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Ram pressure and returning gas

Ram pressure and returning gas · L3

Why global colour needs a history

A galaxy’s colour depends on which generations of stars are shining and on the dust their light crosses. Gas displacement supplies neither history by itself. To calculate global colour, add the light of each generation with its own age and initial mass.

A small young generation can change the light

A massive young star shines brightly and has a short lifetime. Long-lived, lower-mass stars keep contributing after its bright blue light has faded. A population therefore changes colour as it ages even if no star moves out of the aperture.

An SSP, or simple stellar population, is an ideal group born at one time with one specified chemical composition and a distribution of stellar birth masses. Its spectrum gives luminosity as a function of age. Multiplying that spectrum by an initially formed mass tells us how bright that generation is.

Our illustrative input is one fixed solar-labelled BC03/EzGal model with a Salpeter birth-mass distribution. It is normalized per initially formed solar mass. Its later remaining stellar mass is different because stars shed material as they evolve; multiplying by that remaining fraction again would apply mass loss twice.

Reading: Bruzual & Charlot, Stellar population synthesis at the resolution of 2003, astro-ph/0309134v1 · Original fixed-slice and static-restoring-force materials

Add generations at their present ages

Suppose the observation occurs TT million years after the common initial state. Stars born at an earlier time now have age TT minus that birth time. Multiply their present-age spectrum by the mass born during that interval, then add all birth intervals. This weighted sum is called a convolution.

The old population starts at an age of 10000 million years and ages along with the young population. Its initial formed mass is chosen using the fixed model’s remaining-mass convention at that initial age. The gravitational potential remains fixed in the gas exercise; this postprocessing does not feed stellar mass loss back into the gas.

There are two young-star input histories: continuing exponential consumption, and the same history stopped after 650 million years. The latter is a deliberately imposed experiment. The wind model did not predict this global shutdown.

Lν(T)=Moldℓν(aold+T)+∫0Tψform(u)ℓν(T−u) du\begin{aligned}L_\nu(T)&=M_{\rm old}\ell_\nu(a_{\rm old}+T)\\&\quad+\int_0^T\psi_{\rm form}(u)\ell_\nu(T-u)\,du\end{aligned}
ℓν\ell_\nu is luminosity per Hz per initially formed solar mass. ψform\psi_{\rm form} is initially formed mass per unit time. The time unit used for the rate and the integral must agree.

Reading: Original fixed-slice and static-restoring-force materials · Bruzual & Charlot, Stellar population synthesis at the resolution of 2003, astro-ph/0309134v1

A filter counts a weighted part of the spectrum

A broadband filter admits a continuous range of wavelengths with different transmission weights. The g band samples a bluer region than r. For a photon-response curve, averaging a spectrum per unit frequency requires the corresponding wavelength weight; a plain unweighted arithmetic mean generally gives the wrong band flux.

Once the two band luminosities use the same AB convention, their ratio gives g−rg-r. Larger g−rg-r means relatively less blue-band light. Scaling every stellar formation mass by the same factor changes the total brightness but leaves the colour ratio unchanged.

The native EzGal file stores a rest-frame flux convention at 10 parsecs. Multiplying by the area of that sphere gives luminosity per Hz. An option labelled luminosity in the original source additionally multiplies by frequency; that quantity is frequency times luminosity per Hz, so its name alone is not enough to identify units.

g−r=−2.5log⁡10 ⁣(⟨Lν⟩g⟨Lν⟩r)g-r=-2.5\log_{10}\!\left(\frac{\langle L_\nu\rangle_g}{\langle L_\nu\rangle_r}\right)
The shared AB zero point and the same distance factor cancel in the difference. The independent package recomputes this ratio from the supplied own band luminosities.
Four exact global g-r samples for continuing and imposed-shutdown histories with no dust
Own global-band ratios at exact elapsed ages 00, 325325, 650650 and 1300 Myr1300\,\mathrm{Myr}, no dust. Points show the separately specified histories, without assigning stellar colours to gas positions. Original spectra are not reproduced here. Open the full figure

Reading: Original fixed-slice and static-restoring-force materials

Dust changes colour without changing stellar ages

A foreground dust screen removes different fractions of light at different wavelengths. In the chosen empirical Calzetti prescription the bluer light is more strongly attenuated over these optical bands, so changing the screen can redden the same population.

