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Northern Sky Transient Survey w/ Tomo-e Gozen 諸隈 智貴 (東京大学) Tomoki Morokuma (Univ. of Tokyo/IoA)

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  • Northern Sky Transient Survey

    w/ Tomo-e Gozen

    諸隈 智貴 (東京大学)

    Tomoki Morokuma (Univ. of Tokyo/IoA)

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Contents

    New Parameter Space: High Cadence Transient Surveys

    Northern Sky Transient Survey w/ Tomo-e Gozen

    Survey Design / Simulation

    Follow-up Scheme

    Summary

    �2

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �3Kasliwal 2011, Cooke (http://www.astro.caltech.edu/~ycao/B&ETalks/B&E_FRBs_Cooke.pdf)

    128

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak

    Lum

    inos

    ity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Peak

    Lum

    inos

    ity [e

    rg s−

    1 ]

    Figure 8.1 Framework of Cosmic Explosions in the Year 2011. Note that until 2005 (Fig-

    ure 1.1), we only knew about three classes (denoted by gray bands). Systematic surveys,

    serendpitous discoveries and archival searches have yielded multiple, new classes of tran-

    sients. Discoveries presented in thesis Chapters 3, 5, 6 and 7 are denoted by ⋆.

    (Brown et al. 2011) that undergo such an explosion.

    2. Luminous Red Novae: The defining characteristics of the emerging class of luminous

    red novae (LRN) are: large amplitude (> 7mag), peak luminosity intermediate be-

    tween novae and supernovae (−6 to −14mag), very red colors and long-lived infrared

    emission. When the first LRN was discovered (Kulkarni et al. 2007), the similarities

    to three Galactic explosions (including V838Mon) suggested a common origin. Since

    then, 5 more extragalactic and 1 more Galactic LRN have been discovered. Recent

    developments suggest there may be two progenitor channels.

    http://www.astro.caltech.edu/~ycao/B&ETalks/B&E_FRBs_Cooke.pdf

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �4Kasliwal 2011, Cooke (http://www.astro.caltech.edu/~ycao/B&ETalks/B&E_FRBs_Cooke.pdf)

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak L

    um

    inosity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Pe

    ak L

    um

    ino

    sity [

    erg

    s−

    1]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak L

    um

    inosity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Pe

    ak L

    um

    ino

    sity [

    erg

    s−

    1]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak

    Lum

    inos

    ity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Peak

    Lum

    inos

    ity [e

    rg s−1

    ]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak

    Lum

    inos

    ity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Peak

    Lum

    inos

    ity [e

    rg s−

    1 ]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak

    Lum

    inos

    ity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Peak

    Lum

    inos

    ity [e

    rg s−1

    ]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    0

    log ( [sec])

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak

    Lum

    inos

    ity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Peak

    Lum

    inos

    ity [e

    rg s−1

    ]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    1""""""""""""""""""""""""""2""""""""""""""""""""""""""3""""""""""""""""""""""""""4"""""""""""""""""""""""""5"""""""""""""""""""""""""6""""""""""""""""""""""""7"

    Transients in the local Universe 383

    100 101 102

    −24

    −22

    −20

    −18

    −16

    −14

    −12

    −10

    −8

    −6

    Characteristic Timescale [day]

    Peak Lum

    inosity [M

    V]

    V838 MonM85 OT

    M31 RV

    SCP06F6

    SN2006gySN2005ap SN2008es

    SN2007bi

    SN2008S

    NGC300OT

    SN2008ha

    SN2005E

    SN2002bj

    PTF10iuvPTF09dav

    PTF11bijPTF10bhp

    PTF10fqs

    PTF10acbp

    PTF09atuPTF09cnd

    PTF09cwlPTF10cwr

    Thermonuclear Supernovae

    Classical Novae

    Luminous Red

    Novae

    Core−Collapse Supernovae

    Luminous Supernovae

    .Ia Explosions

    Ca−rich Transients

    P60−M81OT−071213

    P60−M82OT−081119

    1038

    1039

    1040

    1041

    1042

    1043

    1044

    1045

    Pe

    ak L

    um

    ino

    sity [e

    rg

    s−

    1]

