The DOI matches its Crossref record; 453 of the 493 references it cites were found in a registry or an index.
Star Formation in the Milky Way and Nearby Galaxies
Open accessAbstract
We review progress over the past decade in observations of large-scale star formation, with a focus on the interface between extragalactic and Galactic studies. Methods of measuring gas contents and star-formation rates are discussed, and updated prescriptions for calculating star-formation rates are provided. We review relations between star formation and gas on scales ranging from entire galaxies to individual molecular clouds.
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“The most direct external comparison to our CMD-based recent SFHs are the tracers that involve UV emission, as both are grounded in similarly young stellar populations”
From The Panchromatic Hubble Andromeda Southern Treasury (PHAST). II. The Spatially Resolved Recent Star Formation History in M31 (2026) · cites this paper as Kennicutt & Evans 2012
In the citing paper
“Physically, the FUV emission is weighted most strongly toward short lived O and B stars with lifetimes shorter than 100 Myr, with a strong weighting toward ages of 30-50 Myr”
From The Panchromatic Hubble Andromeda Southern Treasury (PHAST). II. The Spatially Resolved Recent Star Formation History in M31 (2026) · cites this paper as Kennicutt & Evans 2012
In the citing paper
“the failure of either constant SFR model to explain the observed FUV emission is due to the fact that the FUV is sensitive not just to the averaged rate of star formation over some time interval, but also depends on the detailed timing of star formation within that interval.”
From The Panchromatic Hubble Andromeda Southern Treasury (PHAST). II. The Spatially Resolved Recent Star Formation History in M31 (2026) · cites this paper as Kennicutt & Evans 2012
Citations
Cites
XO-2b: Transiting Hot Jupiter in a Metal-rich Common Proper Motion Binary
Burke, C. J., McCullough, P. R., Valenti, J., Johns-Krull, C., Janes, K. A., Heasley, J., Summers, F. J., Stys, J., Bissinger, R., Fleenor, M., et al. (2007) · The Astrophysical Journal · doi:10.1086/523087 · Cited by 11,857 · cited 1×
“Various objections and caveats to this appealing picture have been registered (e.g., Swift & Williams 2008; Reid et al. 2010; Clark et al. 2007; Hatchell & Fuller 2008).”
BackgroundGalactic Stellar and Substellar Initial Mass Function
Chabrier, G. (2003) · Publications of the Astronomical Society of the Pacific · doi:10.1086/376392 · Cited by 9,071 · cited 2×
“More recent determinations over a wider range of masses, including brown dwarfs, indicate a clear flattening at lower masses, either as broken power laws (Kroupa et al. 1993) or a log-normal distribution (Miller & Scalo 1979; Chabrier 2003).”
BackgroundResultThe Luminosity function and stellar evolution
Salpeter, E. (1955) · The Astrophysical Journal · doi:10.1086/145971 · Cited by 6,816 · cited 46×
“This uncertainty range does not include all possible systematic errors, arising for example from changes in X(CO) or the IMF with increasing surface density or SFR. Major systematic changes in either of these could easily change the derived value of N by as much as 0.2–0.3.”
BackgroundMethodInfluentialSTAR FORMATION IN GALAXIES ALONG THE HUBBLE SEQUENCE
Kennicutt, R. C. (1998) · Annual Review of Astronomy and Astrophysics · doi:10.1146/annurev.astro.36.1.189 · Cited by 6,578 · cited 11×
“The High-density Regime The two regimes discussed above were able to reproduce all of the early observations of the large-scale star formation law by Kennicutt (1989, 1998b) and Martin & Kennicutt (2001).”
BackgroundMethodInfluentialSelf-citationStarburst99: Synthesis Models for Galaxies with Active Star Formation
Leitherer, C., Schaerer, D., Goldader, J. D., Delgado, R. M. G., Robert, C., Kune, D. F., de Mello, D. F., Devost, D., & Heckman, T. M. (1999) · The Astrophysical Journal Supplement Series · doi:10.1086/313233 · Cited by 4,126 · cited 1×
“The results cited here use the Starburst99 models of Leitherer et al. (1999), which are regularly updated in the on-line version of the package.”
MethodThe Global Schmidt law in star forming galaxies
Kennicutt, R., & Jr. (1997) · The Astrophysical Journal · doi:10.1086/305588 · Cited by 4,027 · cited 11×
“The High-density Regime The two regimes discussed above were able to reproduce all of the early observations of the large-scale star formation law by Kennicutt (1989, 1998b) and Martin & Kennicutt (2001).”
BackgroundMethodInfluentialSelf-citationHerschel Space Observatory - An ESA facility for far-infrared and submillimetre astronomy
Pilbratt, G., Riedinger, J., Passvogel, T., Crone, G., Doyle, D., Gageur, U., Heras, A., Jewell, C., Metcalfe, L., Ott, S., et al. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201014759 · Cited by 2,540 · cited 2×
“This section focusses on the transformational results which have come from the Spitzer Space Telescope (Werner et al. 2004) and the Herschel Space Observatory (Pilbratt et al. 2010).”
BackgroundThe physical properties of star-forming galaxies in the low-redshift universe
Brinchmann, J., Charlot, S., White, S. D. M., Tremonti, C., Kauffmann, G., Heckman, T., & Brinkmann, J. (2003) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.07881.x · Cited by 2,513 · cited 3×
“The mass dependence of the SSFR has been explored by numerous investigators (e.g., Brinchmann et al. 2004; Salim et al. 2007; Schiminovich et al. 2007; Lee et al. 2007).”
BackgroundMethodThe Galaxy Evolution Explorer : A Space Ultraviolet Survey Mission
Martin, D. C., Fanson, J., Schiminovich, D., Morrissey, P., Friedman, P. G., Barlow, T. A., Conrow, T., Grange, R., Jelinsky, P. N., Milliard, B., et al. (2005) · The Astrophysical Journal · doi:10.1086/426387 · Cited by 2,470 · cited 4×
“For extragalactic studies, this subject has been revolutionised by the launch of the Galaxy Evolution Explorer (GALEX) mission (Martin et al. 2005a).”
BackgroundMethodInfluentialEmbedded Clusters in Molecular Clouds
Lada, C., & Lada, E. (2003) · Annual Review of Astronomy and Astrophysics · doi:10.1146/annurev.astro.41.011802.094844 · Cited by 2,375 · cited 2×
“The masses of embedded young clusters (Lada & Lada 2003), OB associations (McKee & Williams 1997), and massive open clusters (Elmegreen & Efremov 1997; Zhang & Fall 1999), follow a similar relation with γcluster ∼ 1.”
