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Astronomy & Astrophysics manuscript no. 8189 October 9, 2007

c ESO 2007

Weak magnetic fields in Ap/Bp stars

,

Evidence for a dipole field lower limit and a tentative interpretation of the magnetic dichotomy

arXiv:0710.1554v1 [astro-ph] 8 Oct 2007

M. Auriere1 , G.A. Wade2 , J. Silvester2,3 , F. Lignieres1 , S. Bagnulo4 , K. Bale2 , B. Dintrans1 , J.F. Donati1 , C.P. Folsom2 , ` ` 5 , A. Hui Bon Hoa1 , S. Jeffers6 , N. Johnson2 , J.D. Landstreet7 , A. Lebre8 , T. Lueftinger5 , S. Marsden9 , M. Gruberbauer ` D. Mouillet1 , S. Naseri1 , F. Paletou1 , P. Petit1 , J. Power2 , F. Rincon1 , S. Strasser10 , N. Toque11 Ä
1 2 3 4 5 6 7 8 9 10 11

Laboratoire d'Astrophysique de Toulouse- Tarbes, Universite Paul Sabatier, CNRS, Observatoire Midi-Pyrenees, 57 Avenue Ä ÄÄ d'Azereix, 65008 Tarbes, France Department of Physics, Royal Military College of Canada, PO Box 17000, Station 'Forces', Kingston, Ontario, Canada K7K 4B4 Department of Physics, Queen's University, Kingston, Ontario, Canada Armagh Observatory, College Hill, Armagh BT61 9DG, Northern Ireland Institut fur Astronomy, University of Vienna, Turkenschanzstrasse 17, A-1180 Wien, Austria ? ? Sterrekundig Instituut Utrecht, Universiteit Utrecht, PO Box 80000, 3508 TA Utrecht, The Netherlands Department of Physics & Astronomy, The University of Western Ontario, London, Ontario, Canada, N6A 3K7 GRAAL, Universite Montpellier II, CNRS, 62 Place Eugene Bataillon, 34095 Montpellier, France Ä ` Anglo-Australian Observatory, PO Box 296, Epping, NSW 1710, Australia Department of Astronomy, University of Minnesota, 116 Church Street, S.E., Minnepolis 55455, USA Department of Physics and Astronomy, Saint Mary's University, 923 Robie Street, Halifax, Nova Scotia, B3H3C3, Canada

Received September 15, 1996; accepted March 16, 1997
ABSTRACT

Aims. We have investigated a sample of 28 well-known spectroscopically-identified magnetic Ap/Bp stars, with weak, poorlydetermined or previously undetected magnetic fields. The aim of this study is to explore the weak part of the magnetic field distribution of Ap/Bp stars. Methods. Using the MuSiCoS and NARVAL spectropolarimeters at Telescope Bernard Lyot (Observatoire du Pic du Midi, France) Ä and the cross-correlation technique Least Squares Deconvolution (LSD), we have obtained 282 LSD Stokes V signatures of our 28 sample stars, in order to detect the magnetic field and to infer its longitudinal component with high precision (median = 40 G). Results. For the 28 studied stars, we have obtained 27 detections of Stokes V Zeeman signatures from the MuSiCoS observations. Detection of the Stokes V signature of the 28th star (HD 32650) was obtained during science demonstration time of the new NARVAL spectropolarimeter at Pic du Midi. This result shows clearly that when observed with sufficient precision, all firmly classified Ap/Bp stars show detectable surface magnetic fields. Furthermore, all detected magnetic fields correspond to longitudinal fields which are significantly greater than some tens of G. To better characterise the surface magnetic field intensities and geometries of the sample, we have phased the longitudinal field measurements of each star using new and previously-published rotational periods, and modeled them to infer the dipolar field intensity and the magnetic obliquity. The distribution of derived dipole strengths for these stars exhibits a plateau at about 1 kG, falling off to larger and smaller field strengths. Remarkably, in this sample of stars selected for their presumably weak magnetic fields, we find only 2 stars for which the derived dipole strength is weaker than 300 G. We interpret this "magnetic threshold" as a critical value necessary for the stability of large-scale magnetic fields, and develop a simple quantitative model that is able to approximately reproduce the observed threshold characteristics. This scenario leads to a natural explanation of the small fraction of intermediate-mass magnetic stars. It may also explain the near-absence of magnetic fields in more massive B and O-type stars.
Key words. stars: chemically peculiar - stars: magnetic field

1. Introduction
The magnetic chemically peculiar Ap/Bp stars are the nondegenerate stars for which the strongest magnetic fields have been measured (Landstreet 1992). Although the fields are thought to be fossil remnants of flux swept up during star formation or produced via dynamo action on the pre-main sequence, their origin is not understood in any real detail (e.g. Moss 2001). Furthermore, the role of the magnetic field in the diffusion processes which are responsible for their chemical peculiarity has been studied in only a schematic fashion.

Send offprint requests to: M. Auriere, ` michel.auriere@ast.obs-mip.fr Based on data obtained using the Telescope Bernard Lyot at Ä Observatoire du Pic du Midi, CNRS and Universite Paul Sabatier, Ä France. Fig. 7 to Fig. 32 are only available online. Table 3 is only available in electronic form at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/


2

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Although more than one thousand main sequence A-type stars have been catalogued as magnetic Ap/Bp stars (Renson et al. 1991) following the scheme of Preston (1974), direct measurements of the magnetic field have been obtained for only a few hundred of them (Romanyuk 2000, Bychkov et al. 2003). Examination of the published measurements shows that the majority of the reported values are rather large. For example, 55% of the 210 stars of the catalogue of Romanyuk (2000) with published magnetic field measurements have a maximum unsigned line-of-sight (longitudinal) magnetic field B larger than 1 kG. On the other hand, according to Bohlender & Landstreet (1990), the median root-mean-square (rms) longitudinal magnetic field of Ap stars (based on a small magnitude-limited sample observed by Borra & Landstreet 1980) is only about 300 G (the largest rms field they report is only 710 G). This implies that most Ap stars have relatively weak (< 1 kG) magnetic fields, and that the available observations are strongly biased toward stars with the strongest and most easily-measured fields. One consequence of this bias is that the weak-field part of the magnetic field distribution of Ap stars is poorly studied. It is not known if it increases monotonically toward arbitrarily small field strength, or if it is truncated at a minimum magnetic field strength (as proposed by Glagolevskij & Chountonov 2002). In order to improve our knowledge of the weak-field part of the magnetic field distribution of Ap stars, we have undertaken a study of a sample of 28 well-known spectroscopically-identified Ap/Bp stars, with very weak, poorly-determined or previouslyundetected magnetic fields. We describe our survey in Sect. 2 and report our observational and modeling results in Sect. 3 and Sect. 4. We discuss the implications of our results, suggesting one possible interpretation involving the stability of large scale magnetic fields, in Sect. 5 and give our conclusions in Sect. 6.

2.2. Observations and reduction

2. The weak-field Ap stars survey
2.1. The selected sample

Our sample is composed of spectroscopically-identified Ap/Bp stars belonging to the HD catalogue. Twelve stars were selected based on the observations of Borra & Landstreet (1980) and Bohlender et al. (1993), identifying stars for which no significant detection of the magnetic field was obtained. Thirteen additional targets are stars for which only old photographic measurements of the magnetic field were available, typically by Babcock (1958), and for which measurements have poor precision and do not provide a significant detection of the magnetic field; these stars were generally selected using the catalogues of Romanyuk (2000) or Bychkov et al. (2003). Finally, 3 stars of our sample were selected which had not been observed for magnetic field before this work. The observational properties of the 28 stars are presented in Table 1. Section 3.2 gives more details on each star and on the obtained results. Because all of these stars are relatively bright, most have been known for decades and have been well studied. All appear in the Hipparcos catalogue (Perryman et al., 1997), and all but 6 have / < 0.2. The majority have photometrically-determined rotational periods and published values of v sin i. Many have been studied using high-resolution spectroscopy and Doppler Imaging. Therefore the classification of this sample as bona fide Ap/Bp stars is generally quite firm. As a consequence of this careful selection (and as will be described later in the paper), no non-Ap/Bp star has been mistakenly included in the sample.

Stokes V and Stokes I spectra of the 28 sample stars were obtained during 10 observing runs, from July 2001 to June 2006. We used the MuSiCoS spectropolarimeter attached the Bernard Lyot telescope (TBL) at Observatoire du Pic du Midi. The MuSiCoS spectropolarimeter is composed of a cross-dispersed echelle spectrograph (Baudrand & Bohm 1992) and a dedicated ? polarimeter module (Donati et al. 1999). The spectrograph is a table-top instrument, fed by a double optical fibre directly from the Cassegrain-mounted polarimeter. In one single exposure, this apparatus allows the acquisition of a stellar spectrum in a given polarisation (Stokes V in this case) throughout the spectral range 450 to 660 nm with a resolving power of about 35000. Spectra in both orthogonal polarisations are recorded simultaneously by the CCD detector. A complete Stokes V exposure consists of a sequence of four subexposures, between which the quarter-wave plate is rotated by 90o . This has the effect of exchanging the beams in the whole instrument, and in particular switching the positions of the two orthogonally polarised spectra on the CCD, thereby reducing spurious polarisation signatures. The echelle polarisation spectra were reduced using the ESpRIT package (Donati et al. 1997). The observation and reduction procedures are more thoroughly described by Shorlin et al. (2002). The correct operation of the MuSiCoS instrument, and in particular the absence of spurious magnetic field detections, is supported by other data obtained during these same observing runs, including studies of non-magnetic A-type stars (e.g. Shorlin et al. 2002), magnetic A, B and O-type stars (e.g., Ryabchikova et al. 2005a, Donati et al. 2001, Wade et al. 2006a) and magnetic late-type stars (e.g. Petit et al. 2005). MuSiCoS has recently been decomissioned, and has been replaced with NARVAL (Auriere 2003), the new-generation spec` tropolarimeter which is a copy of the ESPaDOnS instrument in operation at the Canada-France-Hawaii Telescope (Donati 2004, 2007: in preparation). The main improvements of NARVAL in polarisation mode with respect to MuSiCoS are a spectral resolution of about 65000, spectral response between 370 nm and 1000 nm, and an overall sensitivity increased by a factor of about 30.
2.3. Physical proper ties of the sample

For each of the sample stars, we have determined effective temperature T eff , luminosity L and radius R, to allow us to identify the appropriate line mask for Least-Squares Deconvolution (Sect. 2.5) and for determination of the rotational axis inclination for the dipole magnetic field model (Sect. 2.7). Effective temperatures of stars of our sample were derived using Geneva and Stromgren photometry (obtained from the ? General Catalogue of Photometric Data (GCPD); Mermilliod et al. 1997) using the calibrations of Hauck & North (1982) and Moon & Dworetsky (1985). Effective temperatures reported in Table 1 are the average of the two estimates when both were available, or the single one which could be derived when only one photometric set was available. We have assumed for T eff an uncertainty of the order of 3% for propagation of uncertainties in all calculations using the effective temperature. Luminosity was inferred using the GCPD-reported visual magnitude, the Hipparcos parallax and the bolometric correction relations of Balona (1994). Radius was then inferred directly from the luminosity and temperature via the Stefan-Boltzmann equation for a uniform spherical star.


