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ly observables contain
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- Ly observables contain unique information stars & emitting gas about the high-z


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SLIDE 1

現実的なシミュレーション ライマン-αスペクトル

マックス・グロンケ カリフォルニア⼤夨学サンタバーバラ校

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SLIDE 2

Lyα observables contain unique information

stars & emitting gas neutral hydrogen …about the high-z Universe. …to understand the behaviour

  • f cold, neutral gas.

…to constrain galactic subgrid models!

Lots of Lyα data…

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SLIDE 3

Lyα spectra from hydrodynamical simulations

Hydro-sim: Walch, Girichidis, Naab, Gatto, Glover et al. - https://hera.ph1.uni-koeln.de/~silcc/

The SILCC simulations

  • 4pc fixed resolution
  • radiative heating & cooling
  • chemistry (CO & H2)
  • ionizing RT
  • several “subgrid” feedback

mechanisms (SN, winds, …)

The plan: correlate spectral properties with subgrid parameters!

slide-4
SLIDE 4

Lyα spectra from hydrodynamical simulations

Hydro-sim: Walch, Girichidis, Naab, Gatto, Glover et al. - https://hera.ph1.uni-koeln.de/~silcc/

The SILCC simulations

  • 4pc fixed resolution
  • radiative heating & cooling
  • chemistry (CO & H2)
  • ionizing RT
  • several “subgrid” feedback

mechanisms (SN, winds, …)

The plan: correlate spectral properties with subgrid parameters!

slide-5
SLIDE 5

Lyα spectra from hydrodynamical simulations

Hydro-sim: Walch, Girichidis, Naab, Gatto, Glover et al. - https://hera.ph1.uni-koeln.de/~silcc/

The plan: correlate spectral properties with subgrid parameters!

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SLIDE 6

Lyα spectra from hydrodynamical simulations

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SLIDE 7

Lyα spectra from hydrodynamical simulations

“Green Peas” (Henry et al. 2015; Yang et al. 2016, …); z~0 Erb et al. (2014); z~2-3

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SLIDE 8

Lyα spectra from hydrodynamical simulations

“Green Peas” (Henry et al. 2015; Yang et al. 2016, …); z~0 Erb et al. (2014); z~2-3

Do not match observations! Lyα photons escape through cleared channels!

(similar problems with toy models of multiphase media)

MG & Dijkstra (2016)

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SLIDE 9

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

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SLIDE 10

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM

Laursen et al. (2011)

slide-11
SLIDE 11

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM ➞ not at low-z (and problematic at high-z due to fesc≳0.5)

Laursen et al. (2011)

Hayes et al. (2010); Trainor et al. (2015); Sobral et al. (2017)

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SLIDE 12

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM

➞ not at low-z (and problematic at high-z due to fesc≳0.5)

Hayes et al. (2010); Trainor et al. (2015); Sobral et al. (2017)

slide-13
SLIDE 13

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010); Trainor et al. (2015); Sobral et al. (2017)

slide-14
SLIDE 14

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010)

unrealistic! The impact of the CGM on Lyα spectra

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SLIDE 15

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010)

unrealistic! The impact of the CGM on Lyα spectra

for |z| > 1 kpc coarsen the resolution

slide-16
SLIDE 16

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010)

unrealistic! The impact of the CGM on Lyα spectra “realistic”? r e s

  • l

u t i

  • n

for |z| > 1 kpc coarsen the resolution

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SLIDE 17

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM
  • 3. a new shape of cold gas

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010); Trainor et al. (2015); Sobral et al. (2017)

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SLIDE 18

Escape of Lyα photons through a multiphase medium

tmp

esc ∼ fcB

c th

esc ∼Bxesc(NHI)

c

MG, Dijkstra, McCourt, Oh (2016, 2017)

  • 40
  • 30
  • 20
  • 10

10 20 30 40

∆V/Vdop

0.001 0.01 0.1 1

Distribution

Neufeld (1990)

∼ x/xesc

Hansen & Oh (2006)

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SLIDE 19

Escape of Lyα photons through a multiphase medium

tmp

esc ∼ fcB

c th

esc ∼Bxesc(NHI)

c

MG, Dijkstra, McCourt, Oh (2016, 2017)

  • 40
  • 30
  • 20
  • 10

10 20 30 40

∆V/Vdop

0.001 0.01 0.1 1

Distribution

Neufeld (1990)

∼ x/xesc

NHI = 4/3 × 1019 cm−2

Hansen & Oh (2006)

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SLIDE 20

Escape of Lyα photons through a multiphase medium

tmp

esc ∼ fcB

c th

esc ∼Bxesc(NHI)

c

MG, Dijkstra, McCourt, Oh (2016, 2017)

  • 40
  • 30
  • 20
  • 10

10 20 30 40

∆V/Vdop

0.001 0.01 0.1 1

Distribution

Neufeld (1990)