Background
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Cited by
Sorted by citations
Items 401–500 of 1,004
Clark, C., Dunne, L., Gomez, H., Maddox, S., de Vis, P., Smith, M., Eales, S., Baes, M., Bendo, G. J., Bourne, N., et al. (2015) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1276 · Cited by 49
“MIR emission comes primarily from hot dust, heated by short-wavelength photons emitted from newborn stars, and traces star formation on time scales < 100 Myr (Calzetti et al., 2005; Kennicutt & Evans, 2012).”
BackgroundInfluentialCALIBRATING UV STAR FORMATION RATES FOR DWARF GALAXIES FROM STARBIRDS
McQuinn, K. B. W., Skillman, E. D., Dolphin, A. E., & Mitchell, N. P. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/808/2/109 · Cited by 48
“UV scaling relations are widely used because of their relative simplicity and because they have been consistently calibrated against each other (e.g., Kennicutt & Evans 2012, and references therein).”
MethodRosario, D., Burtscher, L., Davies, R., Koss, M., Ricci, C., Lutz, D., Riffel, R., Alexander, D., Genzel, R., Hicks, E., et al. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2670 · Cited by 48
“…by Universidade Federal do Rio Grande do Sul user on 08 March 2018 which is based on the calibration from Kennicutt & Evans (2012), in the limit that all the radiation from the young stars of a continuous star-forming population with a Chabrier IMF is…”
BackgroundEstimating gas masses and dust-to-gas ratios from optical spectroscopy
Brinchmann, J., Charlot, S., Kauffmann, G., Heckman, T., White, S., & Tremonti, C. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt551 · Cited by 48
“(24) Calibrations of XCO against metallicity in the literature show a large variation between different authors (see Bolatto et al. 2008; Leroy et al. 2011; Kennicutt & Evans 2012, for summaries).”
BackgroundHarvey, P., Fallscheer, C., Ginsburg, A., Terebey, S., André, P., Bourke, T., di Francesco, J., Könyves, V., Matthews, B., & Peterson, D. (2012) · doi:10.1088/0004-637x/764/2/133 · Cited by 48
“Kennicutt & Evans (2012) have reviewed this subject extensively in the context of both Galactic and extragalactic star formation.”
BackgroundDelvecchio, I., Daddi, E., Sargent, M., Jarvis, M., Elbaz, D., Jin, S., Liu, D.-Z., Whittam, I., Algera, H., Carraro, R., et al. (2021) · Astronomy & Astrophysics · doi:10.1051/0004-6361/202039647 · Cited by 47
“Given the tight correlation between LIR and SFR, the IR data have been extensively used as proxy for SFR, assuming that most of galaxy star formation is obscured by dust (Kennicutt 1998; Kennicutt & Evans 2012).”
MethodResultResolved [C ii] Emission from z > 6 Quasar Host–Companion Galaxy Pairs
Neeleman, M., Bañados, E., Walter, F., Decarli, R., Venemans, B. P., Carilli, C. L., Fan, X., Farina, E. P., Mazzucchelli, C., Novak, M., et al. (2019) · The Astrophysical Journal · doi:10.3847/1538-4357/ab2ed3 · Cited by 75
“Second, using the conversion between SFR and dust continuum measurement / total infrared luminosity (e.g., Kennicutt & Evans 2012).”
MethodCai, Z., Hamden, E., Matuszewski, M. J., Prochaska, J., Li, Q., Cantalupo, S., Battaia, F. A., Martin, C. D., Neill, J., O'Sullivan, D., et al. (2018) · Astrophysical Journal · doi:10.3847/2041-8213/aacce6 · Cited by 47
“0.3 M yr−1 (Kennicutt & Evans 2012).”
InfluentialThe Fraction of Stars That Form in Clusters in Different Galaxies
Chandar, R., Fall, S., Whitmore, B., & Mulia, A. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa92ce · Cited by 47
“We use the most recent GALEX FUV and Spitzer 24 μm fluxes from the literature and the formulae given in Kennicutt & Evans (2012) to derive an extinctioncorrected FUV-based SFR (by including the 24 μm flux to correct for attenuation by dust) and the 24 μm flux measurements alone to determine an…”
BackgroundMethodInfluentialFang, X., Thompson, T., & Hirata, C. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty472 · Cited by 47
“…the Milky Way SFR range from around 0.68 − 4 M yr−1 (e.g., Diehl et al. 2006; Misiriotis et al. 2006; Murray & Rahman 2010; Robitaille & Whitney 2010; Kennicutt & Evans 2012), which combined with our estimate of f (t < 1010yr) = 0.31 − 0.33 gives an event rate from quadruple systems of ∼ 0.01 −…”
BackgroundInfluentialCO line emission from galaxies in the Epoch of Reionization
Vallini, L., Pallottini, A., Ferrara, A., Gallerani, S., Sobacchi, E., & Behrens, C. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2376 · Cited by 47
Galaxy And Mass Assembly: the 1.4 GHz SFR indicator, SFR-M* relation and predictions for ASKAP-GAMA
Davies, L., Huynh, M., Hopkins, A., Seymour, N., Driver, S., Robotham, A., Baldry, I., Bland-Hawthorn, J., Bourne, N., Bremer, M., et al. (2017) · doi:10.1093/mnras/stw3080 · Cited by 47
Sarbadhicary, S., Badenes, C., Chomiuk, L., Caprioli, D., & Huizenga, D. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2566 · Cited by 47
“We assign locations of CC SNRs in M33 using FUV (Gil de Paz et al. 2007) and 24 µm (Dale et al. 2009) images, which trace recent star formation (Kennicutt & Evans 2012).”
MethodA resolved analysis of cold dust and gas in the nearby edge-on spiral NGC 891
Hughes, T., Baes, M., Fritz, J., Smith, M. W. L., Parkin, T., Gentile, G., Bendo, G. J., Wilson, C., Allaert, F., Bianchi, S., et al. (2014) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201323245 · Cited by 47
“There is a power-law correlation between the surface densities of gas (Σgas) and SFR (ΣSFR), with numerous studies attempting to constrain the power-law index via global quantities from galaxy samples and resolved observations of individual systems (see Kennicutt & Evans 2012, for a review).”
BackgroundTiming the earliest quenching events with a robust sample of massive quiescent galaxies at 2 < z < 5
Carnall, A., Walker, S., McLure, R., Dunlop, J., Mcleod, D., Cullen, F., Wild, V., Amorín, R., Bolzonella, M., Castellano, M., et al. (2020) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/staa1535 · Cited by 46
“It is possible to turn this line flux into an approximation of the SFR for this galaxy, assuming an intrinsic Lyα/Hα ratio of 8.7 (from case B recombination theory; see Osterbrock 1989) and the Kennicutt & Evans (2012) relationship between Hα luminosity and SFR.”
