Precision Weak Lensing Pol Gurri A.Prof. Ned Taylor Prof. Chris - - PowerPoint PPT Presentation

precision weak lensing
SMART_READER_LITE
LIVE PREVIEW

Precision Weak Lensing Pol Gurri A.Prof. Ned Taylor Prof. Chris - - PowerPoint PPT Presentation

Precision Weak Lensing Pol Gurri A.Prof. Ned Taylor Prof. Chris Fluke Swinburne University of Technology Galaxies live inside dark matter halos But How? Stellar to Halo Mass Relation Abundance Matching Weak Lensing Source


slide-1
SLIDE 1

Precision Weak Lensing

Pol Gurri A.Prof. Ned Taylor


  • Prof. Chris Fluke

Swinburne University of Technology

slide-2
SLIDE 2

Galaxies live inside dark matter halos

But How?

slide-3
SLIDE 3

Stellar to Halo Mass Relation

slide-4
SLIDE 4

Abundance Matching

slide-5
SLIDE 5

Weak Lensing

Lens
 (foreground) Source
 (background)

slide-6
SLIDE 6

Weak Lensing

Lens
 (foreground) Source
 (background)

γ shear

slide-7
SLIDE 7

Weak Lensing

Lens
 (foreground) Source
 (background)

slide-8
SLIDE 8

Overcoming shape noise

Lens
 (foreground) Source
 (background)

slide-9
SLIDE 9

Stellar to Halo Mass Relation

slide-10
SLIDE 10

My Research

Develop and exploit a new high-precision weak lensing technique

slide-11
SLIDE 11
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-12
SLIDE 12
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-13
SLIDE 13

Precision Weak Lensing

slide-14
SLIDE 14

Precision Weak Lensing

Circular shape Circular motion

slide-15
SLIDE 15

Precision Weak Lensing

α

Circular shape Circular motion

slide-16
SLIDE 16

Precision Weak Lensing

Unlensed Lensed

β

α

  • n
slide-17
SLIDE 17

γobs = γtrue + σ sin(2ϕ)

Dynamical Shape noise

slide-18
SLIDE 18

γobs = γtrue + σ sin(2ϕ) γobs < 0 γobs < 0 γobs > 0 γobs > 0

slide-19
SLIDE 19

Data

Target Selection Observations Analysis

z < 0.15 & i < 17.5

γpred > 0.001

+30 nights KOALA (3.9m) + WIFES (2.3m) 100 galaxies Custom Data Reduction Vel with shear modelling 21 useful targets 3000 systems

slide-20
SLIDE 20

Precision Weak Lensing

Gurri et. al. 2020a

slide-21
SLIDE 21

Precision Weak Lensing

⟨γ⟩ = 0.021 ± 0.005

Gurri et. al. 2020a

slide-22
SLIDE 22
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-23
SLIDE 23
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-24
SLIDE 24

The Shape of Shear

Dynamical shape noise Dispersion in SHMR

γobs

σ

γobs

ξ

σ ξ

γobs ≠ γpred

slide-25
SLIDE 25

The Shape of Shear

Dynamical shape noise + dispersion in SHMR

γobs ≠ γpred

γobs

γpred

slide-26
SLIDE 26

γobs

σ σ

ξlow

low high

ξhigh

γobs γobs γobs

slide-27
SLIDE 27

The Shape of Shear

Gurri et. al. 2020b

slide-28
SLIDE 28
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-29
SLIDE 29
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-30
SLIDE 30

Dispersion in the SHMR

slide-31
SLIDE 31

Dispersion in the SHMR

ξ = 0.4 dex

slide-32
SLIDE 32

Dispersion in the SHMR

γobs

γpred

slide-33
SLIDE 33
  • 1. Can we detect lensing though velocity fjelds?
  • 2. Can we separate noise from lensing?
  • 3. Can we constrain the SHMR’s dispersion & shape?

My Research

slide-34
SLIDE 34

Contribution to Research Area

  • 1. A new methodology to do weak lensing
  • 2. Published the fjrst dataset of weakly lensed vel. fjelds
  • 3. Opened a way to measure the dispersion in the SHMR