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Synthetic properties of starburst galaxies
Abstract
We present the results of an extensive grid of evolutionary synthesis models for populations of massive stars. The parameter space has been chosen to correspond to conditions typically found in objects like giant H II regions, H II galaxies, blue compact dwarf galaxies, nuclear starbursts, and infrared luminous starburst galaxies. The models are based on the most up-to-date input physics for the theory of stellar atmospheres, stellar winds, and stellar evolution. Observable properties of a population of stars are computed for the two limiting cases of an instantaneous burst and a constant star- formation rate over a time interval of 3 x 10^8^ yr. We also investigate the effects of starformation histories which are intermediate between those two extreme cases. Three choices of the initial mass functions are studied: a Salpeter and a Miller-Scalo type IMF with upper mass limits of 100 M_sun_, and a Salpeter IMF truncated at 30 M_sun_. Metallicities of 0.1 Z_sun_, 0.25 Z_sun_, Z_sun_, and 2 Z_sun_ are considered. The model predictions include the numbers of hot stars, supernova rates, colors in the UBVRIJHKL passbands, slopes of the ultraviolet continuum observable by IUE, HST, and HUT, equivalent widths of hydrogen recombination lines, ionizing fluxes shortward of the H^0^, He^0^, and He^+^ ionization edges, the Lyman discontinuity, and mass- and energy- deposition rates due to stellar winds and supernovae. We discuss the contamination of the stellar ultraviolet, optical, and near-infrared continuum by nebular emission. It is found that under typical starburst conditions the nebular continuum is not negligible. Depending on the wavelength, addition of the nebular continuum leads to significantly redder or bluer broadband colors than obtained from a pure stellar continuum. A population of massive stars is not only important in terms of its output of radiation but also via its deposition of mechanical energy. The output of radiative and mechanical luminosity is compared at various starburst epochs. In a supernova dominated instantaneous starburst, the mechanical luminosity can be as large as almost 10% of the total radiative luminosity. This occurs when most massive O stars have disappeared, and the synthetic spectrum in the optical and near- ultraviolet is dominated by B and A stars. During this epoch, the output of ionizing radiation below 912 A becomes very small, as indicated by a very large Lyman discontinuity and a very small ratio of ionizing over mechanical luminosity. We discuss the relevance of these results for the interpretation of starburst galaxies, active galactic nuclei, and the energetics of the interstellar medium.
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“Massive ( ≳ 8 M ⊙ ) stars generate mechanical energy via stellar winds and SNe (Leitherer & Heckman 1995; Leitherer et al. 1999; Sternberg et al. 2003).”
From The Fermi/eROSITA bubbles: a look into the nuclear outflow from the Milky Way (2024) · cites this paper as Leitherer & Heckman 1995
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Spaxel analysis: probing the physics of star formation in ultraluminous infrared galaxies
Dopita, M. A., Rich, J., Vogt, F. P. A., et al. (2013) · Astrophysics and Space Science · doi:10.1007/s10509-013-1753-2 · Cited by 29
“Here we use the “standard” calibration for starbursts by Kennicutt (1998), based on the Starburst 99 models of Leitherer & Heckman (1995): SFRHα = 7.9× 10−42 [ LHα/erg.s −1] (1) Using the surface brightness per square arc sec. and the distance we can translate this star formation rate to the…”
MethodInfluentialDelgado, R. M. G., Leitherer, C., & Heckman, T. M. (1997) · The Astrophysical Journal · doi:10.1086/304813 · Cited by 29
Self-citationWarm dust as a tracer of galaxies with gaseous halos
Dahlem, M., Lazendic-Galloway, J., Haynes, R. F., et al. (2001) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20010639 · Cited by 29
“SF-related heating sources are photo-ionisation, shocks and/or turbulent mixing layers, but in principle all energy comes from processes relating to the evolution of high-mass stars (winds and type II supernovae; Leitherer & Heckman 1995; Leitherer et al. 1999).”
High-resolution UKIRT observations of circumnuclear star formation in M100
Ryder, S. D., & Knapen, J. H. (1999) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.1999.02204.x · Cited by 29
Absorption line indices in the UV - I. Empirical and theoretical stellar population models
Maraston, C., Nieves Colmárez, L., Bender, R., et al. (2009) · Max Planck Institute for Plasma Physics · doi:10.1051/0004-6361:20066907 · Cited by 28
“The lines of Civ and Si iv already have been studied extensively in the literature (Storchi-Bergmann et al. 1994; Leitherer & Heckman 1995; Leitherer et al. 1999; Heckman et al. 1998; Rix et al. 2004).”