BackgroundInfluentialChruslinska, M., & Nelemans, G. (2019) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stz2057 · Cited by 46
First gas-phase metallicity gradients of 0.1 ∼ < z ∼ < 0.8 galaxies with MUSE
Carton, D., Brinchmann, J., Contini, T., Epinat, B., Finley, H., Richard, J., Patrício, V., Schaye, J., Nanayakkara, T., Weilbacher, P., et al. (2018) · doi:10.1093/mnras/sty1343 · Cited by 46
“Finally, we convert the inferred dust-corrected Hα luminosities to SFRs using a scaling relation between Hα and SFR log10 ( SFR M yr−1 ) = log10 ( L(Hα) ergs−1 ) −41.27, (3) (Murphy et al. 2011; Hao et al. 2011; Kennicutt & Evans 2012).”
MethodInfluentialCatalán-Torrecilla, C., de Paz, A. D., Castillo-Morales, Á., Méndez-Abreu, J., Falcón-Barroso, J., Bekeraitė, S., Costantin, L., de Lorenzo-C'aceres, A., Florido, E., García-Benito, R., et al. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8a6d · Cited by 46
“In this work we use extinction-corrected Hα (Hαcorr) as our SFR reference indicator following the recipe given by Kennicutt & Evans (2012).”
MethodSelf-citationAn instability of feedback regulated star formation in galactic nuclei
Torrey, P., Hopkins, P., Faucher-Giguere, C., Vogelsberger, M., Quataert, E., Kereš, D., & Murray, N. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx254 · Cited by 46
“The smoothed definition of the SFR is therefore more in line with what is measured observationally through UV or nebular emission line SFR tracers (e.g., see Table 1 of Kennicutt & Evans 2012).”
BackgroundThe nebular emission of star-forming galaxies in a hierarchical universe
Orsi, Á., Padilla, N., Groves, B., Cora, S., Tecce, T., Gargiulo, I., & Ruiz, A. (2014) · doi:10.1093/mnras/stu1203 · Cited by 46
Missing [C ii] emission from early galaxies
Carniani, S., Ferrara, A., Maiolino, R., Castellano, M., Gallerani, S., Fontana, A., Kohandel, M., Lupi, A., Pallottini, A., Pentericci, L., et al. (2020) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/staa3178 · Cited by 45
“We note that, if we use the SFR estimated from the UV+FIR luminosity (Kennicutt & Evans 2012), which is the same method used for the other [CII] emitters from the literature (e.g. Matthee et al. 2019) and for the ALPINE survey (Schaerer et al. 2020), our sources are in agreement with the local…”
MethodInfluentialMerging Rates of Compact Binaries in Galaxies: Perspectives for Gravitational Wave Detections
Boco, L., Lapi, A., Goswami, S., Perrotta, F., Baccigalupi, C., & Danese, L. (2019) · Astrophysical Journal · doi:10.3847/1538-4357/ab328e · Cited by 45
“The SFR of a galaxy is directly proportional to the intrinsic UV luminosity; however, the latter can be significantly absorbed by even a modest amount of dust and re-radiated mostly at far-IR/(sub)mm wavelengths (e.g., Kennicutt & Evans 2012).”
BackgroundWhat drives the radio slopes in radio-quiet quasars?
Laor, A., Baldi, R., & Behar, E. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/sty3098 · Cited by 45
“The Kennicutt-Schmidt law implies an associated surface gas density (e.g. Kennicutt & Evans 2012, Fig.11 there) of > 104 − 105 M⊙ pc −2, or a total associated gas mass Mgas > 3× 10 10 − 3× 1011 M⊙ at the core.”
BackgroundColombo, D., Kalinova, V., Utomo, D., Rosolowsky, E., Bolatto, A., Levy, R., Wong, T., Sánchez, S. F., Leroy, A., Ostriker, E., et al. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx3233 · Cited by 45
“Star formation occurs exclusively within molecular clouds, which are local overdensities with respect to the molecular gas density distribution (for a recent review see Kennicutt & Evans 2012).”
BackgroundNear-infrared MOSFIRE Spectra of Dusty Star-forming Galaxies at 0.2 < z < 4
Casey, C., Cooray, A., Killi, M., Capak, P., Chen, C.-C., Hung, C., Kartaltepe, J., Sanders, D., & Scoville, N. (2017) · doi:10.3847/1538-4357/aa6cb1 · Cited by 45
Goldbaum, N., Krumholz, M., & Forbes, J. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/827/1/28 · Cited by 45
“In all three cases, the classical Kennicutt-Schmidt law (Kennicutt 1998; Kennicutt & Evans 2012), where the total gas surface density is on the x-axis, shows a superlinear scaling, as observed in nearby star forming galaxies.”
BackgroundEllsworth-Bowers, T., Rosolowsky, E., Glenn, J., Ginsburg, A., Evans, N. J., Battersby, C., Shirley, Y., & Svoboda, B. (2014) · doi:10.1088/0004-637x/799/1/29 · Cited by 45
“Derived distances to and physical properties of these objects may answer several outstanding questions about massive star formation (Kennicutt & Evans 2012).”
Self-citationJet-induced star formation in 3C 285 and Minkowski Object
Salom'e, Q., Salom'e, P., & Combes, F. (2014) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201424932 · Cited by 45
“The Hα, TIR, FIR, and 24 µm SFR were calculated following Kennicutt & Evans (2012), Kennicutt (1998), and Calzetti et al. (2007).”
BackgroundMethodInfluentialOMEGA: OSIRIS Mapping of Emission-Line Galaxies in A901/2
Chies-Santos, A., del Pino, B. R., Aragón-Salamanca, A., Bamford, S., Gray, M., Wolf, C., Böhm, A., Maltby, D., Pintos-Castro, I., Sánchez-Portal, M., et al. (2014) · Proceedings of the International Astronomical Union · doi:10.1093/mnras/stz007 · Cited by 45
The Star Formation Rate of the Milky Way as Seen by Herschel
Elia, D., Molinari, S., Schisano, E., Soler, J. D., Merello, M., Russeil, D., Veneziani, M., Zavagno, A., Noriega‐Crespo, A., Olmi, L., et al. (2022) · The Astrophysical Journal · doi:10.3847/1538-4357/aca27d · Cited by 95
“Our result, in essence, corroborates the common idea - supported by the fact that a variety of approaches leads to similar values - that the current SFR of the Milky Way lies in the range 1.5-2.5 M⊙ yr −1, which is consistent with the values found for spiral galaxies (e.g., Kennicutt & Evans 2012).”
