1 The cosmic distance scale Distance information is often crucial to understand the physics of astrophysical objects. This requires knowing the basic properties of such an object, like its size, its environment, its location in space... There are essentially two ways to derive distances to astronomical objects, through absolute distance estimators or through relative distance estimators Absolute distance estimators Objects for whose distance can be measured directly. They have physical properties which allow such a measurement. Examples are pulsating stars, supernovae atmospheres, gravitational lensing time delays from multiple quasar images, etc. Relative distance estimators These (ultimately) depend on directly measured distances, and are based on the existence of types of objects that share the same intrinsic luminosity (and whose distance has been determined somehow).
2 For example, there are types of stars that have all the same intrinsic luminosity. If the distance to a sample of these objects has been measured directly (e.g. through trigonometric parallax), then we can use these to determine the distance to a nearby galaxy by comparing their apparent brightness to those in the Milky Way. Essentially we use that log(d 1 /D 2 ) = 1/5 * [(m 1 m 2 ) - (A 1 A 2 )] where D 1 is the distance to system 1, D 2 is the distance to system 2, m 1 is the apparent magnitudes of stars in S 1 and S 2 respectively, and A 1 and A 2 corrects for the absorption towards the sources in S 1 and S 2. Stars or objects which have the same intrinsic luminosity are known as standard candles. If the distance to such a standard candle has been measured directly, then the relative distances will have been anchored to an absolute distance scale.
3 Plan of the day Distance determination for nearby objects (Few) Examples of absolute distance estimators (Many more) Examples of relative distance estimators
4 Brief review of distance determination in the Trigonometric parallax: Solar Neighbourhood Measures the displacement in position of a star on the celestial sphere as the Earth moves around the Sun. This angular displacement is dependent on the distance to the star: Π [arcsec] = 1/d[pc]. This method is currently restricted to nearby stars, within roughly 200 pc, for which the relative error in distance is of the order of 20%. Moving cluster method: All stars in an open cluster have the same velocity vector, which projected onto the celestial sphere is oriented towards a convergence point. The measurement of the proper motion, radial velocity and the convergence point the provides the distance to the cluster. Can be applied to nearby clusters spanning a wide angle on the sky, and for which proper motions can be accurately measured.
5 Absolute distance estimators These estimators can used for very distant objects, and so are not tied to the local calibration of distances using the nearby stars. They provide an additional check for the scales built up from relative distance indicators. This implies that a more robust distance scale is available when the two types of estimators are combined. The Baade-Wesselink method The luminosity of a star is given by L = 4 π R 2 σ T 4 eff Therefore, if the radius R is measured, and the T eff is obtained from the spectrum or color of a star, and the apparent magnitude is known then it would be possible to derive its distance. The most direct way of measuring the radii of stars is by using eclipsing binaries. However, these objects are not very common, and hence not very useful in constructing the ladder of distance scales.
6 It is possible to use this method on variable stars such as cepheids or RR Lyrae. The lines in the spectrum of such a star show periodic shifts that vary with the same period as the star's brightness. These shifts are due to the expansion and contraction of the atmosphere of the star. The amount by which the size of a star varies between t 1 and t 0 can be obtained by integrating the line-of-sight velocity in this time interval r = -p t0 t1 v los (t) dt The negative sign is due to the fact that when r increases the lines are blueshifted, indicating a negative radial velocity, and the other way round. The factor p takes into account that the line of sight velocity we measure comes from different regions from the stellar disc, and so it is not exactly equal to the expansion velocity of the atmosphere.
