M ATTHEW C OLLESS
M ULTI -O BJECT S PECTROSCOPY IN THE N EXT D ECADE S ANTA C RUZ DE L A P ALMA
2-6 M ARCH 2015
C OSMOLOGY
C URRENT S URVEYS
AND I NSTRUMENTATION
W HY S URVEYS ? W HY MOS?
ASTRONOMY IS AN OBSERVATIONAL SCIENCE DEALING WITH LARGE POPULATIONS OF COMPLEX OBJECTS THAT FORM STRUCTURES IN SPACE AND EVOLVE IN TIME
SURVEYS ALLOW US TO STUDY LARGE POPULATIONS ,
TO MAP STRUCTURES , AND TO TRACK EVOLUTION
“ A PICTURE IS WORTH A THOUSAND WORDS ”,
BUT , TO AN ASTRONOMER ,
“ A SPECTRUM IS WORTH A THOUSAND IMAGES ”
M ULTI -O BJECT S PECTROSCOPY (MOS) IS THE
MOST EFFICIENT WAY TO GATHER ASTROPHYSICAL INFORMATION FOR LARGE POPULATIONS SCATTERED OVER TIME AND SPACE
S O … IN THE LAST FEW DECADES MOS SURVEYS
HAVE TRANSFORMED OBSERVATIONAL COSMOLOGY
C OSMOLOGY S URVEYS T IMELINE
WiggleZ, 2.6, 5.5
BOSS, 3.0, 6.2 PSCz, 0, 4.2
LCRS, 2.0, 4.4
SDSS, 2.8, 5.9 2dFGRS, 2.6, 5.3
6dFGS, 2.2, 5.1 CfA, 0, 4.0
1980s 1990s 2000s 2010s
Survey, logM, logN
Survey, logM, logN
Survey, logM, logN
non-MOSslit MOS
fibre MOS
DEEP, ~2, 4.0
MOS INSTRUMENTS FOR COSMOLOGY
1D (M ULTI -F IBRES )
L
ASC
AMPANASF
IBRES
YSTEM(LCRS)
2
DF (2
DFGRS,2QZ)
➡︎AAΩ (W
IGGLEZ,GAMA,O
ZDES)
6
DF (6
DFGS)
➡︎TAIPAN (T
AIPAN)
SDSS (SDSS-I, SDSS-II)
➡︎BOSS (BOSS,
EBOSS)
2D (M ULTI -S LITS )
DEIMOS (DEEP, DEEP-2)
3D (M ULTI -IFU S )
MUSE(?)
HET/VIRUS (HETDEX)
F
IBRES DOMINATEMOS
COSMOLOGY SURVEYS BECAUSE SCIENCE DRIVERS
ARE MULTIPLEX AND AREA
R EDSHIFT S URVEYS
R EDSHIFT S URVEYS : US SURVEYS , E UROPEAN SURVEYS , A USTRALIAN SURVEYS ; CELESTIAL SPHERE IS AT CMB
MOVIE BY SIMON DRIVER
AAO Z - SURVEYS
2 D FGRS, 2QZ, 2SLAQ-LRG, 2SLAQ-QSO, 6 D FGS, GAMA, W IGGLE Z; CELESTIAL SPHERE AT Z =1
MOVIE BY SIMON DRIVER
GAMA: THE VERY
MODEL OF A MODERN REDSHIFT SURVEY
G ALAXY A ND M ASS A SSEMBLY SURVEY
F EDERATIVE , MULTI - l,
AND MULTI - FACILITY
G
ALAXYSED
S FROMUV
TO
R
ADIO USINGEXISTING SURVEYS
&
NEW OBSERVATIONS
A
LSO MULTI-
Z WHENASKAP
PROVIDESHI
REDSHIFTS
… RICH SURVEY DATABASE
… COMPLEX INFORMATION STRUCTURES
WEB
WIKI
DATABASE
MOS S URVEYS /I NSTRUMENTS HERE
T
ELESCOPE: I
NSTRUMENTS
URVEY(
S)
AAT : AAΩ, HERMES, SAMI WIGGLEZ, GAMA, GALAH, SAMI UKST : 6DF, TAIPAN RAVE, 6DFGS, TAIPAN