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

3

Table 1. Observational properties of the weak-field Ap star sample. Columns give ID and HD number, visual magnitude, spectral classification, effective temperature, luminosity and radius (with associated 1 error bars), adopted LSD mask temperature, number of observations obtained and detection level (d=definite detection; m=marginal detection), maximum observed unsigned longitudim nal field in G, 1 error in G, and peak longitudinal field detection significance z = | Bma x| / . Bd in,3.3 is the minimum dipole field l (at 2) inferred from the maximum measured longitudinal field and Eq. (7).
ID HN And 43 Cas Cas 21 Per 9 Tau 56 Tau 11 Ori 137 Tau 15 Cnc 3 Hya 45 Leo EP Uma 65 Uma 21 Com Her 45 Her 19 Lyr 4 Cyg Psc HD 8441 10221 15089 15144 18296 22374 27309 32549 32650 37687 39317 40711 43819 68351 72968 90569 94427 96707 103498 108945 148112 151525 171586 171782 179527 183056 204411 220825 m Spec Type A2p A0sp A5p A6Vsp B9p A2p A0sp A0sp B9sp B8 B9spe A0 B9IIIsp B9sp A1spe A0sp A5 F0sp A1spe A2pvar B9p B9p A2pvar A0p B9sp B9sp A6pe A0p T eff ( K) 9060 Á 300 10660 Á 350 8360 Á 275 8480 Á 280 9360 Á 310 8390 Á 275 12730 Á 420 10220 Á 335 11920 Á 390 9450 Á 310 10130 Á 330 8070 Á 265 10880 Á 355 10290 Á 340 9840 Á 320 10250 Á 335 7250 Á 240 7780 Á 255 9220 Á 300 8870 Á 290 9330 Á 305 9380 Á 310 8760 Á 290 9660 Á 315 10370 Á 340 11710 Á 385 8750 Á 290 9450 Á 310 1. 2. 1. 1. 2. 1. 2. 2. 2. 2. 2. 1. 2. 2. 1. 1. 1. 1. 2. 1. 1. 2. 1. 1. 2. 2. 1. 1. log L (L ) 90 11 38 21 08 48 06 35 11 18 19 94 15 65 55 78 05 54 06 72 86 18 37 76 63 69 97 40 Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 16 09 05 07 11 13 08 12 07 25 14 61 20 21 08 10 11 08 20 09 08 13 10 30 16 11 07 05 3. 3. 2. 1. 4. 2. 2. 4. 2. 4. 4. 4. 3. 6. 2. 2. 2. 3. 4. 3. 3. 4. 2. 2. 6. 5. 4. 1. R (R ) 6 3 3 9 2 6 2 7 7 6 0 8 3 6 0 5 1 2 2 1 2 7 1 7 4 3 2 9 Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á Á 0. 0. 0. 0. 1. 0. 0. 1. 0. 1. 1. 5. 1. 2. 0. 0. 0. 0. 1. 0. 0. 1. 0. 1. 1. 1. 0. 0. 9 7 4 3 0 7 4 2 5 9 1 3 2 4 4 5 5 6 5 6 6 2 5 3 9 2 8 3 Mask (kK) 9 11 9 9 10 9 12 11 12 10 11 9 11 10 10 11 8 8 9 9 10 11 10 10 11 12 9 10 # 8 10 12 6 2 2 12 11 18 2 8 3 8 16 13 10 8 21 14 13 12 14 5 6 11 13 12 12 Det. level 8d 8d 12d 6d 2d 2d 12d 1d3m 2m3d 2d 3d1m 1d1m 8d 1d4m 13d 10d 8d 7d7m 12d1m 12d1m 11d 2d3m 5d 2d1m 8d2m 13d 12d 12d |B |
ma x

V

Á ( G)

z 8.7 4.3 20.8 42.0 10.6 21.7 16.1 4.7 5.0 6.4 3.6 13.8 25.1 6.9 27.4 23.5 8.6 2.3 8.9 4.3 9.7 3.8 6.6 4.2 3.4 6.9 6.0 12.8

B

min,3.3 d

( G)

6. 5. 4. 5. 5. 6. 5. 4. 5. 7. 5. 8. 6. 5. 5. 6. 7. 6. 6. 5. 4. 5. 6. 7. 5. 5. 5. 4.

7 5 5 8 0 7 3 7 4 0 5 5 2 6 7 0 3 0 9 4 6 2 4 8 9 1 3 9

157 Á 18 148 Á 34 486 Á 23 631 Á 15 213 Á 20 523 Á 24 804 Á 50 186 Á 39 91 Á 18 766 Á 119 216 Á 59 528 Á 38 628 Á 25 325 Á 47 427 Á 16 541 Á 23 356 Á 41 69 Á 33 169 Á 19 234 Á 54 204 Á 21 146 Á 38 375 Á 56 333 Á 78 156 Á 46 290 Á 42 88 Á 14 312 Á 25

399 264 1452 1983 571 1568 2323 356 237 1742 323 1492 1907 762 1304 1634 904 128 432 416 535 231 868 584 211 680 198 865

The inferred values of T eff , log L/L and R/R are reported in Table 1. For the 20 stars which we have in common with the study of Kochukhov & Bagnulo (2006), these values are all in good agreement. As pointed out by Landstreet et al. (2007), the assumed uncertainties of Kochukhov & Bagnulo (2006), which are comparable to our own, are probably somewhat underestimated. However, as our fundamental parameters are not to be used for detailed evolutionary studies, we consider them to be sufficient for this study.
2.4. Least-Squares Deconvolution and magnetic field detection

The primary aim of our study is to detect line circular polarisation (a "Stokes V Zeeman signature") which is characteristic of the longitudinal Zeeman effect produced by the presence of a magnetic field in the stellar photosphere. For this we used the Least-Squares Deconvolution (LSD) procedure, first used by Donati et al. (1997) to study the magnetic fields of active latetype stars and by Wade et al. (2000 a,b) for Ap stars. This method enables the "averaging" of several hundred (and possibly several thousand in some stars) lines and thus to obtain Stokes I and Stokes V profiles with greatly improved S/N. LSD provides a single quantitative criterion for the detection of Stokes V Zeeman signatures: we perform a statistical test in which the reduced 2 statistic is computed for the Stokes V pro-

file, both inside and outside the spectral line (Donati et al. 1997). The statistics are then converted into detection probabilities, which are assessed to determine if we have a definite detection (dd, false alarm probability smaller than 10-5 ), a marginal detection (md, false alarm probability greater than 10-5 and smaller than 10-3 ), or no detection at all (nd). A diagnostic null spectrum (called N in the following) is also obtained using the same subexposures obtained for Stokes V , but by pair processing those corresponding to identical azimuths of the quarter-wave plate. By checking that a signal is detected only in V and not in N , and that any detected signature is located within the line profile velocity interval, we can distinguish between real magnetic signatures and (infrequent) spurious signatures. In addition, using the full resolved Stokes V profile enables the detection of the magnetic field, even if the integrated line-of-sight component is very weak, or even null.
2.5. LSD masks

LSD is a cross-correlation method which requires comparison of our observed spectra with synthetic line masks (Donati et al. 1997, Shorlin et al. 2002). To obtain the most realistic masks, we used spectral line lists from the Vienna Atomic Line Database (VALD; Piskunov et al 1995; Ryabchikova et al. 1997; Kupka et al. 1999). To take into account the chemical peculiarities of Ap/Bp stars, we employed an abundance table in which the


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M. Auriere et al.: Magnetic fields of weak-field Ap stars `

abundance of metals (Al, Si, S, Ti, V, Mn, Fe, Co, Ni, Zn, Sr, Y, Zr, Ba, La, Ce, Pr, Nd, Eu, Gd, Dy) is 10x solar, except for Cr which was increased to 100x solar (e.g. Shorlin et al. 2002). Masks were then compiled for effective temperature ranging from 7000-13000 K, with log g = 4.0, a microturbulence of 2 km/s, and including all metal lines with a central depth greater than 10% of the continuum. We also compiled a series of masks assuming solar abundances. We have found in other studies that the magnetic field measurements are not very sensitive to the mask temperature within a couple of thousand K (Wade et al., in preparation). We therefore computed masks spaced every 1 0 0 0 K. Least-Squares Deconvolution was performed for several temperatures and in some cases the most significant magnetic field detection was obtained for a temperature somewhat hotter than that given by the photometric data. This occured several times for the hottest sample stars - this can be seen in Table 1. In the case of the cool Ap star EP UMa, a solar abundance mask gave a better result (better detection of magnetic field and smaller error bars on B ) than Ap abundances as described above. These discrepancies probably result from differences between the true chemical peculiarities of individual stars and those assumed in the line masks. For the discrepant hot stars, we computed the longitudinal magnetic field for a mask temperature between that corresponding to the best detection and the derived effective temperature. For EP UMa, we used solar abundance masks in our analysis. The number of lines used in the LSD ranged from 1500 to 3000, and is anticorrelated with the temperature.
2.6. Longitudinal magnetic field

The longitudinal magnetic field was inferred from each of the Stokes I and V profile sets, using the first-order moment method. According to this method, the longitudinal field B (in G) is calculated from the Stokes I and V profiles in velocity units as: B = -2 .1 4 ç 1 0
11

vV ( v) d v gc [Ic - I (v)]dv

,

(1 )

(Rees & Semel 1979; Donati et al. 1997; Wade et al. 2000b) where , in nm, is the mean wavelength of the LSD profile, c is the velocity of light (in the same units as v), and g is the mean value of the Lande factors of all lines used to construct Ä the LSD profile. Integration ranges used for evaluation of Eq. (1) were computed automatically, beginning and ending 15 km/s before/after the location in the line wings at which the residual flux was equal to 85% of the continuum flux. The accuracy of this technique for determining high-precision longitudinal field measurements has been clearly demonstrated by Wade et al. (2000b), Donati et al. (2001) and Shorlin et al. (2002). The resultant longitudinal magnetic field measurements, which are reported in Table 3, are remarkably precise (this Table is only available on line). The 282 measurements, with a median 1 uncertainty of 40 G, represent the largest compilation of high-precision stellar magnetic field measurements ever published.
2.7. Modeling the longitudinal field variation

good first approximation of the large scale magnetic field of Ap stars (e.g. Landstreet 1988). Because of the weakness of the longitudinal magnetic field observed for the stars of our sample, we do not expect to be able to detect departures from a global dipolar configuration. To begin, we added to our high-precision data set additional good-quality published magnetic field measurements collected by Bychkov et al. (2003). Details of these collected measurements were kindly provided by Dr. Victor Bychkov. Then, we searched the literature for rotational periods for each of our sample stars. For many stars, published rotational periods were available which provided an acceptable folded phase variation B () of the magnetic measurements. However, for some stars, the published rotational period or periods did not provide an acceptable folded magnetic field variation, and for others, no published period was available. For these latter stars, we used a modified Lomb-Scargle technique to attempt to infer the rotational period, both directly from the longitudinal field measurements, as well as from the variations of the LSD Stokes I and V profiles. The period searches of LSD profiles were performed by treating each pixel in the Stokes I and V profiles as an independent timeseries (similar to the technique described by Adelman et al., 2002). Individual periodograms were subsequently weighted according to their amplitude of variation and averaged to characterise variability of the whole LSD profile. Acceptable periods were identified by establishing the 99% confidence threshold, and candidate periods were evaluated by phasing the LSD profiles and longitudinal field measurements. Results of the period searches for individual stars are provided in their appropriate subsections in Sect. 3. Ultimately, acceptable rotational periods were obtained for 24 stars, and these periods are reported in Table 2. We also searched the literature for published values of the projected rotational velocity (v sin i) of each star, which we compared to the value measured from the LSD Stokes I profile by fitting rotationally-broadened synthetic profiles. Sometimes significant discrepancies were found between our values of v sin i and those reported in the literature. These discrepacies are discussed in Sect. 3, and the adopted rotational velocities (generally those obtained from the LSD profiles) are shown in Table 2. Each phased longitudinal field variation B () was then fit using a 1st order sine function: B () = B0 + B1 sin 2( + 0 ). (2 )

To characterise the dipole components of the magnetic fields of our sample stars, we use the oblique rotator model (ORM, Stibbs 1950) as formulated by Preston (1967). This model provides a

The phased and fit longitudinal field variations are shown in Fig. 1. The reduced 2 of this fit (2 ), along with those of linear 2 fits through B = 0 (the "null field" model, 2 ) and through 0 the weighted mean of the measurements (the "constant field" model, 2 ), of each star, are reported in Table 2. 2im , the 2 1 l upper limit for admissible models, computed according to Press et al. (1992), is reported in Table 2 as well . A comparison of these reduced 2 values with each other allows us to evaluate the significance of the detection of the longitudinal magnetic field and its variability. Although variability of the longitudinal field cannot be established for a few stars (2 < 2im ), the only star 1 l for which the longitudinal field is not detected with more than 2 confidence is HD 96707 (for which 2 < 2im ). 0 l For a tilted, centred magnetic dipole, the surface polar field strength Bd is derived from the variation of the longitudinal magnetic field B with rotational phase using Preston's (1967) well-known relation: Bd = B
max

15 + u (cos cos i + sin sin i) 2 0 (3 - u )

-1

,

(3 )