7 Thus if the star has a radius r 0 at t 0, and r 1 at t 1, the change in the bolometric apparent magnitude will be m 1 m 0 = M 1 M 0 = -2.5 log(l 1 /L 0 ) = -5 log(r 1 /r 0 ) - 10 log(t 1 /T 0 ) Since r 1 = r 0 + r, if we measure T 0 and T 1, and r using the lineshifts in the spectrum, we can solve for r 0, and thereby derive its total luminosity and so its distance. We may choose to compare two epochs when the colour of the star is the same, that is when T 0 = T 1. In that case, the above equation becomes r 0 = H r/(1 H) where H = 10 5(m 1 m0) This method relies on some simplifying assumptions which may not be fully correct v los corresponds to expanding atmosphere. But lines detected may originate from different layers moving at different speeds the stellar oscillations may be not purely radial A one-to-one relation between the colour of a star and its Teff. E.g., variable stars observed in different bands do not vary in the same way with time. Need to use realistic models of the atmospheres of variable stars to correct for systematic effects.
8 Distances from time delays If an object changes its brightness in time we may measure its distance D by the delay in the arrival of the time-varying signal. If the physical dimension of the source is d, then d ~ c t. If it is also possible to measure an angular scale, θ associated to the source size d then θ = d/d, and D ~ c t/θ Example: the ring around SN1987A Observations made by the IUE (a UV satellite) showed emission lines from highly ionized atoms in the spectrum of SN1987A. These lines were detected t 0 = 90 days after the initial explosion. Their intensity increased and reached a maximum at t 1 = 400 days. The simplest explanation is that the emission lines come from material that is located at some distance from the supernova. The presence of such material has been indeed observed, and is distributed in an inclined ring structure.
9 The delay in the detection of the first emission lines and their maximum intensity can be attributed to different light-paths (from B and C). t o = R ring /c (1 sin i) and t 1 = R ring /c (1 + sin i) Combining the equations and using the values of t 0 and t 1, one obtains R ring = / pc and i=42+/- 5 deg. Since the angular size of the ring is θ = / arcsec, we derive a distance of 52 +/- 3 kpc to the supernova (and hence to the LMC).
10 Relative distance indicators Luminosities of variable stars: RR Lyrae, cepheids Local Group, nearby groups Luminosity functions of globular clusters and planetary nebulae galaxies and nearby clusters Novae and supernovae galaxies and cosmological distances Kinematics of galaxies: Tully-Fisher and D n σ galaxies, groups of galaxies and clusters
11 Luminosities of variable stars The luminosities of some pulsating variables can be determined accurately from their periods. For example cepheids obey the relation <M V > ~ log (P/10 days) 4.13 with a scatter of 0.3 mag. This relation has been calibrated for cepheids whose distances could be measured directly, for example through trigonometric parallaxes and the Baade-Wesselink method. Cepheids have absolute magnitudes M V ~ - 3, so that they can be observed to distance moduli of (m V M V ) ~ 25 from the ground and (m V M V ) ~ 28 using HST. This allows one to reach the nearest galaxy cluster Virgo. Cepheids are particularly useful because of their characteristic light curves, implying that they can be identified unambiguously.
12 Another example are RR Lyrae stars whose absolute magnitude is M V ~ 0.6. This has been derived from nearby RR Lyrae (not very many because they are characteristic of metal-poor populations) for which the trigonometric parallax could be measured; and also using the main sequence fitting method for globular clusters, which in turn is based on the distance scale to local subdwarf stars. RR Lyrae are less bright, and do not allow us to measure distances beyond the Local Group.
13 Luminosity functions Objects that have a spread in intrinsic luminosities cannot be used as standard candles. However, if the luminosity function of these objects is universal, i.e. it does not vary from system to system, we can compare the distribution of apparent luminosities to derive a relative distance to the systems. By luminosity function we mean the number of objects with absolute magnitude in a given range (i.e. the distribution of absolute magnitudes). Globular clusters The average luminosity of the globular clusters around the Milky Way, the LMC and M31 seems to be the same. Hence we may assume that this should also apply to other systems. We can use the average luminosity of the globular clusters as a standard candle, and hence to derive the relative distance of a given host galaxy. This method is often used to derive distances to elliptical galaxies, because the globular clusters are very easy to identify in this case.
