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astronomers Huchra Da Costaredshift et al universe Shanks et al However rapid jected large visual Over available more recently from ob jective machinebased scanning of the al rst discovery of acomplex celllike D structure structures rep orted b eeing by Jo eveer discovered et starting with the bution puter database to record alland published Meudon information was on formed galax in to establish the rst com empty region of the so called Bo otes void and H connected Received Sept accepted 3 2 1 Are astro-ph/9611211 26 Nov 1996 Mon Not R Astron So c School of Physics UniversityObservatoire of de New Lyon South F Wales SaintGenis Sydney Laval NSW FRANCE AUSTRALIA AngloAustralian Observatory Coonabarabran NSW AUSTRALIA Later Kirshner INTRODUCTION Before the compilation Anticipating their Di recent scale studies Lick catalogue Shane Wirtanen D a collab oration surveys has the Schmidt Nella use galaxy years mapp ed emerged as progress eg de Lapparent a the sky distributio n to ol an distribution largescale growth with WJ increasingly survey b etween the Observatories to with redshift et al describ e the of these large industry plates Key words detected and makes thethat total no length connexion of exists b this etween PP chain of and PI more However than a southern Mp c extension of PP was Pisces region was found b etween thefrom southern the Pavo LEDA database PI is wall and plotted the in northern hypergalactic Perseus co ordinates A signicant empty at Siding Spring Australia Two interesting in the galaxy distribution at sample previous p o or sampling of the galaxies in this region Redshifts for a magnitude selected the ABSTRACT Couch based advent of found a very structures In the FLAIR detailed et al Geller the Collins PP chain This survey this on surveys of lo cal of of D either redshift surveys large redshift question pap er multiob ject from picture G d galaxy et galaxies catalogue redshifts largescale structures led galaxies Printed May systematic sub jective al Paturel chain the or we to more of Lyon surveys of distri that Mp c large present pro and the were sp ectroscopy arises with a obtained and QA ies equal typical ters voids laments the plane by Tully in sp ectively and This most is p opulated tilted plane by ab out MPP also ten degrees claimed to l p ole and the Lo cal Sup ercluster Theeral LEDA team calculated the Paturel et al even The larger structure than any seemedthe previously to LEDA seen connect database Bottinelli sev suggested et al the existence of a structure voids and this alignement via an equal area pro jection of galaxy p ositions lyonfr gion tests new when M pc deg LyonMeudon highly signicant density LEDA Using sup erclusters Huchra of this attened hypergalactic redshift Geller and l area the  and deg login feature all the system Parker covering B of the Lo cal reality of this void which may simply reect discovered the b pro jection the T Around this and deg in galactic longitude and latitude re leda  survey CfA redshift scales M pc currently of sup erclusters PavoIndus Extragalactic on b Huchra Perseus the deg LyndenBell also noticed graphically All the H and of a of undertaken four Sup ercluster 0 lament  kms sheets was b eing time the existence available redshift Mp c redshifts Pisces UKSTSERC m survey De Database enhancements conrmed UK on the sup ergalactic galaxies showed in to In PavoIndus structure to b e ab out de Vaucouleurs 1 the were Mp c Schmidt address that Lapparent telnet wall Coma then the obtained conrmed survey a Flamsteeds 1 of sup erclus this We claim information were existence available the Telescope cluster lmcuniv lament rather elds found Geller plane with with re in of