BackgroundMethodResultInfluentialH i-MaNGA: tracing the physics of the neutral and ionized ISM with the second data release
Stark, D., Masters, K., Avila-Reese, V., Riffel, R., Riffel, R., Boardman, N., Zheng, Z., Weijmans, A., Dillon, S., Fielder, C. E., et al. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab566 · Cited by 44
Thorne, J., Robotham, A., Davies, L., Bellstedt, S., Driver, S., Bravo, M., Bremer, M., Holwerda, B., Hopkins, A., Lagos, C. D. P., et al. (2020) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stab1294 · Cited by 44
From Diffuse Gas to Dense Molecular Cloud Cores
Ballesteros-Paredes, J., André, P., Hennebelle, P., Klessen, R., Inutsuka, S., Kruijssen, J. M. D., Chevance, M., Nakamura, F., Adamo, A., & Vázquez-Semadeni, E. (2020) · Space Science Reviews · doi:10.1007/s11214-020-00698-3 · Cited by 44
“…et al. 2010; Gutermuth et al. 2011) between the molecular gas mass surface density (Σ ) and the star formation rate surface density (ΣSFR), which is observed to have a power law form of ΣSFR ∝ ΣN with N = 1–1.5 (e.g. Kennicutt 1998; Bigiel et al. 2008; Kennicutt and Evans 2012; Leroy et al. 2013).”
BackgroundInfluentialZhang, Z.-Y., Ivison, R., George, R., Zhao, Y.-H., Dunne, L., Herrera-Camus, R., Lewis, A., Liu, D.-Z., Naylor, D., Oteo, I., et al. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2082 · Cited by 44
“Despite calculating almost identical dust emission luminosities, the SFR we derive using our chosen calibration: that presented in Murphy et al. (2011) and recommended by the review of Kennicutt & Evans (2012); is a factor of 3 higher than value reported by Negrello et al. (2014).”
BackgroundMethodInfluentialFarina, E. P., Venemans, B. P., Decarli, R., Hennawi, J. F., Walter, F., Bañados, E., Mazzucchelli, C., Cantalupo, S., Battaia, F. A., & McGreer, I. D. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8df4 · Cited by 63
“These leakage may be associated with short and extreme bursts of star formation as proposed to explain the intrinsically blue rest frame UV slope observed in dusty, star forming galaxies (SFR>50 M yr −1) up to z∼5 (e.g., Casey et al. 2014).”
InfluentialKatsianis, A., Blanc, G., Lagos, C., Tejos, N., Bower, R., Alavi, A., González, V., Theuns, T., Schaller, M., & Lopez, S. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2020 · Cited by 44
The discovery of gas-rich, dusty starbursts in luminous reddened quasars at z ∼ 2.5 with ALMA
Banerji, M., Carilli, C., Jones, G., Wagg, J., McMahon, R. G., Hewett, P., Alaghband-Zadeh, S., & Feruglio, C. (2016) · doi:10.1093/mnras/stw3019 · Cited by 44
“The FIR luminosity here is defined between 40 and 300 µ m and we use the Kennicutt & Evans (2012) relation to convert this FIR luminosity to a star formation rate: Once again, these values can be found in Table 3 and correspond to the average of the T d = 47 K, β = 1.6 and T d = 41 K, β = 1.95 grey…”
InfluentialMID-INFRARED COLORS OF DWARF GALAXIES: YOUNG STARBURSTS MIMICKING ACTIVE GALACTIC NUCLEI
Hainline, K., Reines, A., Greene, J., & Stern, D. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/832/2/119 · Cited by 44
“The luminosity of Hα can be used to measure the SFR for a galaxy, following Kennicutt & Evans (2012): ( [ ]) ( ( ) [ ]) ( )☉ a= -- -”
MethodTHE LINK BETWEEN THE FORMATION RATES OF CLUSTERS AND STARS IN GALAXIES
Chandar, R., Fall, S., & Whitmore, B. (2015) · doi:10.1088/0004-637x/810/1/1 · Cited by 44
“…including flux measurements, corrections made for attenuation by dust, variations in the SFR, uncertainties in the calibration used to convert the measured fluxes to SFR as discussed in the review by Kennicutt & Evans (2012), and the leakage of Lyman continuum photons from the parent galaxy.”
BackgroundMethodInfluentialObservation of self-bound droplets of ultracold dipolar molecules.
Zhang, S.-W., Yuan, W., Bigagli, N., Kwak, H., Karman, T., Stevenson, I., & Will, S. (2025) · Nature · doi:10.1038/s41586-026-10245-9 · Cited by 43
Star formation scaling relations at ∼100 pc from PHANGS: Impact of completeness and spatial scale
Pessa, I., Schinnerer, E., Belfiore, F., Emsellem, E., Leroy, A., Schruba, A., Kruijssen, J., Pan, H.-A., Blanc, G., S'anchez-Bl'azquez, P., et al. (2021) · Astronomy & Astrophysics · doi:10.1051/0004-6361/202140733 · Cited by 43
Curti, M., Maiolino, R., Cirasuolo, M., Mannucci, F., Williams, R. J., Auger, M., Mercurio, A., Hayden-Pawson, C., Cresci, G., Marconi, A., et al. (2019) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stz3379 · Cited by 43
“The global SFR for our sources is calculated from the extinctioncorrected Hα luminosity, which is converted to SFR assuming the Kennicutt & Evans (2012) relation and applying a scaling factor of 1.06 to convert from Kroupa, Tout & Gilmore (1993) to Chabrier (2003) IMF.”
MethodInfluentialThe art of modelling CO, [C i], and [C ii] in cosmological galaxy formation models
Popping, G., Narayanan, D., Somerville, R., Faisst, A., & Krumholz, M. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2969 · Cited by 43
George, K., Poggianti, B., Gullieuszik, M., Fasano, G., Bellhouse, C., Postma, J., Moretti, A., Jaffé, Y., Vulcani, B., Bettoni, D., et al. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1452 · Cited by 43
“> 20M , (O & B spectral type) whose lifetimes are 10-20 Myr or shorter (Kennicutt 1998; Kennicutt & Evans 2012).”
BackgroundA Virgo Environmental Survey Tracing Ionised Gas Emission (VESTIGE)
Boselli, A., Fossati, M., Ferrarese, L., Boissier, S., Consolandi, G., Longobardi, A., Amram, P., Balogh, M., Barmby, P., Boquien, M., et al. (2018) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201732407 · Cited by 43
“…line originates primarily from gas ionised by young and massive OB stars; it is thus an excellent tracer of ongoing star formation (Kennicutt 1998; Boselli et al. 2001, 2009; Kennicutt & Evans 2012), sensitive to stellar populations much younger than those detected in the GALEX UV bands (Hα.”
BackgroundH2 distribution during the formation of multiphase molecular clouds
Valdivia, V., Hennebelle, P., Gérin, M., & Lesaffre, P. (2015) · doi:10.1051/0004-6361/201527325 · Cited by 43
“Moreover, excitation energies are very high and require very high temperatures or strong ultraviolet (UV) fields to excite its rotational levels (Kennicutt & Evans 2012).”