SDSS 2.5M : SDSS, BOSS, MANGA SDSS, BOSS, EBOSS, MANGA
WHT : ISIS, WEAVE WEAVE
GTC : OSIRIS, EMIR, MEGARA
VLT : VIMOS, KMOS, MUSE, MOONS VANDELS, VIPERS, LEGA-C,…
VISTA : 4MOST 4MOST, WAVES
LAMOST LEGUE
CALAR ALTO : CALIFA CALIFA
MAGELLAN : PRIMUS PRIMUS
SUBARU : FMOS, PFS FASTSOUND
HET : VIRUS HETDEX
GAIA GAIA
KPNO 4M : DESI DESI
EUCLID EUCLID
LSST:MOS / MSE / WFIRST …
I MPACT OF MOS S URVEYS - 1
L ITERATURE ANALYSIS BY T RIMBLE & C EJA (2008)
LOOKED AT 11,831 PAPERS PUBLISHED IN 2001-3 ( DATED , BUT RESULTS STILL APPLICABLE )
T HE MOST - CITED OPTICAL / INFRARED FACILITIES …
FACILITY CITATIONS PAPERS
HST 15390 1063.1
Keck 8122 365.6
SDSS 7235 161
VLT 5696 345.5
AAT 4592 170.2
Schmidts 3430 247.8
2MASS 2937 182.9
I MPACT OF MOS S URVEYS - 2
20
MOST-
CITEDPAPERS2001 -3
TRIMBLE & CEJA (2008)
S URVEY I MPACT BY F IELD
P HYSICS FROM L ARGE -S CALE S TRUCTURE
S IDEBAR : S PECTRO - Z ’ S VS P HOTO - Z ’ S
P
HOTO-
Z’
S ARE POTENTIALLY A CHEAP WAY TO MEASURE MANY GALAXY REDSHIFTS AND HENCE THEBAO
PEAK
P
ROBLEM IS LARGE ERRORS-
FOR Z-
ERRORS >1000
KM/
S, BAO
PEAK IS SMEARED OUT& H(
Z)
CANNOT BE MEASURED;
FULL INFORMATION REQUIRES Z
-
ERRORS <300
KM/
S
T
O MEASUREDA(
Z),
A PRECISION OFσ
z/(1+z) ≲ 4%
IS REQUIRED;
WORSE PRECISION CAUSES CATASTROPHIC CANCELLATION OFBAO
SIGNAL OVER WIDTH OF Z-
SHELL
H
OWEVER3-4%
PRECISION YIELDS POOR CONSTRAINTS ON THEBAO
PER UNIT VOLUME;
A PHOTO-
Z SURVEY NEEDS~10
X MORE VOLUME THAN A SPECTRO-
Z SURVEY
B
ETTER PRECISION HELPS,
BUT AT Z<0.7,
SPECTRO-
ZSURVEYS ARE ALREADY COVERING LARGE FRACTION OF SKY
,
SO PHOTO
-
Z SURVEYS ONLY COMPETITIVE AT HIGHER Z’
S
P
HOTO-
Z SURVEYS REQUIRE STRINGENT CALIBRATION AND MORE EXTENSIVE MODELING THAN SPECTRO-
Z SURVEYS
2
DFGRS
MEASURED221,000
Z’
S OVER2000
DEG2
L
ARGE-
SCALE STRUCTURE OF THE GALAXY DISTRIBUTION PRECISELY MAPPED ON SCALES OF10
6–10
9 LIGHT-
YEARS
T
HE FORM OFL
ARGE-
SCALE STRUCTURE IS CONSISTENT WITH GROWTH BY GRAVITATIONAL INSTABILITY
QUANTUMFLUCTUATIONS FROM THE
B
IGB
ANG ARE AMPLIFIED BYGRAVITY TO BECOME GALAXIES
,
CLUSTERS&
SUPERCLUSTERS
T
HE TOTAL DENSITY OF ALL TYPES OF MATTER ISΩ
M= 0.23
THERE IS ONLY
23%
OF THE MATTER NEEDED TO MAKE A CRITICAL-
DENSITY(
I.
E.