14 The globular cluster luminosity function is very similar in all galaxies φ GC exp[-(m <m GC >) 2 /(2 σ GC2 )] (N.B. we have accurate measurements of the absolute magnitude only for the globular clusters in the Milky Way). LF of globular clusters in four E in Virgo.. By fitting this functional formed to the apparent magnitudes of globular clusters around a given galaxy we can obtain <m GC >. The comparison of this quantity for different galaxies will give us a measure of their relative distances Note that to estimate <m GC > reliably implies that the observations should reach faint enough levels so that the turn-over is clearly visible in the distribution. So far, this method has allowed us to measure distances to the Coma cluster.
15 Luminosity functions: Planetary Nebulae Planetary nebulae are easily identifiable through their characteristic emission forbidden lines at 5007 A. They are very common in all types of galaxies, and so their luminosity function can be accurately determined for each host system. The PN luminosity function is very similar in all galaxies φ PN (m) e m [1 e 3(m PN cut m) ] There are no PN brighter than m PN cut, a cut-off apparent magnitude. The fact that there is such an abrupt cut-off at bright end implies that this method can be applied even when a limited number of PN (only the brightest) have been observed around a given system. The maximum luminosity in the PNLF in the bulge of M31 occurs at ± If we adopt a distance of 740 ± 40 kpc (derived from cepheids), then M cut PN = -4.6 ± 0.1.
16 Novae Novae are very bright, and reach peak absolute magnitudes of M v ~ -7, which makes them ideal to probe very large distances. Novae in our Galaxy are sufficiently close that it is possible to derive their distances directly, using the expansion of their shells. If a shell expands with a velocity v exp - measurable from the Doppler shifts in spectral lines-, after a time t, this shell will have an angular size δθ which corresponds to a physical dimension v exp t. Therefore the distance to the novae is v exp t/ δθ. The luminosities derived for novae in our Galaxy show that they are not standard candles, since their peak absolute magnitude range from -4.8 to However, they have a characteristic rate of decline in brightness M V (max) = log(t 2 /day) where M V (max) is the peak magnitude of the novae, and t 2 is the time the novae took to decline in brightness by two magnitudes from its maximum.
17 Supernovae Supernovae type Ia have very similar properties, which is not surprising given that they originate in essentially identical systems (C/O white dwarf that by accretion from a binary companion has reached a mass of 1.38 M sun, which leads to an instability and triggers the explosion.) They are ideal standard candles because of their extreme intrinsic luminosities, implying that they can be observed to cosmological distances M v (max) = /
18 Distances from galaxy kinematics Galaxies themselves are not standard candles, since their brightness vary strongly from system to system (as for example, evidenced by the population of galaxies in distant clusters). However, they obey certain scaling laws: the more massive a galaxy is, the larger its intrinsic luminosity. The more massive the galaxy, the larger the average speed of its stars. (This derives from the virial theorem). Tully-Fisher relation The luminosity of a spiral galaxy correlates strongly with its rotational velocity.
19 The rotational velocity of a spiral galaxy can be measured from the HI integrated spectrum. The HI gas in a spiral follows very closely circular orbits at a speed V c. If the galaxy is inclined at an angle i to the line of sight, the observed line of sight velocity will vary from + V c sin i to - V c sin i relative to the systemic velocity of the galaxy. This results in a double horn line profile. Thus measuring the width of the line we get a direct estimate of the circular velocity. Conventionally, this width is measured by finding the points in the line wings where the intensity has dropped by 20% of the peak value. The difference in Doppler shift between these 2 points is W 20. W 20 needs to be corrected for 2 effects. The first one is that HI does not follow perfectly circular orbits, but has some random motion, whose effect is to broaden the observed lines. This can be estimated to be typically 10 km/s. The second effect is due to the inclination. The width that we measure is essentially 2 V c sin i. Therefore, the quantity W R = (W 20 -W rand )/sin i is an inclination independent measure of the circular velocity of a spiral galaxy.
