Julius Scheiner – 19th century extragalactic spectroscopy

Juluis Scheiner published a lot in German language and made a lot of solar and stellar research. I’m concentrating on his English production on extragalactic issues.

Scheiner (1898) studied the reason why nebular spectra sometimes showed Hβ lines while showing little or no Hα lines, which seemed to go against the common knowledge back then that Hα lines are brighter than Hβ lines. He had trouble of studying the phenomenon with spectrophotometers because they weren’t able to measure so faint light as needed in the study. He then made a remarkable experimental setup:

The Geissler tube was set up at the distance of distinct vision (or at a distance somewhat greater), and viewed with a direct-vision system of prisms, the capillary bore of the tube serving as a slit. Between the tube and the prism-system two Nicol prisms were introduced, one of which could be turned and its angular displacement measured. By turning this prism the hydrogen lines could be made to vanish.

With this setup, he found an interesting thing:

Then on weakening the light, there occurred, at a certain intensity, an apparent equality of the two lines, after which Hα disappeared and then Hβ.

Scheiner & Wilsing (1902) also studied some issues relating to different spectral lines and their intensities in nebulae.

Scheiner (1899) discussed the spectrum of the Andromeda nebula (Messier 31) and showed that it consisted of stars. He then proceeded to discuss the Milky Way in the light of that evidence:

The irregularities of the Milky Way, especially its streams, can be quite well accounted for, as Easton attempted to do, if they are regarded as a system of spirals and not as a ring system.

And further:

In spite of the unfavorable projection under which we see the Milky Way, it does not seem impossible to establish the spiral character of the principal forms, and, furthermore, to bring the proper motions of the stars of the Milky Way into relation with this.

Apparently, this spectrum of Scheiner of M31 was the first succesful spectrum of a galaxy (Rubin, 1995). There seemed to be some minor dispute with Edward Fath and Scheiner over the spectrum of M31 as discussed in Scheiner (1909).

Julius Scheiner links

MNRAS: Obituary
Wikipedia: Julius Scheiner

References

Rubin, 1995, ApJ, 451, 419, “A Century of Galaxy Spectroscopy”

Scheiner, 1898, ApJ, 7, 231, “On the Spectrum of Hydrogen in the nebulæ”

Scheiner, 1899, ApJ, 9, 149, “On the spectrum of the great nebula in Andromeda”

Scheiner, 1909, ApJ, 30, 69, “Note on the Spectrum of the Andromeda Nebula”

Scheiner & Wilsing, 1902, ApJ, 16, 234, “Determination of the intensity-ratios of the principal lines in the spectra of several gaseous nebulae”

UGC 05015 – QSO-galaxy pair

Arp (1980) discussed the companion galaxies of NGC 2859. One of the four discussed companions is UGC 05015 (object 1 in Figure 1). Specifically, Arp studied quasars near companion galaxies. He noted that UGC 05015 had an ultraviolet excess object in its vicinity. Arp studied it spectroscopically, and it turned out to be a quasar (object 2). Arp calculated the probability of 0.01 for a background quasar falling so close to UGC 05020 by chance.

Notes

Objects 3 and 4 have similar redshift, so they are probably physically associated with each other.


Figure 1. The objects with measured redshifts near of UGC 05015. Size of the image is 10 x 10 arcmin. Image is from Digitized Sky Survey (POSS2/UKSTU blue), and it has been adjusted for brightness and contrast to bring out the faint objects in the field.

Objects and their data

NBR NAME TYPE REDSHIFT MAG SEPARATION
1 UGC 05015 SABdm 0.005504 15.3 (g) 0
2 NGC 2859 U3 QSO 1.460000 20.5 (g) 1.263
3 SDSS J092603.02+341319.4 galaxy 0.157844 18.2 (g) 4.533
4 SDSS J092611.06+341320.9 galaxy 0.156371 18.8 (g) 5.785
5 SDSS J092612.57+342104.5 galaxy 0.086866 17.6 (g) 6.748

NED objects within 10′ from UGC 05015.

SDSS image of the system.

References

Arp, 1980, ApJ, 240, 415, “High-redshift objects near the companion galaxies to NGC 2859″

3C 345 – the quasar line

Most of the field around 3C 345 will be handled with NGC 6212, which is close to 3C 345, so here I will only deal with the discordant redshift issues that has been discussed in the scientific literature with 3C 345 as the central object. In addition 3C 345 has been a subject for a huge amount of studies so it makes sense to limit the scope here. Some general information is given in the introduction of Arp (1997). 3C 345 is variable in all wavelengths, has superluminal jet, and is among the earliest found quasars – to give a few reasons why it is so much studied object.

Arp (1997) studied the 3C 345 field as a discordant redshift system. First thing Arp noted was that there was an apparent concentration of quasars around 3C 345, and that the concentration forms a rough line across 3C 345. Arp said:

The first question that poses itself is whether the quasars in the concentration around 3C 345 are different from the quasars in the rest of the field. The answer is yes. The quasars in the rest of the field are fainter and generally of much higher redshift.

He then showed a sketch of the field (his Figure 2) showing only brightest (and lowest redshift) quasars of the field, and there is a clear concentration around 3C 345. The image shows the field so that it has 3C 345 area is in the left. Dividing the image in half shows 13 bright quasars in the 3C 345 side and 2 bright quasars in the other side. So it appears that Arp is correct that at least locally the bright quasars are concentrated to the area where 3C 345 lies (and NGC 6212, let’s not forget that).

Arp then emphasizes this point further by providing a plot of quasar density, again with the brightest quasars, near 3C 345 calculated within concentric circles around 3C 345. The plot shows an apparent trend so that density increases closer to 3C 345. Background density for the bright quasars in question is about 3 quasars per square degree according to Arp, and the density around 3C 345 is from 20 to almost 50 quasars per square degree. Arp says:

Therefore we can confidently compute that the over density close to 3C 345 reaches a factor of 15, falling away at greater distances to an indicated group diameter of the order of a degree.

Arp then discussed the X-ray properties of the quasars. He noted that the quasars are bright X-ray sources and he noted that the X-ray sources were well aligned across 3C 345. He calculated the chance projection probability of five X-ray sources in the line to be P = 3 x 10-8. Based on that he suggested that the quasars in the line were associated with 3C 345. All quasars in the line except one have discordant redshifts compared to 3C 345.

Arp also noted that all the quasars in the field fall close to preferred redshift peaks known as Karlsson peaks. Arp then discussed briefly of the role of NGC 6212 in this. His interpretation is that NGC 6212 has ejected 3C 345 which in turn has subsequently ejected other quasars. However, for some objects in the field he couldn’t say if they were ejected from NGC 6212 or 3C 345. He added further relating to the quantized redshifts:

It is also noticeable that the quasar redshifts on one side of the 3C 345/NGC6212 center, fall systematically higher than the quantized values, and those on the other side fall systematically lower. This effect is to be expected if quasars at quantized values are ejected toward and away from the observer from the center with projected velocities of some hundredths of c.

Notes

The 3C 345 field is within SDSS coverage area and it also has been thoroughly searched (and spectrographed) for quasars. Result is huge amount of objects, so only closest objects to 3C 345 (within 0.5 arcmin) and the objects discussed in the text are shown in Figure 1. Consult NED object list within 10 arcmin for more objects.

There is almost certainly a group of objects at 3C 345’s redshift. According to NED, there is 28 objects within 60 arcmin that have redshift between z = 0.5828 and z = 0.6028 (redshift of 3C 345 is given as 0.5928 so these limits are exactly 0.01 from 3C 345’s redshift to each direction). 26 of them are within 10 arcmin. This seems to suggest that there is a physically associated group of 26 objects in the field at z~0.59. Presence of a group of course makes all the alignments in the field more probable. It is also likely that this group has been discussed in the huge amount of studies on this system.


Figure 1. The field around 3C 345. Upper panel is from Digitized Sky Survey (POSS2/UKSTU Blue) and it has been adjusted for brightness and contrast to bring out faint objects. Width of the upper panel image is about 5 arcmin. Lower panel is a sketch where the positions of the objects have been adopted from Arp (1997) Figure 2. Rough area presented in upper panel has been indicated in lower panel by a gray box.

