Dust effects in the SEDs of simulated galaxies: the GRASIL-3D code and some applications A. OBREJA...
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Transcript of Dust effects in the SEDs of simulated galaxies: the GRASIL-3D code and some applications A. OBREJA...
Dust effects in the SEDs of simulated galaxies: the GRASIL-3D code and some applications
A. OBREJA (UAM, Spain)G.L. GRANATO (INAF, Trieste, Italy)I. SANTOS (UAM, Spain)C. A. BROOK (UAM, Spain)G. STINSON (MPIA, Heidelberg, Germany)L. SILVA (INAF, Trieste, Italy)A. SERNA (UMH,Spain)S. GOTTLOBER, Y. HOFFMAN, G. YEPES & CLUES Collaboration
Rosa Domínguez-TenreiroUniversidad Autónoma de Madrid, Spain
Dust Effects in galaxy SEDsDust Effects in galaxy SEDs Galaxy formed in a hydro simulation Galaxy formed in a hydro simulation
Z=6 t/t_U=0.066
DECREASING UV optical // INCREASING IR submm L
DUST reradiates the overall bolometric luminosity SED has been calculated with GRASIL3D code (D-T et al, 2014)
MOTIVATION: Galaxy Formation Simulations: information on 6D phase
space, ages, composition, gas density and temperature.
Observations: light
Testing simulations (theories & models)
against observations demands SOFTWARE TELESCOPES:
Simulation outputs ----> SEDs, images
DUST EFFECTS: FUNDAMENTAL ROLE in GALAXY SEDs
GRASIL-3D
Application I.- Testing G-3 local galaxies
Application II.- IR-submm emission from CLUES Local Group dwarfs
Application III.- The MS and the Fundamental Plane of star-forming galaxies
GRASIL-3D: An extension of GRASIL to arbitrarygeometries and galaxy evolutionary
histories
(D-T+ 14)
RADIATIVE TRANSFER THROUGH DUST
SUNRISE (Jonsson 04,05; +09)
RADISHE (Chakrabarti+08; & Whitney09)
ART2 (Li + 07; Yajima+12)
MCarlo solve RT for Simu outputs
GRASIL assumesEquatorial & axial symmetry for galaxies
SAMS
PEGASE (Fioc & Rocca-Volmerage 1997)
CIGALE (Burgarella + 14) Parameter determination
SKIRT (Baes+ 03, 11)
GRASIL(-3D) PARTICULARITIESSeparately treats RT in MCs and in cirrus,
different dust composition
Age-dependent dust reprocessing of stellar populations: younger *s in denser ISM embeded in MC until destruction
Detailed non-equilibrium calculation for dust grains with diameter a < 250 A
---> Proper PAH treatment
RT solved in a grid, rather than MCarlo
CHARGE VARIABLES to a GRID
MC & CIRRUS DISTRIBUTIONBased on sub-resolution PDF (Wada+07 ; Federrath + 12)
Choose a density threshold for MC rho_thres
Choose a 2 parameter log-normal PDF for the cold gas f_pd(rho_0, sig)
For the ith particle
Identify <rho>_V = rho_gas(i) (**)
→ Calculate the MC mass fraction at ¨i¨
Calculate cirrus mass fraction at ¨i
(**) provides a link between PDF parameters
and simulation outputs ---> PDF sig
AGE DEPENDENT DUST REPROCESSING OF SP
Light fraction that can escape the StarBurst region, mimicking MC destruction,
f(t) = 1 if t<t_0
0 if t>2t_0
2-t/t_0 in other cases
DUST CONTENT k-th GAS PARTICLE d(Z_k) = Z_gas,k /(110 x Z_sun)
PARAMETERS GRASIL 3D
Grid size simulation resolution
rho_mc,thres 10 – 100 H/ cm^3 (Obs + simu)
1 PDF parameter sig 2 – 3 in simulations
---> cirrus & MC mass fraction f_mc
GRASIL
Dust model
Escape-time-scale t_0 2.5-8 or 18-50 Myrs (N,SB)
Individual MC log(m_mc) = 5 -6 M_o; r_mc= 10-50 pc
SIMULATION: SHAPE, EVOLUTION MODEL, SFRH
SIMULATIONSSIMULATIONS P-DEVA P-DEVA AP3M-SPHAP3M-SPH (Martínez-Serrano+ 08)(Martínez-Serrano+ 08) Entropy conserving; mutual neighbors OKEntropy conserving; mutual neighbors OK Chemical evolutionChemical evolution tracks the full dependence of tracks the full dependence of
metal production on the detailed chemical metal production on the detailed chemical composition of * particles (Q_ij formalism, composition of * particles (Q_ij formalism, Talbot+ 73Talbot+ 73))
Feedback: implicitely through (inefficient) SF Feedback: implicitely through (inefficient) SF parameters parameters (Agertz+ 11)(Agertz+ 11)