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

5

Table 2. Results of the magnetic field modeling. The contents of the columns are described in sect. 2.7. The uncertainties associated with the derived dipole parameters i, and Bd correspond to 2.
star 8441 10221 15089 15144 27309 32549 32650 39317 43819 68351 72968 90569 94427 96707 103498 108945 148112 151525 171586 171782 179527 183056 204411 220825 Period (d) 69.2 3.15459 1.74033 2.99787 1.568884 4.6393 2.7347 2.6541 15.02 4.16 5.6525 1.04404 1.9625 3.515 15.830 2.01011 3.04296 4.1164 2.1308 4.4674 7.098 2.9919 4.8456 1.42539 v sin i (km/s) 2 24 48 13 57 47 30 45 10 33 16 13 8 37 13 65 44.5 35 37 24 33 26 5.4 38 2 0 13.71 5.90 57.83 1305.83 157.42 7.19 4.48 4.97 135.66 7.85 360.16 170.38 37.58 0.82 25.43 5.31 40.67 2.74 10.86 6.88 6.57 25.02 20.75 78.54 2 1 6.69 1.81 56.37 4.57 2.43 8.56 1.92 1.84 59.32 2.17 4.51 36.08 46.61 0.91 29.71 6.00 0.93 2.86 8.27 1.12 7.70 28.74 5.43 90.05 2 2 1. 1. 1. 0. 1. 1. 1. 2. 3. 1. 1. 1. 2. 0. 6. 2. 0. 0. 2. 1. 0. 1. 0. 2. 75 56 83 04 74 75 19 24 45 38 22 93 12 77 55 10 95 97 59 79 30 59 57 29 2i l 3. 2. 2. 2. 2. 2. 1. 3. 4. 2. 2. 3. 3. 1. 7. 2. 1. 1. 6. 3. 1. 2. 1. 3. i ( ) 49 Á 33 27 Á 11 45 Á 11 24 Á 8 53 Á 17 65 Á 27 37 Á 12 36 Á 12 63 Á 66 28 Á 37 61 Á 18 9Á4 8Á4 53 Á 16 75 Á 68 57 Á 18 56 Á 16 37 Á 19 48 Á 19 51 Á 51 74 Á 32 74 Á 8 7Á5 35 Á 54 ( ) 73+17 - 61 42+38 - 41 80+72 -1 9+6 -3 5+11 -5 77+11 - 74 45+31 - 30 20+69 - 20 + 47 42-42 46+36 - 41 5+7 -4 81+5 -7 89+1 -4 +0 90-90 80+10 - 11 85+31 -6 3+11 -3 78+11 - 43 46+40 - 40 5+85 -5 +8 81-34 49+37 - 32 81+72 -1 83+70 -8 Bd (103 G) 0.683 0.375 2.031 2.100 3.673 0.546 0.229 0.560 2.626 0.649 2.388 5.157 8.957 0.100 0.600 0.735 1.042 0.545 1.422 1.651 0.522 1.558 0.968 1.957 B m in d (103 G) 0.415 0.195 1.560 2.007 2.325 0.312 0.153 0.113 2.488 0.437 1.451 2.946 3.806 0.0 0.572 0.333 0.579 0.208 0.716 0.213 0.409 1.172 0.416 1.141 Bmax d (103 G) 2.931 1.202 2.999 2.281 8.022 28.176 0.477 2.252 78.367 71.486 6.702 11.284 25.519 0.492 6.751 1.509 2.370 1.927 4.413 22257.276 1.233 3.938 4.509 21.045

m

35 71 14 71 63 75 72 18 18 00 03 07 72 21 44 83 73 70 60 79 30 32 46 18

where Bmax = | B0 | + B1 and u denotes the limb darkening parameter (equal to approximately u = 0.5 for our sample). The rotational axis inclination and obliquity angles i and are related by tan = 1-r cot i, 1+r (4 )

directly from the maximum measured value of the longitudinal field. The maximum measured longitudinal field is reported in column 11 of Table 1, and the inferred lower limit (2) of Bd , m Bd in,3.3 is reported in column 13 of Table 1. It is clear from these data that Bd for most of our sample is larger than a few hundred G at 2.

wh e r e r = ( | B 0 | - B 1 ) / ( | B 0 | + B 1 ) . We have determined the inclination i for each of our stars assuming rigid rotation, and computing: sin i = Prot v sin i , 5 0 .6 R (5 )

3. Observational results
3.1. Global results as compared to previous work

where Prot is the adopted stellar rotational period in days, v sin i is the adopted projected rotational velocity in km/s, and R is the computed stellar radius in solar units. The magnetic obliquity was then inferred from Eq. (4) and the polar strength of the dipole Bd from Eq. (3). Uncertainties associated with all parameters (at 2, including a max(2 km/s, 10%) uncertainty on v sin i) were propagated through the calculations of i, and Bd . The resultant dipole magnetic field models are reported in Table 2. An important and interesting consequence of Eq. (3), independent of all parameters except limb-darkening, is: Bd 2 0 (3 - u ) B 15 + u
max

,

(6 )

which, for typical limb-darkening u, yields: Bd > 3 .3 B
max

.

(7 )

Therefore, exclusive of the model geometry, a lower limit on the surface dipole component of the magnetic field is obtained

All of the 28 Ap stars studied were found to exhibit significant circular polarisation in their spectral lines. Table 1 gives our global result. For a majority of the sample, the detection of the magnetic field was obtained during the first observation. For some objects, obtaining a positive detection of the magnetic field required several observations, sometimes spanning several observing seasons. This was due to observations at phases in which the polarisation was especially weak, and due to low S/N ratio resulting from poor meteorological conditions. The number of observations and of Zeeman detections of each star is also indicated in Table 1. No significant or recent detection of the magnetic field has been reported in the past for essentially all stars of our sample. Shorlin et al. (2002), using MuSiCoS and the same procedure as in this paper, did not detect the magnetic field of 3 Ap stars they observed. For two of these stars, they suggested a misclassification. We re-observed the third star, HD 148112 ( Her), and easily detected its field. Glagolevskij & Chountonov (2002) observed 11 weakly-magnetic Ap stars and detected no magnetic fields in any of them. More recently, Glagolevskij et al. (2005) presented 9 stars in which they detected no longitudinal fields, with B weaker than 100 G. Five of these stars were observed


6

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Fig. 2. LSD profiles of 21 Per (HD 18296) on 01 Sep 05. From bottom to top, Stokes I and Stokes V are presented. For display purposes, the profiles are shifted vertically, and Stokes V profile is expanded by a factor of 25. The dashed line illustrates the zero level for the Stokes V profile. during this work and the magnetic field was detected for all of them. Hubrig et al. (2006) and Kochukhov & Bagnulo (2006) reduced FORS1 observations of about 100 Ap stars, among which were about 50 stars for which they detected the magnetic field for the first time. Four stars of their sample are in common with ours: 9 Tau, 21 Com, Her and 45 Her. In this study, the magnetic field is detected and measured for each of them, we give details in Sect. 3.2. on the results of the FORS1 investigations. Our higher detection rate of magnetic field with respect to other techniques is certainly due to in part to the S/N improvement associated with the LSD method. In addition, our magnetic field detection criterion is based on measurement of significant circular polarisation within the velocity-resolved line profile (the Stokes V signature). This signature amplitude is only weakly sensitive to the global magnetic field geometry, and generally varies by only a factor of a few during the stellar rotational cycle, unlike the longitudinal field (which frequently varies by orders of magnitude, and which can vanish completely at some phases). Finally, the fact that we insist on performing multiple observations of each star is also an important factor in our superior magnetic field detection rate. One set of LSD profiles will be shown for each of the studied stars in the online version of the paper. However, Figs. 2 and 3 illustrate the case of 21 Per (HD 18296) when the field was respectively 213 Á 20 G (10 longitudinal field detection) and -39 Á 24 G (insignificant longitudinal field detection). However, both of these observations correspond to highly significant detections of the Stokes V Zeeman signatures. Fig. 4 illustrates the non-detection of magnetic field in HD 32650 with MuSiCoS, and Fig. 5 shows the Zeeman detection of this same star obtained with NARVAL on 12 March 2007. We now present our Zeeman detection and modeling results for each star of our sample.
3.2. Results obtained for each star
3.2.1. HN And (HD 8441)

Fig. 3. LSD profiles of 21 Per on 02 sep 05 (same as Fig. 2).

Fig. 4. LSD profiles (ND) of HD 32650 on 12 feb 04 observed with MuSiCoS (same as Fig. 2, no Zeeman detection).

Fig. 5. LSD profiles (DD) of HD 32650 on 12 Mar 07 as observed with NARVAL (same as Fig. 2 but Stokes V profile is expanded by a factor of 50, definite Zeeman detection). measuring its field. We observed this star 8 times and obtained 8 definite Zeeman detections. Fig. 7 shows the LSD Stokes V and Stokes I profiles when the longitudinal magnetic field was B = 1 5 5 Á 1 8 G. In the literature we find periods for HN And of 2.9632 days (Steinitz, 1965) based on magnetic data from Babcock (1958), 106.27 days from radial velocity measurements (Renson, 1965) later shown to be the rotation period of the binary (North et al, 1998), 69.5 days based on Stromgren (Wolff & Morrison, 1973) and Johnson (Rakosch & Fiedler, 1978) photometry, and 1.80889 days (Bychkov et al, 2005) based mostly on the same magnetic data as Steinitz (1965). Examining our periodogram near these periods, we only find a strong 2 minimum near 69.5

HN And is a well-studied SB1 A2p star (e.g. North et al. 1998, Adelman et al. 1995) for which no clear magnetic field detection has been reported. Babcock (1958) presented measurements of a relatively weak (some hundreds of G) field, and Bychkov et al. (2003) did not present any new significant Zeeman detection. Preston (1971) and Mathys & Lanz (1992) did not succeed in


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

7

200 100 0 -100 0 -350 -700 500 0 400 0 -400 0 -200 150 0 -150

HD 8441

150 75 0 150 0 -150

HD 10221

600 300 0 -300 150 75 0 -75 400 200 0

0 -250
HD 15089 HD 32650

HD 15144

-500 300 150 0 500
HD 90569 HD 39317

HD 27309

Longitudinal magnetic field (G)

HD 32549 HD 68351

HD 43819

300 150 0 75 0

HD 72968 HD 103498

250 0 200 0 -200 0 -250
HD 108945

HD 96707

200 0 -200 0 -200 -400 0 -50 -100

HD 94427 HD 148112

-75 150 0 -150 HD 151525

HD 171586 HD 204411

-500 300 0 -300

HD 171782

HD 179527

200 0 -200 -400

HD 183056

HD 220825

Rotational phase
Fig. 1. Phased longitudinal field measurements of sample stars. The vertical (longitudinal field) scale differs in each frame, and is indicated in each frame in units of G. The horizontal (phase) axis in each frame runs from -0.25 to 1.25 cycles. days in both Stokes V and I . The LSD profiles phase in a sensible fashion at this minimum, thus we can be confident that it is the correct period. Based on our analysis we adopt Prot = 69.2+0..6 d, -0 5 where the uncertainties correspond to 99% confidence. The projected rotational velocity of HN And is very low, and is also not well known. North et al. (1998) report v sin i < 2.35 km/s. Our R = 35000 spectra do not allow us to improve upon this estimate. Using a high-resolution (R = 110, 000) CFHT-Gecko spectrum of this star in our possession, we have attempted to estimate v sin i by modeling the 6150 Õ region. The best fit is obtained for v sin i 3 km/s and very weak magnetic field (0 - 500 G). However, acceptable fits are also obtained for moderate fields (1-1.5 kG) and intermediate rotation (1.5-2 km/s). For calculation of the dipole field, we adopt v sin i = 2 km/s which results (at 2 confidence) in i = 49 Á 33, = 73+17 and 415 Bd 2931 G (with Bmin,3,3 = 399 G). -61 d Larger values of v sin i result in an increased value of the inferred Bd , and assuming v sin i = 1 km s-1 (which we believe is the smallest value admissible by the line profiles), the weakest admissible field remains essentially unchanged.
3.2.2. 43 Cas, HD 10221