BackgroundAnisotropic Galactic Outflows and Enrichment of the Intergalactic Medium. I. Monte Carlo Simulations
Pieri, M. M., Martel, H., & Grenon, C. (2007) · The Astrophysical Journal · doi:10.1086/510997 · Cited by 28
Bunker, A. J., Moustakas, L. A., & Davis, M. (2000) · The Astrophysical Journal · doi:10.1086/308432 · Cited by 28
“This is compa-M _ \M* \ 125 M _rable to the relation derived from the models of Leitherer & Heckman (1995).”
MethodPahl, A., Topping, M., Shapley, A., Sanders, R., Reddy, N., Clarke, L., Kehoe, E., Bento, T., & Brammer, G. (2024) · Astrophysical Journal · doi:10.3847/1538-4357/adb1ab · Cited by 32
“Assuming no ionizing photons escape the galaxy ( f esc = 0) and case B recombination, we can relate ˙n ion to L H α ,int via the relation of Leitherer & Heckman (1995): This equation assumes a temperature of 10 4 K and an electron density of 100 cm − 3 , but is not sensitive to the choice of…”
Lin, Y.-H., Scarlata, C. M., Williams, H., et al. (2023) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stad3483 · Cited by 27
Más-Hesse, J. M., Otí-Floranes, H., & Cerviño, M. (2008) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20078398 · Cited by 27
“Leitherer & Heckman (1995) presented the evolution of both supernova rate and the injection rate of mechanical energy for longer term evolution, up to ages of 300 Myr.”
BackgroundUltracompact Blue Dwarf Galaxies:Hubble Space TelescopeImaging and Stellar Population Analysis
Corbin, M. R., Vacca, W. D., Fernandes, R. C., Hibbard, J. E., Somerville, R. S., & Windhorst, R. A. (2006) · The Astrophysical Journal · doi:10.1086/507575 · Cited by 27
“The measured fluxes should thus mainly represent the stellar continuum emission of the objects, with a contribution from nebular continuum emission depending on the strength and age of the starburst (see Leitherer & Heckman 1995; Kruger, Fritze-von Alvensleben, & Loose 1995).”
BackgroundConfidence limits of evolutionary synthesis models III. On time-integrated quantitiesPreprint
Cerviño, M., Gómez-Flechoso, M. Á., Castander, F. J., et al. (2001) · arXiv (Cornell University) · doi:10.48550/arxiv.astro-ph/0107266 · Cited by 27
“…1 2 N ∑ i wiṁi(t)v 2 ∞,i(t), (13) where ṁi(t) is obtained from interpolations of the tracks and v∞,i(t) is derived from the interpolated luminosity, the effective temperature, the mass mi, and the metallicity of the star of initial mass Mi at the given age, following Leitherer and Heckman (1995).”
Modeling Tracers of Young Stellar Population Age in Star-Forming GalaxiesPreprint
Levesque, E. M., & Leitherer, C. (2016) · Cited by 27
Self-citationPiovan, L., Tantalo, R., & Chiosi, C. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.10573.x · Cited by 26
“…the level of SSPs and again no dust at the level of the galaxy model (see e.g. Arimoto & Yoshii 1987; Arimoto & Tarrab 1990; Bruzual & Charlot 1993; Leitherer & Heckman 1995; Leitherer et al. 1999; Tantalo et al. 1996; Kodama & Arimoto 1997; Kodama et al. 1998; Tantalo et al. 1998; Buzzoni 2002,…”
BackgroundStrait, V., Bradač, M., Coe, D., et al. (2021) · The Astrophysical Journal · doi:10.3847/1538-4357/abe533 · Cited by 26
“To do this, we first calculate hydrogen recombination line strength following the relation from Leitherer & Heckman (1995), scaling from integrated Lyman-continuum flux, and then follow the strengths determined with nebular line ratios by Anders & Fritze-v.”
MethodThe ionizing photon production efficiency of bright z ∼ 2 − 5 galaxies
Castellano, M., Belfiori, D., Pentericci, L., et al. (2023) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202346069 · Cited by 26
THE UV CONTINUUM OF z > 1 STAR-FORMING GALAXIES IN THE HUBBLE ULTRAVIOLET ULTRADEEP FIELD
Kurczynski, P., Gawiser, E., Rafelski, M. A., et al. (2014) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/793/1/l5 · Cited by 26
“The lowest expected value, β = −3, corresponds to the spectrum of individual O-type stars (Leitherer & Heckman 1995).”