FLAT = ZERO-
CURVATURE)
UNIVERSE
T
HE TOTAL DENSITY IN ORDINARY MATTER ISΩ
B= 0.04
BARYONS ARE
17% & CDM 83%
OF THE TOTAL MATTER
N
EUTRINOS MAKE UP LESS THAN13%
OF ALL MATTER
TOTAL MASS OF3
NEUTRINO SPECIES IS LESS THAN0.7 eV
B
ARYONA
COUSTICO
SCILLATIONS DETECTED AT2.5 s
C OSMOLOGY FROM 2 D FGRS
C OSMOLOGY FROM MOS – BAO
B
ARYON ACOUSTIC OSCILLATIONS(BAO)
PROVIDE STANDARD RULER
BAO
RESULT FROM PRESSURE WAVES IN PRE-
RECOMBINATIONPHOTON
-
BARYON FLUID IMPRINTING THE SOUND HORIZON SCALE ONTHE MATTER DISTRIBUTION
G
ALAXY REDSHIFT SURVEYS YIELD ANGULAR DIAMETER DISTANCESD
A(
Z) &
EXPANSION RATESH(
Z)
BAO
MAP EXPANSION HISTORYBOTH ALONG AND ACROSS THE LINE OF SIGHT
,
PROBING BOTHD
ARKE
NERGY ANDG
RAVITY
A
WELL-
UNDERSTOOD,
PRECISE TOOL;
MAIN LIMITATION IS THESCALE OF THE SURVEYS REQUIRED
ANDERSON+ (2014)
BAO SURVEYS
BAO
FIRST DETECTED IN GALAXY DISTRIBUTION(
AT2.5 s )
BY2
DFGRS
ANDSDSS (C
OLE+ 2005, E
ISENSTEIN+ 2005)
T
HEW
IGGLEZ
SURVEY OBSERVED2
X10
5 EMISSION-
LINEGALAXIES OVER
800
DEG2 AND MEASUREDBAO
AT0.5<
Z<1
WITH
3.8%
PRECISION AT Z=0.6 (B
LAKE+ 2011)
B
EUTLER+ (2011)
USED6
DFGS
TO MAKE A LOW-
REDSHIFT(
Z0.1) BAO
DISTANCE MEASUREMENT WITH4.5%
PRECISION
K
AZIN+ (2010)
USED THE FULLLRG
SAMPLE FROMDR7
TO MEASURE THE GALAXY CORRELATION FUNCTION AND OBTAIN A3.5%
MEASUREMENT OF THEBAO
SCALE AT Z= 0.35
P
ERCIVAL+ (2010)
USED900,000
GALAXIES OVER9100
DEG2 FROM THE COMBINED2
DFGRS, SDSS DR7/LRG
SAMPLES TO OBTAIN THEBAO
SCALE AT Z=0.27
WITH2.7%
PRECISION
P
ADMANABHAN+ (2012)
SHOWED THAT DENSITY FIELDRECONSTRUCTION COULD IMPROVE THESE
BAO
MEASURES BY ABOUT A FACTOR OF2
C OSMOLOGY FROM MOS - RSD
R
EDSHIFT-S
PACED
ISTORTIONS RESULT FROM PECULIAR MOTIONS DUE TO GRAVITY AND MEASURE THE GROWTH OF STRUCTURE
RSD
MEASURE THE COMBINATIONf(z) s
8(z)
WHERE
f(z)=Ω M (z)
ANDs
8 ISFLUCTUATION IN
8 M
PC/h
SPHERE
RSD
CONSTRAINTS COME FOR FREE WITH ANY LARGE GALAXYz -
SURVEY
M
AIN UNCERTAINTY IS THEORETICAL MODELING OF THE NON-
LINEARGRAVITATIONAL EVOLUTION AND NON
-
LINEAR BIAS
;
CURRENTLY THIS LIMITS APPLICATION OFRSD
METHOD TOCO
-
MOVING SEPARATIONSr
>
10 M
PC/h (
ORk
<0.2 h/M
PC)
SAMUSHIA+ (2014)
KAISER EFFECT
(COHERENT INFALL) BAO
RING
BOSS CORRELATION FUNCTION IN 2D
L OW - Z C OSMOLOGY S URVEYS
6
DFGS,
THOUGH SMALLER THAN2
DFGRS & SDSS,
GIVES VALUABLE CONSTRAINTS ON COSMOLOGY AT LOW Z,
NOTABLY A DIRECT MEASURE OFH
0 ANDG
ROWTH OFS
TRUCTURE
T
HET
AIPAN SURVEY(H
OPKINS TALK)
WILL HAVE4
X THE SAMPLE SIZE&
VOLUME OF6
DFGS
AND GIVEH
0 WITH~1%
PRECISIONAND GROWTH OF STRUCTURE TO
5%
AT⟨
Z⟩≈0.1
D
ARKE
NERGY IS A LATE-
TIME(
LOW-
REDSHIFT)
PHENOMENON!