Objects and their data

NBR NAME TYPE REDSHIFT MAG SEPARATION
1 3C 345 QSO, HPQ, FSRQ 0.592800 16.6 (G) 0
2 SDSS J164259.37+394835.7 galaxy 0.588000 21.47 0.110
3 SDSS J164259.86+394818.0 galaxy 0.281300 23.86 0.375
4 SDSS J164257.38+394821.5 galaxy 0.531900 21.42 0.376
5 SDSS J164300.56+394825.6 galaxy 0.582200 21.01 0.386
6 SDSS J164257.00+394847.7 galaxy 0.412600 22.24 0.391
7 NGC 6212 Sb, Sy1 0.030281 14.7 (G) 4.678
8 [HB89] 1641+399 NED05 QSO 1.088540 19.0 (G) 6.116
9 [HB89] 1641+399 NED04 QSO 0.705320 18.1 (G) 6.992
10 [HB89] 1641+399 NED06 QSO, blazar 0.590692 19.2 (G) 8.627
11 [HB89] 1640+400 NED02 QSO 1.595930 19.7 (G) 11.322
12 [VCV2001] J164211.2+393836 QSO 0.625000 18.0 13.564
13 [HB89] 1641+396 NED01 QSO 1.414000 19.8 13.871
14 [HB89] 1640+401 QSO 1.002800 18.0 (G) 17.198
15 [HB89] 1642+400 QSO 1.376400 19.5 (G) 17.081
16 [HB89] 1640+396 QSO 0.539093 19.7 (G) 19.281
17 [HB89] 1640+395 QSO 1.466000 20.2 21.652
18 [HB89] 1642+401 QSO 1.268000 18.8 22.855
19 [VCV2001] J164338.7+400935 QSO 1.358000 19.5 22.283
20 [VCV2001] J164420.8+401128 QSO 0.610166 19.0 (G) 27.661

NED objects within 10′ from 3C 345 with redshifts available.

NED page for object 11.
NED page for object 12.
NED page for object 13.
NED page for object 14.
NED page for object 15.
NED page for object 16.
NED page for object 17.
NED page for object 18.
NED page for object 19.
NED page for object 20.

SDSS image of 3C 345 system.
SDSS page for object 1.
SDSS page for object 2.
SDSS page for object 3.
SDSS page for object 4.
SDSS page for object 5.
SDSS page for object 6.
SDSS page for object 7.
SDSS page for object 8.
SDSS page for object 9.
SDSS page for object 10.
SDSS page for object 11.
SDSS page for object 12.
SDSS page for object 13.
SDSS page for object 14.
SDSS page for object 15.
SDSS page for object 16.
SDSS page for object 17.
SDSS page for object 18.
SDSS page for object 19.
SDSS page for object 20.

References

Arp, 1997, A&A, 327, 479, “Concentration of quasars around the active extragalactic object 3C 345″

Redshift periodicity papers

Few years ago I compiled a list of papers relating to the quantized redshifts (or periodic redshifts, or preferred redshift peaks, or redshift bands, or…). I have previously posted it to a BAUT forum thread, but I decided to post it here as well. The list is not complete. It is probably quite thorough for older papers but there’s no papers that have been published after 2005. “Paper not available” in the list means that I couldn’t access the full text online (back then, I haven’t checked the situation currently). At some point, I might update this list to contain the newer papers as well. Note also that the subject is tied to a mainstream astronomy subject of large scale distribution of galaxies. There is a huge amount of papers on that subject, and only some of them are included to this list (those that seemed to concentreate on the periodicity issues), starting from Broadhurst et al. (1990). Here goes:

On the Wavelengths of the Absorption Lines in Quasi-Stellar Objects – Burbidge, Geoffrey (1967)

Limits to the Distance of the Quasi-Stellar Objects Deduced from Their Absorption Line Spectra – Burbidge, G. R.; Burbidge, E. M. (1967)

On the Nature of "standard" Absorption Spectrum of the Quasi-Stellar Objects – Shklovsky, J. (1967)

Concerning Redshifts in the Spectra of Quasi-Stellar Objects – Cowan, Clyde L. (1968)

The Distribution of Redshifts in Quasi-Stellar Objects, N-Systems and Some Radio and Compact Galaxies – Burbidge, Geoffrey (1968)

- Cowan, Clyde L. (1969) Nature, 224, 665

- Plagemann, S. H., Feldman, P. A. and Gribben, J. R. (1969) Nature, 224, 875

- Deeming, T. J. (1970) Nature, 225, 620

- Coles, W. A. (1970) unpublished

- Wesselink, A. J. (1970) Nature, 225, 927

QSO redshifts-Possible selection effect – Roeder, R. C. (1971) (paper not available)

Possible Discretization of Quasar Redshifts – Karlsson, K. G. (1971)

Some Trends in the Red-Shift Distribution of Quasi-Stellar Objects and Related Peculiar Galaxies – Basu, D.; Abdu, M. A. (1972)

An Analysis of the Distribution of Redshifts of Quasars and Emission-Line Objects – Lake, R. G.; Roeder, R. C. (1972)

Quasars-Effects of Earth’s atmosphere on redshift measurements – Roeder, R. C.; Dyer, C. C. (1972) (paper not available)

The Correlation of Redshift with Magnitude and Morphology in the Coma Cluster – Tifft, W. G. (1972)

The Distribution of Redshifts of Quasi-Stellar Objects and Related Emission-Line Objects – Burbidge, G. R.; O’dell, S. L. (1972)

Quasars-Selection effects and the nature of redshifts – Karlsson, K. G. (1973) (paper not available)

Properties of the redshift-magnitude bands in the Coma cluster – Tifft, W. G. (1973)

Redshift-Magnitude Bands, Quasi-Stellar Sources, and Systems of Redshift – Tifft, W. G. (1973)

QSOs-Selection in redshift measurement – Basu, D. (1973) (paper not available)

A Quantitative Alternative to the Cosmological Hypothesis for Quasars – Bell, Morley B.; Fort, David N. (1973)

The Distribution of Redshifts of Radio Galaxies with Different Optical Spectra and Forms – Burbidge, G. R.; O’dell, S. L. (1973)

Redshift Magnitude Bands for Quasistellar Sources – Veron, P.; Veron, M. P. (1974)

Remarks on the Magnitude-Redshift Bands in the Coma Cluster – Barnothy, Jeno M.; Barnothy, Madeleine F. (1974)

Fine Structure Within the Redshift-Magnitude Correlation for Galaxies – Tifft, W. G. (1974)

The definition, visibility, and significance of redshift-magnitude bands – Tifft, W. G. (1974)

Distribution of quasars in the universe – Schmidt, M. (1974) (paper not available)

On the Significance of Periodicities in the Observed Quasar Redshifts and in the Intrinsic Redshift Components as Computed from Bell and Fort’s Quasar Model – Corso, G. J.; Barnothy, J. M. (1975)

Possible effect of misidentification of QSOs on the redshift distribution – Basu, D. (1975) (paper not available)

The NGC 507 cluster of galaxies – Tifft, W. G.; Hilsman, K. A.; Corrado, L. C. (1975)

The distribution of redshifts of quasars and related objects – Knight, J. W.; Sturrock, P. A.; Switzer, P. (1976)

Critique of Bell and Fort’s quasar model – Barnothy, J. M.; Corso, G. J. (1976)

Discrete states of redshift and galaxy dynamics. I – Internal motions in single galaxies – Tifft, W. G. (1976)

On the redshift distribution of quasi-stellar objects – Wills, D.; Ricklefs, R. L. (1976)

The ln(l+z) Periodicity in the Redshifts of Quasars – Barnothy, M. F.; Barnothy, J. M. (1976)

Periodicity in the ln/1+z/ distribution of quasars – Barnothy, J. M.; Barnothy, M. F. (1976)

On the reality of periodicities in the redshift distribution of emission-line objects – Green, R. F.; Richstone, D. O. (1976)

Redshift-magnitude bands in clusters of galaxies – Tifft, W. G. (1977) (paper not available)

Discrete states of redshift and galaxy dynamics. II – Systems of galaxies – Tifft, W. G. (1977)

Discrete states of redshift and Galaxy dynamics. III – Abnormal galaxies and stars – Tifft, W. G. (1977)

Distortion of Galaxy Radial Velocity Measurements by the Night Sky Spectrum – Simkin, S. M. (1977)

On the existence of significant peaks in the quasar redshift distribution – Karlsson, K. G. (1977)

Gaps in the emission line redshift distribution of QSOs – Basu, D. (1977)

On the In (I + z) Periodicity in QSO Redshifts – Wills, D. (1977)

A trend in the gaps in redshift distribution of QSOs – Basu, D. (1978)

On the periodicity in the distribution of quasar redshifts – Kjaergaard, P. (1978) (paper not available)

The Simkin effect – Tifft, W. G. (1978)

The discrete redshift and asymmetry in H I profiles – Tifft, W. G. (1978)

The absolute solar motion and the discrete redshift – Tifft, W. G. (1978)

Redshift-magnitude bands and the evolution of galaxies. I – New observations – Tifft, W. G. (1978)