BackgroundSpectroscopic Observations of Merging Galaxies
Donzelli, C. J., & Pastoriza, M. G. (2000) · The Astronomical Journal · doi:10.1086/301420 · Cited by 26
Bransford, M. A., Appleton, P. N., Marston, A. P., et al. (1998) · The Astronomical Journal · doi:10.1086/300629 · Cited by 26
Kennicutt, R. C. (1998) · Saas-Fee Advanced Course · doi:10.1007/3-540-31630-2_1 · Cited by 26
Toward a Unified Model for the “Diffuse Ionized Medium” in Normal and Starburst Galaxies
Wang, J., Heckman, T. M., & Lehnert, M. D. (1998) · The Astrophysical Journal · doi:10.1086/306489 · Cited by 26
“It is not surprising that most of line emission results from photoionization since the ionizing radiation energy from OB stars is about an order of magnitude higher than the total kinetic energy released by supernovae and stellar winds (cf. Leitherer & Heckman 1995).”
BackgroundInfluentialSelf-citationde Grijs, R., Anders, P., Lamers, H. J. G. L. M., et al. (2005) · White Rose Research Online (University of Leeds, The University of Sheffield, University of York) · Cited by 26
Leitherer, C., & Chen, J. (2008) · New Astronomy · doi:10.1016/j.newast.2008.10.007 · Cited by 25
Self-citationAbundance segregation in Virgo spiral galaxies
Dors, O. L., & Copetti, M. V. F. (2006) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20054592 · Cited by 25
Calibration of star formation rate tracers for short- and long-lived star formation episodes
Otí-Floranes, H., & Mas-Hesse, J. M. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/200913384 · Cited by 25
“SB99 synthesis models (Leitherer et al. 1999) are based on the original models by Leitherer & Heckman (1995), but have been continuously updated with new evolutionary tracks and stellar atmospheres.”
MethodJ-PLUS: Synthetic galaxy catalogues with emission lines for photometric surveys
Izquierdo–Villalba, D., Angulo, R. E., Orsi, A. A., et al. (2019) · Springer Link (Chiba Institute of Technology) · doi:10.1051/0004-6361/201936232/pdf · Cited by 25
Star Formation in the Tidal Tail of the Leo Triplet Galaxy NGC 3628
Chromey, F. R., Elmegreen, D. M., Mandell, A., et al. (1998) · The Astronomical Journal · doi:10.1086/300369 · Cited by 25
Evolutionary Synthesis Models of Young Star‐forming Regions: The Influence of Binary Stars
Dionne, D., & Robert, C. (2006) · The Astrophysical Journal · doi:10.1086/500380 · Cited by 25
“A nebular contribution to the SED is also considered, following the recipe of Leitherer & Heckman (1995).”
MethodJarrett, T. H., Polletta, M. D. C., Fournón, I. P., et al. (2006) · The Astronomical Journal · doi:10.1086/498414 · Cited by 25
[C ii ] 158 μm emission as an indicator of galaxy star formation rate
Liang, L., FELDMANN, R. J., Murray, N., et al. (2023) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stad3792 · Cited by 24
Near-infrared [Fe ii] emission from supernova remnants and the supernova rate of starburst galaxies
Morel, T., Doyon, R., & Louis, N. S. (2002) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2002.05026.x · Cited by 24
“…lifetime (t[Fe II]) of a single SNR, one can define the supernova rate, η, as: η = L[Fe II] t[Fe II] L[Fe II] yr−1 (1) This quantity can be used, for instance, to set constraints on the star formation history of starburst galaxies (e.g. Leitherer & Heckman 1995; Kotilainen et al. 1996). c© 2001 RAS”
BackgroundGazak, J. Z., Bastian, N., Kudritzki, R. P., et al. (2012) · Monthly Notices of the Royal Astronomical Society Letters · doi:10.1093/mnrasl/sls043 · Cited by 24
“The third category is to use some feature of the YMC, such as surface brightness fluctuations, the size of the bubble created by the YMC in the surrounding ISM (e.g, Whitmore et al. 2011), or the equivalent width of recombination lines (e.g. Leitherer & Heckman 1995) as a proxy for the cluster age.”
MethodThree-dimensional simulations of the interstellar medium in dwarf galaxies - II. Galactic winds
Marcolini, A., Brighenti, F., & D’Ercole, A. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.07954.x · Cited by 24
“According to Leitherer & Heckman (1995) the assumed injected energy corresponds to an instantaneous starburst of ∼ 2× 106 M⊙.”
BackgroundThe remarkable starburst-driven outflow in NGC 2782
Jogee, S., Kenney, J. D. P., & Smith, B. (1997) · CERN Document Server (European Organization for Nuclear Research) · Cited by 24
Bowman, W. P., Zeimann, G., Nagaraj, G., Ciardullo, R., Gronwall, C., McCarron, A. P., Weiss, L., Molina, M., Belles, A., & Schneider, D. (2020) · Astrophysical Journal · doi:10.3847/1538-4357/ab9f3c · Cited by 19
“As noted by Byler et al. (2017), other combinations of ionizing spectra and photoionization codes, 14 such as those presented in Dopita et al. (2013) using STARBURST99 (Leitherer & Heckman 1995) and MAPPINGS III (Sutherland & Dopita 1993) can produce [O III]/Hβ ratios that more closely resemble our sample.”