Landstreet (1980) nor Glagolevskij & Chountonov (2002) could detect it. Glagolevskij et al. (2005) reported a 4 detection. In this paper, the Stokes V Zeeman signal is clearly detected on 8 occasions. Fig. 8 shows the LSD Stokes V and Stokes I profiles when the longitudinal magnetic field was measured to be B = 148 Á 34 G. Hildebrandt (1975) found a photometric period of 3.1848 d. for 43 Cas, which was refined to 3.15459 d from Hipparcos data (van Leeuwen et al. 1997). The projected rotational velocity, measured from modeling of the strongly-variable LSD Stokes I profiles, is 24 km/s. We derive i = 27 Á 11 , m = 42+38 and 195 Bd 1202 G (with Bd in,3,3 = 264 G). -41
3.2.3. Cas, HD 15089

43 Cas is a classical Ap star in which magnetic field has been sought for around 50 years, but neither Babcock (1958), Borra &

The magnetic field of Cas was not detected by Borra & Landstreet (1980), but was by Kuschnig et al. (1998). As shown in Fig. 9 and Table 3, the field is easily detected (12 definite detections), and a rather large longitudinal field is measured ( B = -348 Á28 G). The rotational period of this star has been recently confirmed by Hipparcos (1.74033 d), and Kuschnig et al. (1998) give v sin i = 48 km/s (consistent with Royer et al. 2002, and somewhat lower than the LSD profiles which give 52 km/s). We adopt v sin i = 48 km/s. We have included 18 additional measurements from Kuschnig et al. (1998), and obtain i = 45 Á 11 , m = 80+72 and 1560 Bd 2999 (with Bd in,3,3 = 1452 G). -1


8

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

3 . 2 . 4 . HD 1 5 1 4 4

3 . 2 . 9 . HD 3 2 6 5 0

Only rather old investigations concerning the magnetic field are published for this star. Our observations confirm the existence of a rather strong negative magnetic field at the surface of HD 15144 as already inferred by Babcock (1958) and Bonsack (1981). Fig. 10 shows the LSD Stokes profiles when the longitudinal magnetic field was measured as B = -631 Á 15 G. We have employed the 2.99787 d photometric period of van Genderen (1971), and we adopt v sin i = 13 km/s from the LSD profiles. We obtain i = 24 Á 8 , = 9+6 and 2007 Bd 2281 -3 m (with Bd in,3,3 = 1983 G).
3.2.5. 21 Per, HD 18296

21 Per was not detected significantly by Borra & Landstreet (1980). Its rather weak longitudinal field was measured by Glagolevskij et al. (1995). We detect it easily on two occasions, and our error bars on B are about 10 times smaller than those of previous measurements. Fig. 2 shows the LSD spectrum when the field was 213 Á 20 G, while Fig. 3 corresponds to a cross-over phase when the longitudinal field is as small as -39 Á 24 G. Although some photographic longitudinal field measurements are reported in the catalogue of Bychkov et al. (2003), their uncertainties appear to be seriously underestimated. Given the small number of precise magnetic field measurements of this star, we are unable to derive a dipole field model. However, from the peak value of the longitudinal field obtained here, we can infer that Bd > 571 G with 2 confidence.
3.2.6. 9 Tau, HD 22374

This star is classified as B9pSi by Cowley & Cowley (1969) and spectrophotometry was obtained by Adelman (1997, 1980). It was found to be a large amplitude variable (up to 0.1 mag in U -band). We did not detect its field with MuSiCoS, although we observed it several times. However the magnetic field of HD 32650 was detected (marginally) during science demonstration observations with NARVAL, and has since been detected definitively and repeatedly with this instrument. Fig. 4 shows our MuSiCoS observation on 12 February 2004. Fig. 5 shows one definite Zeeman detection with NARVAL on 12 March 07 wh e n B = 9 1 Á 1 8 G. Using the rotational period of HD 32650 from Adelman (1997) and v sin i = 30 km/s (from the LSD profiles) we modeled the combined MuSiCoS + NARVAL longitudinal field variation, obtaining i = 37 Á 12 , = 45+31 and 153 Bd 477 (with -30 m Bd in,3,3 = 237 G). This is one of the weakest dipole intensities inferred in this study.
3 . 2 . 1 0 . HD 3 7 6 8 7

9 Tau appears to have been only observed for magnetic field by Babcock (1958). Our two observations provide an easy Zeeman detection. Fig. 11 shows the LSD Stokes profiles when the longitudinal magnetic field was measured to be B = 523 Á 24 G. Although we are unable to model the dipole field, we infer that Bd > 1568 G with 2 confidence.
3.2.7. 56 Tau, HD 27309

This star is located in the direction of the Ori OB1 association. Morrel & Levato (1991) did not find it to be a member. However the Hipparcos parallax and proper motions do not appear conclusive alone, and radial velocity measurements will be necessary to conclude definitively on the membership. Magnetic splitting of the very sharp spectral lines of HD 37687 was not resolved in the investigation of Mathys & Lanz (1992). We detected easily the magnetic field of this star for the very first time (Fig. 14) from only 2 LSD profiles. We find that the longitudinal magnetic field reaches B = 766 Á 119 G (on 17 Feb 05). From the maximum longitudinal field measured, we infer a lower limit of Bd > 1742 G with 2 confidence.
3.2.11. 137 Tau, HD 39317

Neither Borra & Landstreet (1980) nor Glagolevskij (as reported in the catalogue of Bychkov et al. 2003) could detect the field of this star. 56 Tau is generously detected in each of our 12 observations and the longitudinal field reaches B = -775 Á 40 G (Fig. 1 2 ). The rotational period P = 1.5688840 Á 0.00000470 d is from North & Adelman (1995). Although Royer et al. (2002) report v sin i = 44 km/s, we find that this value seriously underestimates the width of the LSD profiles, and adopt v sin i = 57 km/s. Using these values, we derive i = 53 Á 17 , = 5+11 and 2325 Bd -5 m 8022 G (with Bd in,3,3 = 2323 G).
3.2.8. 11 Ori, HD 32549

The magnetic field of this star was not detected by Borra & Landstreet (1980). In this study 137 Tau was observed 8 times and its magnetic field detected 3 times, reaching a peak value B = 222 Á 58 G on 10 Feb 05 (Fig. 15). Using P = 2.6541 d (Renson & Manfroid 1981) and the LSD-measured v sin i of 45 km/s, we obtain i = 36 Á 12 , = 20+69 and 113 Bd -20 m 2252 G (with Bd in,3,3 = 323 G).
3 . 2 . 1 2 . HD 4 0 7 1 1

El'kin et al. (2003) observed this star and obtained a lower limit for the longitudinal magnetic field of more than several hundred G. We obtain three observations of this star, Fig. 16 shows our Stokes V and Stokes I LSD profiles on 13 Feb 04 when the longitudinal magnetic field was B = -528 Á 38 G. We obtain a 2 lower limit on the dipole intensity of Bd > 1492 G.
3 . 2 . 1 3 . HD 4 3 8 1 9

Borra & Landstreet (1980) could not detect the magnetic field of 11 Ori. We detect significant Stokes V signatures in 4 of our 11 observations. Our best circular polarisation detection is obtained at a crossover phase, when the longitudinal field is as weak as -8 Á 26 G (Fig. 13). Using the photometric period of 4.6394 d (van Leeuwen et al. 1997) and the LSD-measured v sin i of 47 km/s, we obtained i = 65 Á 27 , = 77+11 and 312 Bd -74 m 28176 G (with Bd in,3,3 = 356 G).

This star is well studied for photometric and abundance properties (Lopez-Garcia & Adelman 1994; Adelman & Young 2005). Adelman & Young (2005) found a period of 15.0313 days, stable over a 30 year time span, which is compatible with the Hipparcos period (van Leeuwen et al, 1997). Gollnow (1971) reported one insignificant longitudinal field measurement, and Bychkov et al.


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

9

(2003) reported additional observations. Fig. 17 corresponds to a crossover phase when B was as weak as -12 Á 29 G. Using the period of Adelman & Young (2005) and v sin i = 10 km/s from the LSD profiles, and including the better-quality magnetic field measurements reported by Bychkov et al. (2003), we obtain i = 63 Á 66, = 42+47 and 2626 Bd 78367 G -42 m (with Bd in,3,3 = 1907 G).
3.2.14. 15 Cnc, HD 68351

This star was previously observed by Babcock (1958) and Bohlender et al. (1993), who did not obtain any significant magnetic field detection. We observed it 16 times and detected the magnetic field 5 times. Fig. 18 presents our Stokes profiles obtained on 07 Feb 03 when the longitudinal magnetic field was B = 3 2 5 Á 4 5 G. The period is not very well known, and we adopt that of Stepien (1968; P = 4.116 d). With v sin i = 33 km/s from Ä the LSD profiles, we obtain i = 28 Á 37 , = 46+36 and -41 437 Bd 71486 G (with Bmin,3,3 = 762 G). d
3.2.15. 3 Hya, HD 72968

This star has been observed by Babcock (1958) and van den Heuvel (1971) who did not obtain a significant detection of its magnetic field. We detected it easily 13 times. Fig. 19 presents our Stokes profiles when the longitudinal magnetic field was B = 3 9 0 Á 1 6 G. Adelman (1998) reports a photometric period of 11.305 days, which according to our data appears to be twice the magnetic period. With a period of 5.6525 d and v sin i = 16 km/s, we obtain i = 61 Á 18 , = 5+7 and 1451 Bd 6702 G (with -4 m Bd in,3,3 = 1304 G).
3.2.16. 45 Leo, HD 90569

MuSiCoS by Johnson (2004), who obtained 5 detections of Stokes V signatures from 7 observations, but with a longitudinal field never larger than 119 Á 58 G. From the total of 21 LSD Stokes V profiles of EP UMa (the 7 observations of Johnson (1994) plus an additional 14 observations), we have obtained 7 definite Zeeman detections, 7 marginal detections and 7 nondetections, as defined in section 2.2. We confirm the result of Johnson (2004) - the magnetic field of EP UMa is very weak, and the longitudinal component is never larger than about 100 G. Fig. 22 presents our LSD profiles of EP UMa when the longitudinal magnetic field was B = 59 Á 33 G. The period of rotation of EP UMa has been subject of debate, with the main uncertainty being whether to choose the 3.516 d photometric period of Adelman et al (1999), or the magnetic period of twice this value (7.0286 d) reported by Leone & Catanzaro (2001). Using our Stokes profiles, we find independently a magnetic period of P = 3.515+0..009, consistent with the photometric period. -0 026 Adopting therefore the photometric period and v sin i = 37 km/s, we obtain i = 53 Á 16 , = 90+00 , and 0 Bd 492 G (with -9 m Bd in,3,3 = 128 G). EP UMa exhibits one of the weakest dipole fields of any star in the sample, and it is the only star in our sample for which the longitudinal field is not significantly detected (although the presence of a field is confirmed via the Stokes V profiles).
3 . 2 . 1 9 . 6 5 UM a , HD 1 0 3 4 9 8

This star was observed by Babcock (1958) and Bonsack (1976) who detected the magnetic field. However, their measurements have poor precision. Leroy (1993) measured linear polarisation in the direction of this star, but it is likely at least partly due to interstellar polarisation. We detected the magnetic field of 45 Leo easily 10 times. Fig. 20 presents our Stokes profiles when the longitudinal magnetic field was B = 541 Á 23 G. Adopting the period P = 1.04404 d of Adelman (2006) and measuring v sin i = 13 km/s, we find i = 9 Á 4 , = 81+5 and -7 2946 Bd 11284 G (with Bmin,3,3 = 1634 G). d
3 . 2 . 1 7 . HD 9 4 4 2 7

This star is part of a double system. Its magnetic field has been reported by Bychkov et al. (2003), who indicate that it reaches an extreme value of about -800 G. We observed this star 14 times and detected its magnetic field 13 times. We find that the maximum unsigned longitudinal field is never larger than about 200 G. Fig. 23 presents our LSD profiles when the longitudinal magnetic field was B = -166 Á 20 G. Using the LSD Stokes I and V profiles, we have determined a rotational period of 15.830 d and v sin i = 13 km/s. The magnetic field geometry is described by i = 75 Á 68 , = 80+10 and 572 Bd 6751 G -11 m (with Bd in,3,3 = 432 G).
3 . 2 . 2 0 . 2 1 Co m , HD 1 0 8 9 4 5

