SLIDE 1 Masahiro Takada (IPMU)
@GRB conference, Kyoto, April 20
SLIDE 2
- What is the Hyper Suprime-Cam (HSC)?
- HSC surveys
- The major scientific goals
- Synergy with other surveys
- Summary
SLIDE 3 @ summit of Mt. Mauna Kea (4200m), Big Island, Hawaii
Subaru Telescope
SLIDE 4 4
Cassegrain Focus Prime Focus Nasmyth Focus Nasmyth Focus FOCAS Optical imager and spectrograph COMICS IR imager and spectrograph MOIRCS NIR imager (7′×4′) and multi-
Suprime-Cam Optical imager (34′×27′) HDS Optical spectrograph (λ/Δλ=100,000) AO188 188-element curvature sensing adaptive optics system with a laser guide star capability
Illustration by Takaetsu Endo, taken from Nikkei Science 1996
IRCS (AO188) Infrared imager and spectrograph (λ/Δλ=20,000) HiCIAO (AO188) Coronagraphic imager with differential imaging techniques
SLIDE 5
Only Subaru has the prime focus camera, Suprime- Cam, among other 8-10m class telescope: the wide field-of-view (0.25 sq deg) Excellent image quality allows accurate shape measurements of galaxies
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Upgrade the prime focus camera Funded, started since 2006 International collaboration: Japan (NAOJ, IPMU, Tokyo, Tohoku, Nagoya), Princeton, Taiwan Field-of-View: ~10×Suprime-Cam Keep the excellent image quality Instrumentation well underway (S. Miyazaki, NAOJ) HSC survey starting from 2012- (~5 years)
SLIDE 7
SLIDE 8 Developed by Hamamatsu Photonics-NAOJ collaboration
Quantum efficiency
HSC previous S-Cam CCDs
Improved CCDs in red
SLIDE 9
Field of view: 1.5 degrees in diameter Image quality kept same to that of the current camera, Suprime-Cam, in r, i, z, y bands The CCD chips with improved quantum efficiency in red bands
SLIDE 10 Wide-field survey (>1000 sq. deg.; grizy)
- Depth: t_exp~15min, i~26 mag (5σ)
- Probes a comoving volume of ~10Gpc^3 up to z~1.5
- Sciences: later
Deep survey (~20 sq. deg.; grizy+NIBs)
- Depth: t_exp~1 hour, i~27 mag
- Key sciences: z~6-7 Ly-alpha emitters (survey area >
reionization bubbles), z~6 QSOs, SNe, galaxy evolution studies
- ver z~1-2, GRB orphan afterglow, …
Ultra-Deep survey (a few sq. deg.; grizy+NIBs)
- Depth: t_exp~20-30 hours, i~28 mag
- Key sciences: z~7 Ly-alpha emitters (for understanding
reionization history), SNe
- Best targets for spectroscopic follow-ups by TMT
Surveys designed fully utilizing its unique capability (wide FoV and depth)
SLIDE 11
- Ouchi et al. (09): found 22 z~7 z-dropout
candidates (one LEA confirmed spectroscopically) over 0.4 sq. deg. area (~(100Mpc)^3)
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Current in ~5 years
SLIDE 13 UDF (the previous image) The Millennium Simulation (Springel et al., Nature 05)
Exploring the large-scale structure of the Universe
A massive galaxy cluster (>10^3 galaxies) ~10Mpc or ~30Mlight year@z~0.5~0.5deg
Subaru Other 8m telescopes
Hyper-SC
SLIDE 14 Gravitational lensing of the hierarchical structures
- Cosmological lensing: cosmological parameters (DE, neutrino mass)
- Cluster lensing (dark matter, cluster physics)
- Galaxy group; not yet fully explored so far
- Galaxy-scale lensing (weak and strong lensing)
Finding galaxy clusters out to z~1.5 (y-band)
- The expected number of massive clusters with 10^15Msun at z>1
- ver a 1000 sq. deg. area is only O(1) for LCDM model
QSOs at z~7 (SMBHs; GP test)
- 10-100 QSOs can be expected if extrapolating the results at z<6.5
Galaxy evolution out to z~1 Dwarf satelites in our Milky Way out to ~100kpc in distance (compared to ~10kpc for SDSS)
- A few satellites expected to be found, for LCDM model
- Constraining the mass of DM (the current constraint MWDM<a few keV)
SLIDE 15
Lensing strength = (the geometry of the Universe) ×(lensing matter [including DM])
SLIDE 16 γ ∝Ωm0 dzL
zS
∫
dLS(zL,zS)dL(zL) dS(zS) δ(zL,θ)
for a source galaxy at zs
- Lensing efficiency function: Wgl