BackgroundChemical abundances in Seyfert galaxies – IX. Helium abundance estimates
Dors, O. L., Valerdi, M., Freitas-Lemes, P., et al. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac1722 · Cited by 23
On the neutral gas distribution and kinematics in the dwarf irregular galaxy IC 1613
Silich, S., Lozinskaya, T. A., Moiseev, A. V., et al. (2005) · Springer Link (Chiba Institute of Technology) · doi:10.1051/0004-6361:20053326/pdf · Cited by 23
Self-consistent population spectral synthesis with FADO
Cardoso, L. S. M., Gomes, J. M., & Papaderos, P. (2018) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201833438 · Cited by 23
Martin, C. L., & Kennicutt, R. C. (1997) · The Astrophysical Journal · doi:10.1086/304277 · Cited by 23
“The 0.25 Z⊙ evolutionary synthesis models of Leitherer & Heckman (1995), for example, predict a spectral hardness Q(He) / Q(H) = 0.23 and Q(He)/Q(H) = 0.07 from stellar populations continuously forming stars with a Salpeter initial mass function (IMF) and upper mass limits of mu = 100 M⊙ and 30 M⊙…”
MethodInfluentialThe energetics and mass loss of the dwarf starburst Markarian 33
Summers, L. K., Stevens, I. R., & Strickland, D. (2001) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2001.04722.x · Cited by 23
“A first estimate of the mass deposition rate, Ṁ for a 107M⊙ starburst, with Z = 0.3Z⊙ and c© 0000 RAS, MNRAS 000, 000–000 t = 5.8 Myr can be obtained from the starburst evolutionary synthesis models (Leitherer & Heckman 1995; Leitherer et al. 1999), and gives Ṁ ∼ 0.17M⊙ yr−1.”
BackgroundInfluentialA Fresh View of Henize 2‐10 with VLT NAOS‐CONICA
Cabanac, R. A., Vanzi, L., & Sauvage, M. (2005) · The Astrophysical Journal · doi:10.1086/432534 · Cited by 23
“Figure 6 (bottom right panel ) shows the histogram of the H equivalent-width log(EW[H ]) of the 12 central sources in units of log(8) (from Table 2) and the associated ages according to Leitherer & Heckman (1995).”
X‐Ray Properties of Lyman Break Galaxies in the Hubble Deep Field–North Region
Nandra, K., Mushotzky, R. F., Arnaud, K. A., et al. (2002) · The Astrophysical Journal · doi:10.1086/341888 · Cited by 23
“As the FIR luminosity is an excellent indicator of the current SFR (e.g., Leitherer & Heckman 1995; Kennicutt 1998), we can use the David et al. (1992) correlation to convert LX to SFR via the predicted LFIR.”
MethodMid‐Infrared Emission from E+A Galaxies in the Coma Cluster
Quillen, A. C., Rieke, G. H., Rieke, M. J., et al. (1999) · The Astrophysical Journal · doi:10.1086/307307 · Cited by 23
“However, the lack of 12 km emission, corresponding to (using conver-L IR[ 108 L _sion factors discussed in Leitherer & Heckman 1995 and Devereux & Young 1990), limits the current star formation rate even more, to yr~1.”
MethodSpaxel Analysis: Probing the Physics of Star Formation in Ultraluminous Infrared GalaxiesPreprint
Dopita, M. A., Rich, J. A., Vogt, A., et al. (2016) · Cited by 23
Near-Infrared Observations of Hot Spots in the Circumnuclear Rings of NGC 2997 and NGC 6951
Elmegreen, D. M., Chromey, F. R., Sawyer, J. E., et al. (1999) · The Astronomical Journal · doi:10.1086/300970 · Cited by 22
“…the same time, as might be expected from a large-scale gravitational instability, then their J[K colors would be 0.7 mag for an age of 107 yr, based on a comparison of the J[K colors with models of cluster evolution (e.g., Leitherer & Heckman 1995 ; Mayya 1995 ; Girardi & Bertelli 1998).”