2 Di Nel la H et al

all p ossessing their own selection criteria biases and errors

Incompleteness in some of these surveys is also o ccurring just

where the walls are b ecoming p opulated Furthermore our

azimuthal view is incomplete due to the zones of avoidance

in the and p ossible p o or sampling in certain

directions

Thus to ascertain whether the great walls seen are part

of yet larger shelllike structures we have b egun a redshift

survey to map the galaxy distributio n out through and b e

yond the great walls We hop e to determine whether they

truly have an outer edge rather than b eing an artefact of

incomplete data and also to determine whether the appar

ent gaps b etween the walls are real or due to p o or sampling

Apart from b eing pierced by narrow p encilb eam surveys

the galaxy distribution b eyond the walls has so far b een

relatively p o orly studied

In this rst pap er we present results of a new redshift

survey in the direction b etween the PavoIndus and Perseus

Pisces walls This is of particular interest b ecause of the ap

parent deciency of galaxies in this direction seen in Figure

A prime motivator for studying this region rst was to see

if there is a p ossible link b etween these two ma jor walls as

suggested by Dpro jections Paturel et al Santiago

et al

The pap er is organised as follows in section we de

Figure Distribution of galaxies from the LEDA sample in a

scrib e the selection of the galaxies to b e observed the ob

faceon view of the socalled hypergalactic plane see text The

serving pro cedure and the data reduction Section presents

newly observed region is dened by the two continuous lines

the nal redshift results whilst the signicance of our nd

ings are discussed in section

was actually a sheetlike structure that has b ecome known

as the Great Wal l similar to structures predicted in mo dels

by Zeldovich In the comple

OBSERVATIONS

mentary redshift surveys were undertaken by da Costa et al

and Fairall et al A compilation of available

Construction of the sample

published Southern redshifts by Fairall and Jones

revealed another walllike structure in the Pavo Indus PI

To obtain our sample we want to selected galaxies in the

empty region b etween PerseusPisces and PavoIndus This region The PerseusPisces PP region was describ ed either

region corresp onds to the range deg  hg l  deg as a chain Jo ever et al Gregory Thompson and Tit

or a sheetlike structure Haynes and Giovanelli

and deg  hg b  deg in hypergalactic longitude

and latitude resp ectively We decided to limit ourselves in In the years since the inception of LEDA data for

hypergalactic latitude and study only the galaxies lying close some galaxies and more than redshifts have

to the hypergalactic plane This would encompass FLAIR b een collected From LEDA a volumelimited v

1

observations across UKSTSERC survey elds centered kms and diameterlimited logD allsky sample

25

at approximately hgb deg see Table of galaxies was extracted After studying its complete

From the LEDA database which contains published ness in apparent diameter we used this sample to show that

the most p opulated plane in the lo cal Universe actually coin

data on known galaxies we selected all galaxies which are

p ositioned in one of the four UKST elds to b e observed cides with the hypergalactic plane or structure previously

Though entries on more than galaxies are currently found with the Flamsteed Dpro jection Di Nella and Pa

turel and If real this would represent p ossibly

available from LEDA signicant incompleteness exists for a

whole range of LEDA galaxy parameters includin g redshift the largest coherent structure in the Universe

magnitude and apparent diameters Sp ecially for galaxies This plane hereafter the hypergalactic plane is de

fainter than Bmagnitude LEDA b ecomes progressively ned by its up dated p ole and origin in galactic co ordi

incomplete nates l pol e deg bpol e deg and l or ig in

Thus it is necessary to complete the LEDA sample l pol e bor ig in bpol e deg To understand the sig

from a deep er catalogue We used the COSMOS database nicance of this most p opulated plane we calculated that

currently on line at the AAO Drinkwater Barnes and at  deg around this plane of the sample lay in only

Ellison The COSMOS database consists of param of the solid angle The distribution of the galaxies of

eterised image information for all ob jects detected ab ove the sample is shown in Fig

a given isophotal threshold from COSMOS measuring ma Despite the wealth of information in Figure there was

chine scans of the UKSTSERC J survey plates of the whole still a clear need to improve the picture further via additional

of the Southern sky excluding the Milky Way galaxy redshifts Like the Fairall redshift compilation the available

separation is provided up to the limiting magnitude for LEDA redshifts are a collation from a wide variety of sources