Redshift-magnitude bands and the evolution of galaxies. II – Data analysis – Tifft, W. G. (1978)

Band theory applied to the Coma/A1367 supercluster – Tifft, W. G.; Gregory, S. A. (1979)

Structure within redshift-magnitude bands – Morphological evolution – Tifft, W. G. (1979)

Periodicity in the redshift intervals for double galaxies – Tifft, W. G. (1980)

Absorption line redshift distribution of QSOs – Basu, D. (1980)

An analysis of the redshift-magnitude band phenomenon in the Coma Cluster – Nanni, D.; Pittella, G.; Trevese, D.; Vignato, A. (1981)

The periodicity in the distribution of quasar redshifts and the density perturbations in the early universe – Fang, L.-Z.; Chu, Y.-Q.; Liu, Y.; Cao, C. (1982)

Quantum effects in the redshift intervals for double galaxies – Tifft, W. G. (1982)

Double galaxy investigations. II – The redshift periodicity in optically observed pairs – Tifft, W. G. (1982)

The cosmic density wave and its observable vestige – Liu, Y.-Z. (1982)

Effect of search lines on emission and absorption redshift distribution of QSOs – Basu, D. (1983)

Distribution of gaps in emission line redshifts of QSOs – Basu, D. (1983)

Redshift quantization in compact groups of galaxies – Cocke, W. J.; Tifft, W. G. (1983)

The effects of emission line identification on the redshift distribution of QSO’s – Zhou, Y.-Y.; Deng, Z.-G.; Zhou, Z.-L. (1983)

The distribution of quasar emission-line redshifts – Box, T. C.; Roeder, R. C. (1984)

The distribution of absorption line redshifts of quasars and its origin – Chu, Y.; Fang, L.; Liu, Y. (1984) (paper not available)

Status of Quantized Extragalactic Redshifts – Tifft, W. G.; Cocke, W. J. (1984)

Double galaxy redshifts and dynamical analyses – Sharp, N. A. (1984)

Global redshift quantization – Tifft, W. G.; Cocke, W. J. (1984)

Double galaxy investigations. III – The differential redshift distribution and emission-line correlations – Tifft, W. G. (1985)

Theory and interpretation of quantized extragalactic redshifts – Cocke, W. J. (1985)

The redshift distribution law of quasars revisited – Depaquit, S.; Pecker, J.-C.; Vigier, J.-P. (1985)

Emission line redshift distribution of QSOs – Zhou, Y.-Y.; Deng, Z.-G.; Dai, H.-J. (1985)

The distribution of emission line redshift of QSOs – Basu, D. (1985)

Relativistic realization of a proposed model of quantized redshift – Nieto, M. M. (1986) (paper not available)

Results from high precision 21-cm redshift measurements – Cocke, W. J.; Tifft, William G. (1987) (paper not available)

Quantized galaxy redshifts – Tifft, William G.; Cocke, W. John (1987) (paper not available)

Additional members of the Local Group of galaxies and quantized redshifts within the two nearest groups – Arp, Halton (1987)

Quantized Redshifts are Real – Tifft, W. G. (1987) (paper not available)

A different approach to the cosmological quantized redshift problem – Buitrago, J. (1988) (paper not available)

Quantization of redshift differences in isolated galaxy pairs – Tifft, W. G.; Cocke, W. J. (1989)

The periodicity in the redshift distribution of the Lyman-alpha forest – Chu, Yaoquan; Zhu, Xingfen (1989)

Double galaxy redshifts and the statistics of small numbers – Newman, William I.; Haynes, Martha P.; Terzian, Yervant (1989)

Redshift quantization in the Ly-alpha forest and the measurement of q(0) – Cocke, W. J.; Tifft, W. G. (1989)

Periodicities in galaxy redshifts – Croasdale, Martin R. (1989)

Periodicity of quasar redshifts – Arp, H.; Bi, H. G.; Chu, Y.; Zhu, X. (1990)

Deviation from periodicity in the large-scale distribution of galaxies – Kurki-Suonio, H.; Mathews, G. J.; Fuller, G. M. (1990)

Large-scale distribution of galaxies at the Galactic poles – Broadhurst, T. J.; Ellis, R. S.; Koo, D. C.; Szalay, A. S. (1990) (paper not available)

The Virgo cluster as a test for quantization of extragalactic redshifts – Guthrie, B. N. G.; Napier, W. M. (1990)

Double galaxy redshifts and dynamical analyses. II – Sample comparisons – Sharp, N. A. (1990)

A large-scale periodic clustering of galaxies as a result of hydromagnetic ringing of gas in a recombination ERA of the expanding universe – Fujimoto, Mitsuaki (1990)

The redshift peak at Z = 0.06 – Burbidge, G.; Hewitt, A. (1990)

Periodicity of redshift distribution in a T-3 universe – Fang, Li-Zhi (1990)

Oscillating universe – The periodic redshift distribution of galaxies with a scale 128/h megaparsecs at the galactic poles – Morikawa, Masahiro (1990)

Quasar redshifts and nearby galaxies – Karlsson, K. G. (1990)

Can oscillating physics explain an apparently periodic universe? – Hill, Christopher T.; Steinhardt, Paul J.; Turner, Michael S. (1990) (paper not available)

Claims for periodicity in quasar redshifts – Scott, Douglas (1991)

Statistical procedure and the significance of periodicities in double-galaxy redshifts – Cocke, W. J.; Tifft, W. G. (1991)

Coherent peculiar velocities and periodic redshifts – Hill, Christopher T.; Steinhardt, Paul J.; Turner, Michael S. (1991)

Universe with oscillating expansion rate – Morikawa, Masahiro (1991)

Quasi-periodicity in deep redshift surveys – van de Weygaert, Rien (1991)

Against the Delta-ln(1 + z) of about 0.205 periodicity in quasar redshifts – Scott, D. (1991)

Large-scale structure in the Lyman-alpha forest – Fang, L. Z. (1991)

Periodic universe and condensate of pseudo-Goldstone field – Anselm, A. A. (1991)

Quasi-periodic structures in the large-scale galaxy distribution and three-dimensional Voronoi tessellation – Ikeuchi, Satoru; Turner, Edwin L. (1991)

Evidence for redshift periodicity in nearby field galaxies – Guthrie, B. N. G.; Napier, W. M. (1991)

Power-spectrum analysis of one-dimensional redshift surveys – Kaiser, N.; Peacock, J. A. (1991)

Superclusters and pencil-beam surveys – The origin of large-scale periodicity – Bahcall, Neta A. (1991)

Large-scale periodicity – Problems with cellular models – Williams, B. G.; Heavens, A. F.; Peacock, J. A. (1991)

Properties of the redshift. III – Temporal variation – Tifft, W. G. (1991)

Velocity differences in binary galaxies. I – Suggestions for a nonmonotonic, two-component distribution – Schneider, Stephen E.; Salpeter, Edwin E. (1992)

Statistical tests of peaks and periodicities in the observed redshift distribution of quasi-stellar objects – Duari, Debiprosad; Gupta, Patrick D.; Narlikar, Jayant V. (1992)

Possible geometric patterns in 0.1c scale structure – Tully, R. B.; Scaramella, Roberto; Vettolani, Giampaolo; Zamorani, Giovanni (1992)

Statistical methods for investigating periodicities in double-galaxy redshifts – Cocke, W. J. (1992)

Statistical properties of the sky distribution of extragalactic infrared sources – Source-number fluctuations and density peaks – Fabbri, R. (1992)

The distribution of rich clusters of galaxies in the south Galactic pole region – Guzzo, Luigi; Collins, Chris A.; Nichol, Robert C.; Lumsden, Stuart L. (1992)

Large-scale periodicity and Gaussian fluctuations – Dekel, Avishai; Blumenthal, George R.; Primack, Joel R.; Stanhill, David (1992)

The peaks and gaps in the redshift distributions of active galactic nuclei and quasars – Kruogovenko, Andrei A.; Orlov, Viktor V. (1992)

A new method for the detection of a periodic signal of unknown shape and period – Gregory, P. C.; Loredo, Thomas J. (1992)

Cosmological parameters and redshift periodicity – Holba, Agnes; Horvath, I.; Lukacs, B.; Paal, G. (1992)

Redshift quantization in the cosmic background rest frame – Tifft, W. G.; Cocke, W. J. (1993)

The clustering of QSOs at low redshift – Boyle, B. J.; Mo, H. J. (1993)

Upper limit on periodicity in the three-dimensional large-scale distribution of matter – Tytler, David; Sandoval, John; Fan, Xiao-Ming (1993)

High-resolution simulation of deep pencil beam surveys – analysis of quasi-periodicity – Weiss, A. G.; Buchert, T. (1993)