– Overall amplitude is sensitive to Ωm, i.e. Ωde if a flat universe is a prior assumed – Sensitive to Hubble expansion through dA, i.e. DE – Depends on source redshift – uncertainty in weak lensing measurements if redshift info is not available
– Allows to reconstruct the dark matter distribution without resting on any assumptions of the dynamical states – Sensitive to primordial power spectrum (amplitude and shape) – Redshift history of the growth rate is sensitive to DE (structure formation arises from the balance between gravitational instability and cosmic expansion
SLIDE 17 Strong Lensing
- Multiple Images
- Large Arcs, Ring
- Obvious Distortion
Weak Lensing
- Slight Stretching
- Distortion small compared
to initial shape
- Statistical lensing
- The S/N depends on the
number of background gals and the accuracy of shape measurement (PSF)
to center
SLIDE 18 Reyes et al. Nature 2010
theory, lensing is caused by the gravitational potential (g_00) and the curvature perturbation (g_ij)
measurement is distorted by the peculiar velocity field, caused by the gravitational potential (g_00)
the SDSS clustering stats to explore the consistency relation
Ratio: lensing strength/galaxy cluster strength Distance from the center of lensing galaxies
SLIDE 19 Subaru (S-Cam) is currently the best instrument for measuring WL signal, thanks to its image quality and depth
Subaru S-Cam CFHT (blue: mass)
Okabe, MT+ 2010, in press Bardeau, Soucail, Kneib et al.07
A209
SLIDE 20
Okabe, MT+ 2010, in press
A2390
Bardeau, Soucail, Kneib et al.07
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Merging Clusters: Bullet Cluster (1E 0657-56)
HSC-W of 2000 deg.: >10^4 clusters with >10^14Msun WL found clusters are ~ a few x 10^3 O(1) clusters with 10^15 Msun at z>1 ALMA follow-up observations of high-z clusters ~10^2 merging clusters like Bullet Cluster (Hayashi & White 06)
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- Plan to overlap the HSC survey
region with that of the SZ experiment ACT (around the equator)
- SZ independent of redshift
- HSC can determine the redshift of
SZ found clusters
- Statistical studies of ACT-HSC
data for clusters
Atacama Cosmology Telescope (148GHz, 218GHz, 277GHz)
Abell 3128 (z=0.44)
SPT-CL0547 (z=0.88)
- BOSS redshifts of LRGs (z< 0.7) available
- LRGs are landmarks of LSS (most likely bright
central galaxies of clusters)
- HSC will add faint galaxies surrounding every
LRG
- Other synergy with Astro-H, ALMA, eROSITA,
TMT…
SDSS-III (BOSS survey)
SLIDE 23
- Key factors: other datasets, NIR, spec-z, ACT, ALMA
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- Cosmological lensing
- The current most massive survey is
CFHT, 170 sq. deg.
- HSC-W: >1000 sq. deg.: dark energy
and neutrino mass
σ8
WL WMAP combined
σ8(Ωm/0.25)0.64=0.785±0.043 σ8=0.771±0.029 Ωm=0.248±0.019 Fu+0712.0884 Ichiki, MT, Takahashi 09 ΣMν<0.54eV (95% C.L.)
SLIDE 25 ρde(z) ∝(1+ z)3(1+w)
MT & Jain (2004)
DE equation of state: w DE density parameter:Ω_de
0.1 Today(08) 0.05 0.01
σ(w)
2015 2020(?) The first question to be addressed: if or not w=-1? (w=-1: cosmological constant) Complementary to the geometrical tests, SNe, BAO, GRBs.. HSC(+CMB): σ(w)~0.02-0.04 LSST, JEDM σ(w)~0.01 σ(w)~0.1 We may find the evidence of w≠-1 earlier than LSST/JEDM (note: systematics)
SLIDE 26 From S. Miyazaki
SLIDE 27
- Hyper Suprime-Cam (HSC) is the next-generation prime focus
camera of Subaru: a factor 10 improvement in the survey speed
- The fabrication well underway: the survey will start from ~2012
- Many science cases available: wide, deep, ultra-deep surveys
– From the local universe to cosmos: dwarf satellites in our Milky Way, distant galaxies, galaxy clusters, QSO, large-scale structure – Weak lensing adds new information on the data: dark matter distribution, which is essential for a quantitative understanding of structure formation
- Major scientific goals: dark energy, dark matter, neutrinos,
cosmic reionization
- Various synergy with future surveys: ACT (SZ effect), ALMA,
Astro-H, BOSS, JWST, TMT,….