Are the PerseusPisces chain and the PavoIndus wal l connected 3

upp er limit of seconds exp osure was adopted The typ

Table Details of the observations

ical total exp osure time p er eld was in the range  s

to  s  s are normally considered adequate to

ESOSERC Set of Night of Seeing Total exp osure

obtain sp ectra of SN ratio  eld galaxies Sept arcsec time sec

a thth

The GB grating was used giving Amm or

a thth

Apixel CCD resolution The A covered on the CCD

a thth

at this disp ersion was selected for the range A A

a thth

This choice provided

a thth

i sucient sp ectral coverage to give a go o d chance of see

b thth

ing a number of dierent absorption or emission features in

b thth

galaxies at dierent redshifts

ii a high enough disp ersion to get reasonable redshift accu

racy

galaxies of B  though sources can b e detected up to

T

iii a minimum spreading of the galaxy light to get an ac

B  Howeveer we only selected galaxies in the range

T

ceptable SN ratio

 B  This limit suciently deep to provide

T

The current FLAIR system has very p o or eciency b e

go o d sampling at the depths of interest is a go o d match to

low A but this problem has recently b een addressed by

the capabiliti es of FLAIR and provides a target list that can

the commissioning of a new back illumina ted thinned CCD

b e observed in reasonable timescales

which oers times the blue DQE of the previous CCD

Some galaxies fainter than B can b e present in

T

To wavelength calibrate the data arc exp osures were

b oth LEDA and COSMOS subsamples see section Af

taken either side of a set of eld exp osures at the given dis

ter matching galaxies in b oth subsamples and rejectig galax

p ersion and grating angle The extremely stable nature of

ies with known redshift we obtained a total of galaxies

the o ormounted FLAIR sp ectrograph obviates the need

for redshift determination as shown in Table Five nights

for more frequent calibration exp osures eg Parker Wat

of FLAIR observing time were allo cated for the pro ject in

son Light from a selection of arc lamps is simply re

September Even with the bre multiplex advantage

ected o the closed dome Arc exp osures were also taken

and the capabili ty to observe  ob jects a night by us

when we changed plateholders to account for the dierent

ing two FLAIR plateholders it was not p ossible to observe

breformats fo cus values etc Both Neon and HgCd arcs

the total sample of selected galaxies in the nights available

were combined to provide adequate line coverage over the

Hence sets of  galaxies p er UKST eld were randomly

observed wavelength range

selected at the rate of in as this gives a go o d match to the

Flateld exp osures were taken using either the zenith

available bres in each FLAIR plateholder A nal sample

twilight sky or by reection of a featureless quartzhalogen

of galaxies was obtained

lamp o a sp ecially provided dome ateld screen These

exp osures are used to obtain the bretobre transmission

function see Parker and Watson vital to ensure prop er

Observing pro cedure

skysubtraction Dierences b etween bre transmission e

ciencies b etween the twilight sky and dome ats are at the

The survey was undertaken using FLAIR the multibre

 level Parker Lee Bias frames were also

sp ectroscopy system on the m UK Schmidt telescop e at

taken b efore andor after observations in order to correct

Siding Spring Co onabarabran Australia FLAIR is ideal for

for any sensitivity variations cosmetic defects and system

this survey as it combines b oth a large eld of view deg 

atic pixeltopixel variations on the CCD Of the or

deg a large multiplex advantage ob jects simulta

available bres dep ending on which FLAIR plateholder is

neously dep ending on the FLAIR plateholder used and a

used were devoted to the night sky to facilitate satis

suciently faint limiting magnitude B  to eciently

T

factory sky subtraction across the wide eld

sample the volume of interest

The observations spread over ve nights from the th

to the th September are detailed in Table Unfor

Data reduction

tunately the rst night was lost due to p o or weather The

All the data reduction was p erformed using the NOAO second night was only partly clear with typical seeing of

IRAF sp ectral reduction package together with a few ad arcseconds The following nights were mostly go o d with see

ditional FLAIR sp ecic IRAF tasks A FLAIR IRAF data ing in the range arcseconds Two sets of galaxies

reduction manual exists to facilitate the pro cess Drinkwa p er eld were prepared with the idea of observing two sets

ter and Barnes It is based mainly on existing IRAF of galaxies p er night by swapping b etween the two available

packages for multiber sp ectroscopy such as dohydra The plateholders This was accomplished on three nights but due

nal derivation of the radial velocities was done using the to weather conditions and some equipment problems half

rvsao crosscorrelation IRAF package night exp osures were sometimes not enough to obtain data