Can Extra Power Explain Periodicity on Large Scales? – Luo, Shan; Vishniac, Ethan T. (1993)

Quasi-periodical structures in the galaxy populations – Mass and luminosity functions for the cluster galaxies – Litvin, V. F.; Holzmann, F. M.; Smirnov, A. V.; Taibin, B. S.; Orlov, V. V.; Baryshnikov, V. N. (1993)

Apparently periodic Universe – Busarello, G.; Capozziello, S.; de Ritis, R.; Longo, G.; Rifatto, A.; Rubano, C.; Scudellaro, P. (1994)

Redshift data and statistical inference – Newman, William I.; Haynes, Martha P.; Terzian, Yervant (1994)

Once more on quasar periodicities – Holba, Agnes; Horvath, I.; Lukacs, B.; Paal, G. (1994) (paper not available)

Redshift Quantization – A Review – Tifft, W. G. (1995) (paper not available)

The Spontaneous Violation of the Cosmological Principle and the Possible Wave Structures of the Universe – Budinich, P.; Nurowski, P.; Raczka, R.; Ramella, M. (1995)

Global Redshift Periodicities: Association with the Cosmic Background Radiation – Cocke, W. J.; Tifft, W. G. (1996) (paper not available)

Evidence for quantized and variable redshifts in the cosmic backgroung rest frame – Tifft, W. G. (1996) (paper not available)

Statiscal analysis of the occurrence of periodicities in galaxy redshift data – Cocke, W.; Devito, C.; Pitucco, A. (1996) (paper not available)

Redshift periodicity in the Local Supercluster – Guthrie, B. N. G.; Napier, W. M. (1996)

Testing for quantized redshifts. I. The project – Napier, W. M.; Guthrie, B. N. G. (1996) (paper not available)

Testing for quantized redshifts. II. The Local Supercluster – Napier, W. M.; Guthrie, B. N. G. (1996) (paper not available)

The 37.5 km s-1 redshift periodicity of galaxies as the machion frequency – Arp, Halton (1996)

Galactic periodicity and the oscillating G model – Salgado, Marcelo; Sudarsky, Daniel; Quevedo, Hernando (1996)

Global Redshift Periodicities and Periodicity Structure – Tifft, W. G. (1996)

The Periodic Distribution of Redshifts – Carvalho, J. C. (1997) (paper not available)

Global Redshift Periodicities and Periodicity Variability – Tifft, W. G. (1997)

The redshift periodicity of galaxies as a probe of the correctness of general relativity – Valerio Faraoni (1997)

A 120 MPC Periodicity in the Three-Dimensional Distribution of Galaxy Superclusters – Einasto, J.; Einasto, M.; Gottloeber, S.; Mueller, V.; Saar, V.; Starobinsky, A. A.; Tago, E.; Tucker, D.; Andernach, H.; Frisch, P. (1997)

A study of the large-scale distribution of galaxies in the South Galactic Pole region – II. Further evidence for a preferential clustering scale? – Ettori, S.; Guzzo, L.; Tarenghi, M. (1997)

Redshift Quantization in the Cosmic Background Rest Frame – Tifft, W. G. (1997)

The Possible Redshift Clumping of Damped Lyman-alpha Absorbers – Gal, R.; Djorgovski, S. G. (1997)

Quantized Redshifts: A Status Report – Napier, W. M.; Guthrie, B. N. G. (1997)

The supercluster-void network – II. an oscillating cluster correlation function – Einasto, J.; Einasto, M.; Frisch, P.; Gottlober, S.; Muller, V.; Saar, V.; Starobinsky, A. A.; Tago, E.; Tucker, D.; Andernach, H. (1997)

Periodicity in the Redshift Distribution of Quasi Stellar Objects – Duari, Debiprosad (1997)

Periodicity revealed by statistics of the absorption-line redshifts of quasars – Liu, Yong-Zhen; Hu, Fu-Xing (1998)

The spatial and temporal distribution of matter in the redshift interval z = 1.2-3.2 – Ryabinkov, A. I.; Varshalovich, D. A.; Kaminker, A. D. (1998) (paper not available)

Periodicity in quasar redshifts or selection effects? – Basu, D. (1999) (paper not available)

Clustering Properties of Low-Redshift QSO Absorption Systems Toward the Galactic Poles – vanden Berk, Daniel E.; Lauroesch, James T.; Stoughton, Chris; Szalay, Alexander S.; Koo, David C.; Crotts, Arlin P. S.; Blades, J. Chris; Melott, Adrian L.; Boyle, Brian J.; Broadhurst, Thomas J.; York, Donald G. (1999)

Galaxy Clustering and Large-Scale Structure from z=0.2 to z=0.5 in Two Norris Redshift Surveys – Small, Todd A.; Ma, Chung-Pei; Sargent, Wallace L. W.; Hamilton, Donald (1999)

Space-time distributions of QSO absorption systems – Kaminker, A. D.; Ryabinkov, A. I.; Varshalovich, D. A. (2000)

Spatial structure and periodicity in the Universe – González, J. A.; Quevedo, H.; Salgado, M.; Sudarsky, D. (2000)

The Distribution of Redshifts in New Samples of Quasi-stellar Objects – Burbidge, G.; Napier, W. M. (2001)

Periodicity versus selection effects in the redshift distribution of QSOs – Basu, D. (2001) (paper not available)

Electrostatic interaction energy and factor 1.23 – Rubcic, A.; Arp, H.; Rubcic, J. (2002)

No Periodicities in 2dF Redshift Survey Data – E. Hawkins, S.J. Maddox, M.R. Merrifield (2002)

Quantum Perturbative Approach to Discrete Redshift – Mark D. Roberts (2002)

The supercluster-void network V.. The regularity periodogram – Saar, E.; Einasto, J.; Toomet, O.; Starobinsky, A. A.; Andernach, H.; Einasto, M.; Kasak, E.; Tago, E. (2002) (paper not available)

Redshift periodicities, The Galaxy-Quasar Connection – Tifft, W. G. (2003) (paper not available)

The Sources of Gamma-Ray Bursts and Their Connections with QSOs and Active Galaxies – Burbidge, G. R. (2003) (paper not available)

Is the Redshift Clustering of Long-Duration Gamma-Ray Bursts Significant?
- J. S. Bloom (2003)

The detection of periodicity in QSO data sets – Napier, W. M.; Burbidge, G. (2003) (paper not available)

Discrete Components in the Radial Velocities of ScI Galaxies – M.B. Bell, S.P. Comeau, D.G. Russell (2004)

Large Scale Periodicity in Redshift Distribution – K. Bajan, M. Biernacka, P. Flin, W. Godlowski, V. Pervushin, A. Zorin (2004)

Distances of Quasars and Quasar-Like Galaxies: Further Evidence that QSOs may be Ejected from Active Galaxies – M. B. Bell (2004)

Selection Effects in the Redshift Distribution of Gamma-Ray Bursts and Associated Quasi-stellar Objects and Active Galaxies – Basu, D. (2005) (paper not available)

Periodicities of Quasar Redshifts in Large Area Surveys – H. Arp, C. Fulton, D. Roscoe (2005)

Evidence for Cosmological Oscillations in the Gold SnIa Dataset – R. Lazkoz, S. Nesseris, L. Perivolaropoulos (2005)

Critical Examinations of QSO Redshift Periodicities and Associations with Galaxies in Sloan Digital Sky Survey Data – Su Min Tang, Shuang Nan Zhang (2005)

3C 303 – a nearby QSO with possible radio bridge

Kronberg (1976) studied the radio structure of 3C 303 field. Kronberg noted:

Also visible is a low brightness extension of the western component toward the southwest. This extension is approximately superposed on a ~19.5 mag object at ([alpha] = 14h41m22s68, [sigma] = 52[degrees]14′18″0) which is clearly visible in Figure 1 and which we shall call object C.

At that time, object C (object 2 in figure 1) wasn’t yet identified, but there were some spectral knowledge from Burbidge indicating it was not a star or a normal radio galaxy nucleus. Kronberg also showed that there were two other objects very close to object C and that all three objects showed ultraviolet excess. Object that Kronberg called G was best positioned with the end of the radio extension (or rather the second component of the double radio source). Kronberg et al. (1977) published further radio observations and spectra observations. They said on the radio extension:

The existence of the faint features between the two main radio components strongly suggests that the latter are physically connected and are not just a chance superposition of unrelated radio systems (Kronberg 1976).

Kronberg et al. (1977) measured the spectrum of the object C. It turned out to be a quasar with redshift of z = 1.57. They then discussed the possible explanations of the system, one question being if the object C was in the background. They calculated the probability for the chance projection of object C to be about 0.001. Their analysis showed that there were no satisfactory explanation with the information available at that point.