H IGH - Z C OSMOLOGY S URVEYS
REDSHIFT SURVEYS COVERING A RANGE OF EPOCHS
(W IGGLE Z, BOSS…) CONSTRAIN THE EVOLUTION OF THE GEOMETRY OF THE UNIVERSE AND THE
GROWTH OF STRUCTURE OVER COSMIC TIME
PLANCK COLLABORATION (PAPER XIII, 2015) BAO: DEVIATIONS FROM LCDM GEOMETRY RSD: GROWTH RATE OF STRUCTURE
C OSMOLOGICAL P OWER OF MOS
T
HE ADDED INFORMATION GIVEN BYMOS
SURVEYS IS QUANTIFIED BY THETIGHTER CONSTRAINTS ON
D
ARKE
NERGY ANDM
ODIFIEDG
RAVITY RELATIVE TO THOSEFROM THE
CMB
ALONEPLANCKCOLLABORATION(PAPERXIV, 2015)
DARK
ENERGY
MODIFIED
GRAVITY
ΩM VS s8
BOSS: THE STATE OF THE ART
G OAL : MEASURE BAO OVER LARGER VOLUME AND Z - RANGE THAN ALL PREVIOUS Z - SURVEYS
F INAL DATASET IS SDSS DR12 ( TO JULY 2014)
G ALAXIES : 1.4
X10
6AT Z < 0.7 (i < 19.9 ) OVER 10
4DEG
2
F
ORECAST: D
A TO1.0 %
ANDH(
Z)
TO1.8 %
AND1.7 %
AT Z=0.3
AND Z=0.57
Lya: 1.6
X10
5QSO S
WITH g < 22 AT 2.15 < Z < 3.5
F
ORECAST:
OVERALL DILATION FACTOR TO
1.9 %
AT Z 2.5
BOSS AND eBOSS
BOSS: THE STATE OF THE ART
BOSS
DETECTSBAO
FEATURE AT7 s
IN GALAXIES AND
5 s
INLya
FOREST
BAO
ALONE YIELD A HIGH CONFIDENCE DETECTION OF DARK ENERGY AND,
WITH THE
CMB
ACOUSTIC SCALE, BAO
IMPLY A NEARLY FLAT UNIVERSE
BAO+CMB+SN
DATA JOINTLY GIVEH
0= 67.3 ± 1.1
KM/
S/M
PC(1.7%)
ROBUST TO ASSUMPTIONS ABOUT DARK ENERGY OR SPACE CURVATURE
F
OR CONSTANT DARK ENERGY(Λ), BAO+CMB+SN
YIELDSΩ
M= 0.301 ± 0.008 (2.7%) Ω
K= −0.003 ± 0.003
F
OR EVOLVING FORMS DARK ENERGY, BAO+CMB+SN D
ATA ARE ALWAYS CONSISTENT WITH FLATΛCDM
AT~1σ
BAO+P
LANCK-WL
GIVES A SUMMED MASS OF NEUTRINOS
Mν< 0.25 eV
AUBOURG+(2014)
PALANQUE-DELABROUILLE+ (2014)
C OSMOLOGY - P ECULIAR VELOCITIES
MOS
COSMOLOGY IS NOT JUST ABOUT REDSHIFTS!
P
ECULIAR VELOCITY SURVEYS(
V-
SURVEYS)
CAN PROVIDE ADDITIONAL INFORMATION REMOVING SOME DEGENERACIES INTRINSIC TO Z-
SURVEYS(
E.
G.
BETWEENb
ANDr
g)
Z-ONLY
Z+V
1
s
CONTOURSON PAIRS OF PARAMETERS
V-
SURVEYS ARE NECESSARILY LOW-
REDSHIFT DUE TO FIXED FRACTIONAL DISTANCE ERRORS
D
ISTANCE ERRORS ARE TYPICALLY SIGNIFICANT(
E.
G. 20-25%
FORTF
ANDFP,
BUT5-8%
FORSN
E)
6
DFGRS
IS THE CURRENT STATE-
OF-
THE
-
ART Z+V-
SURVEY:
125,000
REDSHIFTS AND9000
PECULIAR VELOCITIES
(
USINGF
UNDAMENTALP
LANE DISTANCES FOR EARLY-
TYPE GALAXIES)
V-
SURVEY COVERS17000
DEG2TO DEPTH OF
~16000
KM/
SV- SURVEY C OSMOLOGY
J
OHNSON+ (2014)
USE THE POWER SPECTRUM OF THE6
DFGS
PECULIAR VELOCITIES TO OBTAIN FIRST SCALE-
DEPENDENT MEASUREMENTS OF THE GROWTH RATE OF STRUCTUREfσ
8(
IN COMBINATION WITH Z<0.07 SN
E)
N
O EVIDENCE FOR A SCALE DEPENDENCE IN GROWTH RATE OR VARIATION FROM PREDICTIONS OFP
LANCKΛCDM
MODEL
C
OMBINING ALL SCALES,
THE GROWTH RATE AT Z=0
IS MEASURED WITH∼ 15%
PRECISION,
INDEPENDENT OF GALAXY BIAS&
IN GOOD AGREEMENT WITHRSD
GROWTH RATE MEASUREMENTS FROM6
DFGS
Z-
SURVEY
F
UTURE PECULIAR VELOCITY SURVEYS WILL ALLOW US TO UNDERSTAND IN DETAIL THE GROWTH OF STRUCTURE IN THE LOW-
REDSHIFT UNIVERSE,
PROVIDING STRONG CONSTRAINTS ON THE NATURE OF DARK ENERGY
M
EASURED THE GROWTH RATE INDk
=0.03 h/M
PC BINS TO~35%
PRECISION,
INCL
.