The rst stage of the pro cess is to combine several bias of adequate SN In these cases plateholder changeover was

exp osures into a single image this is required to remove any delayed to later in the night or to the following night

structure in the bias level across the CCD It is also nec The length of a FLAIR exp osure is determined mainly

essary to combine the at eld frames used to determine by the cosmic ray event rate typically p er minute Af

and correct for the relative transmission eciency of the ter seconds  cosmic ray events may b e detected

dierent bre ap ertures This frame is also used to dene resulting in signicant clutter of a data frame Imp ortant

and identify the bre ap ertures themselves The next stage features in galaxy sp ectra may thus b e compromised An

4 Di Nel la H et al

Table Selection of the target galaxies

HGB range HGL range RA and DEC UKSTSERC number of number of

in deg in deg of eld centre eld number target ob jects observed ob jects

h deg

h deg

h deg

h deg

is to use the IRAF task ccdpro c This task removes the

electronic zero level rst by subtracting the combined bias

image from each frame and secondly by subtracting the av

erage over the columns in the overscan region Finally the

image is trimmed to leave just the part containing useful

data The individu al data frames are now combined to in

crease the SN ratio of the nal sp ectra At this stage the

cosmic ray events on each frame are eectively removed us

ing a suitable sigma clipping algorithm which rejects pixel

whose values deviate signicantly from the mean with min

imal loss of data An ap erture identication le is then cre

ated to sp ecify which ap ertures are sky and which contain

the ob jects The FLAIR data are now ready for nal pro

cessing using the IRAF dohydra task This complex task

was developed for the multibre system on the

KPNO m telescop e but can also b e eectively used with

Figure Typical reduced absorption line galaxy sp ectrum not

FLAIR data From the combined cleaned and trimmed tar

ux calibrated with SN ratio  The vertical axis average

get frames together with the dome ats and arc exp osures

counts p er exp osure e edu The is

fully reduced disp ersion corrected wavelength calibrated

B The combined exp osure was  s and V

T helio

sky subtracted one dimensional sp ectra were pro duced

1

k ms

Derivation of radial velocities

The reduced sp ectra from dohydra can then b e input to the

IRAF rvsao task to derive the galaxy radial velocities via

crosscorrelation against ltered templates provided by QA

Parker Such reduction pro cedures are describ ed in detail by

Parker and Watson and Watson et al

We nally observed sets of  galaxies elds

and were observed twice but lo oking at dierent galax

ies Among the galaxies observed gave reliable ra

dial velocities according to a set of strict criteria ccf p eak

height cuto and match b etween emission and absorption

line velocities An overall success rate of was achieved

Two fully reduced typical sp ectra are shown in Figure

and Figure for an absorption and emission line sp ectrum

resp ectively During the survey a signicant number of ac

Figure Typical reduced emission line galaxy sp ectrum not

tive galaxies were also identied they will b e rep orted in a

ux calibrated with H H and SI I linesThe SN ratio is 

companion pap er

The vertical axis is average counts p er exp osure The apparent

The list of the measured galaxies is given in Table

magnitude is B The combined exp osure is  s and

T

1

together with COSMOS co ordinates and apparent magni

V k ms

helio

tude These parameters plus diameter axis ratio and p o

sition angle were used to p erform crossidentication with

the PGCLEDA ob jects after reduction to the RC system  column in hours minutes seconds

de Vaucouleurs et al Both cross correlation results

tenths for Equinox

from rvsao and emission line results from emsao are

 column in degrees arcminutes and arc

presented A few galaxies with published redshifts were also seconds for Equinox Co ordinates are from the COS