Lonsdale et al. (1983) produced new radio maps of the field. The maps didn’t show much association between the radio sources and the quasar, but they showed that Kronberg’s object G was likely to be associated with the other radio component (commonly referred to as a radio hotspot). Arp (1987) mentioned this system as an example of a possible bridge between lower and higher redshift objects.

Meisenheimer et al. (1997) studied the system in infrared. They detected the bridge between the two radio sources. They weren’t able to determine if the object G was the one associated with the radio hotspot but it seemed very probable as the object G showed the similar structure as the radio hotspot. They concluded that the radio hotspot candidate was not actual radio hotspot, but just a bright knot in the jet of 3C 303. Lähteenmäki & Valtaoja (1999) made some observations that showed that the object G is indeed the optical object that corresponds to the radio hotspot. They didn’t find any connection with the quasar (object C).

Kataoka et al. (2003) studied the system in X-rays. They first showed a radio image of the system where the quasar seems to lie within the general radio feature of the system. Their X-ray image shows the quasar to be “in touch” with the radio hotspot (which in turn is clearly bridged to 3C 303 in radio image) but it is impossible to say that the apparent connection would be anything else than an overlapping effect.

Notes

Objects 4 (cz = 26791 km/s) and 9 (cz = 26806 km/s) have lower redshift than 3C 303. They also have similar redshift to each other, and there’s one more object (SDSS J144314.14+515610.0, cz = 26823 km/s) little outside the pictured field in figure 1 that has similar redshift. They form a probable galaxy group with mean redshift of cz = 26807 km/s. Group’s redshift dispersion is very small, maximum dispersion is only 16 km/s. Object 9 has almost exactly the mean redshift and is brightest of the three, so it would be natural main galaxy candidate for the group. On the other hand, object 4 has largest major diameter (0.33 against 0.25 and 0.12 of objects 9 and the one outside the field respectively). If object 4 would be the main galaxy, the other group members would have slightly higher redshift than the redshift of the main galaxy.

There are three objects that have similar redshift as 3C 303 (cz = 42327 km/s): object 3 (cz = 42049 km/s), object 5 (cz = 42931 km/s), and object 7 (cz = 42574 km/s). They form a probable galaxy group with mean redshift of cz = 42470 km/s. Group’s redshift dispersion is 461 km/s at maximum. There are two good main galaxy candidates; 3C 303 is brightest and object 7 has largest major diameter. Both of these objects are closest to the mean redshift of the group (object 7 being the closest to the mean). Object 3 is smallest and faintest but has lowest redshift.

There is a line of four objects; object 6 (z = 0.43), 3C 303 (z = 0.14), object 3 (z = 0.14), and object 5 (z = 0.14). Line is very straight and one of the objects has discordant redshift (object 6). There is a similar situation with objects 9 (z = 0.09), 4 (z = 0.09), and 8 (z = 0.16), but there object 8 is slightly off the line.


Figure 1. The field around 3C 303. Size of the image is 10 x 10 arcmin. Image is from Digitized Sky Survey (POSS2/UKSTU Blue) and it has been adjusted for brightness and contrast to bring out faint objects.

Objects and their data

NBR NAME TYPE REDSHIFT MAG SEPARATION
1 3C 303 N galaxy, BLRG 0.141186 17.6 (G) 0
2 3C 303C QSO 1.570000 19.97 0.275
3 SDSS J144301.15+520153.9 galaxy 0.140261 19.6 (G) 0.373
4 SDSS J144317.79+520209.5 galaxy 0.089365 17.6 (G) 2.374
5 SDSS J144251.74+520321.6 galaxy 0.143201 17.9 (G) 2.429
6 SDSS J144313.85+515946.6 galaxy 0.433745 21.2 (G) 2.512
7 SDSS J144313.09+520356.4 galaxy 0.142013 17.9 (G) 2.811
8 SDSS J144307.10+520440.0 galaxy 0.157260 18.6 (G) 3.119
9 SDSS J144326.46+515953.4 galaxy 0.089415 17.3 (G) 4.038

NED objects within 10′ from 3C 303 with redshifts available.

SDSS image of 3C 303 system.

References

Arp, 1987, IAUS, 124, 479, “Observations requiring a non-standard approach”

Kataoka et al., 2003, A&A, 399, 91, “Chandra detection of hotspot and knots of 3C 303″

Kronberg, 1976, ApJ, 203, 47, “3C 303: a source with unusual radio and optical properties”

Kronberg et al., 1977, ApJ, 218, 8, “The radio structure and optical field of 3C 303″

Lonsdale et al., 1983, MNRAS, 202, 1, “The radio structure of 3C303 at 408 MHz”

Lähteenmäki & Valtaoja, 1999, AJ, 117, 1168, “Optical Polarization and Imaging of Hot Spots in Radio Galaxies”

Meisenheimer et al., 1997, A&A, 325, 57, “The synchrotron spectra of radio hot spots. II. Infrared imaging”

53W 003 – lot of high-z objects

Pascarelle et al. (1998) reported about a population of objects at z ~ 2.4 in the field containing 53W 003. They suggested that there’s a large scale structure at that redshift. This was followed up by many studies, such as Keel et al. (1999), who show individual images of the objects and a nice map of the field. They also reported a finding of two quasars in the field (objects 6 and 11 in Figure 1 here) having similar redshift as the large scale structure.

Arp (1999) discussed this system as discordant redshift system. Arp noted that the two quasars found by Keel et al. were aligned across 53W 003 and separated from the other group of similar redshift objects. Arp discussed some properties of 53W 003 and noted:

The first important point for this paper, however, is that such galaxies are rare, and finding one this close to a very unusual grouping of high redshift objects is clearly noteworthy.

Arp showed that there were only three medium redshift quasars in the Her I and Her II fields and two of them fell close to 53W 003 (but outside the field presented in figure 1). Third fell close to another similar galaxy as 53W 003. Arp also noted that there seemed to be more quasars near 53W 003 than average density would suggest. The shape of the high redshift objects near 53W 003 also caught Arp’s eye:

All our empirical experience would indicate that the most luminous galaxies are massive, relaxed, equilibrium forms. But in the 53W003 field, as in the typical Hubble Deep Field, there is a preponderance of blue, irregular-shaped objects, which I would argue is prima facie evidence for low-luminosity, intrinsically redshifted young matter in various stages of compactness.

Notes

There are lot of faint objects in the field with redshifts available from The Bright Ages Survey. They are difficult to locate exactly from the DSS image presented here, so most of them have been left out from Figure 1 but at least a few closest to 53W 003 are indicated (objects 3, 4, and 5). Interested readers can check them from NED list of objects within 10′ from 53W 003 with redshifts available.

Object 8 is not the big elliptical object, but it is some very faint object in its vicinity.


Figure 1. The field around 53W 003. Size of the image is 10 x 10 arcmin. Image is from Digitized Sky Survey (POSS2/UKSTU Blue), and it has been adjusted for brightness and contrast to bring out the faint objects.

Objects and their data

NBR NAME TYPE REDSHIFT (cz) MAG SEPARATION
1 53W 003 galaxy pair 0.050000 (14990 km/s) - 0
2 2MASX J17141672+5018167 galaxy 0.045300 (13581 km/s) 13.8 (K) 0.065
3 BAS 1714+5015 M133 IrS 0.045700 (13701 km/s) 17.1 (K) 0.242
4 BAS 1714+5015 M052 galaxy 1.088000 19.2 (K) 0.363
5 BAS 1714+5015 M057 galaxy 0.046000 (13790 km/s) 20.0 (K) 0.494
6 [KCW99] 04 QSO BLAGN 2.393000 24.37 0.706
7 [WBM91] 2 galaxy 2.388000 22.50 2.801
8 [PWK98] 008 galaxy 2.386000 25.6 2.803
9 53W 002d galaxy sp+comp 0.275000 19.63 3.830
10 53W 002c galaxy sp+bar 0.273000 19.81 3.887
11 [KCW99] 02 QSO 2.381000 23.31 4.499
12 53W 002e galaxy sp+comp 0.528000 20.53 4.606

NED objects within 10′ from 53W 003 with redshifts available.

References

Arp, 1999, ApJ, 525, 594, “The Distribution of High-Redshift (z>~2) Quasars near Active Galaxies”

Keel et al., 1999, AJ, 118, 2547, “Evidence for Large-Scale Structure at z ~ 2.4 from Lya Imaging”

Pascarelle et al., 1998, AJ, 116, 2659, “Compact Lyalpha-emitting Candidates at Z ~= 2.4 in Deep Medium-Band Hubble Space Telescope WFPC2 Images”

UGC 05020 – High-z companion, QSO, pair, line

Arp (1980) discussed the companion galaxies of NGC 2859. One of the four discussed companions is UGC 05020 (object 1 in Figure 1). Specifically, Arp studied quasars near companion galaxies. He noted that UGC 05020 had an ultraviolet excess object in its vicinity. Arp studied it spectroscopically, and it turned out to be a quasar (object 2). Arp calculated the probability of 0.01 for a background quasar falling so close to UGC 05020 by chance.