This star is poorly studied, but we detected its magnetic field clearly on 8 occasions. Fig. 21 presents our Stokes profiles when the longitudinal magnetic field was B = 356 Á 41 G. We have determined the rotational period of 1.9625 d from the LSD profile variations. With v sin i = 8 km/s, we obtain i = m 8 Á 4 , = 89+1 and 3806 Bd 25519 G (with Bd in,3,3 = -4 9 0 4 G) .
3 . 2 . 1 8 . E P UM a , HD 9 6 7 0 7

21 Com is a member of the Mel 111 cluster in Coma Ber (Bounatiro, 1993). This star was observed by Borra & Landstreet (1980) who obtained no detection of its magnetic field. Shorlin et al. (2002) detected it with MuSiCoS. Using FORS1 at VLT, Hubrig et al. (2006) presented one measurement of the longitudinal magnetic field as a new detection, B = -347 Á 51 G, whereas Kochukhov & Bagnulo (2006), using the same observational data, could not detect the magnetic field, with B = 65 Á 116 G. We observed 21 Com 13 times with MuSiCoS and detected its magnetic field each time. Fig. 24 presents our LSD profiles when the longitudinal magnetic field was B = -238 Á 55 G. We adopt the best magnetic period near that of Kreidl et al. (1990): P = 2.01011 d, and v sin i = 65 km/s from Shorlin et al. (2002). Our derived magnetic field geometry is i = 57 Á 18 , m = 85+31 and 333 Bd 1509 G (with Bd in,3,3 = 416 G). -6
3.2.21. Her, HD 148112

Several studies of EP UMa measured a rather large magnetic field: van den Heuvel (1971), Bychkov et al. (1997), Leone & Catanzaro (2001). This star was observed previously with

Borra & Landstreet (1980) detected the magnetic field in Her and report 9 measurements, but with rather large uncertainties ( between 115 and 285 G). Shorlin et al. (2002) and Bychkov et al. (2005) add one measurement each, the values of which suggest a


10

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

small amplitude of variation. Kochukhov & Bagnulo (2006) and Hubrig et al. (2006) did not detect the magnetic field. From our 12 observations of Her we obtained 11 definite detections. Fig. 25 presents our LSD profiles when the longitudinal magnetic field was B = -204 Á 21 G. We have adopted the rotational period P = 3.04296 d and v sin i = 44.5 km/s of Hatzes (1991) (we obtained 46 km/s from the LSD profiles). The derived field geometry is i = 56 Á 16 , = 3+11 and 579 Bd 2370 G (with Bmin,3,3 = 535 G). -3 d
3.2.22. 45 Her, HD 151525

Using the photometric period P = 7.098 d of Adelman & Rice (1999) and LSD-derived v sin i = 33 km/s, we obtain i = m 74 Á 32, = 81+84 and 409 Bd 1233 (with Bd in,3,3 = -4 2 1 1 G) .
3.2.26. 4 Cyg, HD 183056

This star is the one for which detection of the magnetic field required the longest time. Babcock (1958) observed it, and Kochukhov & Bagnulo (2006) and Hubrig et al. (2006) did not detect the magnetic field. We observed it 14 times and obtained 2 definite Zeeman detections and 3 marginal detections. Fig. 26 presents our LSD profiles when the longitudinal magnetic field was B = 146 Á 38 G. We used the period P = 4.1164 d and v sin i = 35 km/s of Hatzes (1991) (we obtained 36 km/s from the LSD profiles) to model the magnetic field geometry, obtaining i = 37 Á 19 , = 78+11 and 208 Bd 1927 G (with Bmin,3,3 = 231 G). -43 d
3 . 2 . 2 3 . HD 1 7 1 5 8 6

The magnetic field of 4 Cyg was not detected by Borra & Landstreet (1980). We observed the star 13 times with MuSiCoS and obtained a Zeeman detection each time. Fig. 30 shows the LSD profiles when the longitudinal magnetic field was B = 3 3 0 Á 8 3 G. Using the LSD profile variations of this star, we obtain a rotational period of 2.9919 d and v sin i = 26 km/s. The derived magnetic geometry is i = 74 Á 8 , = 49+37 and 1172 Bd -32 m 3938 G (with Bd in,3,3 = 680 G).
3 . 2 . 2 7 . HD 2 0 4 4 1 1

HD 171586 is a classical Ap star (Babcock 1958), which is located in the direction of the open cluster IC 4756. However, Gray & Corbally (2002) found that HD 171586 is not a cluster member. Only one magnetic observation by Babcock (1958) has been reported (Bychkov et al, 2003). We observed and detected this star 5 times. Fig. 27 shows the LSD profiles when the longitudinal magnetic field was measured as B = -375 Á 56 G. We have adopted the period of Winzer (1974) of P = 2.1308 d which produces a reasonable phasing of the data, along with v sin i = 37 km/s from the LSD profiles. We obtain i = 48 Á 19 , = 46+40 and 716 Bd 4413 G (with -40 m Bd in,3,3 = 868 G).
3 . 2 . 2 4 . HD 1 7 1 7 8 2

The surface magnetic field of HD 204411 was estimated by Preston (1971) to be about 500 G. Johnson (2004) detected the magnetic field with MuSiCoS. Here we have obtained 12 observations of this star with 12 definite Zeeman detections, although the longitudinal field is always smaller than 100 G. Fig. 31 shows the LSD profiles when the longitudinal magnetic field was B = -88 Á 14 G. We have derived a rotational period of 4.8456 d from LSD profiles. Fig. 1 shows that B presents a clear variation, although HD 204411 has been for a long time considered as a very longperiod photometric and/or spectroscopic variable (Preston 1970, Adelman 2003). The spectral lines of this star are sufficiently sharp that v sin i cannot be accurate determined from our spectra, and we adopt v sin i = 5.4 km/s (Ryabchikova et al. 2005b). The derived magnetic geometry is i = 7 Á 5 , = 81+72 and -1 m 416 Bd 4509 G (with Bd in,3,3 = 198 G). This range of field intensities is consistent with the estimate of the surface field reported by Ryabchikova et al. (2005b).
3.2.28. Psc, HD 220825

This star is located in the direction of IC 4556, but Herzog & Sanders (1975) discarded it as a member because of relative proper motion measurements. No magnetic field measurements has been reported for HD 171782. We observed this star 6 times and detected it 3 times. Fig. 28 shows the LSD profiles when the longitudinal magnetic field was measured to be B = - 1 3 3 Á 7 8 G. Adopting the 4.4674 d period of Adelman & Meadows (2002) and v sin i = 24 km/s measured from the LSD profiles, we obtain i = 51 Á 51 , = 5+85 and Bd 213 G (with -5 m Bd in,3,3 = 584 G). Note, due to the large uncertainties associated with i and , that the derived Bd upper limit for this star is unrealistically large.
3.2.25. 19 Lyr, HD 179527

The magnetic field of Psc was not detected by Borra & Landstreet (1980). We observed the star 12 times, detecting it each time. Fig. 32 shows the LSD profiles when the longitudinal magnetic field was B = 350 Á 24 G. We adopt the 1.420 d period of Kreidl & Schneider (1989; the only published period that fits out measurements) and v sin i = 38 km/s from the LSD profiles. We derive i = 35 Á 54 , m = 83+70 and 1141 Bd 21045 G (with Bd in,3,3 = 865 G). -8

4. Modeling results
4.1. Qualitative summary of the survey

The magnetic field of 19 Lyr was not detected by Landstreet (1980). We observed this star 11 times with and obtained 10 Zeeman detections. Fig. 29 shows the files at a cross-over phase, when the longitudinal mag was as weak as B = -42 Á 42 G.

Borra & MuSiCoS LSD pronetic field

Tables 1 and 3, Figs. 2 to 5 and Figs. 7 to 32 show that for all of the 28 weak-field Ap/Bp sample stars, the magnetic field of every sample star could be detected when sufficient tenacity and precision were employed. Thus our first conclusion is that all magnetic Ap/Bp stars, when confidently identified through spectroscopic and photometric observations, can be shown to host a measurable surface magnetic field. In every case, it was found that the longitudinal field measurements could be modeled assuming an oblique, centred dipole without any significant inconsistencies.


M. Auriere et al.: Magnetic fields of weak-field Ap stars `
6

11

5

4 #

3

2

1

0

1

10

100 Bd (G)

1000

10000

A straightforward interpretation of the behaviour observed in Fig. 6 is that there exists a minimum magnetic field strength necessary for the generation of the chemical peculiarities of Ap/Bp stars. One possible implication of this hypothesis is that there may exist a potentially large population of A-type stars which host magnetic fields which are not sufficiently strong to generate Ap-type peculiarities (Vauclair & Vauclair 1982). However, large, high precision investigations of non-Ap tepid stars (e.g. Shorlin et al. 2002, Wade et al. 2006b, Bagnulo et al. 2006), which are able to rule out the presence of dipole fields with intensities below 300 G in many stars, suggest that no such population exists, and that the Ap/Bp stars are the only A-type stars with detectable magnetic fields.

Fig. 6. Histogram of best-fit derived dipole field strengths of the stars in our sample.

5. Interpretation
The 100% Zeeman detection rate obtained in our survey strongly suggests that all Ap/Bp stars host detectable magnetic fields. Moreover, it appears that a threshold magnetic field of about 300 G exists below which fields are very rare, and perhaps altogether absent. A possible interpretation of this result is that there exists a critical field strength above which stable magnetic configurations exist and below which any large scale field configuration is destroyed by some instability. The instability is expected to result in the presence of opposite polarities at small length scales, thus strongly reducing the magnitude of the integrated longitudinal field through cancellation effects. For a sample of stars containing both stable and unstable field configurations, this scenario would imply a strong jump in the measured values of the longitudinal fields or a lower bound of the magnetic field, depending on the detection limit. The existence of stable large scale magnetic fields in stars is primarily supported by the observations of the magnetic fields of Ap stars and white dwarfs. Theoretically, although no stable field configuration is known in an analytical form, it has been proposed that the combination of azimuthal and poloidal field might be stable as a recent numerical simulation tends to confirm (Braithwaite & Spruit, 2004). However, when the magnetic field is sufficiently weak to be wound up by differential rotation, the resulting field, predominantly azimuthal with respect to the rotation axis, can be subject to various instabilities. As recently reviewed by Spruit (1999) (see also Spruit, 2004), the most vigorous of these instabilities is a pinch-type instability first considered in a stellar context by Tayler (1973). Here, we estimate the critical magnetic field below which the winding-up process induces an instability and above which the action of magnetic torques on the differential rotation limits the winding-up before the instability sets in. The winding-up time scale is tw = 1/(q) where q = r / = r/ is a dimensionless measure of the differential rotation. The winding-up of the axisymmetric part of sym the original poloidal field Bp by the differential rotation being sym governed by t B = r sin Bp Ç , the time scale tw corresponds more specifically to the time necessary to produce an azsym imuthal field component B of the same amplitude as Bp . On the other hand, Lorentz forces will affect the differential rotation after a Alfven travel time calculated on the shear length scale , Ä that is tA = (4 )1/2 / B. Equating both time scales gives a local order of magnitude estimate of the critical magnetic field, Bc (4 )1/2r. Its value can be expressed in terms of the equipartition field of a typical Ap star as follows: Bc B eq 2 Prot 5day
-1

4.2. Distribution of dipole intensities Bd of the weakest-field Ap stars

For 24 of our sample stars, a sufficient number of longitudinal field measurements were obtained to allow modeling of the dipolar magnetic field geometry in the manner described in Sect. 2.7. The results of this modeling are summarised in Table 2. Fig. 6 shows the histogram of the derived best-fit dipole strengths Bd . The remarkable characteristic of this diagram is the near-absence of Ap stars in our sample with Bd below 300 G. Only 2 stars (HD 32650 and HD 96707) are found to have bestfit model dipole field intensities below 300 G. This number increases to only 3 stars if we consider the lower limit of the dipole strength (either Bmin or Bmin,3.3 , whichever is larger). Moreover, d d no star is constrained to have Bd below 300 G (i.e. the maximumfield model for every star has Bd larger than 300 G). This result cannot be due to a detection threshold effect, because the magnetic field has been detected for every star in the sample. Nor is it likely that it is due to a selection effect, as our sample was constructed specifically to include the Ap/Bp stars with the weakest magnetic fields. What is clearly demonstrated is that the number of Ap/Bp stars does not continue to increase monotonically to arbitrarily small field strengths. Instead, it appears to plateau around 1 kG, and to decline rapidly below about 300 G. That this result is not an artifact of the modeling technique that we have employed is supported by the distribution of peak longitudinal fields measured for the sample, and the minimum dipole strengths derived directly from those measurements (columns 11 and 13 of Table 1). Because these minimum strengths are dependent on essentially no i, or period (dipole field strength and known limb-darkening are the only model assumptions), they provide firm 2 lower limits on the surface field intensity of each star. In addition, those stars for which the data quality is sufficiently good show excellent agreement bem tween the 2 minimum field intensities Bmin and Bd in,3.3 . d The derived surface field intensities Bd are probably themselves only lower limits on the true surface field. When sufficient data are available, detailed models of magnetic Ap stars nearly always show evidence of higher-order multipolar contributions to the magnetic field (e.g. Landstreet 1988, Landstreet & Mathys 2000). These higher-order field components contribute only weakly to the longitudinal field variation, although they can have surface intensities comparable to that of the dipole component. Therefore the magnetic field models derived here probably systematically underestimate the true surface field intensity.