    Figure 4. Framework of Cosmic Explosions in the Year 2011 (Kasliwal 2011). Note that until 2005 (Fig. 1),we only knew about three classes (denoted by gray bands). In the past six years, systematic searches,serendipitous discoveries and archival searches have uncovered a plethora of novel, rare transients. Discov-eries by the Palomar Transient Factory and P60-FasTING (Kasliwal et al. 2011a) are denoted by ?. Severalnew classes are emerging and the governing physics is being widely debated: luminous red novae (electroncapture induced collapse of rapidly rotating O–Ne–Mg white dwarfs?), luminous supernovae (magnetarsor pair instability explosions?), .Ia explosions (helium detonations in ultra-compact white dwarf binaries),Calcium-rich halo transients (helium deflagrations?).

    (advanced LIGO, advanced VIRGO, LCGT, INDIGO) coming online. Detecting gravitationalwaves from neutron star mergers every month is expected to become routine. A basic common-ality between gravitational wave searches and the electromagnetic search described above is thatboth are limited to the local Universe (say, < 200 Mpc). A known challenge will be the poor skylocalizations of the gravitational wave signal and consequent large false positive rate of electro-magnetic candidates (Kulkarni & Kasliwal 2009). Therefore, prior to the ambitious search for anelectromagnetic counterpart to a gravitational wave signal, it would only be prudent to build thiscomplete inventory of transients in the local Universe.

    2 1 log ( )

    -1 -2 -3 -4

    100 Mpc

    10 Mpc

    http://www.astro.caltech.edu/~ycao/B&ETalks/B&E_FRBs_Cooke.pdf

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �5

    “Moment” of Supernova Explosion

    shock breakout

    afterbefore

    days

    hours

    Supernova Shock Breakout

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �6

    supernova

    GW counterpart / kilonova

    neutrino counterpart

    comet, asteroid

    meteor

    NEO

    space debris

    moving objects

    pulsar

    super-flare, M dwarf flare, CV

    Ultra-Long GRB

    Fast Radio Burst

    AGN

    X-ray transient, UV transient

    Proposed Science Cases@previous workshops

    cadence?survey area?survey region?depth?

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �7

    no filter: effectively g+r bands

    1 visit

    6 (3) sec exposure: [0.5 sec exposure] x 12 (6)

    ~18-19 mag

    2x3 or 2x2 dithering

    ~60 deg2 (partially vignetted by ~30%)

    cadence: ~2 hours

    survey area / 2 hrs: ~7,000 (10,000) deg2, EL>40 (30) deg

    2-4 (3-5) times visits per night

    ~19 mag for daily stacked data

    weather factor: usable (half), photometric (30%)

    reference: PS1?

    10,000 deg2 - 2 hr cadence - 18 mag depth

    10,000 deg2 - 1 day cadence - 19 mag depth

    Northern Sky Transient Survey w/ Tomo-e Gozen

    (): last year

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �8

    Tomo-e SN Survey KISSinstrument Tomo-e Gozen KWFC

    sensor CMOS CCDreadout time ~0 sec 120 sec

    period 2018 fall - 2012/4-2015/9 (3.5 yrs)survey area [deg2] 7,000 50-100

    cadence 2 hours / 1 day 1 hourexposure time / visit 6 sec 180 sec

    depth 18 mag / 19 mag 20-21 magfilter no (~g+r) g

    #(SBOs), #(SNe) / yr 5, 1000 O(0.1)-O(1), 100

    data storage daily-stacked image 
SN cutout images

    all data saved

    reference - TM, Tominaga, Tanaka+2014

    Tomo-e Gozen SN Survey 
 vs Kiso Supernova Survey (KISS) w/ KWFC

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �9

    Tomo-e Gozen SN Survey vs other SN surveys

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Requirements for Survey DesignMultiple visits per night: hopefully N(visit)>=3

    Small motion: not go far away for the next pointing

    To avoid extra time for telescope pointing (14 sec for 9 deg)

    Especially for azimuthal direction (dome rotation)

    Not too short time intervals from previous visits: ∂t > 1.5 hours

    Not avoid Galactic Plane

    Avoid less useful(?) regions?: ~10 < |b| < ~20

    Limit the number of visits?

    special regions even below Dec. limit?