observed to derive our external error see section

MOS database except for a few cases were p ositions were

taken from the LEDA database

The columns of Table are arranged as follows  column Internal eld number

Are the PerseusPisces chain and the PavoIndus wal l connected 5

Figure Comparison of new and published helio centric veloci

Figure Comparison of galaxy Bmagnitudes see text

ties see text

 column PGCLEDA number Paturel et al a

b

 due to p o or sampling of this region by previous surveys

 column Alternative name in a given hierarchy ac

and therefore if there is a link b etween the PerseusPisces

cording to LEDA database NGC IC ESO MCG FAIR and

and PavoIndus Sup erclusters

DRCG Dreyer Laub erts Vorontsov

 due to a real void of galaxies

Velyaminov et al Fairall and Dressler

 due to an apparent void of galaxies caused by high

latitude galactic absorption

 column B magnitude from COSMOS database af

T

ter reduction to the LEDA magnitude system Figure

To address these questions we rst present the new re

B B

T COSMOS

sults of this survey in Figure It is imp ortant to under

 column Helio centric velocity V from the cross

cc

stand that the plane of this cone diagram is exactly the

1

correlation metho d and its mean error in k ms

same as the plane of Figure the hypergalactic or most

 column Helio centric velocity V from the emission

em

p opulated plane There is evidence of two density enhance

1

lines identication metho d and its mean error in k ms

ments at a radial distance of  and  Mp c Their

 column notes

signicance seem more clear with the help of a redshift his

togram shown in Figure It app ears in Figure that these

enhancements delineate two low density regions or voids

Radial velocity external error estimates

When compared to the maps of this region given in the

compilation of Fairall Jones these voids are real

To determine the external mean error we made a comparison

1

and signicant The nearest one with v kms is

Fig b etween our new measured velocities and those avail

known as the Void and the furthest with v

able in LEDA for the few ob jects in common This compari

1

kms was called the Further Sculptor Void by Fairall

son conrms that there is no signicant error for the slop e or

Jones This gure is very interesting b ecause it represents

for the zerop oint Rejecting two uncertain measurements

1

one of the rare regions where two walls p erp endicul ar to the

the residual error is kms If we assume that b oth

line of sight are seen We call these chains seen from our

LEDA and the measurements of this survey have the same

1

survey walls b ecause they are part of structures which ex

mean error we get a mean error of V kms

cc

tend ab ove and under the plane of this cone diagram see

The helio centric velocities measured by the emission

Fairalls catalogue of maps of this region

line detection metho d are also compared to published values

When we add these new redshifts to the data of Figure

despite there b eing only p oints in common No slop e or

no evidence of a link b etween the northern PerseusPisces

zerop oint error is found This is conrmed by a compari

and the southern PavoIndus features can b e seen The cur

son with radial velocities obtained by the crosscorrelation

1

rent survey sampled at a rate of in is highly signicant

metho d The mean error is tentatively  k ms

and thus we conclude that we cannot have missed any link

if one existed

The most prominent feature in Figure is the double

RESULTS

p eaked velocity distribution The rst p eak at V 

hel

1

kms seems to result from galaxies lo cated in a southern The aim of this survey was to study the distributio n of galax

extension of the Perseus Pisces wall which now extends over ies in the region b etween PerseusPisces and PavoIndus see

more than Mp c The second p eak is lo cated at V  gure With this study we hop ed to ascertain whether the