BackgroundSUB-KILOPARSEC IMAGING OF COOL MOLECULAR GAS IN TWO STRONGLY LENSED DUSTY, STAR-FORMING GALAXIES
Spilker, J., Aravena, M., Marrone, D., B'ethermin, M., Bothwell, M., Carlstrom, J., Chapman, S., Collier, J., de Breuck, C., Fassnacht, C., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/811/2/124 · Cited by 43
“One of the most studied correlations is the powerlaw relationship between the gas surface density, Σgas, and the SFR surface density, ΣSFR (Schmidt 1959; Kennicutt 1998; see Kennicutt & Evans 2012 for a recent review).”
BackgroundPROSPECTS FOR CHEMICALLY TAGGING STARS IN THE GALAXY
Ting, Y.-S., Conroy, C., & Goodman, A. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/807/1/104 · Cited by 43
“NGC 6946 has long been thought to be a Milky Way counterpart (e.g., Kennicutt & Evans 2012).”
BackgroundThe Effect of Galaxy Interactions on Molecular Gas Properties
Pan, H.-A., Lin, L.-W., Hsieh, B.-C., Xiao, T., Gao, Y., Ellison, S., Scudder, J., Barrera-Ballesteros, J., Yuan, F.-T., Saintonge, A., et al. (2018) · Astrophysical Journal · doi:10.3847/1538-4357/aaeb92 · Cited by 42
“The SFR (or SFR surface density) is observed to correlate with MH2 (or MH2 surface density) with a power-law index of N≈1–2 (Kennicutt & Evans 2012).”
BackgroundThe starburst galaxy NGC 253 revisited by H.E.S.S. and Fermi-LAT
Abdalla, H., Aharonian, F., Benkhali, F. A., Angüner, E., Arakawa, M., Arcaro, C., Armand, C., Arrieta, M., Backes, M., Barnard, M., et al. (2018) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201833202 · Cited by 42
“Corresponding authors: H.E.S.S. Collaboration, e-mail: contact.hess@hess-experiment.eu † Deceased. starburst phase typically lasts for a few hundred million years (see e.g. Kennicutt & Evans 2012; Krumholz 2014, and references therein).”
BackgroundSpatially resolved cold molecular outflows in ULIRGs
Pereira-Santaella, M., Colina, L., García-Burillo, S., Combes, F., Emonts, B., Aalto, S., Alonso-Herrero, A., Arribas, S., Henkel, C., Labiano, Á., et al. (2018) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201833089 · Cited by 42
“The total IR luminosity (LIR) is a good tracer of the SF in dusty environments such as the nuclei of ULIRGs (e.g., Kennicutt & Evans 2012).”
BackgroundMethodObscured star formation in bright z ≃ 7 Lyman-break galaxies
Bowler, R., Bourne, N., Dunlop, J., McLure, R., & Mcleod, D. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2368 · Cited by 42
“We calculated the FIR star formation rate using the calibration from Kennicutt & Evans (2012), correcting to a Chabrier (2003) IMF.”
MethodSharon, C., Riechers, D., Hodge, J., Carilli, C., Walter, F., Weiss, A., Knudsen, K., & Wagg, J. (2016) · doi:10.3847/0004-637x/827/1/18 · Cited by 42
“While the uncertainties for the SFRs are inhomogeneously de- 19 We assume a CO-to-H2 conversion factor of αCO = 0.8 M (K km s−1 pc2)−1 and determine the SFRs from LFIR using the equations from Kennicutt & Evans (2012) (note that we do not correct to the 3-1100µm LTIR used there).”
BackgroundMethodInfluentialThe dense gas mass fraction in the W51 cloud and its protoclusters
Ginsburg, A., Bally, J., Battersby, C., Youngblood, A., Darling, J., Rosolowsky, E., Arce, H., & Santos, M. E. L. (2014) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201424979 · Cited by 42
“This offset is due to an age difference: the gas is tracing star formation yet to begin up to ∼ 1 Myr, while the infrared emission traces older (0-100 Myr, with a peak at 5 Myr; Kennicutt & Evans 2012) star formation.”
BackgroundMethodTHE CO-TO-H2 CONVERSION FACTOR ACROSS THE PERSEUS MOLECULAR CLOUD
Lee, M.-Y., Stanimirović, S., Wolfire, M., Shetty, R., Glover, S., Molina, F. Z., & Klessen, R. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/784/1/80 · Cited by 42
“Stars form exclusively in molecular clouds, although the question of whether molecular gas is a prerequisite or a byproduct of star formation is currently under debate (e.g., Glover & Clark 2012; Kennicutt & Evans 2012; Krumholz 2012).”
BackgroundEvidence for supernova feedback sustaining gas turbulence in nearby star-forming galaxies
Bacchini, C., Fraternali, F., Iorio, G., Pezzulli, G., Marasco, A., & Nipoti, C. (2020) · Astronomy & Astrophysics · doi:10.1051/0004-6361/202038223 · Cited by 41
“This latter takes into account only core-collapse SNe, A70, page 13 of 27 as they can be directly related to the recent star formation traced by FUV emission from massive stars younger than 100 Myr (e.g. Kennicutt & Evans 2012).”
BackgroundType Ibn Supernovae May not all Come from Massive Stars
Hosseinzadeh, G., McCully, C., Zabludoff, A., Arcavi, I., French, K. D., Howell, D., Berger, E., & Hiramatsu, D. (2019) · Astrophysical Journal · doi:10.3847/2041-8213/aafc61 · Cited by 41
“The only SN Ibn with a direct progenitor detection (albeit in outburst) was SN 2006jc; Tominaga et al. (2008) estimated that this SN came from a MZAMS = 40 M star, which would have a lifetime of ≈5 Myr.”
BackgroundInfluentialAnomalously Low-metallicity Regions in MaNGA Star-forming Galaxies: Accretion Caught in Action?
Hwang, H., Barrera-Ballesteros, J., Heckman, T., Rowlands, K., Lin, L.-W., Rodriguez-Gomez, V., Pan, H.-A., Hsieh, B.-C., Sánchez, S., Bizyaev, D., et al. (2018) · Astrophysical Journal · doi:10.3847/1538-4357/aaf7a3 · Cited by 41
“Moreover, if there were no gas replenishment from the outside, the observed rate of star formation is so high that most star-forming galaxies in the present-day Universe would soon run out of gas and cease to form stars (Kennicutt & Evans 2012).”