MethodInfluentialProbing the Dust‐enshrouded Regions of the Interacting Galaxy System Arp 299:A Near‐Infrared Study
Satyapal, S., Watson, D. M., W. J. Forrest, J. L. P., et al. (1999) · The Astrophysical Journal · doi:10.1086/307130 · Cited by 22
Yun, M. S., & Scoville, N. Z. (1998) · The Astrophysical Journal · doi:10.1086/306369 · Cited by 22
“For a starburst population with a reasonable IMF, the ratio L/Mdyn should be less than 500 L⊙/M⊙ (Leitherer & Heckman 1995, Scoville et al. 1997b), and objects with an LFIR/MH2 ratio > 500 L⊙/M⊙ require a significant luminosity contribution from an active nucleus.”
BackgroundOrjales, J. M. C., Stevens, J. A., Jarvis, M. J., et al. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.22049.x · Cited by 21
“(2) The Kennicutt (1998) relation is dependent on the models of Leitherer & Heckman (1995).”
MethodHoughton, R. C. W., & Thatte, N. (2008) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2008.12893.x · Cited by 21
Hα Imaging of the Candidate Protogalaxy MS 1512−[CLC]cB58[/CLC]
Bechtold, J., Yee, H. K. C., Elston, R. J., et al. (1997) · The Astrophysical Journal · doi:10.1086/310520 · Cited by 21
IC 225: a dwarf elliptical galaxy with a peculiar blue corePreprint
Gu, Q., Zhao, Y., Shi, L., et al. (2005) · Cited by 21
Protocluster detection in simulations of HSC–SSP and the 10-yr LSST forecast, using PCcones
Araya-Araya, P., Vicentin, M. C., Junior, L. S., Overzier, R., & Cuevas, H. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab1133 · Cited by 20
UV Emission and bust properties of high redshift galaxies
Calzetti, D. (1999) · Astrophysics and Space Science · doi:10.1023/a:1002655227201 · Cited by 20
Functional and Physical Parameters of HII Galaxies
Díaz, Á. I. (1998) · Astrophysics and Space Science · doi:10.1023/a:1002129421272 · Cited by 20
Fitting optical source counts with an infrared-defined model: insights into galaxy evolution
King, A. J., & Rowan-Robinson, M. (2003) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2003.06240.x · Cited by 21
“Star formation produces stars with a range of masses, some of which will be sufficiently massive to explode as supernova very quickly (∼ 106 years; Leitherer & Heckman 1995), injecting heavy metals into the interstellar medium and producing large quantities of dust on short time scales (∼ 100 – 200…”
BackgroundOn the Recent History of Star Formation in the Blue Compact Dwarf Galaxy VII Z[CLC]w[/CLC] 403
Silich, S., Tenorio-Tagle, G., Muñoz-Tuñón, C., et al. (2002) · The Astronomical Journal · doi:10.1086/339969 · Cited by 20
Observations of a Tidal Tail in the Interacting Galaxies NGC 4485/4490
Elmegreen, D. M., Chromey, F. R., Knowles, B., et al. (1998) · The Astronomical Journal · doi:10.1086/300301 · Cited by 20
Tenorio‐Tagle, G., Silich, S., Rodriguez‐Gonzalez, A., et al. (2005) · The Astrophysical Journal · doi:10.1086/426962 · Cited by 20
“…would however reach the critical value after 4 Myr and 5 Myr, depending if one assumes solar or 0.1 solar as the original cluster metallicity (see Leitherer & Heckman, 1995; their Figure 37), and the UV radiation a couple of Myr after this will not suffice to sustain even the star cluster volume…”
BackgroundMethodInfluentialNew Wolf‐Rayet Galaxies with Detection of WC Stars
Huang, J. H., Gu, Q. S., Ji, L., et al. (1999) · The Astrophysical Journal · doi:10.1086/306859 · Cited by 20
“It should be pointed out that, at the burst age of 4-5 Myr for our three WR galaxies, the continuum emission from the gas is negligible (Leitherer & Heckman 1995).”
BackgroundNear-Infrared Observations of a Redshift 4.92 Galaxy: Evidence for Significant Dust Absorption
Soifer, B. T., Neugebauer, G. X., Franx, M., et al. (1998) · The Astrophysical Journal · doi:10.1086/311462 · Cited by 20
“63l predict for young, ionizing starburst populations (see, e.g., Leitherer & Heckman 1995).”
Extended gas in Seyfert galaxies: near-infrared observations of 15 active nuclei
Winge, C., Storchi‐Bergmann, T., Ward, M. J., et al. (2000) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2000.03614.x · Cited by 20
“21c and 21g corresponds to the region occupied by a young/intermediate age stellar population component with ages ranging from 106 to 108 years, calculated from the models of Leitherer & Heckman (1995).”
