First results from The Palomar Transient Factory Eran Ofek Einstein fellow CALTECH.
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Transcript of First results from The Palomar Transient Factory Eran Ofek Einstein fellow CALTECH.
First results fromThe
Palomar Transient Factory
Eran OfekEinstein fellow
CALTECH
Talk Layout
PTF goals
System overview
Capabilities and products
What have we found so far?
Next Generation Transients Factory
PTF collaborationPI: S. R. Kulkarni
Caltech, LCOGT, Berkeley, LBL, IPAC, Columbia, Oxford, Weizmann
PTF goals
To study the transient and variable sky
Core collapse SNe
Calibrating SN Ia for cosmology
Explore new regions of transients parameter space
Stellar variability: RR Lyr, AM CVn,…
Solar system: Asteroid rotations
Law et al., Rau et al.
PTF system overview
48” Oschin Schmidt camera (Palomar obs.)
7.2 deg2 FOV (92 Mpix)
Scale: 1”/pix, lim. mag ~21
Robotic telescope & scheduler Full automatic operation Auto. Selection of science targets
PTF system overview
60s exposure + 35s readout ~510,000 deg2 yr-1
Filters: g, R, H+
Real time imageSubtraction andTransientclassification
PTF system overviewReal time transient classification
Galaxy zoo transient
PTF observing strategy Observing strategy
40% : 3-day cadence
40% : 1-day cadence
10% : All sky H survey
10% : Monitoring of star formation regions
PTF followup
What did we observe so far?
Log 1
0(N
imag
es)
Abs. photometry
Abs. photometry calibration good to 2-3%
Using SDSS starsas standard stars tocalibrate fields outsideSDSS footprint(photometric nights)
CCD 4
Relative photometry
Relative photometry ~3-5mmag
Deep coadd
Deep sky:~10 images lim. mag. ~22.5~100 images lim. mag. ~24
Data ReleaseFirst public data release: 2011
GalacticWhat have we found?
Galactic: 51 dwarf novae
3 AM CVn
Planet candidates around M-dwarfs
PTF 10nvg: enhanced accretion and outflow in Class-I protostar
New FU Ori star
Levitan et al., in prep.
Law et al., in prep.
Covey et al., 1011.2565
Miller et al., 1011.2063
AM CVnPrimary background noise for LISA
PTF 09hpkLe
vit
an
et
al.,
in p
rep
.
FU Ori and otherPTF10qpf: new FU Ori star
Miller et al., 1011.2063
Planets around M-dwarfsOnly 16 planetary systems detected around M-dwarfs
Possible to find planets in the habitable zone…
Calibrating the mass-radius relation of M-dwarfs
Law et al., in prep.
Planets around M-dwarfsSome eclipsing M-dwarfs we found…
Planets around M-dwarfs
Consistent with secondary radius ~ 1.5-2.0 RJ
Law
et
al.,
in p
rep.
Planets around M-dwarfsLa
w e
t al.,
in p
rep.
Planets around M-dwarfsLa
w e
t al.,
in p
rep.
Asteroids rotationPoolis
hok
et
al.,
in p
rep
.
Asteroids rotationPoolis
hok
et
al.,
in p
rep
.
ExtragalacticWhat have we found?
Since March 2009: >5,000 transient candidates 1036 spectroscopically confirmed SNe 692 Ia 49 Ibc 257 II~3% of these “SNe” are weird and hard to classify into existing scheme:e.g., faint and fast, Ca rich, luminous, etc. Kasliwal et al., 1005.1455
Kasliwal et al., ApJ 723, 98
HST UV spectra of Ia SNePTF Can find SN Ia early PI: R. Ellis
HST UV spectra of Ia SNeThe first dozen…Cooke et al., 1010.2211
HST UV spectra of Ia SNeCooke et al., 1010.2211
The mean UV spectrum of the z~0 and z~0.5 agree, but somedifferences inmetallicabsorptions
The hosts of CC SNeArcavi et al., ApJ 721, 777
MR<-18 MR>-18
Ic-BL and IIb are more common in dwarf hosts,Stripped CC (Ic) are not seen in dwarf hosts.
Probably because in lower metallicity hosts,Metallicity-driven mass loss is reduced.