BackgroundWalter, F., Riechers, D., Novak, M., Decarli, R., Ferkinhoff, C., Venemans, B., Bañados, E., Bertoldi, F., Carilli, C., Fan, X.-H., et al. (2018) · Astrophysical Journal · doi:10.3847/2041-8213/aaf4fa · Cited by 41
“The resulting LIR–based star formation rates (Kennicutt & Evans 2012) are 125±14 M yr−1 (J2100–”
BackgroundChown, R., Li, C., Athanassoula, E., Li, N., Wilson, C., Lin, L., Mo, H.-J., Parker, L., & Xiao, T. (2018) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stz349 · Cited by 41
“A star formation rate (SFR) is then estimated by multiplying the Hα luminosity by 5.3 × 10−42M yr−1 (erg s−1)−1 as in Murphy et al. (2011); Hao et al. (2011); Kennicutt & Evans (2012).”
BackgroundMethodInfluentialCalibration of Ultraviolet, Mid-infrared, and Radio Star Formation Rate Indicators
Brown, M. J. I., Moustakas, J., Kennicutt, R., Bonne, N. J., Intema, H., de Gasperin, F., Boquien, M., Jarrett, T., Cluver, M., Smith, J. D., et al. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8ad2 · Cited by 41
“For a detailed discussion of these SFR indicators and their calibration, we refer the reader to Kennicutt et al. (2009), Kennicutt & Evans (2012), and references therein.”
BackgroundMethodSelf-citationTHE BRIGHTEST YOUNG STAR CLUSTERS IN NGC 5253
Calzetti, D., Johnson, K., Adamo, A., Gallagher, J., Andrews, J. E., Smith, L., Clayton, G. C., Lee, J., Sabbi, E., Úbeda, L., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/811/2/75 · Cited by 41
“The relatively small Hα and UV half–light radii, ∼100 pc and ∼160 pc, respectively (Calzetti et al. 2004), imply a high star formation rate density, ΣSFR ∼3.5 M yr−1 kpc−2, confirming the star bursting nature of the galaxy (Kennicutt & Evans 2012).”
BackgroundInfluentialSelf-citationEvolution of dwarf galaxies: a dynamical perspective
Lelli, F., Fraternali, F., & Verheijen, M. (2013) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201322658 · Cited by 41
“Other common calibrations, which assume a Kroupa IMF and different stellar evolutionary models, would give SFRs that are lower by a factor of ∼0.68 (see Kennicutt & Evans 2012).”
BackgroundInfluentialSTAR FORMATION ON SUBKILOPARSEC SCALE TRIGGERED BY NON-LINEAR PROCESSES IN NEARBY SPIRAL GALAXIES
Momose, R., Koda, J., Kennicutt, R., Egusa, F., Calzetti, D., Liu, G.-L., Meyer, J. D., Okumura, S., Scoville, N., Sawada, T., et al. (2013) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/772/1/l13 · Cited by 41
“Extensive reviews can be found in K98b and Kennicutt & Evans (2012).”
BackgroundSelf-citationCasey, C. M., Akins, H. B., Kokorev, V., McKinney, J., Cooper, O. R., Long, A. S., Franco, M., & Manning, S. M. (2024) · The Astrophysical Journal Letters · doi:10.3847/2041-8213/ad7ba7 · Cited by 48
Physical Processes in Star Formation
Girichidis, P., Offner, S., Kritsuk, A., Klessen, R., Hennebelle, P., Kruijssen, J. M. D., Krause, M., Glover, S., & Padovani, M. (2020) · Space Science Reviews · doi:10.1007/s11214-020-00693-8 · Cited by 40
“An additional complication is that the slope varies across the range of surface densities probed, with a steeper slope (N ∼ 2) at low (Σ 10 M pc−2) and high (Σ 200 M pc−2) gas surface densities (e.g. Bigiel et al. 2008; Daddi et al. 2010; Genzel et al. 2010; Kennicutt and Evans 2012), It was suggested by Krumholz et a…”
BackgroundResultInfluentialXie, Y.-X., & Ho, L. (2019) · Astrophysical Journal · doi:10.3847/1538-4357/ab4200 · Cited by 40
“Dust-corrected ultraviolet (UV) continuum emission and optical line emission ([O II] λ3727, Hα) have been used frequently to probe star formation on timescales of a few to ∼200Myr (e.g., Gallagher et al. 1989; Kennicutt 1998; Hao et al. 2011; Kennicutt & Evans 2012).”
MethodStar Clusters in Evolving Galaxies
Renaud, F. (2018) · New Astronomy Reviews · doi:10.1016/j.newar.2018.03.001 · Cited by 40
UVUDF: UV Luminosity Functions at the Cosmic High Noon
Mehta, V., Scarlata, C., Rafelski, M., Gburek, T., Teplitz, H., Alavi, A., Boylan-Kolchin, M., Finkelstein, S., Gardner, J., Grogin, N., et al. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa6259 · Cited by 40
“For models with constant star formation histories, we compute the range of expected UV-to-Hα ratios at an age of 100Myr (the generic assumption in SFR conversions, e.g., Kennicutt & Evans (2012)).”
BackgroundMethodInfluentialMOLECULAR GAS ALONG A BRIGHT Hα FILAMENT IN 2A 0335+096 REVEALED BY ALMA
Vantyghem, A., McNamara, B., Russell, H., Hogan, M., Edge, A., Nulsen, P., Fabian, A., Combes, F., Salomé, P., Baum, S., et al. (2016) · doi:10.3847/0004-637x/832/2/148 · Cited by 40
Hagen, A., Zeimann, G., Behrens, C., Ciardullo, R., Gebhardt, H. S. G., Gronwall, C., Bridge, J. S., Fox, D., Schneider, D., Trump, J., et al. (2015) · The Astrophysical Journal · doi:10.3847/0004-637x/817/1/79 · Cited by 40
The resolved star-formation relation in nearby active galactic nuclei
Casasola, V., Hunt, L., Combes, F., & García-Burillo, S. (2015) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201425313 · Cited by 40
“For a comprehensive review of the most recent SF relation studies on sub-kpc scales, we refer to Kennicutt & Evans (2012).”
MethodCLEAR: The Ionization and Chemical-enrichment Properties of Galaxies at 1.1 < z < 2.3
Papovich, C., Simons, R., Estrada-Carpenter, V., Matharu, J., Momcheva, I., Trump, J., Backhaus, B., Brammer, G., Cleri, N., Finkelstein, S., et al. (2022) · Astrophysical Journal · doi:10.3847/1538-4357/ac8058 · Cited by 39
“We compared the SED-derived SFRs for objects in our sample to SFRs estimated from dustcorrected Hβ emission measured in the grism data (assuming 6 Case-B recombination and the calibration of Kennicutt & Evans 2012).”
