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A spatially resolved study of ionized regions in galaxies at different ...

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2.4. Discussion 35<br />

are some traces <strong>of</strong> the blue-plume <strong>at</strong> M V = −9, <strong>in</strong>dic<strong>at</strong><strong>in</strong>g ongo<strong>in</strong>g star form<strong>at</strong>ion. A strip<br />

<strong>of</strong> stars follow<strong>in</strong>g a p<strong>at</strong>ch from [0.6,25] to [1.1,22.5] form the red giant branch.<br />

Mass <strong>in</strong> stars<br />

In order to quantify the rel<strong>at</strong>ive importance <strong>of</strong> the present burst to the star form<strong>at</strong>ion<br />

history dur<strong>in</strong>g the previous 100 Myr <strong>in</strong> NGC 5471, we make a rough estim<strong>at</strong>e <strong>of</strong> the stellar<br />

mass from the CMD. We follow three <strong>different</strong> approaches. One method consists <strong>in</strong> assign<strong>in</strong>g<br />

a mass to each <strong>of</strong> the stars <strong>in</strong> the CMD, correspond<strong>in</strong>g to the closest isochrone, thus count<strong>in</strong>g<br />

the stars <strong>in</strong> the mass range 6-55 M ⊙ and <strong>in</strong>tegr<strong>at</strong><strong>in</strong>g a Salpeter IMF <strong>in</strong> the mass range 1-100<br />

M ⊙ . The result <strong>of</strong> this calcul<strong>at</strong>ion gives ∼ 2 × 10 5 M ⊙ . The second method is as follows:<br />

first we assign a mean stellar mass <strong>of</strong> 6 M ⊙ to the stars <strong>in</strong> the most popul<strong>at</strong>ed b<strong>in</strong> <strong>of</strong> the<br />

lum<strong>in</strong>osity function, m 547M = 23.5. This mass is then scaled up by the r<strong>at</strong>io <strong>of</strong> the total<br />

m 547M <strong>of</strong> NGC 5471 to the magnitude <strong>of</strong> the b<strong>in</strong> m 547M = 23.5. The result<strong>in</strong>g mass is used<br />

to normalize the IMF <strong>at</strong> the b<strong>in</strong> correspond<strong>in</strong>g to 6 M ⊙ . The result <strong>of</strong> <strong>in</strong>tegr<strong>at</strong><strong>in</strong>g a Salpeter<br />

IMF <strong>in</strong> the range 1-100 M ⊙ thus normalized gives a value <strong>of</strong> ∼ 5 × 10 5 M ⊙ .<br />

A third <strong>in</strong>dependent method to estim<strong>at</strong>e the mass is based on the fit <strong>of</strong> the CMD by<br />

means <strong>of</strong> Hess diagrams. We have used the code STARFISH (Harris and Zaritsky, 2001,<br />

2002) to f<strong>in</strong>d a best fit to the CMD by a l<strong>in</strong>ear comb<strong>in</strong><strong>at</strong>ion <strong>of</strong> Hess diagrams <strong>at</strong> <strong>different</strong><br />

ages. The solution found by the code is only sensitive to stars <strong>in</strong> two age b<strong>in</strong>s <strong>in</strong> the range<br />

50-100 Myr, giv<strong>in</strong>g an average SFR ∼ 0.01 M ⊙ yr −1 . Integr<strong>at</strong><strong>in</strong>g this SFR for 50 Myr gives a<br />

total mass <strong>of</strong> ∼ 5 × 10 5 M ⊙ , <strong>in</strong> the same range <strong>of</strong> values found by the previous two methods.<br />

Although these methods give only an order <strong>of</strong> magnitude estim<strong>at</strong>e, we can conclude th<strong>at</strong><br />

the <strong>in</strong>tegr<strong>at</strong>ed mass <strong>of</strong> stars formed <strong>in</strong> the past 10-100 Myr is <strong>of</strong> the order <strong>of</strong> magnitude<br />

or less than the current star form<strong>at</strong>ion event, th<strong>at</strong> we have calcul<strong>at</strong>ed above as ∼ 10 6 M ⊙ .<br />

If the star form<strong>at</strong>ion proceeds <strong>in</strong> an isol<strong>at</strong>ed gas cloud, we would expect th<strong>at</strong> the r<strong>at</strong>e <strong>at</strong><br />

which stars form would decrease with time, as less gas is left available to form new stars.<br />

This is wh<strong>at</strong> is observed <strong>in</strong> many giant H ii <strong>regions</strong> with two or more gener<strong>at</strong>ions <strong>of</strong> star<br />

form<strong>at</strong>ion, where the l<strong>at</strong>est event is less massive than the previous. In the case <strong>of</strong> NGC 5471<br />

the results from the <strong>in</strong>tegr<strong>at</strong>ed photometry and from the CMD <strong>in</strong>dic<strong>at</strong>e th<strong>at</strong> the current star<br />

form<strong>in</strong>g event is more massive than the r<strong>at</strong>e <strong>at</strong> which stars have formed dur<strong>in</strong>g the previous<br />

10-100 Myr. This we can understand <strong>in</strong> the context <strong>of</strong> the large H i spiral arm <strong>in</strong> which the<br />

region is immersed, as mentioned above. In this respect, Waller et al. (1997) conclude from a<br />

morphological <strong>study</strong> <strong>of</strong> M101 th<strong>at</strong> NGC 5471 may be the result <strong>of</strong> tidal <strong>in</strong>teractions <strong>of</strong> M101<br />

with the nearby <strong>galaxies</strong> NGC 5477 and NGC 5474 <strong>in</strong> the time <strong>in</strong>terval 100-1000 Myr ago.<br />

Sp<strong>at</strong>ial distribution <strong>of</strong> the star form<strong>at</strong>ion history<br />

Given the long dur<strong>at</strong>ion <strong>of</strong> the star form<strong>at</strong>ion <strong>in</strong> NGC 5471, ∼ 100 Myr, it is n<strong>at</strong>ural<br />

to question the sp<strong>at</strong>ial loc<strong>at</strong>ion <strong>of</strong> the star form<strong>at</strong>ion through time along the extent <strong>of</strong> the

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