hel

1

kms apparent gap b etween these two walls seen in Figure is

6 Di Nel la H et al

standard parameters M and The func



tion is normalized to our sample total of  galaxies

Assuming Poisson errors b oth p eaks are signicant at a

level of and resp ectively It is also clear that the re

gions corresp onding to the Sculptor and the Further Sculp

tor voids are not consistent with a uniform average space

density of galaxies but really are underp opulated regions

DISCUSSION AND CONCLUSIONS

One could argue that the observed galaxy distribution is the

result of selection eects Indeed if our sample was chosen in

a biased way eg with more time devoted to a given region

at a given distance one could susp ect that the p eaks sim

ply reect the excess of time sp ent at this distance Several

arguments can b e presented against this interpretation

 Our selection was made on the basis of carefully con

trolled criteria  B  and without regard to the

T

lo cal density or to distance Thus the observed density at a

given distance should b e representative In interpreting fea

tures of the redshift distribution in this way one must b e

extremely worry ab out the selection eects which bias our

Figure Distribution of galaxies within the region surveyed in

this study The lled circles represent LEDA galaxies previously

view of the structure that is present For example could the

measured in redshift the op en circles are from this survey This

p eaks observed in the velocity distribution simply indicate

is a view faceon of the hypergalactic plane plane with the Pavo

that our sample is preferentially tuned to galaxies at these

Indus wall and PerseusPisces chain The p osition of the density

distances From the selection function we have computed

p eaks seen in the velocity histogram are indicated by the cir

the answer in our case is no

cle arcs One of this velocity p eak in the redshift survey shows

 A completeness test can b e made to prove that our

a southern extension to PerseusPisces which now extends over

sample constitutes a magnitude limited sample with a well

more than Mp c

dened limit Figure This diagram has the exp ected

slop e of indicatin g that the number of studied galax

ies increases on the mean as the cub e of the distance For

comparison we plotted on the same gure the completeness

curve for the entire sky normalised to the solid angle of the

present survey obtained from LEDA when imp osing that

b oth the apparent magnitude B and the radial velocity v

T

are known The completeness limit in the studied region is

magnitude deep er after our survey

 Another argument comes from the diagram Figure

which shows that the density enhancements are visible in

each covered eld at the same distance

 Finally the nearest of the two walls was already visible

in the cone diagrams compiled by Fairall and Jones

This wall delineates the Sculptor void and the Further Sculp

tor void It is p erp endicul ar to the Sculptor Wall The fur

1

thest wall at kms has never b een noticed b efore

It delineates the end of the Further Sculptor Void and is

p erp endicul ar to the Scuptor Wall

Figure Histogram of helio centric velocities in the studied re

To continue to address the questions exhibited in sec

gion The dashed line represents the selection function of our sur

tion we have explored the map of Burstein Heiles

vey The most imp ortant features are the two highly signicant

to see if a high galactic latitude molecular cloud could b e

p eaks bracketting underp opulated regions

resp onsible for an apparent void in the distributio n of galax

ies such as the Sculptor Void If this was the case the p os

sibility of a hidden connection b etween PerseusPisces and

Pavoindus could still exist However we have already a hint They are compared to the calculated selection function

Fairall Jones didnt see a second wall delimitin g the end of our survey derived from a standard non evolving galaxy

of the Further Sculptor void but we did So it would b e luminosity function Because we are claiming that our sam

very surprising if the galactic absorption could play a role ple is complete b etween B and B we cal

T T

dep ending on distance ie hiding some near galaxies and not culated the selection function b etween these limits using

some more distant ones Reinforcing this answer no mapp ed a Schechter function Schechter and Press with the