MethodCLEAR: Emission-line Ratios at Cosmic High Noon
Backhaus, B., Trump, J., Cleri, N., Simons, R., Momcheva, I., Papovich, C., Estrada-Carpenter, V., Finkelstein, S., Matharu, J., Ji, Z., et al. (2021) · Astrophysical Journal · doi:10.3847/1538-4357/ac3919 · Cited by 39
“The Hβ SFR is found by following the Kennicutt & Evans (2012) SFR relation for Hα and Hα/Hβ = 2.86 (assuming Case B recombination, T = 104 K, and ne = 104 cm−3; Osterbrock 1989): log(SFR)[M /yr] = log[L(Hβ)] − 40.82 (1) This SFR is not corrected for dust attenuation, and so is likely a lower limit…”
MethodInfluentialRathjen, T.-E., Naab, T., Girichidis, P., Walch, S., Wünsch, R., Dinnbier, F., Seifried, D., Klessen, R., & Glover, S. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab900 · Cited by 39
Distances and Statistics of Local Molecular Clouds in the First Galactic Quadrant
Yan, Q.-Z., Yang, J., Su, Y., Sun, Y., & Wang, C. (2020) · Astrophysical Journal · doi:10.3847/1538-4357/ab9f9c · Cited by 39
“…molecular clouds are involved in a number of physical processes occurring in the Milky Way, such as star formation (e.g., McKee & Ostriker 2007; Kennicutt & Evans 2012) and large-scale Galactic structure development (e.g., Dame et al. 1986; RomanDuval et al. 2010), many key mechanisms of…”
BackgroundContribution of starburst nuclei to the diffuse gamma-ray and neutrino flux
Peretti, E., Blasi, P., Aharonian, F., Morlino, G., & Cristofari, P. (2019) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/staa698 · Cited by 39
“We adopt as a prototype the Milky Way Global Model (MWGB) developed by Strong et al. (2010) where the HE gamma–ray flux has a spectral slope ∼ 2.7.”
BackgroundInfluentialKim, J.-G., Kim, W., & Ostriker, E. (2019) · Astrophysical Journal · doi:10.3847/1538-4357/ab3d3d · Cited by 39
“For this reason, combinations of Hα (or UV) and IR measurements have been extensively explored to calibrate the dust absorption (as well as dust attenuation of recombination emission lines) and are widely adopted in Galactic and extragalactic studies (see Kennicutt & Evans 2012 for review).”
MethodStevens, A., & Brown, T. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx1596 · Cited by 39
THE MAIN SEQUENCES OF STAR-FORMING GALAXIES AND ACTIVE GALACTIC NUCLEI AT HIGH REDSHIFT
Mancuso, C., Lapi, A., Shi, J., Cai, Z.-Y., González-Nuevo, J., B'ethermin, M., & Danese, L. (2016) · The Astrophysical Journal · doi:10.3847/1538-4357/833/2/152 · Cited by 39
“In the present paper we adopt the flat cosmology indicated by the Planck Collaboration XIII (2016) data, with round parameters: Hubble constant H0 = 100 h km s −1 Mpc−1 for h = 0.67, matter density ΩM = 0.32, baryon density Ωb = 0.05, and mass variance σ8 = 0.83 on a scale of 8 h−1 Mpc. Galaxy stellar masses and lumin…”
MethodInfluentialHony, S., Gouliermis, D., Galliano, F., Galametz, M., Cormier, D., Chen, C., Dib, S., Hughes, A., Klessen, R., Roman-Duval, J., et al. (2015) · doi:10.1093/mnras/stv107 · Cited by 39
“It is interesting to note that the rms scatter around the bestfitting power law is ±0.4dex, This is similar to the rms observed (±0.3dex) in the SK-relation of integrated ‘normal’ spiral galaxies (Kennicutt & Evans 2012).”
BackgroundResultInfluentialClarke, L., Shapley, A., Sanders, R., Topping, M., Brammer, G., Bento, T., Reddy, N., & Kehoe, E. (2024) · Astrophysical Journal · doi:10.3847/1538-4357/ad8ba4 · Cited by 38
“We also note the possibility of missing nebu-lar emission coming from optically-thick dust-enshrouded star-forming regions (Kennicutt & Evans 2012).”
Star formation and nuclear activity in luminous infrared galaxies: an infrared through radio review
P'erez-Torres, M., Mattila, S., Alonso-Herrero, A., Aalto, S., & Efstathiou, A. (2020) · The Astronomy and Astrophysics Review · doi:10.1007/s00159-020-00128-x · Cited by 38
Zooming in on Individual Star Formation: Low- and High-Mass Stars
Rosen, A., Offner, S., Sadavoy, S., Bhandare, A., Vázquez-Semadeni, E., & Ginsburg, A. (2020) · doi:10.1007/s11214-020-00688-5 · Cited by 38
“A correlation between star formation and gas surface density has been well-studied on galaxy scales (see Kennicutt & Evans, 2012, for a review), and lately extended to individual local clouds using star counts and the masses or surface densities of the host cloud (e.g., Lada et al., 2010; Heiderman…”
BackgroundALMA and HST Kiloparsec-scale Imaging of a Quasar-galaxy Merger at Z ≈ 6.2
Decarli, R., Dotti, M., Bañados, E., Farina, E., Walter, F., Carilli, C., Fan, X.-H., Mazzucchelli, C., Neeleman, M., Novak, M., et al. (2019) · Astrophysical Journal · doi:10.3847/1538-4357/ab297f · Cited by 38
“Following Kennicutt & Evans (2012), these luminosities translate into UV– based SFRs of 11, 13, and 25 M yr −1, respectively.”
BackgroundFrom ‘bathtub’ galaxy evolution models to metallicity gradients
Belfiore, F., Vincenzo, F., Maiolino, R., & Matteucci, F. (2019) · Monthly notices of the Royal Astronomical Society · doi:10.1093/mnras/stz1165 · Cited by 38
“We note that large systematics may affect these determinations, due to uncertainties in the density and geometry of the outflows and because they only refer to a specific phase of the ISM.”
BackgroundInfluentialQuerejeta, M., Schinnerer, E., Schruba, A., Murphy, E. J., Meidt, S., Usero, A., Leroy, A., Pety, J., Bigiel, F., Chevance, M., et al. (2019) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201834915 · Cited by 38
“For a fully sampled IMF, in turn, the ionising photon production rate is proportional to the rate of recent star formation (e.g. Kennicutt 1998; Kennicutt & Evans 2012).”
BackgroundMethodShe, R., Ho, L. C., & Feng, H. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa7634 · Cited by 46
“For HMXBs, their luminosity function scales with the star formation rate (Mineo et al. 2012), which itself depends on the Hα luminosity, SFR ≈ 10−41.27× LHα (erg s −1) M yr −1(Kennicutt & Evans 2012).”
BackgroundInfluentialALMA Reveals Sequential High-mass Star Formation in the G9.62+0.19 Complex
Liu, T., Lacy, J., Li, P., Wang, K., Qin, S., Zhang, Q.-Z., Kim, K.-T., Garay, G., Wu, Y.-F., Mardones, D., et al. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8d73 · Cited by 38
“5 0.1 10 4 ´ -( ) ☉ yr−1 (Kennicutt & Evans 2012).”