GASOLINEGASOLINE SPH SPH (Wadsley + 04,Brook + 11)(Wadsley + 04,Brook + 11) Feedback: blastwave formalism (Stinson+ 06) from Feedback: blastwave formalism (Stinson+ 06) from
Sne & Sne & massive starsmassive stars (Stinson+ 13). (Stinson+ 13). Effective coupling Effective coupling with gas 1%with gas 1%
Blast-wave scenario Blast-wave scenario
OBSERVATIONAL SAMPLES GRASIL-3D TESTINGISO Key Project on the ISM of Normal GalaxiesHelou+96; Dale+ 00 ISO & IRAS broad-band fluxes FIR active, quiescent and intermediate (Vega+05)
Aromatic Features in Emission 6.2,7.7,8.6 & 11.3 micron(Lu+03; a subsample of Dale+00)
Spitzer IR Normal Galaxy Survey (SINGS; Kennicutt+03; Dale+05)
Non-tidally perturbed & non-interacting galaxies(Smith+07, a SINGS subsample & Lanz+13 from KINGFISH)
Key Insights on Nearby Galaxies: FIR Survey w Herschel (KINGFISH, Kennicutt+11)All normal types 61 galaxies imaged with PACS and SPIRE (Dale+12)
MOLECULAR and ATOMIC HYDROGEN & STELLAR CONTENT A test for the MC model in GRASIL-3D
Simulations vs COLD GASS survey(Saintonge+11)
OK
IRAS flux density ratios: simulated (color) vs real (Gray: Dale+00) galaxies
FIR active, quiescent and intermediate (Vega+05)Lines join consecutive results for HD-5103B along a merger phase
LEFT: Merger
RIGHT: Normal
AFE Rel Strengths vs FIR/blueAt z=0 and around a MM
Gray points: data Lu+03 FIR-active,intermediate,quiescent
Color: simulations 8 gal. z=0 BLUE And merger phase Different parameter Sets Codes as in previous Fig.left
Observational results recovered Aromatic Features in Emission 6.2,7.7,8.6 & 11.3 micron(Lu+03; a subsample of Dale+00)
Spitzer IRAC & MIPS non-interacting Histograms: Smith+07 sample from SINGS
Points Averages over parameter sets
Spitzer IR Normal Galaxy Survey (SINGS ; Kennicutt+03; Dale+05)Non-tidally perturbed & non-interacting galaxies(Smith+07, a SINGS subsample & Lanz+13 from KINGFISH)
HERSCHEL BANDS non-interacting
Gray: Lanz+13Color: 8 simulated galaxies,
averages & dispersions over parameter sets
Key Insights on Nearby Galaxies: FIR Survey w Herschel (KINGFISH, Kennicutt+11)All normal types 61 galaxies imaged with PACS and SPIRE (Dale+12)
Non-tidally perturbed & non-interacting galaxies(Smith+07, a SINGS subsample & Lanz+13 from KINGFISH)
UV and optical flux density ratiosNon-interacting
Gray: data Dale+07
Color: 8 simulated galaxies,
averages & dispersions over parameter sets
GRASIL-3D DISCUSSION
Changing rho_mc_thres and PDF sig
Parameter variations: not remarkable effects when kept within their ranges
Energy balances: 98% or better
Find encouranging results when comparing with disk galaxies in detail
THE CLUES PROJECT
CLUES: Constrained I.C. (Hoffman +Ribak 92)
** Observational data imposed as constraintson the IC → local Universe skeleton at Mpc** Random at sub-Mpc
SIMULATION: GASOLINELCDMGrav.softening = 220 pcm_DM, m_*, m_gas 30, 2, 6 x10^4 M_sunFeedback ERIS simulation (Guedes+11)Includes chemical evolution
RESULTS: some relations
Luminosity – colorBLUE, CYAN: SF dwarfsRED: ¨dead¨ dwarfsData from Mateo 1998
Iron vs luminosityBlack Simulated D galaxies Red Data McConnachie+12
Dwarfs are low Z systems
RESULTS: SEDs for low M* & Z SF galaxies
Simulations + GRASIL → Two dust components, as observations demand
Galametz+09
MASS and SFRH DETERMINATION in SPIRAL GALAXIES
GRASIL-3D as a test bed for
Obreja et al., 14
III
Www.star.uclan.ac.uk/Cbb/magicc MAGICC Project, Brook & Stinson 2012
MOTIVATION
Constraining galaxy formation scenarios
MS: correlation SFR vs M_* (Wuyts + 11)
MZ: M_* vs metallicities
Gas phase (Garnett + 02; Tremonti + 04) Stars (Cowie & Berger 08; Pérez-Montero + 09)
COMPARING SIMU OUTPUTS TO OBSERVATIONAL DATA
OBSERVATIONS: M_* & SFR determined from light (SEDs)SIMULATIONS: need to apply the same recipees !!
