Phase-resolved analysis of LS 5039 with Fermi LAT Gene Leung HKU - - PowerPoint PPT Presentation

phase resolved analysis of ls 5039 with fermi lat
SMART_READER_LITE
LIVE PREVIEW

Phase-resolved analysis of LS 5039 with Fermi LAT Gene Leung HKU - - PowerPoint PPT Presentation

Phase-resolved analysis of LS 5039 with Fermi LAT Gene Leung HKU FAN4 Workshop Co-workers:Jumpei Takata, KS Cheng LS 5039 High-mass X-ray binary One of the few HMXBs detected at both GeV and TeV energies Consists of an O6.5V star


slide-1
SLIDE 1

Phase-resolved analysis of LS 5039 with Fermi LAT

Gene Leung HKU FAN4 Workshop

Co-workers:Jumpei Takata, KS Cheng

slide-2
SLIDE 2

LS 5039

  • High-mass X-ray binary
  • One of the few HMXBs detected at both GeV and TeV

energies

  • Consists of an O6.5V star (~28 MSun) and a compact object

(>~1.8MSun)

  • Nature of compact object undetermined
  • Black hole? Neutron star?
slide-3
SLIDE 3

Orbital configuration

Casares et al. Aragona et al. Sarty et al. (2005) (2009) (2011)

Superior conjunction ~0.05 ~0.65 Inferior conjunction

e ~ 0.24-0.35 w ~ 225°-237° f(SUPC) ~ 0.05 f(INFC) ~ 0.65-0.72

Aragona et al. (2009)

slide-4
SLIDE 4

Past Fermi studies

  • Abdo et al. (2009), Hadasch et al. (2012)
  • Spectral analysis in two broad phase intervals
  • Best fitted with power-law with exponential cutoff
  • Hadasch et al. (2012) found high energy (>10 GeV) emission

feature

slide-5
SLIDE 5

Comparison with previous studies

  • Background sources: 1FGL vs 2FGL
  • Data, IRFs, diffuse BG: Pass 6 vs Pass 7
  • Length of observation: 2.5 years vs 4 years
  • Finer binning of orbital phase
slide-6
SLIDE 6

Data set

  • Time span: 2008 Aug 14 to 2012 May 19
  • Energy: 0.1-300 GeV
  • ROI: 20°x20° region centered at LS 5039
  • Event class: Pass 7 source
  • Pass 7 source v6 instrumental response functions
  • Excluded events with zenith angle < 100 degrees to avoid

Earth's albedo

  • Excluded events from pulse phase (0.05,0.2) and (0.6,0.75) of

nearby pulsar PSR J1826-1256

slide-7
SLIDE 7

Phase-averaged spectrum

G = -2.07 +/- 0.07 EC = 2.76 +/- 0.46 GeV

slide-8
SLIDE 8

Light curves

0.1-300 GeV S U P C I N F C A p a s t r

  • n

P e r i a s t r

  • n

S U P C I N F C A p a s t r

  • n
slide-9
SLIDE 9

Light curves

1-100 GeV 0.1-1 GeV S U P C I N F C A p a s t r

  • n

P e r i a s t r

  • n

S U P C I N F C A p a s t r

  • n

Modulation more prominent in low energies

slide-10
SLIDE 10

Hardness ratio

S U P C I N F C A p a s t r

  • n

P e r i a s t r

  • n

S U P C I N F C A p a s t r

  • n
slide-11
SLIDE 11

Phase-resolved spectral analysis

  • Define 3 equally spaced phase intervals:

– [0.83,1.17] (periastron and INFC) – [0.17,0.5] – [0.5,0.83] (SUPC)

  • Perform likelihood fits in each phase intervals, fixing spectral

parameters of sources more than 5 degrees from the target

slide-12
SLIDE 12

Division of orbital phase

S U P C I N F C A p a s t r

  • n

P e r i a s t r

  • n

S U P C I N F C A p a s t r

  • n
slide-13
SLIDE 13

G = 2.18 +/- 0.07 EC = 2.06 +/- 0.42 GeV G = 1.71 +/- 0.14 EC = 2.12 +/- 0.56 GeV G = 2.09 +/- 0.13 EC = 3.87 +/- 1.50 GeV

  • Reduced flux in ~0.1-0.3GeV

compared with previous studies (improved IRFs, diffuse background, etc)

  • Enhancement in ~0.1-1GeV for

0.83<f<1.17, i.e. SUPC and periastron

  • High energy component most

significant in 0.17<f<0.5

SUPC INFC

slide-14
SLIDE 14

Theoretical model (Takata et al. 2013)

  • Pulsar scenario
  • Magnetospheric emissions
  • IC of stellar photons and cold-relativistic pulsar wind
  • Termination shocks at two emission regions
slide-15
SLIDE 15

Theoretical model fitting

0.5<f<0.83

  • Modulation of IC

emissions from cold- relativistic pulsar wind in ~0.1-1 GeV

  • IC of shocked pulsar

wind at ~>10 GeV

SUPC INFC

slide-16
SLIDE 16

Theoretical model fitting

S U P C I N F C A p a s t r

  • n
slide-17
SLIDE 17

Summary

  • Spectral analysis for 3 phase intervals
  • Orbital modulation in 0.1-1 GeV due to cold pulsar wind
  • High energy emissions of shocked pulsar wind
  • Orbital modulation of spectral hardness