InfluentialThe sub-galactic and nuclear main sequences for local star-forming galaxies
Maragkoudakis, A., Zezas, A., Ashby, M., & Willner, S. (2016) · doi:10.1093/mnras/stw3180 · Cited by 38
“Numerous studies have shown that in metal-rich SFGs, polycyclic aromatic hydrocarbon (PAH) luminosity scales relatively well with SFR (Calzetti 2011; Kennicutt & Evans 2012 (KE12) and references within).”
BackgroundRoediger, J., Ferrarese, L., Côté, P., MacArthur, L., Sánchez-Janssen, R., Blakeslee, J., Peng, E., Liu, C.-Z., Muñoz, R., Cuillandre, J., et al. (2016) · The Astrophysical Journal · doi:10.3847/1538-4357/836/1/120 · Cited by 38
“…to which galaxies adhere: star formation rate versus stellar mass or gas density (Daddi et al. 2007; Elbaz et al. 2007; Noeske et al. 2007; Kennicutt & Evans 2012), rotational velocity versus luminosity or baryonic mass for disks (Courteau et al. 2007; McGaugh 2012; Lelli et al. 2016),…”
BackgroundRahmani, S., Lianou, S., & Barmby, P. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv2951 · Cited by 38
“Kennicutt & Evans (2012) reviewed star formation in the Milky Way and nearby galaxies and described that there might be a breakdown of SFR laws for small size regions.”
BackgroundGoldbaum, N., Krumholz, M., & Forbes, J. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/814/2/131 · Cited by 38
“Thus the inner parts of galaxies will become gas-depleted and cease star formation unless fresh gas is supplied at an equal rate, which for L∗ galaxies is a few M yr −1 (Kennicutt & Evans 2012).”
BackgroundKrause, M., Diehl, R., Bagetakos, Y., Brinks, E., Burkert, A., Gerhard, O., Greiner, J., Kretschmer, K., & Siegert, T. (2015) · doi:10.1051/0004-6361/201525847 · Cited by 38
“Uncertainties in this parameter are substantial (compare also Kennicutt & Evans 2012).”
BackgroundDRIVERS OF H i TURBULENCE IN DWARF GALAXIES
Stilp, A., Dalcanton, J., Skillman, E., Warren, S., Ott, J., & Koribalski, B. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/773/2/88 · Cited by 38
“Compared with Hα, FUV estimates of star formation are more likely to provide correct estimates of the SFR as they rely on both O and B stars instead of only those with M & 15 M (Lee et al. 2011; Kennicutt & Evans 2012).”
MethodChastenet, J., Sutter, J., Sandstrom, K., Belfiore, F., Egorov, O., Larson, K., Leroy, A., Liu, D.-Z., Rosolowsky, E., Thilker, D., et al. (2023) · Astrophysical Journal Letters · doi:10.3847/2041-8213/acac94 · Cited by 37
“…21 cm observations for NGC 1365, so we assume it to have a uniform neutral gas surface density of 8Me pc −2 everywhere, based on the observed flatness of the atomic gas distribution in the disks of galaxies (e.g., Schruba et al. 2011; Bigiel & Blitz 2012; Kennicutt & Evans 2012; Wong et al. 2013).”
BackgroundPHANGS–JWST First Results: Variations in PAH Fraction as a Function of ISM Phase and Metallicity
Chastenet, J., Sutter, J., Sandstrom, K., Belfiore, F., Egorov, O., Larson, K., Leroy, A., Liu, D.-Z., Rosolowsky, E., Thilker, D., et al. (2023) · Astrophysical Journal Letters · doi:10.3847/2041-8213/acadd7 · Cited by 37
“Based on the observed flatness of the atomic gas surface density over the inner parts of galaxy disks (e.g., Schruba et al. 2011; Bigiel & Blitz 2012; Kennicutt & Evans 2012; Wong et al. 2013), we assume that the atomic gas has a flat distribution with ΣHI= 8Me pc −2 (including helium).”
BackgroundIlluminating the Dark Side of Cosmic Star Formation Two Billion Years after the Big Bang
Talia, M., Cimatti, A., Giulietti, M., Zamorani, G., B'ethermin, M., Faisst, A., Fèvre, O. L., & Smolčić, V. (2020) · Astrophysical Journal · doi:10.3847/1538-4357/abd6e3 · Cited by 37
Chung, D., Viero, M., Church, S., Wechsler, R., Alvarez, M. A., Bond, J., Breysse, P., Cleary, K., Eriksen, H., Foss, M. K., et al. (2018) · Astrophysical Journal · doi:10.3847/1538-4357/ab0027 · Cited by 37
“Before dust absorption and other attenuation mechanisms, the Lyα line is 8.7 times stronger (for case B recombination) than Hα, a frequently chosen emission-line tracer of star formation activity(Kennicutt & Evans 2012).”
BackgroundInfluentialTesting star formation laws in a starburst galaxy at redshift 3 resolved with ALMA
Sharda, P., Federrath, C., da Cunha, E., Swinbank, M., & Dye, S. (2017) · doi:10.1093/mnras/sty886 · Cited by 37
“Although this is quite high compared to nearby galaxies (see Kennicutt & Evans (2012) and references therein), it falls in the range of Mach numbers associated with starburst galaxies (Gao & Solomon 2004; Bouché et al. 2007; Cresci et al. 2009; Förster Schreiber et al. 2009; Tacconi et al. 2010).”
Background
Metadata
- Authors
- Kennicutt, R. C., & Evans, N. J.
- Affiliations
- University of Cambridge (GB)
- European Southern Observatory (CL)
- Venue
- Annual Review of Astronomy and Astrophysics
- Publisher
- Annual Reviews
- Published
- 2012-09-22
- Volume
- 50
- Issue
- 1
- Pages
- 531-608
- ISSN
- 0066-4146 (ISSN-L)
- 1545-4282
- OpenAlex
- W2123267088
- Cited by
- 2,902
- References
- 493
- Citations by year
- 2026: 174 · 2025: 239 · 2024: 287 · 2023: 236 · 2022: 257 · 2021: 208 · 2020: 226 · 2019: 227 · 2018: 232 · 2017: 203 · 2016: 185 · 2015: 175 · 2014: 137 · 2013: 102 · 2012: 13
- FWCI
- 11.04
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Annual Review of Astronomy and Astrophysics (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- arXiv (Cornell University)
- Funders
- Science and Technology Facilities Council (ST/H00243X/1, ST/J001538/1)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astrophysics and Star Formation Studies
- 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
- Keywords
- star formation, Milky Way, nearby galaxies, star formation rate, gas content, molecular clouds
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