A MEASUREMENT ON SCALES >300 h/M
PC,
THELARGEST
-
SCALEMEASUREMENT OF THE GROWTH RATE TO DATE
GROWTH RATE W.R.T. PLANCK MODEL
D ARK E NERGY – FUTURE PROGRESS
ALL OBSERVATIONS TO DATE OF THE COSMIC
EXPANSION HISTORY AND THE GROWTH OF
STRUCTURE ARE
CONSISTENT WITH A FLAT
ΛCDM + GR
MODEL WITH
Ω
M≈ 0.3
AND
Ω
Λ≈ 0.7
Z
-
SURVEY METHODS(BAO, RSD)
AREEXPECTED IN FUTURE TO PROVIDE
10
X BETTER CONSTRAINTS ON THED
ARKE
NERGYEQUATION OF STATE
Weinberg+ (2013) 33
C ONSTRAINTS FROM MOS S URVEYS
FISHER MATRIX
PREDICTIONS FOR PRECISION OF BAO
DISTANCE SCALE MEASUREMENTS AS A FUNCTION OF REDSHIFT
THE BOSS SURVEY
ACHIEVES ~2% FOR
Z < 1 AND AT Z ~2.5
THE DESI &
E UCLID SURVEYS WILL ACHIEVE 0.5- 1% OUT TO Z = 2
P
ERCIVAL(2013)
MOS C OSMOLOGY IN 2025
WHAT WILL MOS COSMOLOGY LOOK LIKE IN 2025?
SOME SAFE PREDICTIONS …
1.
R
EDSHIFT SURVEYS EXIST TOTALING A FEW X10
7 GALAXIES OUT TO Z~1.7
AND A FEW X10
6 GALAXIES/QSO
S OUT TO Z~3
2.
P
ECULIAR VELOCITY SURVEYS(
OPTICAL ANDHI)
EXIST TOTALING >10
5 GALAXIES IN THE NEARBY UNIVERSE3.
LSST
PROVIDES ULTIMATE TARGET LIST FORMOS
SURVEYS;
HOW CAN WE FULLY EXPLOIT THIS
? N
EED DEDICATED8
MMOS!
4.
A
COMMON FEDERATED DATABASE SYSTEM HAS EMERGED FROM A HETEROGENEOUS SET OF SURVEYS AND SOFTWARE5.
M
ANY MORE PAPERS ARE BASED ON ARCHIVALMOS
SPECTRA AND DATABASES THAN ON FRESH OBSERVATIONS6.
‘D
ATAS
CIENTISTS’
OUTNUMBER‘O
BSERVERS’ (
AND HAVEMORE KUDOS AND BETTER CAREER PROSPECTS
)
7.
T
EAM LEADERS ARE STILL COMPLAINING THAT SCIENCE OUTPUTS FROM THEIR SURVEYS ARE PERSON-/
BRAIN-
POWER-
LIMITEDF UTURE MOS I NSTRUMENTS
E VERY SELF - RESPECTING GENERAL - PURPOSE 4 M
OR 8 M - CLASS TELESCOPE NEEDS MOS CAPABILITY
MOS IS EXPANDING IN NEW DIRECTIONS : NOT JUST
HIGH - MULTIPLEX BUT ALSO HIGH - RESOLUTION AND MULTI -IFU S (& EVENTUALLY MOAO MULTI -IFU S )
I N THE ELT ERA , MOST 8 M - CLASS TELESCOPES WILL HAVE A MOS INSTRUMENT OF SOME VARIETY AS THEIR CUTTING - EDGE FACILITY
GMT TO HAVE HIGHLY VERSATILE MOS/ MULTI -IFU
CAPABILITY PROVIDED BY THE MANIFEST FACILITY
C
OUPLED TO LARGE OPTICAL/
NIR SPECTROGRAPHS(
BOTH MEDIUM AND HIGH RESOLUTION)
AΩ = 25
M APERTURE X20
ARCMIN DIAMETER FIELD