The three specified screen strengths have colour-excess parameters 0, 0.2 and 0.4. They are inputs. Applying the screen does not infer its strength from a galaxy image, and the attenuation curve does not determine how much new dust the tail produces.

We apply this prescription only across its declared 1200–22000 Angstrom wavelength range. All used filter supports are covered, including the supplied response tails. There is no invented continuation outside that range or a new infrared emission calculation.

Reading: Calzetti et al., The Dust Content and Opacity of Actively Star-Forming Galaxies, astro-ph/9911459v1 / ApJ533 (2000) · Original fixed-slice and static-restoring-force materials

Use global light for the question it can answer

The public subset shows four exact ages:0, 325, 650 and 1300 million years. Points compare the continuing and separately stopped histories; they do not assign a colour to each visible gas sample. The independent package repeats the colour ratio, while the original native-spectrum convolution has its own source and numerical checks.

All five wind paths share the same global gas-consumption history and therefore the same global light in this experiment. A disk-only SFR curve cannot simply be substituted for a stellar population inside today’s disk: stars born earlier can later change position, and the gas birth inventories do not track those positions.

A colour change can motivate a history question, but age, recent formation and dust can produce overlapping effects. To infer a shutdown time, specify a population model, a dust model and data with enough independent information to compare them. First decide which stars and which region the colour actually includes.

Reading: Original fixed-slice and static-restoring-force materials · Bruzual & Charlot, Stellar population synthesis at the resolution of 2003, astro-ph/0309134v1

Exercises and explained answers

  1. Double both the old and young initially formed masses. What happens to g−rg-r?

    Read the explanation

    The two band luminosities double, their ratio stays the same, and g−rg-r is unchanged. The object becomes brighter.

  2. Could a redder global colour prove that wind removed all star-forming fuel?

    Read the explanation

    No. Older populations or a stronger dust screen can also redden the light. In this controlled exercise the wind paths have identical global formation histories.

Try the prediction

Follow gas lifted by a cluster wind

  1. Open the separate global-light experiment and change dust while retaining the same path and age.
  2. Compare continuing and imposed-shutdown colours at an age after 650 Myr, then check that changing q leaves both global colours unchanged.

Sources and calculation scope

  1. Bruzual & Charlot, Stellar population synthesis at the resolution of 2003, astro-ph/0309134v1

    Section 2.3 supplies the initially formed-mass convention and population convolution. The fixed numerical input is easyGalaxy commit 133c62b383fae964701b673e62517293161b41d5, tests/data/bc03_ssp_z_0.02_salp.model, SHA5b2e2f9f2ecdbbd329ff4993f84a5d4bd7f8bfef6877b38d2042e9a0cf96e1fd. Its Salpeter label is retained; an unspecified track release is not invented.

  2. Calzetti et al., The Dust Content and Opacity of Actively Star-Forming Galaxies, astro-ph/9911459v1 / ApJ533 (2000)

    Empirical attenuation context for the separately specified screens. The own calculation restricts the prescription to 1200–22000 Angstrom; it does not fit a measured dust parameter or solve infrared re-emission.

  3. Original fixed-slice and static-restoring-force materials

    Our five exact synthetic slices with sixty-four sheets and thirteen fields, initial common arrays, two global-light histories/three screens/four-age band subset, independent Python static maxima and mask/energy/colour diagnostics. Original trajectory and native SSP production are distinct earlier calculations; this offline package repeats diagnostics and band ratios. No browser Engine, original FITS/SED, paper, author code or observed-galaxy data is included.

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