MethodLyα Escape from Low-mass, Compact, High-redshift Galaxies
Pucha, R., Reddy, N. A., Dey, A. T., et al. (2022) · The Astronomical Journal · doi:10.3847/1538-3881/ac83a9 · Cited by 19
“Assuming Case-B recombination, the intrinsic Hα luminosity is LHα[erg s −1] = 1.36 × 10−12Q(H0) (Leitherer & Heckman 1995), and the SFR [Me yr −1] ≈ 2.09× 10−42 L(Hα) [erg s−1] (Reddy et al. 2022).”
InfluentialCastellanos, M., Díaz, Á. I., & Terlevich, R. J. (2002) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2002.05934.x · Cited by 19
“This has been achieved in the last few years by several independent groups (e.g. Cerviño & Mas-Hesse 1994; Garcı́a-Vargas, Bressan & Dı́az 1995; Leitherer & Heckman 1995).”
BackgroundBeirão, P., Appleton, P. N., Brandl, B. R., et al. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/693/2/1650 · Cited by 19
“A K-band flux excess was also reported in previous studies that fitted SEDs with Starburst99 (Surace & Sanders (1999) for warm ULIGs; Mazzarella et al. (1992) for the nuclei of Arp 220), which was compensated adding a hot dust (800 K) component contributing to 10-30% of the emission (Surace & Sanders 1999).”
MethodInfluentialBarros, S. D., Reddy, N., & Shivaei, I. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/820/2/96 · Cited by 19
“The UV β slope depends on the age and dust attenuation of the galaxy (and the SFH, Leitherer & Heckman 1995; Meurer et al. 1999).”
BackgroundResultImaging and Spectrophotometry of Markarian 1094: Implications for the Recent Star Formation
Méndez, D. I., Cairós, L. M., Esteban, C., et al. (1999) · The Astronomical Journal · doi:10.1086/300803 · Cited by 19
“9), which is almost constant in the inner 3 kpc. Applying the population synthesis models for instantaneous bursts described by Leitherer & Heckman (1995) and assuming (as we explained in ° 3) that the e†ect of the underlying population is not signiÐcant, it is possible to derive the age of each…”
MethodInfluentialImaging and Spectroscopy of the Multiphase Halo of NGC 4631
Martin, C., & Kern, B. (2001) · The Astrophysical Journal · doi:10.1086/323161 · Cited by 19
Lopsidedness in dwarf irregular galaxies
Heller, A. B., Brosch, N., Almoznino, E., et al. (2000) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2000.03532.x · Cited by 19
“This latter component may be contaminated by nebular continuum emission from HII regions, but nebular emission amounts to only 30% of the light during the first few Myrs of a starburst, and becomes negligible as soon as the first red supergiants appear, at about 106.9 yr (Leitherer & Heckman 1995).”
BackgroundInfluentialA fresh view on Henize 2-10 with VLT/NAOS-CONICA
Cabanac, R. A., Vanzi, L., & Sauvage, M. (2005) · CERN Document Server (European Organization for Nuclear Research) · Cited by 19
New age estimates of M31 globular clusters from multi-colour photometry
Fan, Z., Ma, J., De Grijs, R., et al. (2006) · CERN Document Server (European Organization for Nuclear Research) · Cited by 19
Seeyave, L. T. C., Wilkins, S. M., Kuusisto, J. K., et al. (2023) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stad2487 · Cited by 18
Mao, Y.-W., Kennicutt, R. C., Hao, C.-N., et al. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/757/1/52 · Cited by 18
“−2.0, as suggested in Calzetti et al. 1994; Leitherer & Heckman 1995; Meurer et al. 1999), and any change in this slope results from wavelength-selective absorption of photons by dust grains.”
BackgroundInfluentialAn XMM–Newton view of M101 – III. Diffuse X-ray emission
Warwick, R. S., Jenkins, L. P., Read, A. M., Roberts, T. P., & Owen, R. A. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11571.x · Cited by 17
“The rate of energy deposition into the ISM from the subsequent supernovae rises at this time and remains fairly constant for∼ 3 × 107 yr (Leitherer & Heckman 1995; Cervino, Mas-Hesse & Kunth 2002).”
BackgroundA Grid of Composite Models for the Simulation of Starburst Galaxy and H ii Region Spectra
Contini, M., & Viegas, S. M. (2001) · The Astrophysical Journal Supplement Series · doi:10.1086/322527 · Cited by 18
“As shown by the models of Leitherer & Heckman (1995), the ratio between the mechanical energy and the ionizing Lyman continuum, both injected in the ISM by the massive star population, rapidly increases during the stellar cluster evolution.”
MethodThe tidally disturbed luminous compact blue galaxy Mkn 1087 and its surroundings
López-Sánchez, Á. R., Esteban, C., & Rodríguez, M. (2004) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20041457 · Cited by 18
“They used Leitherer & Heckman (1995) population synthesis models to estimate the ages of the emission zones detected in their images, finding that some of these emission knots are around 5 Myr old.”