∼ x/xesc

NHI = 4/3 × 1019 cm−2

Hansen & Oh (2006)

slide-21
SLIDE 21

Escape of Lyα photons through a multiphase medium

tmp

esc ∼ fcB

c th

esc ∼Bxesc(NHI)

c

MG, Dijkstra, McCourt, Oh (2016, 2017)

  • 40
  • 30
  • 20
  • 10

10 20 30 40

∆V/Vdop

0.001 0.01 0.1 1

Distribution

Neufeld (1990)

∼ x/xesc

NHI = 4/3 × 1019 cm−2

Hansen & Oh (2006)

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SLIDE 22

Escape of Lyα photons through a multiphase medium

tmp

esc ∼ fcB

c th

esc ∼Bxesc(NHI)

c

MG, Dijkstra, McCourt, Oh (2016, 2017)

  • 40
  • 30
  • 20
  • 10

10 20 30 40

∆V/Vdop

0.001 0.01 0.1 1

Distribution

Neufeld (1990)

∼ x/xesc

NHI = 4/3 × 1019 cm−2

Hansen & Oh (2006)

fc, crit ∼ xesc

Transition at

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SLIDE 23

Ubiquitous droplets lead to realistic Lyα spectra

MG, Dijkstra, McCourt, Oh (2016, 2017)

NHI = 4/3 × 1019 cm−2

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SLIDE 24

Ubiquitous droplets lead to realistic Lyα spectra

(asymmetry of spectra)

MG, Dijkstra, McCourt, Oh (2016, 2017)

NHI = 4/3 × 1019 cm−2

more stratification leads to:

✓less flux at v~0 ✓more asymmetry

…in agreement with

  • bservations.
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SLIDE 25

Ubiquitous droplets lead to realistic Lyα spectra

(asymmetry of spectra)

MG, Dijkstra, McCourt, Oh (2016, 2017)

increasing resolution?

NHI = 4/3 × 1019 cm−2

more stratification leads to:

✓less flux at v~0 ✓more asymmetry

…in agreement with

  • bservations.
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SLIDE 26

Other evidence for tiny “droplets”

Prochaska et al. (2017) Arav et al. (1997)

Dv ~ 6km/s

+ many more…

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SLIDE 27

Other evidence for tiny “droplets”

  • smooth absorption &

emission profiles over v

≳1000 km/s in BLR & CGM

  • dense cold gas out to in

galactic halos (large areal but

low volume filling fraction; ➞ e.g., Ting-

Wen Lan’s talk)

Prochaska et al. (2017) Arav et al. (1997)

Dv ~ 6km/s

+ many more…

slide-28
SLIDE 28

Other evidence for tiny “droplets”

  • smooth absorption &

emission profiles over v

≳1000 km/s in BLR & CGM

  • dense cold gas out to in

galactic halos (large areal but

low volume filling fraction; ➞ e.g., Ting-

Wen Lan’s talk)

  • “shattering” instability

(theory predicting droplets of size ~0.1 ncgs-1pc)

Prochaska et al. (2017) Arav et al. (1997)

Dv ~ 6km/s

McCourt et al. (2018)

+ many more…

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SLIDE 29

The “Lyα puzzle”

Problem: Simulated Lyα spectra “look different”

  • too much flux at line center
  • too symmetric

➞ diminishing constraining power of Lyα.

vs

Solutions?

  • 1. IGM
  • 2. CGM
  • 3. a new shape of cold gas
  • 4. another form of feedback

➞ not at low-z (and problematic at high-z due to fesc≳0.5) ➞ does not affect Lyα spectrum by much (?)

Wisotzki et al. (2016); Kakiichi & Dijkstra (2017) Hayes et al. (2010); Trainor et al. (2015); Sobral et al. (2017)

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SLIDE 30

Girichidis et al. (2018)

“old” “new”

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SLIDE 31

Girichidis et al. (2018)

“old” “new”

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SLIDE 32

Girichidis et al. (2018) no CRs with CRs

no CRs with CRs

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SLIDE 33

Impact of cosmic-ray feedback

  • n Lyα spectra
  • non-thermal feedback moves

gas without heating it

  • doesn’t clear channels Lyα

can escape through

MG, Girichidis, Naab, Walch (in prep.)

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SLIDE 34

Impact of cosmic-ray feedback

  • n Lyα spectra
  • non-thermal feedback moves

gas without heating it

  • doesn’t clear channels Lyα

can escape through

MG, Girichidis, Naab, Walch (in prep.)

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SLIDE 35

Simulating realistic Lyman-α spectra

  • Lyα spectra can be used to probe
  • ur understanding of (cold) gas

behaviour

  • Modelling realistic spectra is

crucial but problematic in high- resolution, multiphase systems

  • Two proposes mechanisms to

successfully model realistic Lyα spectra:

  • 1. ubiquitous droplets
  • 2. cosmic ray feedback

…not exclusive!

spectra SB polarization

see: Eide, MG, Dijkstra, Hayes (2018)

Model small-scale gas dynamics Compare to the the “Lyα triangle of truth”

➔The future is (Lyα) bright! Work in progress…

(spatially resolved)