Are the PerseusPisces chain and the PavoIndus wal l connected 7

Dynamique des Structures Gravitationnelles Observatoire de

Lyon

Burstein and Heiles ApJ Suppl

Da Costa LN Pellegrini PS Sargent WLW Tonry J Davis

M Meiksin A Latham DW Menziers JW Coulson IA

ApJ

Di Nella H and Paturel G Comptes rendus de lacademiedes

sciences serieI I t p

Di Nella H and Paturel G Pro ceedings of the Astronomical So

ciety of Australia vol

Dressler A Astrophys J Suppl Ser

Dreyer JLE MNRAS NGC

Dreyer JLE MNRAS IC

Drinkwater MJ Barnes DG Ellison SL Publ Astron

So c Aust

Einasto J Corwin HG Huchra J Miller RH Tarenghi M

Highlights of Astronomy Vol ed R West Reidel

Dordrecht p

Einasto M Einasto J Tago E Dalton GB and Andernach

H Mon Not R astr Soc EETDA

Fairall A MNRAS FAIR

Figure Test to show that our sample constitutes a magnitude

Fairall A Jones A Southern Redshifts Catalogue Plots

limited sample with a welldened cuto at B The solid

Publications of the Department of Astro

T

line represents the exp ected slop e The mean completeness

Fairall AP Palumbo GGC Vettolani G Kaumann G Jones

curve obtainied from LEDA for the same solid angle is shown in

A BaiesiPillastrini G MNRAS P

op en circles A gain of magnitude results from our survey

Geller M Huchra J Science

Gregory SA Thompson LA Tit W ApJ

Haynes MP Giovanelli R ApJ L

absorbing cloud is present in the available absorption maps

Jo eveer M Einasto J Tago E MNRAS

Kirshner RP Oemler A Schechter PL Shectman SA

in this direction

ApJ Lett L

In conclusion we no longer susp ect a link b etween the

Lapparent Vde Geller M Huchra J ApJ L

Perseus Pisces and PavoIndus walls despite evidences from

Laub erts A The ESOUppsala Survey of the ESOB At

Dpro jections Paturel et al Santiago et al

las Europ ean Southern Observatory ESO

Nevertheless Figure is still a very go o d representation of

LyndenBell D in Clusters and Sup erclusters Ed AC

our neighbourho o d Up dating this gure will b e done only

Fabian p

by studying the outer regions of the ma jor walls and trying

Parker QA Lee D AAO do cument on FLAIR p erfor

to ll in the missing data across the zones of avoidance The

mance

Further Sculptor Void can now b e considered delimited by

Parker QA Watson FG AA Suppl

1

a wall at kms and PerseusPisces is extended in

Parker QA Watson FG SPIE vol

Paturel G Bottinelli L Gouguenheim L FouqueP AA

the Southern hemisphere The total length of this chain is

now more than Mp c

Santiago BX Strauss MA Lahav O Davis M Dressler A

Huchra JP ApJ

Shane CD Wirtanen CA Pub Lick Obs

ACKNOWLEDGEMENTS

Schechter P Press W ApJ

Tully RB ApJ

We are grateful to those who have managed the LEDA

Tully RB ApJ

extragalactic database over the last years N Durand

Vaucouleurs Gde Astronomical Journal

P Fouque AM Garcia RGarnier M Loulergue MC

Vaucouleurs Gde Vistas Astr

Marthinet and C Petit We are also grateful to those who

Vaucouleurs Gde Vaucouleurs Ade Corwin HG Jr Buta

assisted during the observations the UKST sta S Besier

RJ Paturel G FouqueP Third Reference Cata

logue of Bright Galaxies SpringerVerlag RC

and K Sealey We acknowledge the COSMOSUKST South

Vettolani G In Astronomy from Wide Field Imaging edt

ern Sky Catalogue supplied by the COSMOS group at the

MacGillivray HT in press

Royal Observatory Edinburgh to the AngloAustralian Ob

Vettolani G Studying the Universe with Clusters of Galaxies

servatory This work has b een supp orted by grants from the

eds BohringerH and Schindler S MPE Rep ort

Conseil Regional RhoneAlp es F and by the Institut Na

tional des Sciences de lUnivers F We thank the University

VorontsovVelyaminovBA Arkip ova VP Kranogorskaja AA

of New South Wales for welcoming us and for providing us

Morphological Catalogue of Galaxies Trudy

the facilities with which we have conducted this study QA

Sternberg Stat AstrInst

Parker is on sp ecial leave from the ROE to work at the AAO

Watson FG Oates AP Shanks T HaleSutton D MN

We thank the referee for his comments

RAS

Zeldovich YB AA

REFERENCES

Bottinelli L Gouguenheim L FouqueP Paturel G in La

8 Di Nel la H et al

Table The measured galaxies

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