Arp also noted the presence of the apparent companion galaxy (object 3). He said:

…, it is noticeable that a second galaxy, nearly as bright, lies close by to the southwest. The comparable brightness, the closeness, and above all the signs of interaction naturally led to the assumption that these two galaxies were at the same distance. It was a considerable surprise therefore when the spectrum of this second component clearly exhibited a much larger redshift of z = 7442 km s-1.

Arp then mentioned that the redshift difference of UGC 05020 and object 3 is similar to the redshift differences found in Stephan’s quintet. He studied the spectrum of object 3 and noted that some spectral features didn’t fit to a large background galaxy and that some features were similar to typical small companion galaxies. Arp concluded:

We see that there are several kinds of evidence which indicate that the z = 7,442 km s-1 galaxy is also physically associated with an NGC 2859 companion and therefore at the same distance.

New evidence

Objects 6 and 7 are roughly aligned across UGC 05020. The alignment is quite closely along the minor axis of UGC 05020. Objects 6 and 7 have almost the same redshift, but not quite close enough to be clearly a galaxy pair (the radial velocity difference is about 2700 km/s). Their distance from UGC 05020 is similar, so is their appearance, and their G band magnitude is the same.

Objects 2 and 10 form a line that is very accurately aligned with the nucleus of UGC 05020. They are both quasars with redshifts over 2. Lower redshift quasar is closer to UGC 05020, though, which would go against decreasing redshift hypothesis. Object 5 also falls close to the line, and it also is a quasar but with lower redshift. It is interesting to note that within 9 arcminutes from UGC 05020 we have three objects that are labelled as QSO’s in NED and all those three are quite accurately in same direction from UGC 05020. There’s a fourth quasar (SDSS J092548.59+344809.1, z = 0.5405) slightly outside of the field shown in Figure 1. It is not exactly in the same direction, but quite close (it is roughly in the same direction as object 6). On the other side, object 4 also falls to the line, but is not similar to other objects.

In summary, we have here:

- a quasar that is very close to the main galaxy.
- a higher redshift companion galaxy, and the situation is very similar to that of NGC 1232 and NGC 1232A.
- a pair of very similar higher redshift objects aligned along the minor axis of the main galaxy.
- a line of quasars from the main galaxy containing all the nearby quasars.

Notes

There’s no sign of a bridge between UGC 05020 and object 3 or object 2 in DSS os SDSS images.


Figure 1. Objects with available redshift near UGC 05020 (all objects within 9 arcmin are presented). The arrow at lower right points to the approximate direction of NGC 2859. Size of the image is 15 x 15 arcmin. Image is from Digitized Sky Survey (POSS2/UKSTU Blue) and it has been adjusted for brightness and contrast to bring out fainter objects more clearly.

Objects and their data

NBR NAME TYPE REDSHIFT (cz) MAG SEPARATION
1 UGC 05020 Scd 0.005420 (1625 km/s) 14.9 (g) 0
2 NGC 2859 U2 QSO 2.250000 19.2 (g) 1.008
3 MCG +06-21-036 Sc 0.024177 (7248 km/s) 15.8 (g) 1.607
4 SDSS J092616.68+343708.6 galaxy 0.150899 18.8 (g) 3.744
5 SDSS J092542.32+344108.6 QSO 1.066320 16.5 (g) 4.390
6 SDSS J092549.67+344439.7 galaxy 0.080995 (24282 km/s) 17.7 (g) 5.972
7 SDSS J092606.74+343240.7 galaxy 0.071833 (21535 km/s) 17.7 (g) 6.616
8 SDSS J092527.26+343917.7 galaxy 0.235684 18.8 (g) 7.039
9 SDSS J092533.04+343441.0 galaxy 0.017219 (5162 km/s) 17.0 (g) 7.398
10 SDSS J092527.51+344357.7 QSO 2.784200 20.4 (g) 8.449

NED objects within 10′ from NGC 0010.

SDSS image of the system.

References

Arp, 1980, ApJ, 240, 415, “High-redshift objects near the companion galaxies to NGC 2859″

George Paddock – early work on cosmological redshift

In addition to the work on extragalactic objects, George Paddock did some work on planets, stars, and galactic nebulae. He also worked on the radial velocity equations of binary stars. Here, I will concentrate on his extragalactic work (which contains only couple of papers).

Paddock (1916) discussed spiral galaxies in their relation to the galactic stellar system (this was well before it was established that spiral galaxies are not part of our own galaxy). He made an observation from the radial velocities of different objects:

The average radial velocities except the spirals range in increasing magnitude from zero to fifty kilometers per second. But a considerable jump is noticed from the fifty kilometers to 400 kilometers for the average of the spirals.

Based on this he presented a question:

Are the spirals dissociated from the star system?

Paddock then mentioned some Slipher’s arguments of the radial velocities of spiral galaxies. Paddock also discussed solar motion and its possible effect to the radial velocities of spiral galaxies. He noted that the spirals having measured radial velocities by that time were distributed in two groups and the Magellanic clouds were a third group, but he also said:

These objects, however, can hardly be considered to form a unitary system of associated objects, for it must be noticed that the average velocity of each of the three groups of objects is decisively positive, which means that they are receding not only from the observer or star system but from another.

What he describes here is an expanding motion. He continued:

Accordingly a solution for the motion of the observer thru space should doubtless contain a constant term to represent the expanding or systematic component whether there be actual expansion or a term in the spectroscopic line displacements not due to velocities. This brings up the question whether these large displacements are to be interpreted as due entirely to velocities.

13 years before Hubble’s redshift-luminosity relation, Paddock was already pondering similar questions. He brought up NGC 1068 with its fuzzy and broad spectroscopic lines as a possible example showing that all of the redshift might not be due to velocity (note that later there has been lot of discussion on the possible discordant redshifts in NGC 1068 system). He suggested that there might be a constant term resembling the K-term of stellar radial velocities and went on to quantify the term from the solar motion derived from the radial velocities of galaxies. He got a rather large value for the K-term (about 250-350 km/s) but he concluded that it is likely be due to small sample size and that he expected it to diminish with larger sample.

Campbell & Paddock (1918) discussed their spectroscopy on NGC 4151. They first mentioned that according to a photograph by Curtis, they thought that NGC 4151 was a planetary nebula. They then descibed their spectroscopy. They mentioned not finding the expected spectrum of a planetary nebula, and determined the radial velocity of 940 +/- 40 km/s for NGC 4151. They also noted that a new photograph by Curtis clearly showed a spiral structure, and that the character of the spectrum resembled the spectrum of NGC 1068.

References

Paddock, 1916, PASP, 28, 109, “The Relation of the System of Stars to the Spiral Nebulæ”

Campbell & Paddock, 1918, PASP, 30, 68, “The Spectrum and Radial Velocity of the Spiral Nebula N. G. C. 4151″

Links

(University of California: in memoriam) George Frederic Paddock: Lick Observatory

Knut Lundmark – extragalactic distance scale

Lundmark & Lindblad (1917) studied the spectral types of spiral galaxies. For NGC 3031 (Messier 81) they noted that Edward Fath had earlier determined that the spectrum resembles that of a K star, and their analysis also showed that if the spectral types of stars were applied to NGC 3031 spectrum, it would belong to spectral class K. They proceeded to analyse some other galaxies in the same manner. They ended their analysis by studying the differences in calculated and observed spectral types:

Hence it follows that the spectral type calculated by us should on an average differ from those determined in the usual way, where the spectral lines have been observed, by an interval at least twice as large as A-K. This not being the case, it seems to us that our investigation can be considered as a confirmation of the result found by Shapley, Hertzsprung and others, that no sensible absorption exists in space.

In a follow-up paper Lundmark & Lindblad (1919) continued these studies.

Lundmark (1921) discussed Messier 33 and wondered about possible distance indicators:

Another question is: As the only difference between the rifts in Messier 33 and those in Milky Way seems to be that the former have dimensions about 1/100 of the latter’s, will that mean that the objects in the spiral are 100 times as far away as the corresponding objects in the Milky Way?