r 3R

T 104 K

-1/2

(8 )


12

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

As Beq = 170 G at the surface (5000 = 2/3) of a typical Ap star (log g = 4, T e f f = 104 K ) the derived critical field is close to the 300 G observational threshold ( B2q = 8 P, P is the pressure). e Calculation of the critical field Bc for each star in the sample also shows that most stars satisfy Bd > Bc, and all stars satisfy Bma x > Bc . Moreover, the magnetic field of the 5 stars with rod tational period under 2d (HD 10589, HD 27309, HD 90569, HD 94427, HD 220825) is compatible with the dependence of Bc on Prot ( Bc P-o1t ) since their dipolar fields Bd = 2 - 9 kG are r substantially greater than the sample median Bd 1.4 kG. It is however important to stress that although the local order of magnitude estimate of Bc is coherent with the present observational data, a detailed and non-local modeling is required to specify the critical field strength below which differential rotation destabilizes large scale field configurations. Note that the threshold value of the magnetic field is also higher than the magnetic field threshold necessary to trigger the Tayler instability, according to the criterion given by Spruit (1999). The large scale field is then destroyed by the development of the instability. An example of the non-linear evolution of such unstable configurations has been recently considered in a solar context (Brun & Zahn 2006) confirming that the resulting field is structured on small latitudinal length scales. The above scenario can thus qualitatively explain the existence of an apparent lower bound in the strength of magnetic fields of Ap stars. By extension, such a model could provide a basis to explain why magnetic fields are observed in only a small fraction of intermediate-mass stars. If the initial magnetic field strength probability distribution of intermediate-mass stars increases (say) exponentially toward weak fields, the large majority of A-type stars, after formation, would have fields weaker than the critical field described by Eq. (8). The fields of such stars would be unstable and decay; they would therefore appear at the main sequence showing no evidence of a magnetic field. Another advantage of the scenario described above is that it may also naturally explain the even greater rarity of magnetic fields detected in massive stars. For a typical main sequence A0p star (with P = 5 d, R = 3 R and T eff = 10000 K), Eq. (8) yields Bc 2 Beq 300 G. However, for a main sequence B0p star (with T eff = 31000 K, R = 7.2 R and P = 2 d), Bc 7 Beq 2 kG. With a substantially larger critical field strength, massive stars are substantially less likely to retain their magnetic fields (assuming an initial field probability distribution similar to that of Ap stars, decreasing toward strong fields). Massive stars in which relatively weak magnetic fields have been detected are all quantitatively in agreement with Eq. (8): Cep (Donati et al. 2001; B0, Bc 361 G, observed Bd = 360 G), Sco (Donati et al. 2006b; B0, Bc 70 G, observed B 500 G), 1 Ori C (Donati et al. 2002; O7, Bc 300 G, observed Bd 1 . 1 k G) , HD 191612 (Donati et al. 2006a, Bc 20 G, estimated minimum B d 1 . 5 k G) .

distribution of derived dipole strengths for these stars exhibits a plateau at about 1 kG, falling off to larger and smaller field strengths. Remarkably, in this sample of stars selected for their presumably weak magnetic fields, we find only 2 stars for which the derived dipole strength is weaker than 300 G. Interpreting this "magnetic threshold" as a critical value necessary for the stability of large-scale magnetic fields leads to a natural explanation of the small fraction of intermediate-mass magnetic stars. It may also explain the near-absence of magnetic fields in more massive B and O-type stars.
Acknowledgements. This research has made use of databases operated by CDS, Strasbourg, France, Vienna Atomic Line Database (VALD), Austria, and Observatoire de Geneve, Switzerland. GAW and JDL acknowledge Discovery ` Grant support from the Natural Sciences and Engineering Research Council of Canada (NSERC). We are very grateful to Dr. Victor Bychkov for providing his collected magnetic field measurements and to Dr. Thierry Roudier for providing IDL routines and making the final LSD figures.

References
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6. Conclusion
We have investigated a sample of 28 well-known spectroscopically-identified magnetic Ap/Bp stars, obtaining 282 new Stokes V Zeeman signatures and longitudinal magnetic field measurements using the MuSiCoS spectropolarimeter. Magnetic field is detected in all sample stars, and the inferred longitudinal fields are significantly greater than some tens of G. To characterise the surface magnetic field intensities of the sample, we modeled the longitudinal field data to infer the intensity of the dipolar field component. The


M. Auriere et al.: Magnetic fields of weak-field Ap stars `
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13


14

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Fig. 7. LSD profiles of HN And (HD 8441) on 25 bottom to top, Stokes I and Stokes V are presente purposes, the profiles are shifted vertically, and the file is expanded by a factor of 25. The dashed line zero level for the Stokes V profile.

Jan 06. From d. For display Stokes V proillustrates the

Fig. 10. LSD profiles of HD 15144 on 10 Dec 01 (same as Fig. 7 ).

Fig. 11. LSD profiles of 9 Tau (HD 22374) on 02 Feb 04 (same as Fig. 7). Fig. 8. LSD profiles of 43 Cas (HD 10221) on 14 Jan 06 (same as Fig. 7).

Fig. 12. LSD profiles of 56 Tau (HD 27309) on 11 Dec 01 (same as Fig. 7). Fig. 9. LSD profiles of Cas (HD 15089) on 24 Aug 04 (same as Fig. 7).


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

15

Fig. 13. LSD profiles of 11 Ori (HD 32549) on 20 Jan 06 (same as Fig. 7).

Fig. 16. LSD profiles of HD 40711 on 13 Feb 04 (same as Fig. 7 ).

Fig. 14. LSD profiles of HD 37687 on 17 Feb 04 (same as Fig. 7 ).

Fig. 17. LSD profiles of HD 43819 on 17 Dec 01 (same as Fig. 7 ).

Fig. 15. LSD profiles of 137 Tau (HD 39317) on 10 Feb 05 (same as Fig. 7).

Fig. 18. LSD profiles of 15 Cnc (HD 68351) on 07 Feb 03 (same as Fig. 7).


16

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Fig. 19. LSD profiles of 3 Hya (HD 72968) on 18 Dec 01 (same as Fig. 7).

Fig. 22. LSD profiles of EP Uma (HD 96707) on 06 Feb 06 (same as Fig. 7).

Fig. 20. LSD spectrum of 45 Leo (HD 90569) on 17 Dec 01 (same as Fig. 7).

Fig. 23. LSD profiles of 65 Uma (HD 103498) on 11 Dec 01 (same as Fig. 7).

Fig. 21. LSD profiles of HD 94427 on 11 Feb 04 (same as Fig. 7 ).

Fig. 24. LSD profiles of 21 Com (HD 108945) on 07 Feb 03 (same as Fig. 7).


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

17

Fig. 25. LSD profiles of Her (HD 148112) on 03 Jul 01 (same as Fig. 7).

Fig. 28. LSD profiles of HD 171782 on 30 Aug 05 (same as Fig. 7 ).

Fig. 26. LSD profiles of 45 Her (HD 151525) on 29 Jul 03 (same as Fig. 7).

Fig. 29. LSD profiles of 19 Lyr (HD 179527) on 13 Aug 05 (same as Fig. 7).

Fig. 27. LSD profiles of HD 171586 on 31 Jul 04 (same as Fig. 7 ).

Fig. 30. LSD profiles of 4 Cyg (HD 183056) on 24 Jun 03 (same as Fig. 7).


18

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Fig. 31. LSD profiles of HD 204411 on 27 May 06 (same as Fig. 7 ).

Fig. 32. LSD profiles of Psc (HD 220825)on 14 Jul 04 (same as Fig. 7).


M. Auriere et al.: Magnetic fields of weak-field Ap stars `

19

Table 3. Dates, magnetic field Detection and Longitudinal magnetic field measurements. Columns give Name and HD numbers, Date, Julian Date, Signal to Noise, 2 , Detection, longitudinal field in G, error in G.

Na m e HN An d

HD 8441

43 Cas

10221

Cas

15089

15144

21 Per 9 Tau 56 Tau

18296 22374 27309

1 1 Or i

32549

Date 12 Jul 03 30 Jul 04 3 1 Au g 0 4 25 Jan 06 31 Jan 06 02 Feb 06 04 Feb 06 05 Feb 06 0 1 De c 0 1 1 1 De c 0 1 1 2 De c 0 1 1 6 De c 0 1 06 Feb 04 12 Feb 04 10 Jan 06 12 Jan 06 14 Jan 06 21 Jan 06 04 Feb 04 06 Feb 04 2 4 Au g 0 4 2 9 Au g 0 4 0 3 Au g 0 5 0 4 Au g 0 5 0 6 Au g 0 5 0 7 Au g 0 5 0 8 Au g 0 6 1 1 Au g 0 5 2 4 Au g 0 5 02 Sep 05 0 9 De c 0 1 1 0 De c 0 1 08 Feb 05 3 0 Au g 0 5 01 Sep 05 03 Sep 05 01 Sep 05 02 Sep 05 02 Feb 04 2 3 Au g 0 5 0 1 De c 0 1 1 1 De c 0 1 1 7 De c 0 1 06 Jan 02 12 Jan 03 2 4 Au g 0 4 3 1 Au g 0 4 16 Jan 03 1 1 Au g 0 5 1 3 Au g 0 5 1 4 Au g 0 5 03 Sep 05 0 2 De c 0 1 0 8 De c 0 1 1 2 De c 0 1 05 Feb 04 17 Feb 04 11 Jan 06 12 Jan 06 16 Jan 06

Julian 24528 24532 24532 24537 24537 24537 24537 24537 24522 24522 24522 24522 24530 24530 24537 24537 24537 24537 24530 24530 24532 24532 24535 24535 24535 24535 24535 24535 24536 24536 24522 24522 24534 24536 24536 24536 24536 24536 24530 24536 24522 24522 24522 24522 24526 24532 24532 24526 24535 24535 24535 24536 24522 24522 24522 24530 24530 24537 24537 24537

Date 3 8 .6 5 1 7 .6 4 4 9 .6 6 6 1 .3 5 6 7 .2 8 6 9 .2 9 7 1 .2 8 7 2 .2 6 4 5 .4 0 5 5 .4 2 5 6 .3 7 6 0 .3 7 4 2 .2 9 4 8 .2 9 4 6 .3 7 4 8 .3 7 5 0 .3 7 5 7 .3 4 4 0 .3 4 4 2 .3 3 4 2 .6 0 4 7 .6 5 8 6 .5 4 8 7 .6 3 8 9 .6 5 9 0 .5 6 9 1 .5 9 9 4 .5 5 0 7 .5 5 1 6 .5 1 5 3 .3 8 5 4 .4 0 1 0 .3 2 1 3 .5 7 1 5 .5 5 1 7 .5 6 1 5 .6 4 1 6 .5 9 3 8 .3 0 0 6 .6 1 4 5 .5 1 5 5 .5 1 6 1 .4 7 8 1 .4 2 5 2 .4 1 4 2 .6 6 4 9 .6 3 5 6 .4 0 9 4 .6 6 9 6 .6 7 9 7 .6 7 1 7 .6 4 4 6 .5 2 5 2 .4 0 5 6 .7 3 4 1 .4 5 5 3 .4 6 4 7 .5 7 4 8 .5 3 5 2 .5 6