MethodAn Intermediate-Band Imaging Survey for High-Redshift Lyman Alpha Emitters: The Mahoroba-11
Yamada, S. F., Sasaki, S. S., Sumiya, R., et al. (2005) · Publications of the Astronomical Society of Japan · doi:10.1093/pasj/57.6.881 · Cited by 18
“Then we can estimate Hβ luminosity, L(Hβ) using the following formula (Leitherer & Heckman 1995), L(Hβ) = 4.76× 10−13NLyc erg s −1.”
MethodInfluentialThe Ionization Source in the Nucleus of M84
Bower, G., Green, R. F., Quillen, A. C., et al. (2000) · The Astrophysical Journal · doi:10.1086/308741 · Cited by 18
Photometric and spectroscopic studies of star-forming regions within Wolf–Rayet galaxies
Karthick, M. C., López-Sánchez, Á. R., Sahu, D. K., et al. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt2301 · Cited by 17
“The estimated age of the most-recent star forming event can be derived from the Hα equivalent width, W(Hα), of the star-forming knots, because this value decreases with time (e.g. Leitherer & Heckman 1995; Johnson & Conti 2000).”
Similarities and uniqueness of Lyα emitters among star-forming galaxies at z = 2.5
Shimakawa, R., Kodama, T., Shibuya, T., et al. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx091 · Cited by 17
Shock Excitation in Interacting Galaxies: Markarian 266
Davies, R., Ward, M. J., & Sugai, H. (2000) · The Astrophysical Journal · doi:10.1086/308890 · Cited by 17
Hogg, D. W., & Phinney, E. S. (1997) · The Astrophysical Journal · doi:10.1086/310929 · Cited by 17
“7 of Leitherer & Heckman (1995); (b) the mass functions φ(logM) ∝ M φ(M) (number per decade in mass), really the distributions of starburst masses, arbitrarily choosing M∗ = 106 M⊙; (c) the bolometric luminosity functions φ(logLbol) ∝ Lbol φ(Lbol) (number per decade in luminosity) produced by the…”
BackgroundMethodInfluentialOriglia, L., & Oliva, E. (2000) · New Astronomy Reviews · doi:10.1016/s1387-6473(00)00054-3 · Cited by 17
Madau, P. (2000) · Philosophical Transactions of the Royal Society A Mathematical Physical and Engineering Sciences · doi:10.1098/rsta.2000.0627 · Cited by 17
Deep Spectroscopy in the Field of 3C 212
Stockton, A. N., & Ridgway, S. E. (1998) · The Astronomical Journal · doi:10.1086/300298 · Cited by 17
“Nevertheless, models for starbursts (Leitherer & Heckman 1995), which have been found to be generally consistent with observations (Stasińska & Leitherer 1996), indicate that Hα EWs can be as high as 3000 for ages up to 3 × 106 years and can remain above ∼ 300 up to ages of 108 years (these models…”
Age and Dust Degeneracy for Starburst Galaxies Solved?Preprint
Takagi, T., Arimoto, N., & Čius, V. V. (1999) · Cited by 17
Dissecting the Mid-infrared Heart of M83 with JWST
Hernández, S., Jones, L., Smith, L. J., et al. (2023) · The Astrophysical Journal · doi:10.3847/1538-4357/acc837 · Cited by 16
“Overall, starburst galaxies cover a broad range in morphology from blue compact dwarfs (BCDs, which share common properties with the high-z environments; e.g., Izotov et al. 2021) to spiral galaxies and merging systems (Leitherer & Heckman 1995; Leitherer et al. 1995; Annibali & Tosi 2022).”
BackgroundYang, C., Omont, A., Martín, S., et al. (2023) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202347610 · Cited by 16
KINEMATICS OF SUPERBUBBLES AND SUPERSHELLS IN THE IRREGULAR GALAXY, NGC 1569
Sánchez-Cruces, M., Rosado, M., Rodríguez‐González, A., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/799/2/231 · Cited by 16
Faro, B. L., Silva, L., Franceschini, A., et al. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu2593 · Cited by 16
“This calibration assumes that the Lbol of a constant SF lasting 100 Myr is totally emitted in the IR (K98; Leitherer & Heckman,1995 LH95 hereafter).”
BackgroundLOW-METALLICITY STAR FORMATION IN HIGH-REDSHIFT GALAXIES ATz∼ 8
Taniguchi, Y., Shioya, Y., & Trump, J. R. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/724/2/1480 · Cited by 16
“First, we calculate the luminosity of Hβ emission line, L(Hβ), using the following relation (Leitherer & Heckman 1995): L(Hβ) (erg s−1) = 4.76×10−13NLyc (s−1), (1) whereNLyc is the ionizing photon production rate estimated in each SED model.”