    Higher elevation preferred

    �10

    b=10b=20

    https://faun.rc.fas.harvard.edu/eschlafly/2dmap/Schafly+2014

    Extinction map

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �11

    ELmin delta t min Dec_min Dec_max20180707a 40 90 -5 80

    20180707b 40 180 -5 80

    20180707c 45 90 -5 80

    20180707d 50 90 -5 80

    20180707e 35 90 -5 80

    20180707f 30 90 -5 80

    Survey Simulation

    2x2 dithering: some gaps on the sky

    too much overlaps in 2x3 dithering

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �12

    2x3 dithering8.8 deg (diameter)

    no gap

    but large overlap

    2x2 dithering

    small gap

    small overlap

    (to be quantified)

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Survey Simulation 1

    �13

    ELmin delta t min Dec_min Dec_max20180707a 40 90 -5 80

    20180707b 40 180 -5 80

    20180707c 45 90 -5 80

    20180707d 50 90 -5 80

    20180707e 35 90 -5 80

    20180707f 30 90 -5 80

    581 visits (~35,000 deg2)

    for 10 hours

    # of visits

    time interval [hrs]

    separation [deg]

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Survey Simulation 3

    �14

    ELmin delta t min Dec_min Dec_max20180707a 40 90 -5 80

    20180707b 40 180 -5 80

    20180707c 45 90 -5 80

    20180707d 50 90 -5 80

    20180707e 35 90 -5 80

    20180707f 30 90 -5 80

    581 visits (~35,000 deg2)

    for 10 hours

    separation [deg]

    time interval [hrs]

    # of visits

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Survey Simulation 5

    �15

    ELmin delta t min Dec_min Dec_max20180707a 40 90 -5 80

    20180707b 40 180 -5 80

    20180707c 45 90 -5 80

    20180707d 50 90 -5 80

    20180707e 35 90 -5 80

    20180707f 30 90 -5 80

    X: increase small-#-visit fields

    581 visits (~35,000 deg2)

    for 10 hours

    separation [deg]

    time interval [hrs]

    # of visits

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11 �16

    ELmin delta t min Dec_min Dec_max20180707a 40 90 -5 80

    20180707b 40 180 -5 80

    20180707c 45 90 -5 80

    20180707d 50 90 -5 80

    20180707e 35 90 -5 80

    20180707f 30 90 -5 80

    Survey Simulation Comparison581 visits (~35,000 deg2)

    for 10 hours

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Follow-up Scheme

    �17

    After discovering SN candidates…

    spectroscopic identification

    multi-band light curves

    KISS: KISS international collaboration + OISTER

    # of spectroscopic observations (29 spec-ID+) limited: too faint

    TM+2014, Tanaka+2014, TM+2017, Gabanyi+2018, Kokubo+ in prep.

    Tomo-e survey: bright enough for OISTER domestic telescopes

    SN: discovery ==> follow-up within the same night

    Tomo-e SN Survey

    KISS (w/ KWFC)

    ©Sako

    Kyoto/Seimei 3.8m

    KOOLS-IFU

    optical spectroscopy

    optical imaging

  • Northern Sky Transient Survey 木曽シュミットシンポジウム2018 2018/07/10-11

    Northern Sky Transient Survey is being planned and started soon (from this fall).

    2x2 dithering, 7,000 deg / 2 hours, 18 mag depth

    2-4 visits / night

    Do these survey parameter match your sciences?

    If yes, suggest any (minor) changes or special options to realize your science cases.

    (domestic) Quick follow-up observations

    Test observations were done based on previous (worse) simulation.

    Image subtraction, data management (DB etc.), quick (and low false-positive) discovery machine development works are being done.

    plan to consider weather conditions (avoid cloudy region and choose clear sky region)

    need to name the survey (after Tomo-e?)

    �18

    Summary