NEED SEDS as close to observed ones as possible
SOFTWARE TELESCOPES
through
Projections of a fundamental relation? Ellison +08
Figure 1 from Galaxy Structure and Mode of Star Formation in the SFR-Mass Plane z ~ 2.5 to z ~ 0.1Stijn Wuyts et al. 2011
Constant slopeZero point ---> high-z galaxies form stars faster than local ones with same M_*Scatter independent of z Increases at lower M_*
METHODS SIMULATIONS
Disk gal. from the MaGICC project (Brook + 12; Stinson + 13)
GRASIL-3D post-processing
Face-on SB in r-band ----> Petrosian radii R_p (Blanton + 01)
** Luminosities, fluxes & colors from SEDs within 2R_p
ready to apply observational techniques
including dust effects MIMIC OBSERVATIONS ¨observed¨as they evolve from z=3.5 upto
z=0 (324 snapshots)
METHODS STELLAR MASS DETERMINATIONColor dependent mass-to-light relations B- and
V-band (McGaugh et al. in prep)
GLOBAL SFR IR-corrected far UV tracer of Hao + 11:
FUV flux corrected using the total IR emission WARNINGTest that simulated galaxy
** B-V and M_V are within those of the sample used for calibration
** IRX vs FUV -NUV used for calibration
RESULTS: M_* Testing observational methods
M_* assembly history, scatter is shownBlack: as predicted by simulationsBlue: B-band mass-to-light ratiosGreen: V-band
RESULTS: THE GLOBAL SFRH ¨Observational¨ SFRs vs real ones OK
BLACK: SFRHs predicted by simulationsBLUE: SFRHs from IR-corrected FUV
RESULTS: SCATTER IN THE MS
Independent of redshiftDecreases with increasing M_*
May trust simulations !!---> Reflects bursting/variable SFR in the SF population
RESULTS: THE FUNDAMENTAL METALLICITY RELATIONM_* - SFR – (O/H) in gas (Lara-López + 10)
GREY POINTS: simulated at z<3.5RED POINTS: simulations in equally populated M_* binsBLUE LINES: solid - linear fit with slope 1, as in Lara-López + 10 Dashed – 0.16 dex scatterBLACK LINES: solid & dashed - fit Lara-López data & scatter
** Tight correlation ** Same scatter as obs** Same coefficients** 0.09 dex lower normalization
CONCLUSIONS APPLICATION III
GRASIL-3D METHOD to test outthe observational methods to determine M_* and the SFRH in star forming galaxies
Consistency observations -simulations
The MS and MZ relation for star forming galaxiesAre projections of the Fundamental Plane M_*-SFR-O/H (Mannucci+ 10; Lara-López+ 10)
Prediction: the FP holds also for lower M_* star-forming galaxies
GENERAL CONCLUSIONS
GRASIL-3D particular strengths follow GRASIL (Silva+ 98; 99)
General applicability to systems with arbitrary geometry, in particular those produced in hydrodynmical simulations (evolutionary history, SFRH ..)
Subresolution PDF formalism to describe MC/cirrus density field
Comparison to observations of local galaxy samples are encouraging, particularly remarkable for PAH features
Detailed analysis of parameter space from literature gives consistent results
Many specific applications possible: different predictions on individual & statistical galaxy properties, directly comparable to observations
Applications so far give encouraging results
STAR FORMATION STAR FORMATION
A few parsec resolution Sne II E_II = 10^51 (mass/10 M_sun) erg injected in the ISM after 10 Myear a 8 – 40 M_sun star is formedSne Blast wave in adiabatic expansion if parsec-scale resolution (McKee & Ostriker 1977; Stinson et al. 2006; Brook 2010 . 2011)
SnIa E_I = E_II, but with slower timescale
+ metals
UNRESOLVED ISM (a few 100 pc for discs) mimic through tuning resolved physics: H_2 formation, small-scale turbulence, radiative effects free parameters, based upon core-scale physics : stocastic model(Katz 1992; parameter testing in Agertz et al. 2011)
d rho_g/dt = - e_ff rho_g/t_ff , rho_g>rho_t (K-S-like)
SNE BLAST WAVE MODELSNE BLAST WAVE MODEL** Sne explosions large volumes of hot, low-densitygas McKee & Ostriker analytical blast wave model
** Mimic its effect in SPH codes: Sne feedback from m_* >8M_o(Thacker & Couchman 2000; Stinson et al. 2006; Brook et al. 2011)Energy from massive stars prior to their explosions (Stinson+ 13)weak coupling of stellar energy to the sorrounding gas 1% Flow outwards + SFR regulated GASOLINE RUNS: 3 galaxies m_bar = 2 and 0.25 x 10^5 M_o e_g = 312,5 pc - 156,2 pc M_* = 2.3 - 0.6 x 10^10 M_o Disk & bulge scales, kine, B/D consistent with observations