a abs

a PGC ESO abs

b emi

b emi

b abs

a emi

a emi

b PGC ESO emi Sb

a emi

b abs

a emi

a absemi

b PGC ESO abs SO

a absemi

a abs

b PGC ESO emi Scd

b PGC ESO emi Sb

a emi

b LEDA abs

b emi

b absemi

a PGC ESO abs

a emi

b PGC ESOA abs

a absemi

b abs

a absemi

b emi

b absemi

b emi

b abs

a emi

b emi

b abs

b emi

b emi

b emi

b PGC ESO emi

a abs

b emi

b emi

b abs

b emi

b emi

a abs

a abs

a emi

b abs

a abs

b emi

a emi

b emi

a PGC ESO abs SO

a PGC ESO absemi

a abs

Are the PerseusPisces chain and the PavoIndus wal l connected 9

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

b PGC ESO abs E

b emi

b abs

a abs

a absemi

a emi

b PGC ESO emi Sa

b emi

b emi

a abs

b emi

b emi

b abs

a abs

a emi

b emi

a abs

b abs

b PGC ESO emi Irr

a abs

b emi

b abs

b emi

a abs

a emi

a emi

b PGC NGC absESo

a abs

a emi

a PGC ESO emi

b PGC ESO abs

b abs

b LEDA emi

a emi

b abs

a absemi

a emi

a abs

a LEDA emi

b PGC ICB abs

a emi

b emi

a absemi

a emi

a emi

b PGC ESO emi

a PGC ESO emi

b PGC ESO emi

a absemi

a abs

b abs

b PGC ESO emi

a abs

b emi

a emi

10 Di Nel la H et al

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

a abs

b emi

a emi

a absemi

a emi

b emi

a abs

b emi

b abs

b abs

b PGC ESO emi

a emi

a emi

a LEDA emi

a abs

a PGC ESO emi

b emi

b emi

a abs

a emi

b PGC ESO abs

a absemi

b PGC ESO emi

a PGC ESO emi

a emi

a PGC FAIR abs

b PGC ESOA absemi

a emi

b abs

b emi

a emi

b abs

a abs

a emi

b abs

a emi

a emi

a PGC FAIR absemi

b abs

b PGC ESO emi

a emi

a PGC ESO emi

b emi

b PGC ESO emi

a abs

b PGC ESO abs

a absemi

a abs

a abs

b emi

b emi

b emi

a abs

b emi

a abs

Are the PerseusPisces chain and the PavoIndus wal l connected 11

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

b emi

a PGC ESO emi

a emi

b abs

a abs

b emi

a emi

b abs

b emi

a abs

a abs

a emi

b emi

a emi

a emi

a emi

a emi

a emi

a emi

a abs

a emi

a emi

a emi

a LEDA emi

a emi

a emi

a emi

a emi

a emi

a emi

a abs

a emi

a abs

a emi

a emi

a emi

a emi

a emi

a emi

a PGC NGC abs

a emi

a abs

a abs

a emi

a emi

a LEDA emi

a LEDA abs

a emi

a abs

a absemi

a emi

a emi

a emi

a abs

a PGC ESO abs

12 Di Nel la H et al

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

a abs

a emi

a emi

a PGC IC emi

a emi

a PGC ESO emi

a emi

a PGC ESO emi

a emi

a emi

a emi

a emi

a emi

a abs

a emi

a emi

a abs

a abs

a PGC MCG abs

a abs

a emi

a emi

a emi

a emi

a emi

a abs

a PGC abs

a PGC ESO emi

a emi

a emi

a emi

a emi

a emi

a abs

a emi

a emi

a emi

a emi

a LEDA emi

a abs

a emi

a abs

a PGC ESO abs

a emi

a emi

a PGC ESO abs

a PGC ESO emi

a abs

a abs

a abs

a emi

a PGC ESO emi

a PGC ESO absemi

a abs

Are the PerseusPisces chain and the PavoIndus wal l connected 13

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

a PGC ESO emi

a LEDA emi

a abs

a emi

a emi

a abs

a LEDA emi

a emi

a abs

a LEDA DRCG abs

a emi

a abs

a LEDA DRCG emi

a abs

a LEDA DRCG abs

a PGC NGC abs

a emi

a PGC ESO emi

a LEDA DRCG emi

a abs

a PGC ESO abs

a abs

a emi

a PGC ESO emi

a PGC ESO emi

a abs

a abs

a emi

a abs

a emi

a emi

a PGC ESO abs

a emi

a PGC ESO emi

a PGC ESO emi

a PGC ESO emi

a emi

a emi

a emi

a emi

a PGC ESO emi

a PGC MCG abs

a abs

a abs

a abs

a abs

a emi

a emi

a emi

a abs

a emi

a abs

a absemi

a emi

14 Di Nel la H et al

Table continued

RA DEC field PGCLEDA Alternat BT Vcc Err Vem Err Notes

h m s d number number name kms kms kms kms

b abs

b abs

b abs

a abs

a abs

a PGC ESO emi

a abs

a abs

a abs

a abs

b LEDA abs

b emi

b emi

b emi

a abs

a abs

b emi

b emi

b abs

b abs

b abs

b abs

b abs

b abs

b abs

b abs

b LEDA abs

a LEDA abs

a abs

a absemi

a LEDA abs

a abs

a abs

a abs

a LEDA emi

a absemi

a abs

a LEDA abs

a abs

a abs

b emi

b abs

b abs

b abs

b LEDA abs

b abs

b abs

b abs

a abs

Note the in the notes column indicates a poor determination of the redshift

abs denotes redshift measured from absorption lines emi denotes redshift measured from emission lines