) 12CO(2-1) Gas density histogram ▶ Statistics of averaged gas density ■ Relative volume in Msun pc-3 bin ▶ Conversion from observational data ■ ■ Line intensity → molecular gas mass Line velocity → distance & geometrical depth Conversion: volume ▶ Distance estimation of each voxel ■ ■ The kinetic distance v → d Cross section area in the beam W d= A ▶ Depth of each voxel ■ Differential of the kinetic distance Dv → Dd ▶ Volume of each voxel ■ V= W d Dd Conversion: mass density ▶ Molecular gas mass ■ ■ XCO=1.8x1020 cm-2/(K km s-1) Dame et al. 2001 Typical intensity ratio T12, T13 → T1-0 Intensity ■ correlation / simple excitation N(H2)=XCO ∫T dv → M(H2) ▶ Volume of each voxel ■ V= W d Dd ▶ Molecular gas density in Msun pc-3 ■ r =M/V XCO for 3 CO lines ▶ for 12CO(2-1) ■ ■ Observed standard ratio R12/1-0=0.64 X12= X1-0 /R12/1-0=2.9x1020 cm-2 /(K km s-1) ▶ for 13CO(2-1) ■ assumptions LTE with 10 K optically thin 13CO(2-1) abundance 12CO/13CO=60, 12CO/H2=4.3x10-5 ■ X13= 1.1x1021 cm-2 /(K km s-1) Kinetic model of MWG ▶ The pure circular rotating disk ▶ with IAU standard kinematics ■ Q0=220km s-1, R0=8.5kpc ▶ Geometrical thickness of Gal. disk ■ ■ assume: gas is confined in a ±100pc uniform disk not include the far side volume beyond z>100pc Gas density histogram ▶ Gas density – volume in MWG ■ ■ fairly well fit by log-normal slight depression at high density end Simple empirical relations ▶ Only simple radiation transfer eq. ■ TMB,13=η13 Tc,13 (1-exp(-τ13)); TMB,12=η12 Tc,12 ▶ Linear relations ■ ■ ■ (η13 Tc,13)/(η12 Tc,12)=α; η13 Tc,13=β τ13 α, β : 2 constants Tc,13 → typical τ13 Optical depth correction ▶ Gas density – volume in MWG ■ t-corrected : well fit by log-normal Model dependence ▶ Galactic constants (recent VLBI obs.) W0=Q0/R0=30 km s-1 kpc-1 Nagayama et al. 2010 -1 ■ → Q0=210km s , R0=7kpc ■ ▶ Radial variation of XCO ■ X1-0=1.4x1020 exp(r/11) Arimoto et al. 1996 ▶ Thickness of the galactic disk ■ without any consideration (infinite thick disk) ▶ Reject local gas near the Sun ■ only Vfar<100 Vnear GDH with different models ▶ Still log-normal like variable XCO Galactic constants infinitly thick disk only near subcentral Why log-normal? Vazquez-Semadeni 1994 ▶ 密度:直前の密度を増幅・減衰する過程 ■ ■ ■ ランダムな増幅度決定←乱流? 増幅度は直前の密度の値によらない 多数の変化 ▶ この場合の現在の密度は… ■ ■ ρ = ρ 0 f1 f2 f3 … fn よって、logρ = log ρ0 +log f1 +log f2 … +log fn ▶ 中心極限定理からlog ρは正規分布 Nearby galaxies ▶ Sample: Nobeyama CO atlas ■ ■ Nobeyama 45m telescope 12CO(1-0) ▶ Gas “Column” Density Histogram Nobeyama CO atlas Kuno et al. 2007 ▶ 12CO (1-0) survey ▶ with Nobeyama 45m telescope ■ ■ ■ beamsize: 15 arcsec RX: BEARS (25 beam SIS) Spectrometer: AOS Sample galaxies ▶ 40 spiral galaxies Kuno et al. 2007 ■ ■ ■ ■ ■ morphology: Sa-Sc distance: d<25Mpc inclination: i<70deg (face-on) IRAS 100um flux >10Jy no/less interacting method ▶ ICO(1-0) → N(H2) ■ using XCO=1.8x1020 cm-2/(K km s-1) Dame et al. 2001 ▶ Inclination correction ■ assume a disk with constant thickness Results ■ lognormal type: ~24/40 ■ Non-lognormal type: ~16/40 What controll GDH shape? ▶ correlation coefficient ■ compare with some parameters ▶ observational effect? ■ ■ N(pixel), linear resolution, noise level, inclination No correlation → not due to obs. effects ▶ other obs. property of galaxy? ■ ■ morphology(SA/SB), molecular mass No correlation → to study more! summary ▶ H2 density histogram over MWG ■ observational counter part of PDF ▶ Some galaxies shows log-normal, although about 40% do not. logr=-2.0[Msun pc-3], s=0.80[dex]