Lundmark then noted that M33 seemed to have nearby background galaxies:

A long exposure Crossley photograph by Sanford shows that some of the nebulae apparently belonging to Messier 33 must have spiral structure. It is too early to speculate about spirals of different order, primary and secondary systems. The most natural explanation is perhaps that in this region we must expect to see several far away small spirals mixed up with nebular objects belonging to the great spiral.

Then follows what I think is quite remarkable thought from the point of view of the subject here in this blog. Lundmark had earlier noted that there has been some nebulous objects found near M33 that seemingly are extensions of M33’s spiral arms, then he said:

If the spaces between the spiral arms are filled with absorbing dark matter we get the impression of an arrangement in the extension of the spiral arms also of these background objects.

(Note that dark matter here doesn’t refer to the modern concept of dark matter, instead it refers just to regular matter that is not bright and therefore not visible to us, and absorbs the background light.) Remarkable thing here is that it is an example of how alignments between unassociated objects can occur sometimes with quite natural explanations. At the end of the paper, Lundmark gave some arguments of the large distance of M33; size of star clusters compared to Milky Way and the presence of apparent foreground stars.

Lundmark (1922) addressed some of the questions raised by parallax measurements made by van Maanen that differed from Lundmark’s measurements. Lundmark argued that the measured proper motions in that time only represented an upper limit. He also presented a calculation of parallax based on assumed systematic motions of spiral galaxies based on their measured radial velocities. He then mentioned a method to determine distance:

Parallaxes obtained by assigning to the brightest resolved stars in spirals an absolute magnitude equal to that of the brightest stars of our stellar system give still larger distances.

He didn’t specify any distances but he did give a range:

To sum up: different methods give for spiral nebulae distances ranging from about 10,000 light-years to 1,500,000 light-years.

He also suggested that diameters of galaxies could be distance indicators:

We have very likely to deal with millions of spirals, and it would be strange if we should have the largest of the spirals in our neighborhood. It is more natural to assume the spirals to have roughly the same linear dimensions, and that the smaller angular diameters in the mean indicate the more distant object.

He then estimated that visible universe extends out to 2,000,000 lightyears. He returned to van Maanen’s measurements, first discussing the extent of the Milky Way briefly and then using van Maanen’s measurements to derive masses for a few spiral galaxies. He got enormous masses as result, larger than the estimates of our own galaxy by that time. He then proceeded to discuss the motions in galaxies and made an interesting remark, showing how spiral galaxies was thought to work back then:

The matter we see in the measured spirals, if moving with a rather constant velocity, as indicated by the measures, must have been ejected during an interval of time of about 100,000 to 300,000 years.

He then made some arguments, based on this, about development stage of spiral galaxies and about the stellar ages. He also noted that amount of stars and supposed young ages of the galaxies meant that star production must be very rapid. But he ended the discussion with a note of doubt of the correctness of it.

Lundmark (1924) discussed the problem of redshifts and specifically the high redshifts of galaxies. He stated the problem:

Another question is, whether such a large Doppler shift represents motion in the line of sight alone or is caused in other ways? The validity of the Doppler principle has been proved by laboratory experiments only for velocities smaller than 1 km./sec. or so. The measures of stellar spectrograms giving such velocities as can be computed from the laws of gravitational astronomy… …have proved the correctness of the Doppler formula for velocities as high as 100 km./sec., and thus it seems allowable to assume that the displacements found for globular clusters and spiral nebulae are due to motions of the objects in the non-relativistic sense or to motions and the above mentioned effect of the curvature of the space-time.

He then proceeded to discuss the apex of the solar motion derived from the redshifts of globular clusters and spiral galaxies. He noted that they gave a different motion than nearby stars and hypothesized that our local system has a motion as a whole relative to the globular clusters and sipral galaxies. He also noted that our own motion seemed to suggesting that we are revolving around galactic centre, but he calculated the orbital period to be 3 billion years (3 x 109 years).

He then turned to de Sitter’s suggestions of the curvature of the space. He studied if there’s relation between the radial velocity of objects and their distance. He first compared the radial velocities of globular clusters to their distance estimations, and found no correlation. He did the same with different type of stellar objects (cepheids, novae, O stars, eclipsing variables, R stars, N stars). He then started analysing spiral galaxies in same manner. He started with a discussion of the situation on their distance estimates. As a sidenote, he argued that nearest spiral galaxies cannot be at distances of many millions of lightyears because some of them had shown to be resolved into stars and that novae and variable stars had been observed in them.

He used a distance scale based on the angular dimensions and magnitudes of the spiral galaxies assuming that they only depend on their distance. He plotted the resulting distance estimates against the radial velocities of spiral galaxies and concluded:

Plotting the radial velocities against these relative distances (fig. 5), we find that there may be a relation between the two quantities, although not a very definite one.

Lundmark was very close here to establish the redshift-distance relation five years before Hubble, probably only restricted by his distance indicators which were not very good ones. He also derived the value for the curvature radius of space-time, and got R = 2.4 x 1012 km as result.

Lundmark (1924b) studied the distance to Large Magellanic Cloud (LMC). He first argued that LMC was in many ways similar as spiral galaxies but decided to call objects like LMC as “nebulae of the Magellanic Cloud type”. He then determined the parallax of LMC with different methods. From the mean of these parallaxes, he determined the distance to the LMC to be 100,000 lightyears.

Lundmark (1924c) derived solar motion based on spiral galaxy measurements and the mean parallax of the spiral galaxies, and finally derived the mean distance to spiral galaxies. He got two values, 76,000 and 61,000 lightyears. Lundmark (1925) reviewed the distance determination methods to spiral galaxies. He noted that spiral galaxies seem to be out of reach of parallax measurements. Proper motion measurements seemed to be too noisy at the time. He then started discussing radial velocities. He first briefly noted that redshift doesn’t seem to correlate with the inclination of the spiral galaxy, indicating that they don’t “move like a discus thrown through space”. There were no correlation with redshift and galactic position either, but there was a correlation between the redshift and the dimensions of the spiral galaxies.

Lundmark then noted a kind of redshift-type relation. He assumed an evolutionary sequence where redshift got smaller when objects get older. “Globular” nebulae were youngest and had highest mean redshift, sequence then continued: “early spirals”, “late” spirals, Magellanic cloud nebulae, Magellanic clouds. This is of course interesting in the context of this blog because here we have the first suggestion of age dependent redshift. Lundmark interpreted this as a sort of K-effect (calling it “Campbell shift”):

The most characteristic feature of the radial velocities of spirals is the presence of a very large Campbell shift of the same nature as is found in most classes of giant stars.

Lundmark then proceeded to derive a value for the Campbell shift of spiral galaxies. Very interesting thing here is that his result included distance. His result is:

VCs = 513 + 10.365r – 0.047r2 km/s

Here r has unit of Andromeda distance multiples. He interpreted the result:

According to the above expression the shift reaches its maximum value, 2250 km./sec. at some 110 Andromeda units, which, according to results given later on, corresponds to a distance of 108 light-years. As the peculiar velocities of spirals seems to be smaller than 800 km./sec. one would scarcely expect to find any radial velocity larger than 3000 km./sec. among the spirals.

The last comment is of course wrong, but it is worth emphasizing that Lundmark gave a redshift-distance relation here. Whether it was the first one ever made, I don’t know, but this was four years before Hubble published his redshift-distance relation.

Lundmark then discussed some details on our own motion in space and the efforts to determine parallax of spiral galaxies. Then he discussed novae as standard candles for measuring distance to spiral galaxies. He reviewed the evidence that novae really occur in spiral galaxies, and then he described the research of Curtis on the subject and how he had arrived to a conclusion that closest spiral galaxies are millions of lightyears away from us based on the magnitude difference of novae in our galaxy and novae in spiral galaxies.

Lundmark then gave results of his studies of distances to the novae in our own galaxies, determined by their parallax. He determined the absolute magnitude of novae in our own galaxy, and did the same with the novae in Andromeda galaxy (M31). He also presented arguments for the similarity of the novae in Andromeda galaxy to the novae in our own galaxy, and for the Andromeda galaxy being a galaxy of its own instead of a stellar system in our own galaxy. Finally, he used the absolute magnitudes he had derived to calculate the distance to the Andromeda galaxy, and got 1.4 million lightyears, a very good estimate by that time (Hubble published his famous result when Lundmark was writing this paper, Hubble’s result was 930,000 lightyears, current value is about 2.7 million lightyears). Lundmark repeated this to NGC 4486 and got a distance of 8 million lightyears (current value is about 53 million lightyears).