The SN2005E family
>23 kpc from NGC 1032No host: MR>-7Spec: He burning products Ca reach
Possibilities:Acc. Induced Collapse.Ia
May solve puzzles:
44Ca in Solar System44Ti->44Ca via b decayPositrons annihilationin Galactic bulge
Perets et al. Nature 465, 322
The SN2005E family: 09dav40kpc from putative spiral hostAbs R mag ~-15Fast: 1 mag in 10 dayVery red, g-r = 1.2
Similar to SN1991bg but with HeHydrogen in nebular phase
Kasliwal et al., in prep.Sullivan et al., in prep.
The SN2005E family: 10iuv
37 kpc from putative hostAbs R. mag ~ -15.Fast: 1 mag in 10 daysIntriguing Nebular Spectra
Kasliwal et al., in prep.
Luminous supernovae
Galactic: 51 dwarf novae; 2 AM CVn;…
Luminous supernovaeQuimby et al., 0910.0059
Luminous supernovaeQuimby et al., 0910.0059
Shock breakout / PTF
PTF detects SNe early -> can detect shock breakout (but still limited by cadence).
GALEX + PTF synergy
PTF + rapid follow up with Swift/UVOT/XRT
Shock breakout / PTFO
fek et al., Apj in press
PTF 09uj
Shock breakout / PTFO
fek et al., Apj in press
PTF 09uj
Shock breakout / PTF
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c
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422
24
24
2
7
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7
ergE
yearMM
MM
KT
cmn
skmv
sun
sun
50
310
105~
/1.0~
3.0~
000,90~
105~
/000,13~
PTF 09uj
Ofek et al., A
pj in press
Shock breakout / PTFPTF 09dah
NGTFThinking about the next project…
PTF-2 will have a ~30-40 deg2 cameraMounted on the 48” schmidt telescope
Simple scheduling – one day cadence objective: find them young
~8000 deg2 day-1
Scheduled for 2014
EndThank you!
Shock breakout / Intro
Photons first emerge from SN (breakout) when they diffuse ahead of the shockfaster than the shock propogates
Happens at optical depth: =c/v
duration: ~r/c
Decay time: ~r/v
Fast supernovae: 10bhpKasliwal et al., ApJ 723, 98
Very fast: decay ~5 days, MR~-17(e.g., similar to SN200bj, [Poznanski+10])
Fast supernovae: 10bhpKasliwal et al., ApJ 723, 98
If powered by 56Ni then Ni mass ~0.02 Msun and SN quickly becomes optically thin to -rays.
AIC (?).Ia (?)
Luminous red novaPTF 10fqs in M99
Kasliwal et al., 1005.1455
Faint/slow event in M99: MR~-11
PTF 10fqsKasliwal et al., 1005.1455
~10,000 km/s (?)
Search for SB in Chandra archive with Mike Muno
Downloaded the entire Chandra archive
Search for transients and highly variableObjects (on short time scale)
First pass completed: complete for events brighter than 40 counts
No SN 2008D-like events (Soderberg et al. 2008)
Next: calc. efficiency and extend to faint sources
Relative photometrySolution using linear least squares
mij – instrumental mag
i-star (1..p), j-image (1..q)
Solving per field (overlap between fields not guaranteed)
ij – instrumental mag err
ijij zmm
Relative photometryUsing linear least squares
23
22
21
13
12
11
100
010
001
010
010
010
100
010
001
001
001
001
m
m
m
m
m
m
P
?
?
?
i
j
m
z
P
H (“design matrix”)
Observations
Free p
ara
mete
rs
ijij zmm
Relative photometrySolution using linear least squares
ijij zmm
)()(1
22 HPmHPm ijT
ij ij
We need to solve (in the presence of errors):
Relative photometrySimultaneous absolute calibration
23
22
21
13
12
11
100
010
001
010
010
010
100
010
001
001
001
001
m
m
m
m
m
m
P H is (pq)x(p+q) matrixHowever, rank is p+q-1
jM
M1
100
010
001
000
000
000 Adding calibration block
Relative photometryAdditional de-trending
We can add more columns to H and P.For example: Airmass x color term
Positional terms
Multiple CCDs (i.e, overlap)
obsbm