S 2 1 1 2 2 3 1 2 3 3 4 4 2 3 4 4 3 4 1 4 4 3 4 5 6 6 5 4 4 6 2 3 2 3 4 3 6 6 1 2 3 3 4 4 2 2 2 3 4 4 5 4 6 5 6 5 4 2 6 5

/ 2 8 8 2 1 0 9 4 1 1 2 1 7 1 4 2 2 5 8 2 5 6 8 5 0 3 4 6 2 2 9 4 6 0 2 6 8 3 9 5 1 7 0 2 8 1 6 3 6 4 3 9 1 2 3 0 4 0 0 5

N 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0

2 3 .9 3 2 .1 6 1 .9 2 7 .6 2 4 .3 4 3 .9 8 2 .8 1 3 .5 3 3 .0 5 1 .5 2 4 .0 6 0 .8 2 0 .8 5 2 .3 5 3 .9 0 2 .3 5 2 .4 2 4 .0 7 1 .9 1 6 .1 8 6 .3 5 5 .4 1 6 .5 2 1 3 .8 9 1 1 .8 0 9 .5 1 8 .2 4 1 0 .7 4 5 .1 4 8 .7 7 3 2 .2 3 3 8 .9 5 1 7 .7 1 3 1 .2 4 4 4 .5 1 3 8 .1 4 8 .0 1 1 2 .2 7 1 8 .5 1 1 9 .2 8 3 .0 1 5 .1 9 5 .7 8 4 .9 0 4 .4 1 2 .5 2 2 .8 0 3 .5 8 4 .8 5 7 .1 7 6 .8 1 5 .1 5 1 .4 4 1 .2 7 1 .2 1 1 .3 7 0 .9 7 0 .8 7 1 .2 6 1 .4 9

Detection DD DD DD DD DD DD DD DD DD DD DD nd nd DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD md nd nd md nd nd nd md

B l ( G) 61 -2 0 40 157 74 88 -4 28 89 67 87 30 -4 1 49 121 57 148 77 182 -2 2 2 -3 4 8 -1 5 2 448 -4 2 389 -2 9 8 486 -1 4 2 433 8 -5 6 8 -6 3 1 -5 5 8 -5 5 8 -6 2 3 -5 8 0 213 -3 9 523 -1 9 5 -6 9 3 -6 1 5 -7 6 8 -6 8 1 -7 1 7 -6 5 4 -7 1 4 -7 7 1 -6 2 5 -8 0 4 -7 7 5 -5 7 4 172 30 171 44 11 -4 7 -1 5 0 -1 8 6

( G) 21 31 30 18 23 18 27 18 38 34 32 29 48 43 30 30 34 31 125 38 28 45 26 25 20 24 23 27 37 29 15 15 24 15 13 14 20 24 24 18 72 49 56 50 61 86 90 68 46 50 40 39 46 43 37 42 69 104 37 39


20 Table 3. continued.

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Na m e

HD

32650

37687 137 Tau 39317

40711 43819

15 Cnc

68351

3 Hy a

72968

Date 20 Jan 06 21 Jan 06 22 Jan 06 0 9 De c 0 1 1 0 De c 0 1 05 Feb 04 12 Feb 04 10 Jan 06 13 Jan 06 19 Jan 06 21 Jan 06 22 Jan 06 27 Nov 06 29 Nov 06 30 Nov 06 1 4 De c 0 6 1 1 M ar 0 7 1 2 M ar 0 7 1 3 M ar 0 7 1 4 M ar 0 7 1 5 M ar 0 7 17 Feb 04 17 Feb 05 0 1 De c 0 1 1 2 De c 0 1 10 Feb 05 23 Jan 06 24 Jan 06 31 Jan 06 01 Feb 06 03 Feb 06 13 Feb 04 08 Feb 05 09 Feb 05 1 0 De c 0 1 1 1 De c 0 1 1 3 De c 0 1 1 6 De c 0 1 1 7 De c 0 1 06 Jan 02 04 Feb 06 05 Feb 06 0 8 De c 0 1 1 1 De c 0 1 07 Feb 03 08 Feb 03 29 Jan 04 13 Feb 04 14 Feb 04 23 Jan 06 24 Jan 06 25 Jan 06 29 Jan 06 31 Jan 06 01 Feb 06 02 Feb 06 03 Feb 06 07 Feb 06 1 0 De c 0 1 1 3 De c 0 1 1 5 De c 0 1

Julian 24537 24537 24537 24522 24522 24530 24530 24537 24537 24537 24537 24537 24540 24540 24540 24540 24541 24541 24541 24541 24541 24530 24534 24522 24522 24534 24537 24537 24537 24537 24537 24530 24534 24534 24522 24522 24522 24522 24522 24522 24537 24537 24522 24522 24526 24526 24530 24530 24530 24537 24537 24537 24537 24537 24537 24537 24537 24537 24522 24522 24522

Date 5 6 .4 1 5 7 .3 9 5 8 .5 2 5 3 .5 5 5 4 .5 4 4 1 .4 8 4 8 .4 6 4 6 .5 6 4 9 .5 8 5 5 .5 3 5 7 .5 0 5 8 .4 0 6 7 .4 8 6 9 .5 7 7 0 .5 4 8 4 .5 5 7 1 .3 4 7 2 .3 9 7 3 .3 4 7 4 .3 8 7 5 .3 6 5 3 .4 2 1 9 .4 5 4 5 .5 5 5 6 .5 2 1 2 .4 7 5 9 .3 9 6 0 .4 1 6 7 .4 5 6 8 .3 8 7 0 .4 5 4 9 .4 4 1 0 .4 8 1 1 .5 0 5 4 .6 4 5 5 .5 4 5 7 .7 5 6 0 .6 1 6 1 .6 0 8 1 .5 6 7 1 .4 7 7 2 .4 6 5 2 .6 4 5 5 .6 3 7 8 .4 6 7 9 .5 4 3 4 .5 9 4 9 .4 8 5 0 .5 4 5 9 .5 5 6 0 .5 7 6 1 .5 5 6 5 .5 0 6 7 .5 0 6 8 .5 0 6 9 .4 7 7 0 .5 0 7 4 .4 8 5 4 .6 9 5 7 .6 0 5 9 .6 1

S/N 780 590 520 370 400 390 420 500 510 390 480 430 562 734 866 684 1188 918 1439 1070 862 130 120 330 410 490 360 330 360 390 460 83 100 44 230 180 150 230 240 200 230 340 350 370 340 320 180 250 300 350 300 400 210 370 400 410 490 490 300 200 200

2 2 .3 9 1 .2 2 1 .1 9 1 .1 5 0 .8 4 0 .9 5 0 .8 7 1 .0 0 1 .1 4 1 .1 4 1 .0 7 0 .7 6 1 .1 2 1 .4 2 1 .0 4 0 .8 3 1 .7 3 2 .2 4 2 .3 7 0 .7 4 1 .7 8 4 .5 7 5 .6 3 1 .1 1 1 .9 6 1 .6 0 1 .1 6 1 .4 8 0 .9 2 1 .8 4 1 .3 8 1 3 .3 8 1 .6 4 1 .2 9 2 2 .0 4 1 6 .6 1 1 4 .6 6 2 1 .1 6 1 5 .6 9 1 7 .0 4 2 1 .5 0 2 9 .0 0 1 .4 4 1 .3 8 2 .0 7 9 0 .9 8 0 .9 2 1 .0 9 0 .8 6 1 .1 6 1 .2 9 1 .0 6 1 .2 4 1 .1 3 1 .2 9 1 .5 3 1 .3 4 1 .1 5 7 .7 3 9 .3 4 8 .5 8

Detection DD nd nd nd nd nd nd nd nd nd nd nd nd md nd nd DD DD DD nd md DD DD nd DD DD nd md nd DD nd DD md nd DD DD DD DD DD DD DD DD md md DD nd nd nd nd nd nd nd nd nd nd md md nd DD DD DD

B l ( G) -8 -9 6 66 55 47 73 98 105 105 122 72 -4 2 29 47 4 3 0 91 39 24 47 565 766 68 200 222 199 129 -1 8 94 59 -5 2 8 -9 7 40 631 642 724 93 -1 2 74 534 628 148 70 276 124 -1 6 117 58 88 137 80 306 72 146 140 84 62 283 379 359

( G) 26 33 57 57 69 59 54 39 43 67 42 63 27 16 18 23 14 18 10 16 19 108 119 70 53 58 66 73 68 58 52 38 71 184 31 34 43 30 29 35 36 25 46 47 41 62 102 75 61 46 57 47 69 51 42 37 39 35 19 27 28


M. Auriere et al.: Magnetic fields of weak-field Ap stars ` Table 3. continued.

21

Na m e

HD

4 5 L eo

90569

94427

E P Um a

96707

6 5 Um a

103498

Date 1 6 De c 0 1 1 7 De c 0 1 1 8 De c 0 1 05 Jan 02 06 Jan 02 12 Jan 06 13 Jan 06 19 Jan 06 20 Jan 06 04 Feb 06 0 7 De c 0 1 1 3 De c 0 1 1 5 De c 0 1 1 6 De c 0 1 1 7 De c 0 1 1 8 De c 0 1 05 Jan 02 06 Jan 02 03 Feb 06 05 Feb 06 07 Feb 03 21 Jan 04 11 Feb 04 0 9 M ay 0 6 1 8 M ay 0 6 2 4 M ay 0 6 2 8 M ay 0 6 01 Jun 06 1 0 De c 0 1 1 1 De c 0 1 1 5 De c 0 1 11 Jan 03 16 Jan 03 19 Jan 03 29 Jan 04 01 Feb 04 02 Feb 04 05 Feb 04 08 Feb 04 13 Feb 04 17 Feb 04 23 Jan 06 24 Jan 06 25 Jan 06 31 Jan 06 05 Feb 06 06 Feb 06 07 Feb 06 08 Feb 06 1 1 De c 0 1 1 3 De c 0 1 1 5 De c 0 1 1 5 De c 0 1 1 6 De c 0 1 1 7 De c 0 1 1 8 De c 0 1 06 Jan 02 06 Feb 05 06 Feb 05 08 Feb 05 10 Feb 05

Julian 24522 24522 24522 24522 24522 24537 24537 24537 24537 24537 24522 24522 24522 24522 24522 24522 24522 24522 24537 24537 24526 24530 24530 24538 24538 24538 24538 24538 24522 24522 24522 24526 24526 24526 24530 24530 24530 24530 24530 24530 24530 24537 24537 24537 24537 24537 24537 24537 24537 24522 24522 24522 24522 24522 24522 24522 24522 24534 24534 24534 24534

Date 6 0 .6 5 6 1 .6 4 6 2 .6 5 8 0 .5 8 8 1 .5 9 4 8 .5 8 4 9 .5 4 5 5 .4 2 5 6 .5 2 7 1 .5 1 5 1 .6 5 5 7 .6 4 5 9 .6 5 6 0 .6 8 6 1 .6 8 6 2 .6 8 8 0 .6 5 8 1 .6 3 7 0 .6 3 7 2 .5 3 7 8 .5 5 2 6 .6 5 4 7 .5 8 6 5 .3 6 7 4 .3 9 8 0 .3 8 8 4 .3 6 8 8 .3 7 5 4 .7 4 5 5 .6 7 5 9 .6 8 5 0 .6 6 5 5 .5 7 5 8 .6 8 3 4 .6 5 3 7 .6 7 3 8 .6 3 4 1 .6 4 4 4 .6 4 4 9 .6 3 5 3 .6 2 5 9 .5 9 6 0 .6 1 6 1 .5 9 6 7 .5 8 7 2 .6 2 7 3 .5 0 7 4 .5 5 7 5 .4 9 5 5 .7 3 5 7 .6 9 5 9 .7 2 5 9 .7 5 6 0 .7 2 6 1 .7 1 6 2 .7 2 8 1 .6 7 0 8 .5 8 0 8 .6 0 1 0 .6 2 1 2 .6 5

S/N 240 330 340 280 280 330 360 150 370 310 320 150 160 260 260 310 240 300 270 290 120 64 110 150 100 120 110 79 290 320 180 240 270 180 170 160 170 280 250 310 260 280 260 350 340 330 340 400 330 200 100 100 100 170 150 150 170 57 89 190 150