Following Hubble’s lead, Lundmark determined the distance to Andromeda galaxy also by using Cepheids. He got few distance estimates; 620,000, 880,000, and 1,500,000 lightyears. Lundmark also used “Oepik’s method” to derive the distance to NGC 4594. The method uses rotation velocity of the spiral galaxy, so it seems to have some similarity to Tully-Fisher relation. The resulting distance to NGC 4594 was 56 million lightyears (current value is about 35 million lightyears). Lundmark mentioned having determined the distance to Messier 33 in 1920 as 1.5 million light years (current value is about 3 million lightyears) using the absolute magnitudes of regular stars. Lundmark closes this remarkable paper by presenting rather mathematically heavy discussion of the extent of the universe.

Lundmark (1930) studied the question if globular clusters and elliptical galaxies are related. Based on some similar features, he suggested that elliptical galaxies are made of stars just like spiral galaxies. He then mentioned the difference of the mean radial velocity between spiral and elliptical galaxies. He also argued that the two elliptical galaxies near Andromeda galaxy were associated with it because they were practically in same direction and had almost the same radial velocity. He then compared the absolute magnitudes of elliptical galaxies and globular clusters and found:

[The absolute magnitude of brightest globular cluster] is a considerably lower value for M than the value of the Andromeda companion, but, on the other hand, there seems to be no real cleft between the absolute magnitudes of several elliptical anagalactic nebulae and those of the brightest globular clusters.

Overall, he built a case where globular clusters are slightly outside of our own galaxy. Elliptical galaxies seemed generally to be companions to spiral galaxies, and as their appearance was also quite similar, it was natural to suggest that globular clusters and elliptical galaxies are related objects. This goes against current thinking, though. He closed the paper by saying:

If the sequence of globular clusters here suggested exists and if the smaller ones have a rapid motion, it might very well be that the globular clusters keep up the relations between the stellar systems and travel from Galaxy to Galaxy. These clusters are then something like what the comets were thought to be in the cosmogonies of Laplace and Schiaparelli – they are “the wandering boys of the Universe”.

In addition to the works mentioned here, Lundmark worked on different properties of stars and nebulae, and made a galaxy catalog. He also published in German and in Swedish, which papers were not considered here due to my poor skills in those languages. Lundmark (1956) would be very interesting paper with apparently a thorough historical overview on extragalactic research and distance indicators, but not freely available. I’ll just finish with the abstract of that paper:

First, an historical outline is given of the “Island-Universe” conception (Galilei, 1609), and of the development of our knowledge of the nebulae. The cosmological views of the eighteenth century are surveyed, and in particular the developments in England during the Restoration Period (1660-1700), the Augustan Age (1700-1745), and the era of Rationalism and Neo-Romanticism (1750-1820), due to Newton, Halley, Hooke, Bradley, Thomas Wright, and John mitchell. The latter’s work founded on stellar-statistical principles resulted in 1767 in the derivation of an average distance of nebulae. Herschel’s work, and Herbert Spencer’s dictum of 1858 are discussed. Bolin’s attempt of 1907 referring to the parallax of the Andromeda nebula, and other work by Curtis in 1917 and Lundmark in 1919 are described. The various distance-indicators are introduced ( e.g. the use of novae since 1919, of supergiants since 1920, of Cepheids since 1924, and of globular clusters since 1931), and absorption effects are considered. On the basis of these indicators a distance of the Andromeda nebula of 1.23 × 106 light-years is derived. The importance of supernovae in this connection is indicated, and also the facts pointing towards a necessary increase in the metagalactic distance-scale.

Links

1959, MNRAS, 119, 342, “Obituary Notices : Knut Emil Lundmark”.

Hetherington, 1976, JHA, 7, 73, “New Source Material on Shapley, Van Maanen and Lundmark”

There seems to have been a dispute between Lundmark and Hubble about their galaxy classification systems published in 1926:
Hart & Berendzen, 1971, JHA, 2, 200, “Hubble, Lundmark and the Classification of Non-Galactic Nebulae”. A brief note on the subject.
Teerikorpi, 1989, JHA, 20, 165, “Lundmark’s Unpublished 1922 Nebula Classification”. See this article for the new piece of information about Lundmark’s unpublished work on galaxy classifications in 1922.

Wikipedia: Knut Lundmark

References

Lundmark & Lindblad, 1917, ApJ, 46, 206, “Photographic effective wavelengths of some spiral nebulae and globular clusters”

Lundmark & Lindblad, 1919, ApJ, 50, 376, “Photographic effective wavelengths of nebulae and clusters”

Lundmark, 1921, ApJ, 50, 376, “The Spiral Nebula Messier 33″

Lundmark, 1922, PASP, 34, 108, “On the Motions of Spirals”

Lundmark, 1924, MNRAS, 84, 747, “The determination of the curvature of space-time in de Sitter’s world”

Lundmark, 1924b, Obs, 47, 276, “The distance of the Large Magellanic Cloud”

Lundmark, 1924c, Obs, 47, 279, “Determination of the apices and the mean parallax of the spirals”

Lundmark, 1925, MNRAS, 85, 865, “Nebulæ, The motions and the distances of spiral”

Lundmark, 1930, PASP, 42, 23, “Are the Globular Clusters and the Anagalactic Nebulae Related?”

Lundmark, 1956, VA, 2, 1607, “On metagalactic distance-indicators”

Updates

- November 22: Changed the “radius of the curvature of the universe” to “curvature radius of space-time”. Added the missing names and characters of the abstract of Lundmark (1956), the abstract has parts missing in ADS too (probably due to careless copy-pasting), so it wasn’t exactly my mistake.

NGC 0010 – some pair alignments

To my knowledge, NGC 0010 has not been discussed as a discordant redshift system before. Of nearby objects, there is one, object 3 in Figure 1, that has similar redshift as NGC 0010. Object 3 is therefore a probable companion to NGC 0010, and it has about 20 km/s higher radial velocity than NGC 0010, according to nominal values in NED. Only other object that can be considered as a companion is object 2, but it has about 1900 km/s lower radial velocity than NGC 0010, which is generally considered too high velocity difference, so it is not likely to be physically associated to NGC 0010 in traditional view. Small apparent size of object 2 suggests that it is some kind of dwarf galaxy. Only object within 20 arcmin from object 2 with similar redshift is 2dFGRS S495Z200 with cz = 4317 km/s and about 15 arcmin angular distance from object 2. 2dFGRS S495Z200 also seems to be quite a small galaxy.

Object 5 is a star, but there’s a galaxy-like object right next to it. One wonders if 2dF galaxy redshift survey’s target selection made a little mistake there and measured the star instead of the galaxy in almost the same position (the galaxy’s redshift would have been interesting to find out, as it seems to be almost exactly aligned across NGC 0010 with object 3).

There’s a rough pair alignment across NGC 0010 with objects 4 and 8. Redshifts of the two are not particularly close to each other but not radically different, either. Alignment is roughly along the minor axis of NGC 0010. The two objects are quite similar in appearance and their magnitudes are quite similar.

Objects 6 and 9 are roughly aligned across NGC 0010. Redshifts of the two are quite close to each other. The two objects are quite similar in appearance and their magnitudes are not that far from each other. Alignment is roughly along the major axis of NGC 0010, and quite accurately perpendicular to alignment line of objects 4 and 8. Other option for pair alignment is objects 7 and 9, but that alignment is worse than in the pair of 6 and 9, and redshifts are not so close to each other as in 6 – 9 pair, but still quite close.

Objects 8 and 9 have the same redshift, so they are a probable galaxy pair or members of same galaxy group. Looking further out from NGC 0010, there are few objects with almost the same redshift so there might be a loose galaxy group present at that redshift.

ngc0010
Figure 1. Objects with available redshift near NGC 0010 (all objects except one within 10 arcmin are presented). Size of the image is 15 x 15 arcmin. Image is from Digitized Sky Survey (POSS2/UKSTU Blue) and it has been adjusted for brightness and contrast to bring out fainter objects more clearly.

Objects and their data

NBR NAME TYPE REDSHIFT (cz) MAG SEPARATION
1 NGC 0010 SAB(rs)bc HII 0.022719 (6811 km/s) 13.3 0
2 2dFGRS S495Z164 galaxy 0.016400 (4917 km/s) 18.84 3.761
3 2dFGRS S495Z331 galaxy 0.022800 (6835 km/s) 18.02 5.068
4 2dFGRS S495Z152 galaxy 0.072000 (21585 km/s) 18.71 5.528
5 2dFGRS S495Z158 star 0.000200 (60 km/s) 19.30 6.738
6 2dFGRS S495Z146 galaxy 0.092600 (27761 km/s) 18.62 6.947
7 2dFGRS S495Z150 galaxy 0.149400 19.13 8.144
8 2dFGRS S495Z182 galaxy 0.114500 19.24 8.252
9 2dFGRS S495Z335 galaxy 0.114400 19.28 9.062

NED objects within 10′ from NGC 0010.