MethodInfluentialOngoing massive star formation in the bulge of M51
Lamers, H. J. G. L. M., Panagia, N., Scuderi, S., et al. (2001) · CERN Document Server (European Organization for Nuclear Research) · Cited by 16
A 'super' star cluster grown old: the most massive star cluster in the Local Group
Ma, J., de Grijs, R., Yang, Y., et al. (2006) · White Rose Research Online (University of Leeds, The University of Sheffield, University of York) · Cited by 16
From Gas to Stars: Regulation of Star Formation
Kennicutt, R. C. (1997) · Astrophysics and space science library · doi:10.1007/978-94-011-5620-2_7 · Cited by 16
A search for intergalactic H I gas in the NGC 1808 group of galaxies
Dahlem, M., Ehle, M., & Ryder, S. D. (2001) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20010614 · Cited by 16
“The major difference between the two galaxies does not lie in the total energy output, but in the size of the region over which the energy is produced in stellar winds and supernovae (Leitherer & Heckman 1995) and released into the ISM.”
BackgroundShioya, Y., & Bekki, K. (2000) · The Astrophysical Journal · doi:10.1086/312832 · Cited by 16
“If all the Lyman continuum photons are used for ionizing the surrounding gas, the luminosity of Hβ is calculated according to the following formula; L(Hβ)(erg s−1) = 4.76 × 10−13NLy(s −1) (5) (Leitherer & Heckman 1995).”
InfluentialThe ionizing photon production efficiency of star-forming galaxies at z ∼ 4–10
Llerena, M., Pentericci, L., Napolitano, L., et al. (2025) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202453251 · Cited by 15
CANUCS: UV and ionizing properties of dwarf star-forming galaxies at z ~ 5–7
Harshan, A., Bradač, M., Abraham, R. G., et al. (2024) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stae1574 · Cited by 15
Characterizing the signatures of star-forming galaxies in the extragalactic γ-ray background
Owen, E. R., Lee, K., & Kong, A. K. H. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab1707 · Cited by 15
ON THE EXTREME POSITIVE STAR FORMATION FEEDBACK CONDITION IN SCUBA SOURCES
Silich, S., Tenorio‐Tagle, G., Munõz-Tuñón, C., et al. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/711/1/25 · Cited by 15
“If one scales the evolutionary synthesis models (e.g. Leitherer & Heckman 1995) for star clusters generated by a constant star formation rate to the values inferred from the SCUBA sources (≥ 100 M⊙ yr −1; e.g. Greve et al. 2005; Swinbank et al. 2006; Tacconi et al. 2006), one sees that as a result…”
MethodFilaments in Galactic Winds Driven by Young Stellar Clusters
Rodríguez‐González, A., Esquivel, A., Velázquez, P. F., et al. (2008) · The Astrophysical Journal · doi:10.1086/592492 · Cited by 15
“We estimate the mass-loss rate ṀSC using the Starburst99 models (Leitherer & Heckman1995; Leitherer et al.1999)3 with the appropriate cluster masses and a Salpeter initial mass function (IMF) including stars between 1 and 100M .”
BackgroundMethod
Metadata
- Authors
- Leitherer, C., & Heckman, T. M.
- Affiliations
- Space Telescope Science Institute (US)
- Johns Hopkins University (US)
- Venue
- The Astrophysical Journal Supplement Series
- Publisher
- American Astronomical Society
- Published
- 1995-01
- Volume
- 96
- Pages
- 9
- ISSN
- 0067-0049 (ISSN-L)
- 1538-4365
- OpenAlex
- W2063361568
- Cited by
- 672
- References
- 0
- Citations by year
- 2026: 11 · 2025: 14 · 2024: 11 · 2023: 17 · 2022: 6 · 2021: 11 · 2020: 8 · 2019: 13 · 2018: 10 · 2017: 10 · 2016: 23 · 2015: 14 · 2014: 12 · 2013: 11 · 2012: 24
- Type
- conference abstract
- Language
- en
- Open access
- closed
- Locations
- The Astrophysical Journal Supplement Series (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Galaxies: Formation, Evolution, Phenomena
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Stellar, planetary, and galactic studies
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astrophysics and Star Formation Studies
- Keywords
- starburst galaxies, massive star populations, stellar population synthesis, H II regions, blue compact dwarf galaxies, nuclear starburst, luminous infrared galaxies, star formation history, initial mass function, stellar winds, supernova feedback, ionizing flux, mechanical luminosity, stellar colors, supernova rate
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