2 6 .5 9 1 5 .5 1 1 6 .2 4 1 2 .6 0 1 2 .9 7 1 6 .4 9 1 7 .1 2 6 .9 9 1 6 .8 4 1 5 .0 6 2 9 .7 8 1 4 .5 7 1 0 .6 4 2 0 .2 9 2 2 .2 0 3 2 5 .8 3 2 4 .1 3 2 6 .8 7 2 2 .8 9 2 3 .2 9 8 .7 1 3 .8 1 7 .2 6 2 .7 5 5 .7 9 8 .0 2 6 .7 6 4 .7 2 1 .5 1 1 .6 7 0 .8 5 1 .1 4 1 .4 1 1 .4 4 0 .9 2 1 .2 3 1 .4 5 1 .3 7 1 .4 4 2 .1 6 1 .5 8 1 .6 4 0 .8 7 2 .0 3 0 .9 7 1 .6 2 1 .8 1 1 .1 2 1 .7 3 6 .2 8 2 .9 7 2 .8 7 2 .2 6 4 .4 4 4 .5 4 5 .6 7 6 .4 1 1 .6 7 1 .1 8 4 .5 4 3 .4 5

Detection DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD md DD nd nd md md nd nd md md md DD md DD nd DD nd DD DD nd DD DD DD DD DD DD DD DD DD MD ND DD DD

B l ( G) 300 338 390 375 378 389 427 430 376 390 430 311 71 171 541 154 438 382 465 195 277 -5 3 4 356 -5 6 -3 5 8 -3 8 6 -4 0 3 -3 0 4 10 -2 50 41 3 24 -3 3 145 13 30 -1 5 -4 8 -1 7 -2 3 -2 -1 6 -4 2 28 59 -1 8 -2 9 -1 6 6 -2 3 1 -1 4 2 -1 1 2 16 88 183 176 388 202 33 -1 6 3

( G) 23 17 16 20 19 16 16 35 15 18 23 43 40 24 23 22 27 27 27 26 40 94 41 33 55 45 57 82 38 31 66 44 44 63 65 62 75 38 40 33 40 40 47 28 33 32 33 28 29 20 43 44 45 24 26 27 25 143 153 28 42


22 Table 3. continued.

M. Auriere et al.: Magnetic fields of weak-field Ap stars `

Na m e 21 Com

HD 108945

He r

148112

4 5 He r

151525

171586

171782

19 Lyr

179527

Date 02 Feb 06 05 Feb 06 1 3 De c 0 1 1 6 De c 0 1 1 7 De c 0 1 1 8 De c 0 1 06 Jan 02 16 Jan 03 07 Feb 03 03 Feb 05 08 Feb 05 08 Feb 05 16 Jan 06 19 Jan 06 20 Jan 06 03 Jul 01 28 Jul 01 16 Jul 03 20 Jul 03 0 4 Au g 0 3 0 3 Au g 0 5 0 5 Au g 0 5 0 6 Au g 0 5 0 7 Au g 0 5 0 8 Au g 0 5 1 5 Au g 0 5 04 Sep 05 07 Jul 01 28 Jun 03 30 Jun 03 07 Jul 03 11 Jul 03 21 Jul 03 29 Jul 03 15 Jan 04 08 Feb 04 14 Feb 04 11 Jul 04 12 Jul 04 15 Jul 04 17 Jul 04 31 Jul 04 0 6 Au g 0 4 1 3 Au g 0 4 01 Jun 06 03 Jun 06 0 5 Au g 0 4 1 2 Au g 0 4 2 8 Au g 0 5 3 0 Au g 0 5 01 Jun 06 04 Jun 06 18 Jul 01 06 Jul 03 08 Jul 03 09 Jul 03 27 Jul 03 0 4 Au g 0 5 1 2 Au g 0 5 1 3 Au g 0 5 1 4 Au g 0 5

Julian 24537 24537 24522 24522 24522 24522 24522 24526 24526 24534 24534 24534 24537 24537 24537 24520 24521 24528 24528 24528 24535 24535 24535 24535 24535 24535 24536 24520 24528 24528 24528 24528 24528 24528 24530 24530 24530 24531 24531 24532 24532 24532 24532 24532 24538 24538 24532 24532 24536 24536 24538 24538 24521 24528 24528 24528 24528 24535 24535 24535 24535

Date 6 9 .6 0 7 2 .5 7 5 7 .7 3 6 0 .7 5 6 1 .7 5 6 2 .7 5 8 1 .7 0 5 6 .6 3 7 8 .6 3 0 5 .6 7 1 0 .6 6 1 0 .6 9 5 2 .6 6 5 5 .5 7 5 6 .5 8 9 4 .4 0 1 9 .4 1 3 7 .3 9 4 1 .3 9 5 1 .3 8 8 6 .4 1 8 8 .3 9 8 9 .3 9 9 0 .4 0 9 1 .3 9 9 8 .3 8 1 8 .3 6 9 8 .4 1 1 9 .4 1 2 1 .3 9 2 8 .4 2 3 2 .4 0 4 2 .3 8 5 0 .3 7 2 0 .7 0 4 4 .7 2 5 0 .7 1 9 8 .4 6 9 9 .4 7 0 2 .4 8 0 4 .4 4 1 8 .4 5 2 4 .4 6 3 1 .4 1 8 8 .4 9 9 0 .5 2 2 3 .4 5 3 0 .4 4 1 1 .4 1 1 3 .3 7 8 8 .5 3 9 1 .5 1 0 9 .4 2 2 7 .4 9 2 9 .5 1 3 0 .5 2 4 8 .3 7 8 7 .4 1 9 5 .4 5 9 6 .3 9 9 7 .3 9

S/N 240 220 160 320 330 340 290 380 340 420 440 270 320 310 440 700 330 620 420 590 400 710 310 700 270 670 590 340 460 180 300 450 380 470 180 350 370 260 410 420 300 200 140 220 200 230 120 93 100 160 80 100 250 310 230 270 240 340 470 430 490

2 9 .0 1 7 .7 2 1 .4 6 2 .6 4 2 .7 3 2 .7 9 1 .6 7 2 .5 1 2 .2 9 2 .6 4 2 .1 9 1 .5 0 2 .1 4 1 .8 5 3 .6 6 3 .6 0 1 .7 5 2 .9 6 1 .5 8 2 .0 7 2 .0 7 3 .1 1 1 .6 3 2 .3 8 1 .2 1 3 .3 5 2 .4 2 0 .8 5 1 .6 0 0 .9 9 0 .7 7 1 .3 1 1 .2 5 1 .8 1 0 .6 3 1 .2 1 1 .3 5 1 .1 3 1 .3 7 1 .2 3 1 .4 8 3 .0 1 1 .5 9 3 .8 4 2 .5 4 2 .9 8 1 .4 4 0 .8 6 1 .6 9 2 .5 7 1 .2 8 1 .1 7 1 .9 2 1 .7 5 1 .4 6 2 .1 1 1 .2 8 1 .5 2 2 .4 4 3 .7 8 3 .3 8

Detection DD DD md DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD nd DD DD nd DD nd nd nd nd DD nd nd md nd md nd md DD DD DD DD DD md nd DD DD nd nd DD DD md DD nd md DD DD DD

B l ( G) 169 -7 3 -1 3 0 -1 3 1 75 -1 0 8 204 -1 9 9 -2 3 8 -2 4 75 80 174 15 -7 0 -2 0 4 -2 1 1 -1 8 1 -2 1 8 -1 8 3 -2 1 7 -1 7 5 -2 3 3 -1 7 2 -1 8 2 -1 8 7 -1 4 9 -1 9 9 -7 9 66 -6 3 -5 9 43 146 84 44 40 -1 3 0 98 0 179 -3 7 5 -3 7 1 -9 6 -4 0 -3 9 -2 0 0 -2 9 0 -3 8 6 -3 3 3 -6 6 8 -2 1 4 78 156 -2 1 -1 7 3 85 137 113 -4 2 -1 2 7

( G) 19 20 139 55 62 53 60 48 55 55 58 102 59 84 43 21 44 22 44 31 34 20 45 24 73 20 26 136 40 96 90 51 49 38 128 63 58 75 46 45 62 56 93 55 51 46 99 276 118 78 194 144 79 46 75 59 92 45 35 42 31


M. Auriere et al.: Magnetic fields of weak-field Ap stars ` Table 3. continued.

23

Na m e 4 Cyg

HD 183056

204411

Psc

220825

Date 1 4 Au g 0 5 2 3 Au g 0 5 24 Jul 01 24 Jun 03 0 2 Au g 0 5 0 4 Au g 0 5 0 5 Au g 0 5 0 6 Au g 0 5 1 2 Au g 0 5 1 3 Au g 0 5 1 4 Au g 0 5 1 4 Au g 0 5 1 5 Au g 0 5 3 0 Au g 0 5 01 Sep 05 04 Jul 03 07 Jul 03 21 Jul 04 23 Jul 04 0 8 Au g 0 5 1 5 Au g 0 5 2 4 Au g 0 5 0 8 M ay 0 6 1 0 M ay 0 6 2 4 M ay 0 6 2 7 M ay 0 6 06 Jun 06 03 Jul 01 24 Jun 03 14 Jul 04 21 Jul 04 22 Jul 04 0 2 Au g 0 5 0 4 Au g 0 5 0 5 Au g 0 5 0 6 Au g 0 5 0 7 Au g 0 5 1 5 Au g 0 5 2 4 Au g 0 5

Julian 24535 24536 24521 24528 24535 24535 24535 24535 24535 24535 24535 24535 24535 24536 24536 24528 24528 24532 24532 24535 24535 24536 24538 24538 24538 24538 24538 24520 24528 24532 24532 24532 24535 24535 24535 24535 24535 24535 24536

Date 9 7 .4 3 0 6 .3 8 1 5 .4 9 1 5 .5 3 8 5 .4 7 8 7 .4 4 8 8 .4 3 8 9 .4 7 9 5 .4 2 9 6 .5 1 9 7 .4 7 9 7 .5 6 9 8 .4 1 1 3 .4 1 1 5 .4 0 2 5 .5 6 2 8 .5 8 0 8 .5 7 1 0 .4 8 9 1 .4 3 9 8 .4 5 0 7 .3 9 6 4 .6 5 6 6 .6 6 8 0 .5 6 8 3 .5 5 9 3 .6 3 9 4 .6 0 1 5 .6 2 0 1 .5 3 0 8 .6 0 0 9 .6 1 8 5 .6 2 8 7 .6 0 8 8 .5 5 8 9 .6 2 9 0 .5 2 9 8 .5 8 0 7 .5 1

S 4 3 2 2 5 4 4 4 5 5 5 5 4 5 5 3 3 2 2 2 4 3 2 3 4 2 4 2 2 4 2 1 4 4 5 5 5 4 3

/ 9 5 7 8 3 1 9 3 8 2 5 8 7 4 8 4 7 1 1 1 5 2 6 1 8 8 2 2 8 1 9 6 8 5 2 9 5 5 0

N 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0

2 3 .2 2 2 .3 6 6 .3 4 5 .2 8 3 .9 3 6 .3 0 3 .4 8 8 .7 9 1 1 .4 8 9 .1 4 3 .9 2 4 .6 8 9 .2 6 9 .3 4 3 .7 7 6 .0 2 6 9 .3 7 4 .6 4 4 .0 0 4 .9 7 9 .8 6 6 .9 5 4 .8 1 3 .1 3 1 3 .5 7 6 .1 6 7 .5 8 4 .8 5 9 .1 9 7 .2 3 5 .6 1 4 .6 4 8 .1 1 1 5 .5 0 5 .3 6 1 8 .0 8 1 4 .6 1 6 .0 1 7 .9 3

Detection DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD DD

B l ( G) -1 3 6 -2 1 -4 6 -3 4 1 281 -2 5 5 237 -2 6 5 -2 5 4 -2 5 9 226 268 -2 9 1 -1 7 7 290 -3 7 -3 3 -2 5 -8 7 -9 -6 8 -8 2 -8 7 -3 -2 8 -8 8 -7 5 -1 9 1 156 350 345 -3 1 -2 0 7 141 -2 8 5 133 299 -3 1 7 263

( G) 31 52 90 85 47 60 52 61 46 49 43 43 55 45 42 12 14 20 19 20 9 13 16 13 9 14 10 57 42 29 35 70 23 25 22 21 20 25 38