20 The best bands to measure the brightness of a spiral galaxy are the infrared bands. The reason is twofold: spiral galaxies have large amounts of dust, which produce extinction. The effect of extinction in the infrared is very small the light will be dominated by old stars, which are more representative of the overall stellar populations. The observed light does not depend therefore on current star formation activity. The relations obtained are M H = 9.5 (log W R 2.5) ± 0.08 M I = 8.72(log W R 2.5) ± 0.1 and have been calibrated using cepheid distances.
21 The D n - σ relation Elliptical galaxies also follow scaling laws which relate their size, velocity dispersion and luminosity (or surface brightness). The most useful relation to measure distances to elliptical galaxies is the D n - σ relation
22 The parameter D n is the diameter within which the mean surface brightness is µ n = mag/arcsec 2 in the blue. σ is the central velocity dispersion. The calibrated relation is D n = 2.05 (σ/100 km/s) 1.33 kpc To obtain the distance we only need to compare the angular size of D n to the scale predicted by this equation. There is a 15% scatter in the relation from galaxy to galaxy, which will imply a 15% intrinsic uncertainty in the distance. However, if one is interested in measuring the distance to a cluster of galaxies, the uncertainty to the cluster distance can be reduced by observing large numbers of elliptical galaxies.
24 Distances within the Local Group Distance to the Galactic center The only absolute distance estimator for the Galactic center are the water masers in star forming regions in SgrB2. In this case, we use the statistical parallax method: radial velocity and proper motions. The relative distance estimators that can be used are RR Lyrae in globular clusters (one looks for the maximum density of halo globular clusters. This point should coincide with the location of the Galactic center). RR Lyrae in the bulge Cepheids water masers 7.2 +/-.7 RR Lyrae 7.8 +/- 0.4 globular clusters 8.0 +/- 0.8 cepheids 8.0 +/- 0.5
25 Distance to the LMC: 50 +/- 2 kpc (It is the extragalactic zero-point of the distance scale) The absolute distance estimator for the LMC is SN 1987A using timedelay arguments, or the Baade-Wesselink method. The relative distance estimators that can be used are Main sequence fitting of globular clusters RR Lyrae stars SN 1987 A time delay Cepheids SN 1987A Baade- Wesselink RR Lyrae Cepheids main sequence fitting 52 +/- 3 kpc 55 +/- 5 kpc 44 +/- 2 kpc 50 +/- 2 kpc 50 +/- 5 kpc
26 Distance to the M31: 740 +/- 40 kpc Its distance is always referred to the LMC Comparison of cepheids in LMC and M31 show that the latter lies /- 0.8 times farther away. Comparison of RR Lyraes give a distance ratio of 15 +/- 1. The PN luminosity function also provides a distance ratio wrt LMC of 15 +/- 1. The peak in the GCLF can be compared to that of the Milky Way, and the distance derived in this way is 700 +/- 60 kpc. This is directly calibrated wrt Milky rather than the LMC. The fact that there is such good agreement between different estimators and zero-points gives good confidence that the scale is correct. Novae RR Lyrae Cepheids 710 +/- 80 kpc 750 +/- 50 kpc 760 +/- 50 kpc PNLF GCLF 750 +/- 50 kpc 700 +/- 60 kpc
27 Distances beyond the Local Group Different methods can be applied to nearby galaxies just outside the Local Group. These methods show good agreement for distances less than ~ 20 Mpc. PNLF and GCLF are generally in good agreement. Distances using the Tully-Fisher for spiral galaxies in clusters are in worse agreement with those distances derived from elliptical galaxies, which could be related to their different physical location in the clusters. The distance to the Virgo cluster is crucial in the extragalactic distance scale: nearest galaxy cluster contains large numbers of spirals and ellipticals has been the site of a few SN it has been recently possible to observe cepheids, and hence to derive a distance which involves less intermediate calibrations it is a fairly average type of cluster: distances beyond it are referred to it.
28 Comparison of various distance determination methods for galaxies in the Virgo cluster
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